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env-llmeval/lib/python3.10/site-packages/sympy/functions/special/benchmarks/bench_special.py

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+from sympy.core.symbol import symbols
+from sympy.functions.special.spherical_harmonics import Ynm
+
+x, y = symbols('x,y')
+
+
+def timeit_Ynm_xy():
+    Ynm(1, 1, x, y)

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/bessel.py

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+from functools import wraps
+
+from sympy.core import S
+from sympy.core.add import Add
+from sympy.core.cache import cacheit
+from sympy.core.expr import Expr
+from sympy.core.function import Function, ArgumentIndexError, _mexpand
+from sympy.core.logic import fuzzy_or, fuzzy_not
+from sympy.core.numbers import Rational, pi, I
+from sympy.core.power import Pow
+from sympy.core.symbol import Dummy, Wild
+from sympy.core.sympify import sympify
+from sympy.functions.combinatorial.factorials import factorial
+from sympy.functions.elementary.trigonometric import sin, cos, csc, cot
+from sympy.functions.elementary.integers import ceiling
+from sympy.functions.elementary.exponential import exp, log
+from sympy.functions.elementary.miscellaneous import cbrt, sqrt, root
+from sympy.functions.elementary.complexes import (Abs, re, im, polar_lift, unpolarify)
+from sympy.functions.special.gamma_functions import gamma, digamma, uppergamma
+from sympy.functions.special.hyper import hyper
+from sympy.polys.orthopolys import spherical_bessel_fn
+
+from mpmath import mp, workprec
+
+# TODO
+# o Scorer functions G1 and G2
+# o Asymptotic expansions
+#   These are possible, e.g. for fixed order, but since the bessel type
+#   functions are oscillatory they are not actually tractable at
+#   infinity, so this is not particularly useful right now.
+# o Nicer series expansions.
+# o More rewriting.
+# o Add solvers to ode.py (or rather add solvers for the hypergeometric equation).
+
+
+class BesselBase(Function):
+    """
+    Abstract base class for Bessel-type functions.
+
+    This class is meant to reduce code duplication.
+    All Bessel-type functions can 1) be differentiated, with the derivatives
+    expressed in terms of similar functions, and 2) be rewritten in terms
+    of other Bessel-type functions.
+
+    Here, Bessel-type functions are assumed to have one complex parameter.
+
+    To use this base class, define class attributes ``_a`` and ``_b`` such that
+    ``2*F_n' = -_a*F_{n+1} + b*F_{n-1}``.
+
+    """
+
+    @property
+    def order(self):
+        """ The order of the Bessel-type function. """
+        return self.args[0]
+
+    @property
+    def argument(self):
+        """ The argument of the Bessel-type function. """
+        return self.args[1]
+
+    @classmethod
+    def eval(cls, nu, z):
+        return
+
+    def fdiff(self, argindex=2):
+        if argindex != 2:
+            raise ArgumentIndexError(self, argindex)
+        return (self._b/2 * self.__class__(self.order - 1, self.argument) -
+                self._a/2 * self.__class__(self.order + 1, self.argument))
+
+    def _eval_conjugate(self):
+        z = self.argument
+        if z.is_extended_negative is False:
+            return self.__class__(self.order.conjugate(), z.conjugate())
+
+    def _eval_is_meromorphic(self, x, a):
+        nu, z = self.order, self.argument
+
+        if nu.has(x):
+            return False
+        if not z._eval_is_meromorphic(x, a):
+            return None
+        z0 = z.subs(x, a)
+        if nu.is_integer:
+            if isinstance(self, (besselj, besseli, hn1, hn2, jn, yn)) or not nu.is_zero:
+                return fuzzy_not(z0.is_infinite)
+        return fuzzy_not(fuzzy_or([z0.is_zero, z0.is_infinite]))
+
+    def _eval_expand_func(self, **hints):
+        nu, z, f = self.order, self.argument, self.__class__
+        if nu.is_real:
+            if (nu - 1).is_positive:
+                return (-self._a*self._b*f(nu - 2, z)._eval_expand_func() +
+                        2*self._a*(nu - 1)*f(nu - 1, z)._eval_expand_func()/z)
+            elif (nu + 1).is_negative:
+                return (2*self._b*(nu + 1)*f(nu + 1, z)._eval_expand_func()/z -
+                        self._a*self._b*f(nu + 2, z)._eval_expand_func())
+        return self
+
+    def _eval_simplify(self, **kwargs):
+        from sympy.simplify.simplify import besselsimp
+        return besselsimp(self)
+
+
+class besselj(BesselBase):
+    r"""
+    Bessel function of the first kind.
+
+    Explanation
+    ===========
+
+    The Bessel $J$ function of order $\nu$ is defined to be the function
+    satisfying Bessel's differential equation
+
+    .. math ::
+        z^2 \frac{\mathrm{d}^2 w}{\mathrm{d}z^2}
+        + z \frac{\mathrm{d}w}{\mathrm{d}z} + (z^2 - \nu^2) w = 0,
+
+    with Laurent expansion
+
+    .. math ::
+        J_\nu(z) = z^\nu \left(\frac{1}{\Gamma(\nu + 1) 2^\nu} + O(z^2) \right),
+
+    if $\nu$ is not a negative integer. If $\nu=-n \in \mathbb{Z}_{<0}$
+    *is* a negative integer, then the definition is
+
+    .. math ::
+        J_{-n}(z) = (-1)^n J_n(z).
+
+    Examples
+    ========
+
+    Create a Bessel function object:
+
+    >>> from sympy import besselj, jn
+    >>> from sympy.abc import z, n
+    >>> b = besselj(n, z)
+
+    Differentiate it:
+
+    >>> b.diff(z)
+    besselj(n - 1, z)/2 - besselj(n + 1, z)/2
+
+    Rewrite in terms of spherical Bessel functions:
+
+    >>> b.rewrite(jn)
+    sqrt(2)*sqrt(z)*jn(n - 1/2, z)/sqrt(pi)
+
+    Access the parameter and argument:
+
+    >>> b.order
+    n
+    >>> b.argument
+    z
+
+    See Also
+    ========
+
+    bessely, besseli, besselk
+
+    References
+    ==========
+
+    .. [1] Abramowitz, Milton; Stegun, Irene A., eds. (1965), "Chapter 9",
+           Handbook of Mathematical Functions with Formulas, Graphs, and
+           Mathematical Tables
+    .. [2] Luke, Y. L. (1969), The Special Functions and Their
+           Approximations, Volume 1
+    .. [3] https://en.wikipedia.org/wiki/Bessel_function
+    .. [4] https://functions.wolfram.com/Bessel-TypeFunctions/BesselJ/
+
+    """
+
+    _a = S.One
+    _b = S.One
+
+    @classmethod
+    def eval(cls, nu, z):
+        if z.is_zero:
+            if nu.is_zero:
+                return S.One
+            elif (nu.is_integer and nu.is_zero is False) or re(nu).is_positive:
+                return S.Zero
+            elif re(nu).is_negative and not (nu.is_integer is True):
+                return S.ComplexInfinity
+            elif nu.is_imaginary:
+                return S.NaN
+        if z in (S.Infinity, S.NegativeInfinity):
+            return S.Zero
+
+        if z.could_extract_minus_sign():
+            return (z)**nu*(-z)**(-nu)*besselj(nu, -z)
+        if nu.is_integer:
+            if nu.could_extract_minus_sign():
+                return S.NegativeOne**(-nu)*besselj(-nu, z)
+            newz = z.extract_multiplicatively(I)
+            if newz:  # NOTE we don't want to change the function if z==0
+                return I**(nu)*besseli(nu, newz)
+
+        # branch handling:
+        if nu.is_integer:
+            newz = unpolarify(z)
+            if newz != z:
+                return besselj(nu, newz)
+        else:
+            newz, n = z.extract_branch_factor()
+            if n != 0:
+                return exp(2*n*pi*nu*I)*besselj(nu, newz)
+        nnu = unpolarify(nu)
+        if nu != nnu:
+            return besselj(nnu, z)
+
+    def _eval_rewrite_as_besseli(self, nu, z, **kwargs):
+        return exp(I*pi*nu/2)*besseli(nu, polar_lift(-I)*z)
+
+    def _eval_rewrite_as_bessely(self, nu, z, **kwargs):
+        if nu.is_integer is False:
+            return csc(pi*nu)*bessely(-nu, z) - cot(pi*nu)*bessely(nu, z)
+
+    def _eval_rewrite_as_jn(self, nu, z, **kwargs):
+        return sqrt(2*z/pi)*jn(nu - S.Half, self.argument)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        nu, z = self.args
+        try:
+            arg = z.as_leading_term(x)
+        except NotImplementedError:
+            return self
+        c, e = arg.as_coeff_exponent(x)
+
+        if e.is_positive:
+            return arg**nu/(2**nu*gamma(nu + 1))
+        elif e.is_negative:
+            cdir = 1 if cdir == 0 else cdir
+            sign = c*cdir**e
+            if not sign.is_negative:
+                # Refer Abramowitz and Stegun 1965, p. 364 for more information on
+                # asymptotic approximation of besselj function.
+                return sqrt(2)*cos(z - pi*(2*nu + 1)/4)/sqrt(pi*z)
+            return self
+
+        return super(besselj, self)._eval_as_leading_term(x, logx, cdir)
+
+    def _eval_is_extended_real(self):
+        nu, z = self.args
+        if nu.is_integer and z.is_extended_real:
+            return True
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        # Refer https://functions.wolfram.com/Bessel-TypeFunctions/BesselJ/06/01/04/01/01/0003/
+        # for more information on nseries expansion of besselj function.
+        from sympy.series.order import Order
+        nu, z = self.args
+
+        # In case of powers less than 1, number of terms need to be computed
+        # separately to avoid repeated callings of _eval_nseries with wrong n
+        try:
+            _, exp = z.leadterm(x)
+        except (ValueError, NotImplementedError):
+            return self
+
+        if exp.is_positive:
+            newn = ceiling(n/exp)
+            o = Order(x**n, x)
+            r = (z/2)._eval_nseries(x, n, logx, cdir).removeO()
+            if r is S.Zero:
+                return o
+            t = (_mexpand(r**2) + o).removeO()
+
+            term = r**nu/gamma(nu + 1)
+            s = [term]
+            for k in range(1, (newn + 1)//2):
+                term *= -t/(k*(nu + k))
+                term = (_mexpand(term) + o).removeO()
+                s.append(term)
+            return Add(*s) + o
+
+        return super(besselj, self)._eval_nseries(x, n, logx, cdir)
+
+
+class bessely(BesselBase):
+    r"""
+    Bessel function of the second kind.
+
+    Explanation
+    ===========
+
+    The Bessel $Y$ function of order $\nu$ is defined as
+
+    .. math ::
+        Y_\nu(z) = \lim_{\mu \to \nu} \frac{J_\mu(z) \cos(\pi \mu)
+                                            - J_{-\mu}(z)}{\sin(\pi \mu)},
+
+    where $J_\mu(z)$ is the Bessel function of the first kind.
+
+    It is a solution to Bessel's equation, and linearly independent from
+    $J_\nu$.
+
+    Examples
+    ========
+
+    >>> from sympy import bessely, yn
+    >>> from sympy.abc import z, n
+    >>> b = bessely(n, z)
+    >>> b.diff(z)
+    bessely(n - 1, z)/2 - bessely(n + 1, z)/2
+    >>> b.rewrite(yn)
+    sqrt(2)*sqrt(z)*yn(n - 1/2, z)/sqrt(pi)
+
+    See Also
+    ========
+
+    besselj, besseli, besselk
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/Bessel-TypeFunctions/BesselY/
+
+    """
+
+    _a = S.One
+    _b = S.One
+
+    @classmethod
+    def eval(cls, nu, z):
+        if z.is_zero:
+            if nu.is_zero:
+                return S.NegativeInfinity
+            elif re(nu).is_zero is False:
+                return S.ComplexInfinity
+            elif re(nu).is_zero:
+                return S.NaN
+        if z in (S.Infinity, S.NegativeInfinity):
+            return S.Zero
+        if z == I*S.Infinity:
+            return exp(I*pi*(nu + 1)/2) * S.Infinity
+        if z == I*S.NegativeInfinity:
+            return exp(-I*pi*(nu + 1)/2) * S.Infinity
+
+        if nu.is_integer:
+            if nu.could_extract_minus_sign():
+                return S.NegativeOne**(-nu)*bessely(-nu, z)
+
+    def _eval_rewrite_as_besselj(self, nu, z, **kwargs):
+        if nu.is_integer is False:
+            return csc(pi*nu)*(cos(pi*nu)*besselj(nu, z) - besselj(-nu, z))
+
+    def _eval_rewrite_as_besseli(self, nu, z, **kwargs):
+        aj = self._eval_rewrite_as_besselj(*self.args)
+        if aj:
+            return aj.rewrite(besseli)
+
+    def _eval_rewrite_as_yn(self, nu, z, **kwargs):
+        return sqrt(2*z/pi) * yn(nu - S.Half, self.argument)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        nu, z = self.args
+        try:
+            arg = z.as_leading_term(x)
+        except NotImplementedError:
+            return self
+        c, e = arg.as_coeff_exponent(x)
+
+        if e.is_positive:
+            term_one = ((2/pi)*log(z/2)*besselj(nu, z))
+            term_two = -(z/2)**(-nu)*factorial(nu - 1)/pi if (nu).is_positive else S.Zero
+            term_three = -(z/2)**nu/(pi*factorial(nu))*(digamma(nu + 1) - S.EulerGamma)
+            arg = Add(*[term_one, term_two, term_three]).as_leading_term(x, logx=logx)
+            return arg
+        elif e.is_negative:
+            cdir = 1 if cdir == 0 else cdir
+            sign = c*cdir**e
+            if not sign.is_negative:
+                # Refer Abramowitz and Stegun 1965, p. 364 for more information on
+                # asymptotic approximation of bessely function.
+                return sqrt(2)*(-sin(pi*nu/2 - z + pi/4) + 3*cos(pi*nu/2 - z + pi/4)/(8*z))*sqrt(1/z)/sqrt(pi)
+            return self
+
+        return super(bessely, self)._eval_as_leading_term(x, logx, cdir)
+
+    def _eval_is_extended_real(self):
+        nu, z = self.args
+        if nu.is_integer and z.is_positive:
+            return True
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        # Refer https://functions.wolfram.com/Bessel-TypeFunctions/BesselY/06/01/04/01/02/0008/
+        # for more information on nseries expansion of bessely function.
+        from sympy.series.order import Order
+        nu, z = self.args
+
+        # In case of powers less than 1, number of terms need to be computed
+        # separately to avoid repeated callings of _eval_nseries with wrong n
+        try:
+            _, exp = z.leadterm(x)
+        except (ValueError, NotImplementedError):
+            return self
+
+        if exp.is_positive and nu.is_integer:
+            newn = ceiling(n/exp)
+            bn = besselj(nu, z)
+            a = ((2/pi)*log(z/2)*bn)._eval_nseries(x, n, logx, cdir)
+
+            b, c = [], []
+            o = Order(x**n, x)
+            r = (z/2)._eval_nseries(x, n, logx, cdir).removeO()
+            if r is S.Zero:
+                return o
+            t = (_mexpand(r**2) + o).removeO()
+
+            if nu > S.Zero:
+                term = r**(-nu)*factorial(nu - 1)/pi
+                b.append(term)
+                for k in range(1, nu):
+                    denom = (nu - k)*k
+                    if denom == S.Zero:
+                        term *= t/k
+                    else:
+                        term *= t/denom
+                    term = (_mexpand(term) + o).removeO()
+                    b.append(term)
+
+            p = r**nu/(pi*factorial(nu))
+            term = p*(digamma(nu + 1) - S.EulerGamma)
+            c.append(term)
+            for k in range(1, (newn + 1)//2):
+                p *= -t/(k*(k + nu))
+                p = (_mexpand(p) + o).removeO()
+                term = p*(digamma(k + nu + 1) + digamma(k + 1))
+                c.append(term)
+            return a - Add(*b) - Add(*c) # Order term comes from a
+
+        return super(bessely, self)._eval_nseries(x, n, logx, cdir)
+
+
+class besseli(BesselBase):
+    r"""
+    Modified Bessel function of the first kind.
+
+    Explanation
+    ===========
+
+    The Bessel $I$ function is a solution to the modified Bessel equation
+
+    .. math ::
+        z^2 \frac{\mathrm{d}^2 w}{\mathrm{d}z^2}
+        + z \frac{\mathrm{d}w}{\mathrm{d}z} + (z^2 + \nu^2)^2 w = 0.
+
+    It can be defined as
+
+    .. math ::
+        I_\nu(z) = i^{-\nu} J_\nu(iz),
+
+    where $J_\nu(z)$ is the Bessel function of the first kind.
+
+    Examples
+    ========
+
+    >>> from sympy import besseli
+    >>> from sympy.abc import z, n
+    >>> besseli(n, z).diff(z)
+    besseli(n - 1, z)/2 + besseli(n + 1, z)/2
+
+    See Also
+    ========
+
+    besselj, bessely, besselk
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/Bessel-TypeFunctions/BesselI/
+
+    """
+
+    _a = -S.One
+    _b = S.One
+
+    @classmethod
+    def eval(cls, nu, z):
+        if z.is_zero:
+            if nu.is_zero:
+                return S.One
+            elif (nu.is_integer and nu.is_zero is False) or re(nu).is_positive:
+                return S.Zero
+            elif re(nu).is_negative and not (nu.is_integer is True):
+                return S.ComplexInfinity
+            elif nu.is_imaginary:
+                return S.NaN
+        if im(z) in (S.Infinity, S.NegativeInfinity):
+            return S.Zero
+        if z is S.Infinity:
+            return S.Infinity
+        if z is S.NegativeInfinity:
+            return (-1)**nu*S.Infinity
+
+        if z.could_extract_minus_sign():
+            return (z)**nu*(-z)**(-nu)*besseli(nu, -z)
+        if nu.is_integer:
+            if nu.could_extract_minus_sign():
+                return besseli(-nu, z)
+            newz = z.extract_multiplicatively(I)
+            if newz:  # NOTE we don't want to change the function if z==0
+                return I**(-nu)*besselj(nu, -newz)
+
+        # branch handling:
+        if nu.is_integer:
+            newz = unpolarify(z)
+            if newz != z:
+                return besseli(nu, newz)
+        else:
+            newz, n = z.extract_branch_factor()
+            if n != 0:
+                return exp(2*n*pi*nu*I)*besseli(nu, newz)
+        nnu = unpolarify(nu)
+        if nu != nnu:
+            return besseli(nnu, z)
+
+    def _eval_rewrite_as_besselj(self, nu, z, **kwargs):
+        return exp(-I*pi*nu/2)*besselj(nu, polar_lift(I)*z)
+
+    def _eval_rewrite_as_bessely(self, nu, z, **kwargs):
+        aj = self._eval_rewrite_as_besselj(*self.args)
+        if aj:
+            return aj.rewrite(bessely)
+
+    def _eval_rewrite_as_jn(self, nu, z, **kwargs):
+        return self._eval_rewrite_as_besselj(*self.args).rewrite(jn)
+
+    def _eval_is_extended_real(self):
+        nu, z = self.args
+        if nu.is_integer and z.is_extended_real:
+            return True
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        nu, z = self.args
+        try:
+            arg = z.as_leading_term(x)
+        except NotImplementedError:
+            return self
+        c, e = arg.as_coeff_exponent(x)
+
+        if e.is_positive:
+            return arg**nu/(2**nu*gamma(nu + 1))
+        elif e.is_negative:
+            cdir = 1 if cdir == 0 else cdir
+            sign = c*cdir**e
+            if not sign.is_negative:
+                # Refer Abramowitz and Stegun 1965, p. 377 for more information on
+                # asymptotic approximation of besseli function.
+                return exp(z)/sqrt(2*pi*z)
+            return self
+
+        return super(besseli, self)._eval_as_leading_term(x, logx, cdir)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        # Refer https://functions.wolfram.com/Bessel-TypeFunctions/BesselI/06/01/04/01/01/0003/
+        # for more information on nseries expansion of besseli function.
+        from sympy.series.order import Order
+        nu, z = self.args
+
+        # In case of powers less than 1, number of terms need to be computed
+        # separately to avoid repeated callings of _eval_nseries with wrong n
+        try:
+            _, exp = z.leadterm(x)
+        except (ValueError, NotImplementedError):
+            return self
+
+        if exp.is_positive:
+            newn = ceiling(n/exp)
+            o = Order(x**n, x)
+            r = (z/2)._eval_nseries(x, n, logx, cdir).removeO()
+            if r is S.Zero:
+                return o
+            t = (_mexpand(r**2) + o).removeO()
+
+            term = r**nu/gamma(nu + 1)
+            s = [term]
+            for k in range(1, (newn + 1)//2):
+                term *= t/(k*(nu + k))
+                term = (_mexpand(term) + o).removeO()
+                s.append(term)
+            return Add(*s) + o
+
+        return super(besseli, self)._eval_nseries(x, n, logx, cdir)
+
+
+class besselk(BesselBase):
+    r"""
+    Modified Bessel function of the second kind.
+
+    Explanation
+    ===========
+
+    The Bessel $K$ function of order $\nu$ is defined as
+
+    .. math ::
+        K_\nu(z) = \lim_{\mu \to \nu} \frac{\pi}{2}
+                   \frac{I_{-\mu}(z) -I_\mu(z)}{\sin(\pi \mu)},
+
+    where $I_\mu(z)$ is the modified Bessel function of the first kind.
+
+    It is a solution of the modified Bessel equation, and linearly independent
+    from $Y_\nu$.
+
+    Examples
+    ========
+
+    >>> from sympy import besselk
+    >>> from sympy.abc import z, n
+    >>> besselk(n, z).diff(z)
+    -besselk(n - 1, z)/2 - besselk(n + 1, z)/2
+
+    See Also
+    ========
+
+    besselj, besseli, bessely
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/Bessel-TypeFunctions/BesselK/
+
+    """
+
+    _a = S.One
+    _b = -S.One
+
+    @classmethod
+    def eval(cls, nu, z):
+        if z.is_zero:
+            if nu.is_zero:
+                return S.Infinity
+            elif re(nu).is_zero is False:
+                return S.ComplexInfinity
+            elif re(nu).is_zero:
+                return S.NaN
+        if z in (S.Infinity, I*S.Infinity, I*S.NegativeInfinity):
+            return S.Zero
+
+        if nu.is_integer:
+            if nu.could_extract_minus_sign():
+                return besselk(-nu, z)
+
+    def _eval_rewrite_as_besseli(self, nu, z, **kwargs):
+        if nu.is_integer is False:
+            return pi*csc(pi*nu)*(besseli(-nu, z) - besseli(nu, z))/2
+
+    def _eval_rewrite_as_besselj(self, nu, z, **kwargs):
+        ai = self._eval_rewrite_as_besseli(*self.args)
+        if ai:
+            return ai.rewrite(besselj)
+
+    def _eval_rewrite_as_bessely(self, nu, z, **kwargs):
+        aj = self._eval_rewrite_as_besselj(*self.args)
+        if aj:
+            return aj.rewrite(bessely)
+
+    def _eval_rewrite_as_yn(self, nu, z, **kwargs):
+        ay = self._eval_rewrite_as_bessely(*self.args)
+        if ay:
+            return ay.rewrite(yn)
+
+    def _eval_is_extended_real(self):
+        nu, z = self.args
+        if nu.is_integer and z.is_positive:
+            return True
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        nu, z = self.args
+        try:
+            arg = z.as_leading_term(x)
+        except NotImplementedError:
+            return self
+        _, e = arg.as_coeff_exponent(x)
+
+        if e.is_positive:
+            term_one = ((-1)**(nu -1)*log(z/2)*besseli(nu, z))
+            term_two = (z/2)**(-nu)*factorial(nu - 1)/2 if (nu).is_positive else S.Zero
+            term_three = (-1)**nu*(z/2)**nu/(2*factorial(nu))*(digamma(nu + 1) - S.EulerGamma)
+            arg = Add(*[term_one, term_two, term_three]).as_leading_term(x, logx=logx)
+            return arg
+        elif e.is_negative:
+            # Refer Abramowitz and Stegun 1965, p. 378 for more information on
+            # asymptotic approximation of besselk function.
+            return sqrt(pi)*exp(-z)/sqrt(2*z)
+
+        return super(besselk, self)._eval_as_leading_term(x, logx, cdir)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        # Refer https://functions.wolfram.com/Bessel-TypeFunctions/BesselK/06/01/04/01/02/0008/
+        # for more information on nseries expansion of besselk function.
+        from sympy.series.order import Order
+        nu, z = self.args
+
+        # In case of powers less than 1, number of terms need to be computed
+        # separately to avoid repeated callings of _eval_nseries with wrong n
+        try:
+            _, exp = z.leadterm(x)
+        except (ValueError, NotImplementedError):
+            return self
+
+        if exp.is_positive and nu.is_integer:
+            newn = ceiling(n/exp)
+            bn = besseli(nu, z)
+            a = ((-1)**(nu - 1)*log(z/2)*bn)._eval_nseries(x, n, logx, cdir)
+
+            b, c = [], []
+            o = Order(x**n, x)
+            r = (z/2)._eval_nseries(x, n, logx, cdir).removeO()
+            if r is S.Zero:
+                return o
+            t = (_mexpand(r**2) + o).removeO()
+
+            if nu > S.Zero:
+                term = r**(-nu)*factorial(nu - 1)/2
+                b.append(term)
+                for k in range(1, nu):
+                    denom = (k - nu)*k
+                    if denom == S.Zero:
+                        term *= t/k
+                    else:
+                        term *= t/denom
+                    term = (_mexpand(term) + o).removeO()
+                    b.append(term)
+
+            p = r**nu*(-1)**nu/(2*factorial(nu))
+            term = p*(digamma(nu + 1) - S.EulerGamma)
+            c.append(term)
+            for k in range(1, (newn + 1)//2):
+                p *= t/(k*(k + nu))
+                p = (_mexpand(p) + o).removeO()
+                term = p*(digamma(k + nu + 1) + digamma(k + 1))
+                c.append(term)
+            return a + Add(*b) + Add(*c) # Order term comes from a
+
+        return super(besselk, self)._eval_nseries(x, n, logx, cdir)
+
+
+class hankel1(BesselBase):
+    r"""
+    Hankel function of the first kind.
+
+    Explanation
+    ===========
+
+    This function is defined as
+
+    .. math ::
+        H_\nu^{(1)} = J_\nu(z) + iY_\nu(z),
+
+    where $J_\nu(z)$ is the Bessel function of the first kind, and
+    $Y_\nu(z)$ is the Bessel function of the second kind.
+
+    It is a solution to Bessel's equation.
+
+    Examples
+    ========
+
+    >>> from sympy import hankel1
+    >>> from sympy.abc import z, n
+    >>> hankel1(n, z).diff(z)
+    hankel1(n - 1, z)/2 - hankel1(n + 1, z)/2
+
+    See Also
+    ========
+
+    hankel2, besselj, bessely
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/Bessel-TypeFunctions/HankelH1/
+
+    """
+
+    _a = S.One
+    _b = S.One
+
+    def _eval_conjugate(self):
+        z = self.argument
+        if z.is_extended_negative is False:
+            return hankel2(self.order.conjugate(), z.conjugate())
+
+
+class hankel2(BesselBase):
+    r"""
+    Hankel function of the second kind.
+
+    Explanation
+    ===========
+
+    This function is defined as
+
+    .. math ::
+        H_\nu^{(2)} = J_\nu(z) - iY_\nu(z),
+
+    where $J_\nu(z)$ is the Bessel function of the first kind, and
+    $Y_\nu(z)$ is the Bessel function of the second kind.
+
+    It is a solution to Bessel's equation, and linearly independent from
+    $H_\nu^{(1)}$.
+
+    Examples
+    ========
+
+    >>> from sympy import hankel2
+    >>> from sympy.abc import z, n
+    >>> hankel2(n, z).diff(z)
+    hankel2(n - 1, z)/2 - hankel2(n + 1, z)/2
+
+    See Also
+    ========
+
+    hankel1, besselj, bessely
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/Bessel-TypeFunctions/HankelH2/
+
+    """
+
+    _a = S.One
+    _b = S.One
+
+    def _eval_conjugate(self):
+        z = self.argument
+        if z.is_extended_negative is False:
+            return hankel1(self.order.conjugate(), z.conjugate())
+
+
+def assume_integer_order(fn):
+    @wraps(fn)
+    def g(self, nu, z):
+        if nu.is_integer:
+            return fn(self, nu, z)
+    return g
+
+
+class SphericalBesselBase(BesselBase):
+    """
+    Base class for spherical Bessel functions.
+
+    These are thin wrappers around ordinary Bessel functions,
+    since spherical Bessel functions differ from the ordinary
+    ones just by a slight change in order.
+
+    To use this class, define the ``_eval_evalf()`` and ``_expand()`` methods.
+
+    """
+
+    def _expand(self, **hints):
+        """ Expand self into a polynomial. Nu is guaranteed to be Integer. """
+        raise NotImplementedError('expansion')
+
+    def _eval_expand_func(self, **hints):
+        if self.order.is_Integer:
+            return self._expand(**hints)
+        return self
+
+    def fdiff(self, argindex=2):
+        if argindex != 2:
+            raise ArgumentIndexError(self, argindex)
+        return self.__class__(self.order - 1, self.argument) - \
+            self * (self.order + 1)/self.argument
+
+
+def _jn(n, z):
+    return (spherical_bessel_fn(n, z)*sin(z) +
+            S.NegativeOne**(n + 1)*spherical_bessel_fn(-n - 1, z)*cos(z))
+
+
+def _yn(n, z):
+    # (-1)**(n + 1) * _jn(-n - 1, z)
+    return (S.NegativeOne**(n + 1) * spherical_bessel_fn(-n - 1, z)*sin(z) -
+            spherical_bessel_fn(n, z)*cos(z))
+
+
+class jn(SphericalBesselBase):
+    r"""
+    Spherical Bessel function of the first kind.
+
+    Explanation
+    ===========
+
+    This function is a solution to the spherical Bessel equation
+
+    .. math ::
+        z^2 \frac{\mathrm{d}^2 w}{\mathrm{d}z^2}
+          + 2z \frac{\mathrm{d}w}{\mathrm{d}z} + (z^2 - \nu(\nu + 1)) w = 0.
+
+    It can be defined as
+
+    .. math ::
+        j_\nu(z) = \sqrt{\frac{\pi}{2z}} J_{\nu + \frac{1}{2}}(z),
+
+    where $J_\nu(z)$ is the Bessel function of the first kind.
+
+    The spherical Bessel functions of integral order are
+    calculated using the formula:
+
+    .. math:: j_n(z) = f_n(z) \sin{z} + (-1)^{n+1} f_{-n-1}(z) \cos{z},
+
+    where the coefficients $f_n(z)$ are available as
+    :func:`sympy.polys.orthopolys.spherical_bessel_fn`.
+
+    Examples
+    ========
+
+    >>> from sympy import Symbol, jn, sin, cos, expand_func, besselj, bessely
+    >>> z = Symbol("z")
+    >>> nu = Symbol("nu", integer=True)
+    >>> print(expand_func(jn(0, z)))
+    sin(z)/z
+    >>> expand_func(jn(1, z)) == sin(z)/z**2 - cos(z)/z
+    True
+    >>> expand_func(jn(3, z))
+    (-6/z**2 + 15/z**4)*sin(z) + (1/z - 15/z**3)*cos(z)
+    >>> jn(nu, z).rewrite(besselj)
+    sqrt(2)*sqrt(pi)*sqrt(1/z)*besselj(nu + 1/2, z)/2
+    >>> jn(nu, z).rewrite(bessely)
+    (-1)**nu*sqrt(2)*sqrt(pi)*sqrt(1/z)*bessely(-nu - 1/2, z)/2
+    >>> jn(2, 5.2+0.3j).evalf(20)
+    0.099419756723640344491 - 0.054525080242173562897*I
+
+    See Also
+    ========
+
+    besselj, bessely, besselk, yn
+
+    References
+    ==========
+
+    .. [1] https://dlmf.nist.gov/10.47
+
+    """
+    @classmethod
+    def eval(cls, nu, z):
+        if z.is_zero:
+            if nu.is_zero:
+                return S.One
+            elif nu.is_integer:
+                if nu.is_positive:
+                    return S.Zero
+                else:
+                    return S.ComplexInfinity
+        if z in (S.NegativeInfinity, S.Infinity):
+            return S.Zero
+
+    def _eval_rewrite_as_besselj(self, nu, z, **kwargs):
+        return sqrt(pi/(2*z)) * besselj(nu + S.Half, z)
+
+    def _eval_rewrite_as_bessely(self, nu, z, **kwargs):
+        return S.NegativeOne**nu * sqrt(pi/(2*z)) * bessely(-nu - S.Half, z)
+
+    def _eval_rewrite_as_yn(self, nu, z, **kwargs):
+        return S.NegativeOne**(nu) * yn(-nu - 1, z)
+
+    def _expand(self, **hints):
+        return _jn(self.order, self.argument)
+
+    def _eval_evalf(self, prec):
+        if self.order.is_Integer:
+            return self.rewrite(besselj)._eval_evalf(prec)
+
+
+class yn(SphericalBesselBase):
+    r"""
+    Spherical Bessel function of the second kind.
+
+    Explanation
+    ===========
+
+    This function is another solution to the spherical Bessel equation, and
+    linearly independent from $j_n$. It can be defined as
+
+    .. math ::
+        y_\nu(z) = \sqrt{\frac{\pi}{2z}} Y_{\nu + \frac{1}{2}}(z),
+
+    where $Y_\nu(z)$ is the Bessel function of the second kind.
+
+    For integral orders $n$, $y_n$ is calculated using the formula:
+
+    .. math:: y_n(z) = (-1)^{n+1} j_{-n-1}(z)
+
+    Examples
+    ========
+
+    >>> from sympy import Symbol, yn, sin, cos, expand_func, besselj, bessely
+    >>> z = Symbol("z")
+    >>> nu = Symbol("nu", integer=True)
+    >>> print(expand_func(yn(0, z)))
+    -cos(z)/z
+    >>> expand_func(yn(1, z)) == -cos(z)/z**2-sin(z)/z
+    True
+    >>> yn(nu, z).rewrite(besselj)
+    (-1)**(nu + 1)*sqrt(2)*sqrt(pi)*sqrt(1/z)*besselj(-nu - 1/2, z)/2
+    >>> yn(nu, z).rewrite(bessely)
+    sqrt(2)*sqrt(pi)*sqrt(1/z)*bessely(nu + 1/2, z)/2
+    >>> yn(2, 5.2+0.3j).evalf(20)
+    0.18525034196069722536 + 0.014895573969924817587*I
+
+    See Also
+    ========
+
+    besselj, bessely, besselk, jn
+
+    References
+    ==========
+
+    .. [1] https://dlmf.nist.gov/10.47
+
+    """
+    @assume_integer_order
+    def _eval_rewrite_as_besselj(self, nu, z, **kwargs):
+        return S.NegativeOne**(nu+1) * sqrt(pi/(2*z)) * besselj(-nu - S.Half, z)
+
+    @assume_integer_order
+    def _eval_rewrite_as_bessely(self, nu, z, **kwargs):
+        return sqrt(pi/(2*z)) * bessely(nu + S.Half, z)
+
+    def _eval_rewrite_as_jn(self, nu, z, **kwargs):
+        return S.NegativeOne**(nu + 1) * jn(-nu - 1, z)
+
+    def _expand(self, **hints):
+        return _yn(self.order, self.argument)
+
+    def _eval_evalf(self, prec):
+        if self.order.is_Integer:
+            return self.rewrite(bessely)._eval_evalf(prec)
+
+
+class SphericalHankelBase(SphericalBesselBase):
+
+    @assume_integer_order
+    def _eval_rewrite_as_besselj(self, nu, z, **kwargs):
+        # jn +- I*yn
+        # jn as beeselj: sqrt(pi/(2*z)) * besselj(nu + S.Half, z)
+        # yn as besselj: (-1)**(nu+1) * sqrt(pi/(2*z)) * besselj(-nu - S.Half, z)
+        hks = self._hankel_kind_sign
+        return sqrt(pi/(2*z))*(besselj(nu + S.Half, z) +
+                               hks*I*S.NegativeOne**(nu+1)*besselj(-nu - S.Half, z))
+
+    @assume_integer_order
+    def _eval_rewrite_as_bessely(self, nu, z, **kwargs):
+        # jn +- I*yn
+        # jn as bessely: (-1)**nu * sqrt(pi/(2*z)) * bessely(-nu - S.Half, z)
+        # yn as bessely: sqrt(pi/(2*z)) * bessely(nu + S.Half, z)
+        hks = self._hankel_kind_sign
+        return sqrt(pi/(2*z))*(S.NegativeOne**nu*bessely(-nu - S.Half, z) +
+                               hks*I*bessely(nu + S.Half, z))
+
+    def _eval_rewrite_as_yn(self, nu, z, **kwargs):
+        hks = self._hankel_kind_sign
+        return jn(nu, z).rewrite(yn) + hks*I*yn(nu, z)
+
+    def _eval_rewrite_as_jn(self, nu, z, **kwargs):
+        hks = self._hankel_kind_sign
+        return jn(nu, z) + hks*I*yn(nu, z).rewrite(jn)
+
+    def _eval_expand_func(self, **hints):
+        if self.order.is_Integer:
+            return self._expand(**hints)
+        else:
+            nu = self.order
+            z = self.argument
+            hks = self._hankel_kind_sign
+            return jn(nu, z) + hks*I*yn(nu, z)
+
+    def _expand(self, **hints):
+        n = self.order
+        z = self.argument
+        hks = self._hankel_kind_sign
+
+        # fully expanded version
+        # return ((fn(n, z) * sin(z) +
+        #          (-1)**(n + 1) * fn(-n - 1, z) * cos(z)) +  # jn
+        #         (hks * I * (-1)**(n + 1) *
+        #          (fn(-n - 1, z) * hk * I * sin(z) +
+        #           (-1)**(-n) * fn(n, z) * I * cos(z)))  # +-I*yn
+        #         )
+
+        return (_jn(n, z) + hks*I*_yn(n, z)).expand()
+
+    def _eval_evalf(self, prec):
+        if self.order.is_Integer:
+            return self.rewrite(besselj)._eval_evalf(prec)
+
+
+class hn1(SphericalHankelBase):
+    r"""
+    Spherical Hankel function of the first kind.
+
+    Explanation
+    ===========
+
+    This function is defined as
+
+    .. math:: h_\nu^(1)(z) = j_\nu(z) + i y_\nu(z),
+
+    where $j_\nu(z)$ and $y_\nu(z)$ are the spherical
+    Bessel function of the first and second kinds.
+
+    For integral orders $n$, $h_n^(1)$ is calculated using the formula:
+
+    .. math:: h_n^(1)(z) = j_{n}(z) + i (-1)^{n+1} j_{-n-1}(z)
+
+    Examples
+    ========
+
+    >>> from sympy import Symbol, hn1, hankel1, expand_func, yn, jn
+    >>> z = Symbol("z")
+    >>> nu = Symbol("nu", integer=True)
+    >>> print(expand_func(hn1(nu, z)))
+    jn(nu, z) + I*yn(nu, z)
+    >>> print(expand_func(hn1(0, z)))
+    sin(z)/z - I*cos(z)/z
+    >>> print(expand_func(hn1(1, z)))
+    -I*sin(z)/z - cos(z)/z + sin(z)/z**2 - I*cos(z)/z**2
+    >>> hn1(nu, z).rewrite(jn)
+    (-1)**(nu + 1)*I*jn(-nu - 1, z) + jn(nu, z)
+    >>> hn1(nu, z).rewrite(yn)
+    (-1)**nu*yn(-nu - 1, z) + I*yn(nu, z)
+    >>> hn1(nu, z).rewrite(hankel1)
+    sqrt(2)*sqrt(pi)*sqrt(1/z)*hankel1(nu, z)/2
+
+    See Also
+    ========
+
+    hn2, jn, yn, hankel1, hankel2
+
+    References
+    ==========
+
+    .. [1] https://dlmf.nist.gov/10.47
+
+    """
+
+    _hankel_kind_sign = S.One
+
+    @assume_integer_order
+    def _eval_rewrite_as_hankel1(self, nu, z, **kwargs):
+        return sqrt(pi/(2*z))*hankel1(nu, z)
+
+
+class hn2(SphericalHankelBase):
+    r"""
+    Spherical Hankel function of the second kind.
+
+    Explanation
+    ===========
+
+    This function is defined as
+
+    .. math:: h_\nu^(2)(z) = j_\nu(z) - i y_\nu(z),
+
+    where $j_\nu(z)$ and $y_\nu(z)$ are the spherical
+    Bessel function of the first and second kinds.
+
+    For integral orders $n$, $h_n^(2)$ is calculated using the formula:
+
+    .. math:: h_n^(2)(z) = j_{n} - i (-1)^{n+1} j_{-n-1}(z)
+
+    Examples
+    ========
+
+    >>> from sympy import Symbol, hn2, hankel2, expand_func, jn, yn
+    >>> z = Symbol("z")
+    >>> nu = Symbol("nu", integer=True)
+    >>> print(expand_func(hn2(nu, z)))
+    jn(nu, z) - I*yn(nu, z)
+    >>> print(expand_func(hn2(0, z)))
+    sin(z)/z + I*cos(z)/z
+    >>> print(expand_func(hn2(1, z)))
+    I*sin(z)/z - cos(z)/z + sin(z)/z**2 + I*cos(z)/z**2
+    >>> hn2(nu, z).rewrite(hankel2)
+    sqrt(2)*sqrt(pi)*sqrt(1/z)*hankel2(nu, z)/2
+    >>> hn2(nu, z).rewrite(jn)
+    -(-1)**(nu + 1)*I*jn(-nu - 1, z) + jn(nu, z)
+    >>> hn2(nu, z).rewrite(yn)
+    (-1)**nu*yn(-nu - 1, z) - I*yn(nu, z)
+
+    See Also
+    ========
+
+    hn1, jn, yn, hankel1, hankel2
+
+    References
+    ==========
+
+    .. [1] https://dlmf.nist.gov/10.47
+
+    """
+
+    _hankel_kind_sign = -S.One
+
+    @assume_integer_order
+    def _eval_rewrite_as_hankel2(self, nu, z, **kwargs):
+        return sqrt(pi/(2*z))*hankel2(nu, z)
+
+
+def jn_zeros(n, k, method="sympy", dps=15):
+    """
+    Zeros of the spherical Bessel function of the first kind.
+
+    Explanation
+    ===========
+
+    This returns an array of zeros of $jn$ up to the $k$-th zero.
+
+    * method = "sympy": uses `mpmath.besseljzero
+      <https://mpmath.org/doc/current/functions/bessel.html#mpmath.besseljzero>`_
+    * method = "scipy": uses the
+      `SciPy's sph_jn <https://docs.scipy.org/doc/scipy/reference/generated/scipy.special.jn_zeros.html>`_
+      and
+      `newton <https://docs.scipy.org/doc/scipy/reference/generated/scipy.optimize.newton.html>`_
+      to find all
+      roots, which is faster than computing the zeros using a general
+      numerical solver, but it requires SciPy and only works with low
+      precision floating point numbers. (The function used with
+      method="sympy" is a recent addition to mpmath; before that a general
+      solver was used.)
+
+    Examples
+    ========
+
+    >>> from sympy import jn_zeros
+    >>> jn_zeros(2, 4, dps=5)
+    [5.7635, 9.095, 12.323, 15.515]
+
+    See Also
+    ========
+
+    jn, yn, besselj, besselk, bessely
+
+    Parameters
+    ==========
+
+    n : integer
+        order of Bessel function
+
+    k : integer
+        number of zeros to return
+
+
+    """
+    from math import pi as math_pi
+
+    if method == "sympy":
+        from mpmath import besseljzero
+        from mpmath.libmp.libmpf import dps_to_prec
+        prec = dps_to_prec(dps)
+        return [Expr._from_mpmath(besseljzero(S(n + 0.5)._to_mpmath(prec),
+                                              int(l)), prec)
+                for l in range(1, k + 1)]
+    elif method == "scipy":
+        from scipy.optimize import newton
+        try:
+            from scipy.special import spherical_jn
+            f = lambda x: spherical_jn(n, x)
+        except ImportError:
+            from scipy.special import sph_jn
+            f = lambda x: sph_jn(n, x)[0][-1]
+    else:
+        raise NotImplementedError("Unknown method.")
+
+    def solver(f, x):
+        if method == "scipy":
+            root = newton(f, x)
+        else:
+            raise NotImplementedError("Unknown method.")
+        return root
+
+    # we need to approximate the position of the first root:
+    root = n + math_pi
+    # determine the first root exactly:
+    root = solver(f, root)
+    roots = [root]
+    for i in range(k - 1):
+        # estimate the position of the next root using the last root + pi:
+        root = solver(f, root + math_pi)
+        roots.append(root)
+    return roots
+
+
+class AiryBase(Function):
+    """
+    Abstract base class for Airy functions.
+
+    This class is meant to reduce code duplication.
+
+    """
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate())
+
+    def _eval_is_extended_real(self):
+        return self.args[0].is_extended_real
+
+    def as_real_imag(self, deep=True, **hints):
+        z = self.args[0]
+        zc = z.conjugate()
+        f = self.func
+        u = (f(z)+f(zc))/2
+        v = I*(f(zc)-f(z))/2
+        return u, v
+
+    def _eval_expand_complex(self, deep=True, **hints):
+        re_part, im_part = self.as_real_imag(deep=deep, **hints)
+        return re_part + im_part*I
+
+
+class airyai(AiryBase):
+    r"""
+    The Airy function $\operatorname{Ai}$ of the first kind.
+
+    Explanation
+    ===========
+
+    The Airy function $\operatorname{Ai}(z)$ is defined to be the function
+    satisfying Airy's differential equation
+
+    .. math::
+        \frac{\mathrm{d}^2 w(z)}{\mathrm{d}z^2} - z w(z) = 0.
+
+    Equivalently, for real $z$
+
+    .. math::
+        \operatorname{Ai}(z) := \frac{1}{\pi}
+        \int_0^\infty \cos\left(\frac{t^3}{3} + z t\right) \mathrm{d}t.
+
+    Examples
+    ========
+
+    Create an Airy function object:
+
+    >>> from sympy import airyai
+    >>> from sympy.abc import z
+
+    >>> airyai(z)
+    airyai(z)
+
+    Several special values are known:
+
+    >>> airyai(0)
+    3**(1/3)/(3*gamma(2/3))
+    >>> from sympy import oo
+    >>> airyai(oo)
+    0
+    >>> airyai(-oo)
+    0
+
+    The Airy function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(airyai(z))
+    airyai(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(airyai(z), z)
+    airyaiprime(z)
+    >>> diff(airyai(z), z, 2)
+    z*airyai(z)
+
+    Series expansion is also supported:
+
+    >>> from sympy import series
+    >>> series(airyai(z), z, 0, 3)
+    3**(5/6)*gamma(1/3)/(6*pi) - 3**(1/6)*z*gamma(2/3)/(2*pi) + O(z**3)
+
+    We can numerically evaluate the Airy function to arbitrary precision
+    on the whole complex plane:
+
+    >>> airyai(-2).evalf(50)
+    0.22740742820168557599192443603787379946077222541710
+
+    Rewrite $\operatorname{Ai}(z)$ in terms of hypergeometric functions:
+
+    >>> from sympy import hyper
+    >>> airyai(z).rewrite(hyper)
+    -3**(2/3)*z*hyper((), (4/3,), z**3/9)/(3*gamma(1/3)) + 3**(1/3)*hyper((), (2/3,), z**3/9)/(3*gamma(2/3))
+
+    See Also
+    ========
+
+    airybi: Airy function of the second kind.
+    airyaiprime: Derivative of the Airy function of the first kind.
+    airybiprime: Derivative of the Airy function of the second kind.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Airy_function
+    .. [2] https://dlmf.nist.gov/9
+    .. [3] https://encyclopediaofmath.org/wiki/Airy_functions
+    .. [4] https://mathworld.wolfram.com/AiryFunctions.html
+
+    """
+
+    nargs = 1
+    unbranched = True
+
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_Number:
+            if arg is S.NaN:
+                return S.NaN
+            elif arg is S.Infinity:
+                return S.Zero
+            elif arg is S.NegativeInfinity:
+                return S.Zero
+            elif arg.is_zero:
+                return S.One / (3**Rational(2, 3) * gamma(Rational(2, 3)))
+        if arg.is_zero:
+            return S.One / (3**Rational(2, 3) * gamma(Rational(2, 3)))
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return airyaiprime(self.args[0])
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n < 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            if len(previous_terms) > 1:
+                p = previous_terms[-1]
+                return ((cbrt(3)*x)**(-n)*(cbrt(3)*x)**(n + 1)*sin(pi*(n*Rational(2, 3) + Rational(4, 3)))*factorial(n) *
+                        gamma(n/3 + Rational(2, 3))/(sin(pi*(n*Rational(2, 3) + Rational(2, 3)))*factorial(n + 1)*gamma(n/3 + Rational(1, 3))) * p)
+            else:
+                return (S.One/(3**Rational(2, 3)*pi) * gamma((n+S.One)/S(3)) * sin(Rational(2, 3)*pi*(n+S.One)) /
+                        factorial(n) * (cbrt(3)*x)**n)
+
+    def _eval_rewrite_as_besselj(self, z, **kwargs):
+        ot = Rational(1, 3)
+        tt = Rational(2, 3)
+        a = Pow(-z, Rational(3, 2))
+        if re(z).is_negative:
+            return ot*sqrt(-z) * (besselj(-ot, tt*a) + besselj(ot, tt*a))
+
+    def _eval_rewrite_as_besseli(self, z, **kwargs):
+        ot = Rational(1, 3)
+        tt = Rational(2, 3)
+        a = Pow(z, Rational(3, 2))
+        if re(z).is_positive:
+            return ot*sqrt(z) * (besseli(-ot, tt*a) - besseli(ot, tt*a))
+        else:
+            return ot*(Pow(a, ot)*besseli(-ot, tt*a) - z*Pow(a, -ot)*besseli(ot, tt*a))
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        pf1 = S.One / (3**Rational(2, 3)*gamma(Rational(2, 3)))
+        pf2 = z / (root(3, 3)*gamma(Rational(1, 3)))
+        return pf1 * hyper([], [Rational(2, 3)], z**3/9) - pf2 * hyper([], [Rational(4, 3)], z**3/9)
+
+    def _eval_expand_func(self, **hints):
+        arg = self.args[0]
+        symbs = arg.free_symbols
+
+        if len(symbs) == 1:
+            z = symbs.pop()
+            c = Wild("c", exclude=[z])
+            d = Wild("d", exclude=[z])
+            m = Wild("m", exclude=[z])
+            n = Wild("n", exclude=[z])
+            M = arg.match(c*(d*z**n)**m)
+            if M is not None:
+                m = M[m]
+                # The transformation is given by 03.05.16.0001.01
+                # https://functions.wolfram.com/Bessel-TypeFunctions/AiryAi/16/01/01/0001/
+                if (3*m).is_integer:
+                    c = M[c]
+                    d = M[d]
+                    n = M[n]
+                    pf = (d * z**n)**m / (d**m * z**(m*n))
+                    newarg = c * d**m * z**(m*n)
+                    return S.Half * ((pf + S.One)*airyai(newarg) - (pf - S.One)/sqrt(3)*airybi(newarg))
+
+
+class airybi(AiryBase):
+    r"""
+    The Airy function $\operatorname{Bi}$ of the second kind.
+
+    Explanation
+    ===========
+
+    The Airy function $\operatorname{Bi}(z)$ is defined to be the function
+    satisfying Airy's differential equation
+
+    .. math::
+        \frac{\mathrm{d}^2 w(z)}{\mathrm{d}z^2} - z w(z) = 0.
+
+    Equivalently, for real $z$
+
+    .. math::
+        \operatorname{Bi}(z) := \frac{1}{\pi}
+                 \int_0^\infty
+                   \exp\left(-\frac{t^3}{3} + z t\right)
+                   + \sin\left(\frac{t^3}{3} + z t\right) \mathrm{d}t.
+
+    Examples
+    ========
+
+    Create an Airy function object:
+
+    >>> from sympy import airybi
+    >>> from sympy.abc import z
+
+    >>> airybi(z)
+    airybi(z)
+
+    Several special values are known:
+
+    >>> airybi(0)
+    3**(5/6)/(3*gamma(2/3))
+    >>> from sympy import oo
+    >>> airybi(oo)
+    oo
+    >>> airybi(-oo)
+    0
+
+    The Airy function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(airybi(z))
+    airybi(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(airybi(z), z)
+    airybiprime(z)
+    >>> diff(airybi(z), z, 2)
+    z*airybi(z)
+
+    Series expansion is also supported:
+
+    >>> from sympy import series
+    >>> series(airybi(z), z, 0, 3)
+    3**(1/3)*gamma(1/3)/(2*pi) + 3**(2/3)*z*gamma(2/3)/(2*pi) + O(z**3)
+
+    We can numerically evaluate the Airy function to arbitrary precision
+    on the whole complex plane:
+
+    >>> airybi(-2).evalf(50)
+    -0.41230258795639848808323405461146104203453483447240
+
+    Rewrite $\operatorname{Bi}(z)$ in terms of hypergeometric functions:
+
+    >>> from sympy import hyper
+    >>> airybi(z).rewrite(hyper)
+    3**(1/6)*z*hyper((), (4/3,), z**3/9)/gamma(1/3) + 3**(5/6)*hyper((), (2/3,), z**3/9)/(3*gamma(2/3))
+
+    See Also
+    ========
+
+    airyai: Airy function of the first kind.
+    airyaiprime: Derivative of the Airy function of the first kind.
+    airybiprime: Derivative of the Airy function of the second kind.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Airy_function
+    .. [2] https://dlmf.nist.gov/9
+    .. [3] https://encyclopediaofmath.org/wiki/Airy_functions
+    .. [4] https://mathworld.wolfram.com/AiryFunctions.html
+
+    """
+
+    nargs = 1
+    unbranched = True
+
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_Number:
+            if arg is S.NaN:
+                return S.NaN
+            elif arg is S.Infinity:
+                return S.Infinity
+            elif arg is S.NegativeInfinity:
+                return S.Zero
+            elif arg.is_zero:
+                return S.One / (3**Rational(1, 6) * gamma(Rational(2, 3)))
+
+        if arg.is_zero:
+            return S.One / (3**Rational(1, 6) * gamma(Rational(2, 3)))
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return airybiprime(self.args[0])
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n < 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            if len(previous_terms) > 1:
+                p = previous_terms[-1]
+                return (cbrt(3)*x * Abs(sin(Rational(2, 3)*pi*(n + S.One))) * factorial((n - S.One)/S(3)) /
+                        ((n + S.One) * Abs(cos(Rational(2, 3)*pi*(n + S.Half))) * factorial((n - 2)/S(3))) * p)
+            else:
+                return (S.One/(root(3, 6)*pi) * gamma((n + S.One)/S(3)) * Abs(sin(Rational(2, 3)*pi*(n + S.One))) /
+                        factorial(n) * (cbrt(3)*x)**n)
+
+    def _eval_rewrite_as_besselj(self, z, **kwargs):
+        ot = Rational(1, 3)
+        tt = Rational(2, 3)
+        a = Pow(-z, Rational(3, 2))
+        if re(z).is_negative:
+            return sqrt(-z/3) * (besselj(-ot, tt*a) - besselj(ot, tt*a))
+
+    def _eval_rewrite_as_besseli(self, z, **kwargs):
+        ot = Rational(1, 3)
+        tt = Rational(2, 3)
+        a = Pow(z, Rational(3, 2))
+        if re(z).is_positive:
+            return sqrt(z)/sqrt(3) * (besseli(-ot, tt*a) + besseli(ot, tt*a))
+        else:
+            b = Pow(a, ot)
+            c = Pow(a, -ot)
+            return sqrt(ot)*(b*besseli(-ot, tt*a) + z*c*besseli(ot, tt*a))
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        pf1 = S.One / (root(3, 6)*gamma(Rational(2, 3)))
+        pf2 = z*root(3, 6) / gamma(Rational(1, 3))
+        return pf1 * hyper([], [Rational(2, 3)], z**3/9) + pf2 * hyper([], [Rational(4, 3)], z**3/9)
+
+    def _eval_expand_func(self, **hints):
+        arg = self.args[0]
+        symbs = arg.free_symbols
+
+        if len(symbs) == 1:
+            z = symbs.pop()
+            c = Wild("c", exclude=[z])
+            d = Wild("d", exclude=[z])
+            m = Wild("m", exclude=[z])
+            n = Wild("n", exclude=[z])
+            M = arg.match(c*(d*z**n)**m)
+            if M is not None:
+                m = M[m]
+                # The transformation is given by 03.06.16.0001.01
+                # https://functions.wolfram.com/Bessel-TypeFunctions/AiryBi/16/01/01/0001/
+                if (3*m).is_integer:
+                    c = M[c]
+                    d = M[d]
+                    n = M[n]
+                    pf = (d * z**n)**m / (d**m * z**(m*n))
+                    newarg = c * d**m * z**(m*n)
+                    return S.Half * (sqrt(3)*(S.One - pf)*airyai(newarg) + (S.One + pf)*airybi(newarg))
+
+
+class airyaiprime(AiryBase):
+    r"""
+    The derivative $\operatorname{Ai}^\prime$ of the Airy function of the first
+    kind.
+
+    Explanation
+    ===========
+
+    The Airy function $\operatorname{Ai}^\prime(z)$ is defined to be the
+    function
+
+    .. math::
+        \operatorname{Ai}^\prime(z) := \frac{\mathrm{d} \operatorname{Ai}(z)}{\mathrm{d} z}.
+
+    Examples
+    ========
+
+    Create an Airy function object:
+
+    >>> from sympy import airyaiprime
+    >>> from sympy.abc import z
+
+    >>> airyaiprime(z)
+    airyaiprime(z)
+
+    Several special values are known:
+
+    >>> airyaiprime(0)
+    -3**(2/3)/(3*gamma(1/3))
+    >>> from sympy import oo
+    >>> airyaiprime(oo)
+    0
+
+    The Airy function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(airyaiprime(z))
+    airyaiprime(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(airyaiprime(z), z)
+    z*airyai(z)
+    >>> diff(airyaiprime(z), z, 2)
+    z*airyaiprime(z) + airyai(z)
+
+    Series expansion is also supported:
+
+    >>> from sympy import series
+    >>> series(airyaiprime(z), z, 0, 3)
+    -3**(2/3)/(3*gamma(1/3)) + 3**(1/3)*z**2/(6*gamma(2/3)) + O(z**3)
+
+    We can numerically evaluate the Airy function to arbitrary precision
+    on the whole complex plane:
+
+    >>> airyaiprime(-2).evalf(50)
+    0.61825902074169104140626429133247528291577794512415
+
+    Rewrite $\operatorname{Ai}^\prime(z)$ in terms of hypergeometric functions:
+
+    >>> from sympy import hyper
+    >>> airyaiprime(z).rewrite(hyper)
+    3**(1/3)*z**2*hyper((), (5/3,), z**3/9)/(6*gamma(2/3)) - 3**(2/3)*hyper((), (1/3,), z**3/9)/(3*gamma(1/3))
+
+    See Also
+    ========
+
+    airyai: Airy function of the first kind.
+    airybi: Airy function of the second kind.
+    airybiprime: Derivative of the Airy function of the second kind.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Airy_function
+    .. [2] https://dlmf.nist.gov/9
+    .. [3] https://encyclopediaofmath.org/wiki/Airy_functions
+    .. [4] https://mathworld.wolfram.com/AiryFunctions.html
+
+    """
+
+    nargs = 1
+    unbranched = True
+
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_Number:
+            if arg is S.NaN:
+                return S.NaN
+            elif arg is S.Infinity:
+                return S.Zero
+
+        if arg.is_zero:
+            return S.NegativeOne / (3**Rational(1, 3) * gamma(Rational(1, 3)))
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return self.args[0]*airyai(self.args[0])
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_evalf(self, prec):
+        z = self.args[0]._to_mpmath(prec)
+        with workprec(prec):
+            res = mp.airyai(z, derivative=1)
+        return Expr._from_mpmath(res, prec)
+
+    def _eval_rewrite_as_besselj(self, z, **kwargs):
+        tt = Rational(2, 3)
+        a = Pow(-z, Rational(3, 2))
+        if re(z).is_negative:
+            return z/3 * (besselj(-tt, tt*a) - besselj(tt, tt*a))
+
+    def _eval_rewrite_as_besseli(self, z, **kwargs):
+        ot = Rational(1, 3)
+        tt = Rational(2, 3)
+        a = tt * Pow(z, Rational(3, 2))
+        if re(z).is_positive:
+            return z/3 * (besseli(tt, a) - besseli(-tt, a))
+        else:
+            a = Pow(z, Rational(3, 2))
+            b = Pow(a, tt)
+            c = Pow(a, -tt)
+            return ot * (z**2*c*besseli(tt, tt*a) - b*besseli(-ot, tt*a))
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        pf1 = z**2 / (2*3**Rational(2, 3)*gamma(Rational(2, 3)))
+        pf2 = 1 / (root(3, 3)*gamma(Rational(1, 3)))
+        return pf1 * hyper([], [Rational(5, 3)], z**3/9) - pf2 * hyper([], [Rational(1, 3)], z**3/9)
+
+    def _eval_expand_func(self, **hints):
+        arg = self.args[0]
+        symbs = arg.free_symbols
+
+        if len(symbs) == 1:
+            z = symbs.pop()
+            c = Wild("c", exclude=[z])
+            d = Wild("d", exclude=[z])
+            m = Wild("m", exclude=[z])
+            n = Wild("n", exclude=[z])
+            M = arg.match(c*(d*z**n)**m)
+            if M is not None:
+                m = M[m]
+                # The transformation is in principle
+                # given by 03.07.16.0001.01 but note
+                # that there is an error in this formula.
+                # https://functions.wolfram.com/Bessel-TypeFunctions/AiryAiPrime/16/01/01/0001/
+                if (3*m).is_integer:
+                    c = M[c]
+                    d = M[d]
+                    n = M[n]
+                    pf = (d**m * z**(n*m)) / (d * z**n)**m
+                    newarg = c * d**m * z**(n*m)
+                    return S.Half * ((pf + S.One)*airyaiprime(newarg) + (pf - S.One)/sqrt(3)*airybiprime(newarg))
+
+
+class airybiprime(AiryBase):
+    r"""
+    The derivative $\operatorname{Bi}^\prime$ of the Airy function of the first
+    kind.
+
+    Explanation
+    ===========
+
+    The Airy function $\operatorname{Bi}^\prime(z)$ is defined to be the
+    function
+
+    .. math::
+        \operatorname{Bi}^\prime(z) := \frac{\mathrm{d} \operatorname{Bi}(z)}{\mathrm{d} z}.
+
+    Examples
+    ========
+
+    Create an Airy function object:
+
+    >>> from sympy import airybiprime
+    >>> from sympy.abc import z
+
+    >>> airybiprime(z)
+    airybiprime(z)
+
+    Several special values are known:
+
+    >>> airybiprime(0)
+    3**(1/6)/gamma(1/3)
+    >>> from sympy import oo
+    >>> airybiprime(oo)
+    oo
+    >>> airybiprime(-oo)
+    0
+
+    The Airy function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(airybiprime(z))
+    airybiprime(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(airybiprime(z), z)
+    z*airybi(z)
+    >>> diff(airybiprime(z), z, 2)
+    z*airybiprime(z) + airybi(z)
+
+    Series expansion is also supported:
+
+    >>> from sympy import series
+    >>> series(airybiprime(z), z, 0, 3)
+    3**(1/6)/gamma(1/3) + 3**(5/6)*z**2/(6*gamma(2/3)) + O(z**3)
+
+    We can numerically evaluate the Airy function to arbitrary precision
+    on the whole complex plane:
+
+    >>> airybiprime(-2).evalf(50)
+    0.27879516692116952268509756941098324140300059345163
+
+    Rewrite $\operatorname{Bi}^\prime(z)$ in terms of hypergeometric functions:
+
+    >>> from sympy import hyper
+    >>> airybiprime(z).rewrite(hyper)
+    3**(5/6)*z**2*hyper((), (5/3,), z**3/9)/(6*gamma(2/3)) + 3**(1/6)*hyper((), (1/3,), z**3/9)/gamma(1/3)
+
+    See Also
+    ========
+
+    airyai: Airy function of the first kind.
+    airybi: Airy function of the second kind.
+    airyaiprime: Derivative of the Airy function of the first kind.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Airy_function
+    .. [2] https://dlmf.nist.gov/9
+    .. [3] https://encyclopediaofmath.org/wiki/Airy_functions
+    .. [4] https://mathworld.wolfram.com/AiryFunctions.html
+
+    """
+
+    nargs = 1
+    unbranched = True
+
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_Number:
+            if arg is S.NaN:
+                return S.NaN
+            elif arg is S.Infinity:
+                return S.Infinity
+            elif arg is S.NegativeInfinity:
+                return S.Zero
+            elif arg.is_zero:
+                return 3**Rational(1, 6) / gamma(Rational(1, 3))
+
+        if arg.is_zero:
+            return 3**Rational(1, 6) / gamma(Rational(1, 3))
+
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return self.args[0]*airybi(self.args[0])
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_evalf(self, prec):
+        z = self.args[0]._to_mpmath(prec)
+        with workprec(prec):
+            res = mp.airybi(z, derivative=1)
+        return Expr._from_mpmath(res, prec)
+
+    def _eval_rewrite_as_besselj(self, z, **kwargs):
+        tt = Rational(2, 3)
+        a = tt * Pow(-z, Rational(3, 2))
+        if re(z).is_negative:
+            return -z/sqrt(3) * (besselj(-tt, a) + besselj(tt, a))
+
+    def _eval_rewrite_as_besseli(self, z, **kwargs):
+        ot = Rational(1, 3)
+        tt = Rational(2, 3)
+        a = tt * Pow(z, Rational(3, 2))
+        if re(z).is_positive:
+            return z/sqrt(3) * (besseli(-tt, a) + besseli(tt, a))
+        else:
+            a = Pow(z, Rational(3, 2))
+            b = Pow(a, tt)
+            c = Pow(a, -tt)
+            return sqrt(ot) * (b*besseli(-tt, tt*a) + z**2*c*besseli(tt, tt*a))
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        pf1 = z**2 / (2*root(3, 6)*gamma(Rational(2, 3)))
+        pf2 = root(3, 6) / gamma(Rational(1, 3))
+        return pf1 * hyper([], [Rational(5, 3)], z**3/9) + pf2 * hyper([], [Rational(1, 3)], z**3/9)
+
+    def _eval_expand_func(self, **hints):
+        arg = self.args[0]
+        symbs = arg.free_symbols
+
+        if len(symbs) == 1:
+            z = symbs.pop()
+            c = Wild("c", exclude=[z])
+            d = Wild("d", exclude=[z])
+            m = Wild("m", exclude=[z])
+            n = Wild("n", exclude=[z])
+            M = arg.match(c*(d*z**n)**m)
+            if M is not None:
+                m = M[m]
+                # The transformation is in principle
+                # given by 03.08.16.0001.01 but note
+                # that there is an error in this formula.
+                # https://functions.wolfram.com/Bessel-TypeFunctions/AiryBiPrime/16/01/01/0001/
+                if (3*m).is_integer:
+                    c = M[c]
+                    d = M[d]
+                    n = M[n]
+                    pf = (d**m * z**(n*m)) / (d * z**n)**m
+                    newarg = c * d**m * z**(n*m)
+                    return S.Half * (sqrt(3)*(pf - S.One)*airyaiprime(newarg) + (pf + S.One)*airybiprime(newarg))
+
+
+class marcumq(Function):
+    r"""
+    The Marcum Q-function.
+
+    Explanation
+    ===========
+
+    The Marcum Q-function is defined by the meromorphic continuation of
+
+    .. math::
+        Q_m(a, b) = a^{- m + 1} \int_{b}^{\infty} x^{m} e^{- \frac{a^{2}}{2} - \frac{x^{2}}{2}} I_{m - 1}\left(a x\right)\, dx
+
+    Examples
+    ========
+
+    >>> from sympy import marcumq
+    >>> from sympy.abc import m, a, b
+    >>> marcumq(m, a, b)
+    marcumq(m, a, b)
+
+    Special values:
+
+    >>> marcumq(m, 0, b)
+    uppergamma(m, b**2/2)/gamma(m)
+    >>> marcumq(0, 0, 0)
+    0
+    >>> marcumq(0, a, 0)
+    1 - exp(-a**2/2)
+    >>> marcumq(1, a, a)
+    1/2 + exp(-a**2)*besseli(0, a**2)/2
+    >>> marcumq(2, a, a)
+    1/2 + exp(-a**2)*besseli(0, a**2)/2 + exp(-a**2)*besseli(1, a**2)
+
+    Differentiation with respect to $a$ and $b$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(marcumq(m, a, b), a)
+    a*(-marcumq(m, a, b) + marcumq(m + 1, a, b))
+    >>> diff(marcumq(m, a, b), b)
+    -a**(1 - m)*b**m*exp(-a**2/2 - b**2/2)*besseli(m - 1, a*b)
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Marcum_Q-function
+    .. [2] https://mathworld.wolfram.com/MarcumQ-Function.html
+
+    """
+
+    @classmethod
+    def eval(cls, m, a, b):
+        if a is S.Zero:
+            if m is S.Zero and b is S.Zero:
+                return S.Zero
+            return uppergamma(m, b**2 * S.Half) / gamma(m)
+
+        if m is S.Zero and b is S.Zero:
+            return 1 - 1 / exp(a**2 * S.Half)
+
+        if a == b:
+            if m is S.One:
+                return (1 + exp(-a**2) * besseli(0, a**2))*S.Half
+            if m == 2:
+                return S.Half + S.Half * exp(-a**2) * besseli(0, a**2) + exp(-a**2) * besseli(1, a**2)
+
+        if a.is_zero:
+            if m.is_zero and b.is_zero:
+                return S.Zero
+            return uppergamma(m, b**2*S.Half) / gamma(m)
+
+        if m.is_zero and b.is_zero:
+            return 1 - 1 / exp(a**2*S.Half)
+
+    def fdiff(self, argindex=2):
+        m, a, b = self.args
+        if argindex == 2:
+            return a * (-marcumq(m, a, b) + marcumq(1+m, a, b))
+        elif argindex == 3:
+            return (-b**m / a**(m-1)) * exp(-(a**2 + b**2)/2) * besseli(m-1, a*b)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_Integral(self, m, a, b, **kwargs):
+        from sympy.integrals.integrals import Integral
+        x = kwargs.get('x', Dummy('x'))
+        return a ** (1 - m) * \
+               Integral(x**m * exp(-(x**2 + a**2)/2) * besseli(m-1, a*x), [x, b, S.Infinity])
+
+    def _eval_rewrite_as_Sum(self, m, a, b, **kwargs):
+        from sympy.concrete.summations import Sum
+        k = kwargs.get('k', Dummy('k'))
+        return exp(-(a**2 + b**2) / 2) * Sum((a/b)**k * besseli(k, a*b), [k, 1-m, S.Infinity])
+
+    def _eval_rewrite_as_besseli(self, m, a, b, **kwargs):
+        if a == b:
+            if m == 1:
+                return (1 + exp(-a**2) * besseli(0, a**2)) / 2
+            if m.is_Integer and m >= 2:
+                s = sum([besseli(i, a**2) for i in range(1, m)])
+                return S.Half + exp(-a**2) * besseli(0, a**2) / 2 + exp(-a**2) * s
+
+    def _eval_is_zero(self):
+        if all(arg.is_zero for arg in self.args):
+            return True

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/beta_functions.py

@@ -0,0 +1,389 @@
+from sympy.core import S
+from sympy.core.function import Function, ArgumentIndexError
+from sympy.core.symbol import Dummy
+from sympy.functions.special.gamma_functions import gamma, digamma
+from sympy.functions.combinatorial.numbers import catalan
+from sympy.functions.elementary.complexes import conjugate
+
+# See mpmath #569 and SymPy #20569
+def betainc_mpmath_fix(a, b, x1, x2, reg=0):
+    from mpmath import betainc, mpf
+    if x1 == x2:
+        return mpf(0)
+    else:
+        return betainc(a, b, x1, x2, reg)
+
+###############################################################################
+############################ COMPLETE BETA  FUNCTION ##########################
+###############################################################################
+
+class beta(Function):
+    r"""
+    The beta integral is called the Eulerian integral of the first kind by
+    Legendre:
+
+    .. math::
+        \mathrm{B}(x,y)  \int^{1}_{0} t^{x-1} (1-t)^{y-1} \mathrm{d}t.
+
+    Explanation
+    ===========
+
+    The Beta function or Euler's first integral is closely associated
+    with the gamma function. The Beta function is often used in probability
+    theory and mathematical statistics. It satisfies properties like:
+
+    .. math::
+        \mathrm{B}(a,1) = \frac{1}{a} \\
+        \mathrm{B}(a,b) = \mathrm{B}(b,a)  \\
+        \mathrm{B}(a,b) = \frac{\Gamma(a) \Gamma(b)}{\Gamma(a+b)}
+
+    Therefore for integral values of $a$ and $b$:
+
+    .. math::
+        \mathrm{B} = \frac{(a-1)! (b-1)!}{(a+b-1)!}
+
+    A special case of the Beta function when `x = y` is the
+    Central Beta function. It satisfies properties like:
+
+    .. math::
+        \mathrm{B}(x) = 2^{1 - 2x}\mathrm{B}(x, \frac{1}{2})
+        \mathrm{B}(x) = 2^{1 - 2x} cos(\pi x) \mathrm{B}(\frac{1}{2} - x, x)
+        \mathrm{B}(x) = \int_{0}^{1} \frac{t^x}{(1 + t)^{2x}} dt
+        \mathrm{B}(x) = \frac{2}{x} \prod_{n = 1}^{\infty} \frac{n(n + 2x)}{(n + x)^2}
+
+    Examples
+    ========
+
+    >>> from sympy import I, pi
+    >>> from sympy.abc import x, y
+
+    The Beta function obeys the mirror symmetry:
+
+    >>> from sympy import beta, conjugate
+    >>> conjugate(beta(x, y))
+    beta(conjugate(x), conjugate(y))
+
+    Differentiation with respect to both $x$ and $y$ is supported:
+
+    >>> from sympy import beta, diff
+    >>> diff(beta(x, y), x)
+    (polygamma(0, x) - polygamma(0, x + y))*beta(x, y)
+
+    >>> diff(beta(x, y), y)
+    (polygamma(0, y) - polygamma(0, x + y))*beta(x, y)
+
+    >>> diff(beta(x), x)
+    2*(polygamma(0, x) - polygamma(0, 2*x))*beta(x, x)
+
+    We can numerically evaluate the Beta function to
+    arbitrary precision for any complex numbers x and y:
+
+    >>> from sympy import beta
+    >>> beta(pi).evalf(40)
+    0.02671848900111377452242355235388489324562
+
+    >>> beta(1 + I).evalf(20)
+    -0.2112723729365330143 - 0.7655283165378005676*I
+
+    See Also
+    ========
+
+    gamma: Gamma function.
+    uppergamma: Upper incomplete gamma function.
+    lowergamma: Lower incomplete gamma function.
+    polygamma: Polygamma function.
+    loggamma: Log Gamma function.
+    digamma: Digamma function.
+    trigamma: Trigamma function.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Beta_function
+    .. [2] https://mathworld.wolfram.com/BetaFunction.html
+    .. [3] https://dlmf.nist.gov/5.12
+
+    """
+    unbranched = True
+
+    def fdiff(self, argindex):
+        x, y = self.args
+        if argindex == 1:
+            # Diff wrt x
+            return beta(x, y)*(digamma(x) - digamma(x + y))
+        elif argindex == 2:
+            # Diff wrt y
+            return beta(x, y)*(digamma(y) - digamma(x + y))
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @classmethod
+    def eval(cls, x, y=None):
+        if y is None:
+            return beta(x, x)
+        if x.is_Number and y.is_Number:
+            return beta(x, y, evaluate=False).doit()
+
+    def doit(self, **hints):
+        x = xold = self.args[0]
+        # Deal with unevaluated single argument beta
+        single_argument = len(self.args) == 1
+        y = yold = self.args[0] if single_argument else self.args[1]
+        if hints.get('deep', True):
+            x = x.doit(**hints)
+            y = y.doit(**hints)
+        if y.is_zero or x.is_zero:
+            return S.ComplexInfinity
+        if y is S.One:
+            return 1/x
+        if x is S.One:
+            return 1/y
+        if y == x + 1:
+            return 1/(x*y*catalan(x))
+        s = x + y
+        if (s.is_integer and s.is_negative and x.is_integer is False and
+            y.is_integer is False):
+            return S.Zero
+        if x == xold and y == yold and not single_argument:
+            return self
+        return beta(x, y)
+
+    def _eval_expand_func(self, **hints):
+        x, y = self.args
+        return gamma(x)*gamma(y) / gamma(x + y)
+
+    def _eval_is_real(self):
+        return self.args[0].is_real and self.args[1].is_real
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate(), self.args[1].conjugate())
+
+    def _eval_rewrite_as_gamma(self, x, y, piecewise=True, **kwargs):
+        return self._eval_expand_func(**kwargs)
+
+    def _eval_rewrite_as_Integral(self, x, y, **kwargs):
+        from sympy.integrals.integrals import Integral
+        t = Dummy('t')
+        return Integral(t**(x - 1)*(1 - t)**(y - 1), (t, 0, 1))
+
+###############################################################################
+########################## INCOMPLETE BETA FUNCTION ###########################
+###############################################################################
+
+class betainc(Function):
+    r"""
+    The Generalized Incomplete Beta function is defined as
+
+    .. math::
+        \mathrm{B}_{(x_1, x_2)}(a, b) = \int_{x_1}^{x_2} t^{a - 1} (1 - t)^{b - 1} dt
+
+    The Incomplete Beta function is a special case
+    of the Generalized Incomplete Beta function :
+
+    .. math:: \mathrm{B}_z (a, b) = \mathrm{B}_{(0, z)}(a, b)
+
+    The Incomplete Beta function satisfies :
+
+    .. math:: \mathrm{B}_z (a, b) = (-1)^a \mathrm{B}_{\frac{z}{z - 1}} (a, 1 - a - b)
+
+    The Beta function is a special case of the Incomplete Beta function :
+
+    .. math:: \mathrm{B}(a, b) = \mathrm{B}_{1}(a, b)
+
+    Examples
+    ========
+
+    >>> from sympy import betainc, symbols, conjugate
+    >>> a, b, x, x1, x2 = symbols('a b x x1 x2')
+
+    The Generalized Incomplete Beta function is given by:
+
+    >>> betainc(a, b, x1, x2)
+    betainc(a, b, x1, x2)
+
+    The Incomplete Beta function can be obtained as follows:
+
+    >>> betainc(a, b, 0, x)
+    betainc(a, b, 0, x)
+
+    The Incomplete Beta function obeys the mirror symmetry:
+
+    >>> conjugate(betainc(a, b, x1, x2))
+    betainc(conjugate(a), conjugate(b), conjugate(x1), conjugate(x2))
+
+    We can numerically evaluate the Incomplete Beta function to
+    arbitrary precision for any complex numbers a, b, x1 and x2:
+
+    >>> from sympy import betainc, I
+    >>> betainc(2, 3, 4, 5).evalf(10)
+    56.08333333
+    >>> betainc(0.75, 1 - 4*I, 0, 2 + 3*I).evalf(25)
+    0.2241657956955709603655887 + 0.3619619242700451992411724*I
+
+    The Generalized Incomplete Beta function can be expressed
+    in terms of the Generalized Hypergeometric function.
+
+    >>> from sympy import hyper
+    >>> betainc(a, b, x1, x2).rewrite(hyper)
+    (-x1**a*hyper((a, 1 - b), (a + 1,), x1) + x2**a*hyper((a, 1 - b), (a + 1,), x2))/a
+
+    See Also
+    ========
+
+    beta: Beta function
+    hyper: Generalized Hypergeometric function
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Beta_function#Incomplete_beta_function
+    .. [2] https://dlmf.nist.gov/8.17
+    .. [3] https://functions.wolfram.com/GammaBetaErf/Beta4/
+    .. [4] https://functions.wolfram.com/GammaBetaErf/BetaRegularized4/02/
+
+    """
+    nargs = 4
+    unbranched = True
+
+    def fdiff(self, argindex):
+        a, b, x1, x2 = self.args
+        if argindex == 3:
+            # Diff wrt x1
+            return -(1 - x1)**(b - 1)*x1**(a - 1)
+        elif argindex == 4:
+            # Diff wrt x2
+            return (1 - x2)**(b - 1)*x2**(a - 1)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_mpmath(self):
+        return betainc_mpmath_fix, self.args
+
+    def _eval_is_real(self):
+        if all(arg.is_real for arg in self.args):
+            return True
+
+    def _eval_conjugate(self):
+        return self.func(*map(conjugate, self.args))
+
+    def _eval_rewrite_as_Integral(self, a, b, x1, x2, **kwargs):
+        from sympy.integrals.integrals import Integral
+        t = Dummy('t')
+        return Integral(t**(a - 1)*(1 - t)**(b - 1), (t, x1, x2))
+
+    def _eval_rewrite_as_hyper(self, a, b, x1, x2, **kwargs):
+        from sympy.functions.special.hyper import hyper
+        return (x2**a * hyper((a, 1 - b), (a + 1,), x2) - x1**a * hyper((a, 1 - b), (a + 1,), x1)) / a
+
+###############################################################################
+#################### REGULARIZED INCOMPLETE BETA FUNCTION #####################
+###############################################################################
+
+class betainc_regularized(Function):
+    r"""
+    The Generalized Regularized Incomplete Beta function is given by
+
+    .. math::
+        \mathrm{I}_{(x_1, x_2)}(a, b) = \frac{\mathrm{B}_{(x_1, x_2)}(a, b)}{\mathrm{B}(a, b)}
+
+    The Regularized Incomplete Beta function is a special case
+    of the Generalized Regularized Incomplete Beta function :
+
+    .. math:: \mathrm{I}_z (a, b) = \mathrm{I}_{(0, z)}(a, b)
+
+    The Regularized Incomplete Beta function is the cumulative distribution
+    function of the beta distribution.
+
+    Examples
+    ========
+
+    >>> from sympy import betainc_regularized, symbols, conjugate
+    >>> a, b, x, x1, x2 = symbols('a b x x1 x2')
+
+    The Generalized Regularized Incomplete Beta
+    function is given by:
+
+    >>> betainc_regularized(a, b, x1, x2)
+    betainc_regularized(a, b, x1, x2)
+
+    The Regularized Incomplete Beta function
+    can be obtained as follows:
+
+    >>> betainc_regularized(a, b, 0, x)
+    betainc_regularized(a, b, 0, x)
+
+    The Regularized Incomplete Beta function
+    obeys the mirror symmetry:
+
+    >>> conjugate(betainc_regularized(a, b, x1, x2))
+    betainc_regularized(conjugate(a), conjugate(b), conjugate(x1), conjugate(x2))
+
+    We can numerically evaluate the Regularized Incomplete Beta function
+    to arbitrary precision for any complex numbers a, b, x1 and x2:
+
+    >>> from sympy import betainc_regularized, pi, E
+    >>> betainc_regularized(1, 2, 0, 0.25).evalf(10)
+    0.4375000000
+    >>> betainc_regularized(pi, E, 0, 1).evalf(5)
+    1.00000
+
+    The Generalized Regularized Incomplete Beta function can be
+    expressed in terms of the Generalized Hypergeometric function.
+
+    >>> from sympy import hyper
+    >>> betainc_regularized(a, b, x1, x2).rewrite(hyper)
+    (-x1**a*hyper((a, 1 - b), (a + 1,), x1) + x2**a*hyper((a, 1 - b), (a + 1,), x2))/(a*beta(a, b))
+
+    See Also
+    ========
+
+    beta: Beta function
+    hyper: Generalized Hypergeometric function
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Beta_function#Incomplete_beta_function
+    .. [2] https://dlmf.nist.gov/8.17
+    .. [3] https://functions.wolfram.com/GammaBetaErf/Beta4/
+    .. [4] https://functions.wolfram.com/GammaBetaErf/BetaRegularized4/02/
+
+    """
+    nargs = 4
+    unbranched = True
+
+    def __new__(cls, a, b, x1, x2):
+        return Function.__new__(cls, a, b, x1, x2)
+
+    def _eval_mpmath(self):
+        return betainc_mpmath_fix, (*self.args, S(1))
+
+    def fdiff(self, argindex):
+        a, b, x1, x2 = self.args
+        if argindex == 3:
+            # Diff wrt x1
+            return -(1 - x1)**(b - 1)*x1**(a - 1) / beta(a, b)
+        elif argindex == 4:
+            # Diff wrt x2
+            return (1 - x2)**(b - 1)*x2**(a - 1) / beta(a, b)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_is_real(self):
+        if all(arg.is_real for arg in self.args):
+            return True
+
+    def _eval_conjugate(self):
+        return self.func(*map(conjugate, self.args))
+
+    def _eval_rewrite_as_Integral(self, a, b, x1, x2, **kwargs):
+        from sympy.integrals.integrals import Integral
+        t = Dummy('t')
+        integrand = t**(a - 1)*(1 - t)**(b - 1)
+        expr = Integral(integrand, (t, x1, x2))
+        return expr / Integral(integrand, (t, 0, 1))
+
+    def _eval_rewrite_as_hyper(self, a, b, x1, x2, **kwargs):
+        from sympy.functions.special.hyper import hyper
+        expr = (x2**a * hyper((a, 1 - b), (a + 1,), x2) - x1**a * hyper((a, 1 - b), (a + 1,), x1)) / a
+        return expr / beta(a, b)

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/bsplines.py

@@ -0,0 +1,351 @@
+from sympy.core import S, sympify
+from sympy.core.symbol import (Dummy, symbols)
+from sympy.functions import Piecewise, piecewise_fold
+from sympy.logic.boolalg import And
+from sympy.sets.sets import Interval
+
+from functools import lru_cache
+
+
+def _ivl(cond, x):
+    """return the interval corresponding to the condition
+
+    Conditions in spline's Piecewise give the range over
+    which an expression is valid like (lo <= x) & (x <= hi).
+    This function returns (lo, hi).
+    """
+    if isinstance(cond, And) and len(cond.args) == 2:
+        a, b = cond.args
+        if a.lts == x:
+            a, b = b, a
+        return a.lts, b.gts
+    raise TypeError('unexpected cond type: %s' % cond)
+
+
+def _add_splines(c, b1, d, b2, x):
+    """Construct c*b1 + d*b2."""
+
+    if S.Zero in (b1, c):
+        rv = piecewise_fold(d * b2)
+    elif S.Zero in (b2, d):
+        rv = piecewise_fold(c * b1)
+    else:
+        new_args = []
+        # Just combining the Piecewise without any fancy optimization
+        p1 = piecewise_fold(c * b1)
+        p2 = piecewise_fold(d * b2)
+
+        # Search all Piecewise arguments except (0, True)
+        p2args = list(p2.args[:-1])
+
+        # This merging algorithm assumes the conditions in
+        # p1 and p2 are sorted
+        for arg in p1.args[:-1]:
+            expr = arg.expr
+            cond = arg.cond
+
+            lower = _ivl(cond, x)[0]
+
+            # Check p2 for matching conditions that can be merged
+            for i, arg2 in enumerate(p2args):
+                expr2 = arg2.expr
+                cond2 = arg2.cond
+
+                lower_2, upper_2 = _ivl(cond2, x)
+                if cond2 == cond:
+                    # Conditions match, join expressions
+                    expr += expr2
+                    # Remove matching element
+                    del p2args[i]
+                    # No need to check the rest
+                    break
+                elif lower_2 < lower and upper_2 <= lower:
+                    # Check if arg2 condition smaller than arg1,
+                    # add to new_args by itself (no match expected
+                    # in p1)
+                    new_args.append(arg2)
+                    del p2args[i]
+                    break
+
+            # Checked all, add expr and cond
+            new_args.append((expr, cond))
+
+        # Add remaining items from p2args
+        new_args.extend(p2args)
+
+        # Add final (0, True)
+        new_args.append((0, True))
+
+        rv = Piecewise(*new_args, evaluate=False)
+
+    return rv.expand()
+
+
+@lru_cache(maxsize=128)
+def bspline_basis(d, knots, n, x):
+    """
+    The $n$-th B-spline at $x$ of degree $d$ with knots.
+
+    Explanation
+    ===========
+
+    B-Splines are piecewise polynomials of degree $d$. They are defined on a
+    set of knots, which is a sequence of integers or floats.
+
+    Examples
+    ========
+
+    The 0th degree splines have a value of 1 on a single interval:
+
+        >>> from sympy import bspline_basis
+        >>> from sympy.abc import x
+        >>> d = 0
+        >>> knots = tuple(range(5))
+        >>> bspline_basis(d, knots, 0, x)
+        Piecewise((1, (x >= 0) & (x <= 1)), (0, True))
+
+    For a given ``(d, knots)`` there are ``len(knots)-d-1`` B-splines
+    defined, that are indexed by ``n`` (starting at 0).
+
+    Here is an example of a cubic B-spline:
+
+        >>> bspline_basis(3, tuple(range(5)), 0, x)
+        Piecewise((x**3/6, (x >= 0) & (x <= 1)),
+                  (-x**3/2 + 2*x**2 - 2*x + 2/3,
+                  (x >= 1) & (x <= 2)),
+                  (x**3/2 - 4*x**2 + 10*x - 22/3,
+                  (x >= 2) & (x <= 3)),
+                  (-x**3/6 + 2*x**2 - 8*x + 32/3,
+                  (x >= 3) & (x <= 4)),
+                  (0, True))
+
+    By repeating knot points, you can introduce discontinuities in the
+    B-splines and their derivatives:
+
+        >>> d = 1
+        >>> knots = (0, 0, 2, 3, 4)
+        >>> bspline_basis(d, knots, 0, x)
+        Piecewise((1 - x/2, (x >= 0) & (x <= 2)), (0, True))
+
+    It is quite time consuming to construct and evaluate B-splines. If
+    you need to evaluate a B-spline many times, it is best to lambdify them
+    first:
+
+        >>> from sympy import lambdify
+        >>> d = 3
+        >>> knots = tuple(range(10))
+        >>> b0 = bspline_basis(d, knots, 0, x)
+        >>> f = lambdify(x, b0)
+        >>> y = f(0.5)
+
+    Parameters
+    ==========
+
+    d : integer
+        degree of bspline
+
+    knots : list of integer values
+        list of knots points of bspline
+
+    n : integer
+        $n$-th B-spline
+
+    x : symbol
+
+    See Also
+    ========
+
+    bspline_basis_set
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/B-spline
+
+    """
+    # make sure x has no assumptions so conditions don't evaluate
+    xvar = x
+    x = Dummy()
+
+    knots = tuple(sympify(k) for k in knots)
+    d = int(d)
+    n = int(n)
+    n_knots = len(knots)
+    n_intervals = n_knots - 1
+    if n + d + 1 > n_intervals:
+        raise ValueError("n + d + 1 must not exceed len(knots) - 1")
+    if d == 0:
+        result = Piecewise(
+            (S.One, Interval(knots[n], knots[n + 1]).contains(x)), (0, True)
+        )
+    elif d > 0:
+        denom = knots[n + d + 1] - knots[n + 1]
+        if denom != S.Zero:
+            B = (knots[n + d + 1] - x) / denom
+            b2 = bspline_basis(d - 1, knots, n + 1, x)
+        else:
+            b2 = B = S.Zero
+
+        denom = knots[n + d] - knots[n]
+        if denom != S.Zero:
+            A = (x - knots[n]) / denom
+            b1 = bspline_basis(d - 1, knots, n, x)
+        else:
+            b1 = A = S.Zero
+
+        result = _add_splines(A, b1, B, b2, x)
+    else:
+        raise ValueError("degree must be non-negative: %r" % n)
+
+    # return result with user-given x
+    return result.xreplace({x: xvar})
+
+
+def bspline_basis_set(d, knots, x):
+    """
+    Return the ``len(knots)-d-1`` B-splines at *x* of degree *d*
+    with *knots*.
+
+    Explanation
+    ===========
+
+    This function returns a list of piecewise polynomials that are the
+    ``len(knots)-d-1`` B-splines of degree *d* for the given knots.
+    This function calls ``bspline_basis(d, knots, n, x)`` for different
+    values of *n*.
+
+    Examples
+    ========
+
+    >>> from sympy import bspline_basis_set
+    >>> from sympy.abc import x
+    >>> d = 2
+    >>> knots = range(5)
+    >>> splines = bspline_basis_set(d, knots, x)
+    >>> splines
+    [Piecewise((x**2/2, (x >= 0) & (x <= 1)),
+               (-x**2 + 3*x - 3/2, (x >= 1) & (x <= 2)),
+               (x**2/2 - 3*x + 9/2, (x >= 2) & (x <= 3)),
+               (0, True)),
+    Piecewise((x**2/2 - x + 1/2, (x >= 1) & (x <= 2)),
+              (-x**2 + 5*x - 11/2, (x >= 2) & (x <= 3)),
+              (x**2/2 - 4*x + 8, (x >= 3) & (x <= 4)),
+              (0, True))]
+
+    Parameters
+    ==========
+
+    d : integer
+        degree of bspline
+
+    knots : list of integers
+        list of knots points of bspline
+
+    x : symbol
+
+    See Also
+    ========
+
+    bspline_basis
+
+    """
+    n_splines = len(knots) - d - 1
+    return [bspline_basis(d, tuple(knots), i, x) for i in range(n_splines)]
+
+
+def interpolating_spline(d, x, X, Y):
+    """
+    Return spline of degree *d*, passing through the given *X*
+    and *Y* values.
+
+    Explanation
+    ===========
+
+    This function returns a piecewise function such that each part is
+    a polynomial of degree not greater than *d*. The value of *d*
+    must be 1 or greater and the values of *X* must be strictly
+    increasing.
+
+    Examples
+    ========
+
+    >>> from sympy import interpolating_spline
+    >>> from sympy.abc import x
+    >>> interpolating_spline(1, x, [1, 2, 4, 7], [3, 6, 5, 7])
+    Piecewise((3*x, (x >= 1) & (x <= 2)),
+            (7 - x/2, (x >= 2) & (x <= 4)),
+            (2*x/3 + 7/3, (x >= 4) & (x <= 7)))
+    >>> interpolating_spline(3, x, [-2, 0, 1, 3, 4], [4, 2, 1, 1, 3])
+    Piecewise((7*x**3/117 + 7*x**2/117 - 131*x/117 + 2, (x >= -2) & (x <= 1)),
+            (10*x**3/117 - 2*x**2/117 - 122*x/117 + 77/39, (x >= 1) & (x <= 4)))
+
+    Parameters
+    ==========
+
+    d : integer
+        Degree of Bspline strictly greater than equal to one
+
+    x : symbol
+
+    X : list of strictly increasing real values
+        list of X coordinates through which the spline passes
+
+    Y : list of real values
+        list of corresponding Y coordinates through which the spline passes
+
+    See Also
+    ========
+
+    bspline_basis_set, interpolating_poly
+
+    """
+    from sympy.solvers.solveset import linsolve
+    from sympy.matrices.dense import Matrix
+
+    # Input sanitization
+    d = sympify(d)
+    if not (d.is_Integer and d.is_positive):
+        raise ValueError("Spline degree must be a positive integer, not %s." % d)
+    if len(X) != len(Y):
+        raise ValueError("Number of X and Y coordinates must be the same.")
+    if len(X) < d + 1:
+        raise ValueError("Degree must be less than the number of control points.")
+    if not all(a < b for a, b in zip(X, X[1:])):
+        raise ValueError("The x-coordinates must be strictly increasing.")
+    X = [sympify(i) for i in X]
+
+    # Evaluating knots value
+    if d.is_odd:
+        j = (d + 1) // 2
+        interior_knots = X[j:-j]
+    else:
+        j = d // 2
+        interior_knots = [
+            (a + b)/2 for a, b in zip(X[j : -j - 1], X[j + 1 : -j])
+        ]
+
+    knots = [X[0]] * (d + 1) + list(interior_knots) + [X[-1]] * (d + 1)
+
+    basis = bspline_basis_set(d, knots, x)
+
+    A = [[b.subs(x, v) for b in basis] for v in X]
+
+    coeff = linsolve((Matrix(A), Matrix(Y)), symbols("c0:{}".format(len(X)), cls=Dummy))
+    coeff = list(coeff)[0]
+    intervals = {c for b in basis for (e, c) in b.args if c != True}
+
+    # Sorting the intervals
+    #  ival contains the end-points of each interval
+    ival = [_ivl(c, x) for c in intervals]
+    com = zip(ival, intervals)
+    com = sorted(com, key=lambda x: x[0])
+    intervals = [y for x, y in com]
+
+    basis_dicts = [{c: e for (e, c) in b.args} for b in basis]
+    spline = []
+    for i in intervals:
+        piece = sum(
+            [c * d.get(i, S.Zero) for (c, d) in zip(coeff, basis_dicts)], S.Zero
+        )
+        spline.append((piece, i))
+    return Piecewise(*spline)

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/delta_functions.py

@@ -0,0 +1,664 @@
+from sympy.core import S, diff
+from sympy.core.function import Function, ArgumentIndexError
+from sympy.core.logic import fuzzy_not
+from sympy.core.relational import Eq, Ne
+from sympy.functions.elementary.complexes import im, sign
+from sympy.functions.elementary.piecewise import Piecewise
+from sympy.polys.polyerrors import PolynomialError
+from sympy.polys.polyroots import roots
+from sympy.utilities.misc import filldedent
+
+
+###############################################################################
+################################ DELTA FUNCTION ###############################
+###############################################################################
+
+
+class DiracDelta(Function):
+    r"""
+    The DiracDelta function and its derivatives.
+
+    Explanation
+    ===========
+
+    DiracDelta is not an ordinary function. It can be rigorously defined either
+    as a distribution or as a measure.
+
+    DiracDelta only makes sense in definite integrals, and in particular,
+    integrals of the form ``Integral(f(x)*DiracDelta(x - x0), (x, a, b))``,
+    where it equals ``f(x0)`` if ``a <= x0 <= b`` and ``0`` otherwise. Formally,
+    DiracDelta acts in some ways like a function that is ``0`` everywhere except
+    at ``0``, but in many ways it also does not. It can often be useful to treat
+    DiracDelta in formal ways, building up and manipulating expressions with
+    delta functions (which may eventually be integrated), but care must be taken
+    to not treat it as a real function. SymPy's ``oo`` is similar. It only
+    truly makes sense formally in certain contexts (such as integration limits),
+    but SymPy allows its use everywhere, and it tries to be consistent with
+    operations on it (like ``1/oo``), but it is easy to get into trouble and get
+    wrong results if ``oo`` is treated too much like a number. Similarly, if
+    DiracDelta is treated too much like a function, it is easy to get wrong or
+    nonsensical results.
+
+    DiracDelta function has the following properties:
+
+    1) $\frac{d}{d x} \theta(x) = \delta(x)$
+    2) $\int_{-\infty}^\infty \delta(x - a)f(x)\, dx = f(a)$ and $\int_{a-
+       \epsilon}^{a+\epsilon} \delta(x - a)f(x)\, dx = f(a)$
+    3) $\delta(x) = 0$ for all $x \neq 0$
+    4) $\delta(g(x)) = \sum_i \frac{\delta(x - x_i)}{\|g'(x_i)\|}$ where $x_i$
+       are the roots of $g$
+    5) $\delta(-x) = \delta(x)$
+
+    Derivatives of ``k``-th order of DiracDelta have the following properties:
+
+    6) $\delta(x, k) = 0$ for all $x \neq 0$
+    7) $\delta(-x, k) = -\delta(x, k)$ for odd $k$
+    8) $\delta(-x, k) = \delta(x, k)$ for even $k$
+
+    Examples
+    ========
+
+    >>> from sympy import DiracDelta, diff, pi
+    >>> from sympy.abc import x, y
+
+    >>> DiracDelta(x)
+    DiracDelta(x)
+    >>> DiracDelta(1)
+    0
+    >>> DiracDelta(-1)
+    0
+    >>> DiracDelta(pi)
+    0
+    >>> DiracDelta(x - 4).subs(x, 4)
+    DiracDelta(0)
+    >>> diff(DiracDelta(x))
+    DiracDelta(x, 1)
+    >>> diff(DiracDelta(x - 1), x, 2)
+    DiracDelta(x - 1, 2)
+    >>> diff(DiracDelta(x**2 - 1), x, 2)
+    2*(2*x**2*DiracDelta(x**2 - 1, 2) + DiracDelta(x**2 - 1, 1))
+    >>> DiracDelta(3*x).is_simple(x)
+    True
+    >>> DiracDelta(x**2).is_simple(x)
+    False
+    >>> DiracDelta((x**2 - 1)*y).expand(diracdelta=True, wrt=x)
+    DiracDelta(x - 1)/(2*Abs(y)) + DiracDelta(x + 1)/(2*Abs(y))
+
+    See Also
+    ========
+
+    Heaviside
+    sympy.simplify.simplify.simplify, is_simple
+    sympy.functions.special.tensor_functions.KroneckerDelta
+
+    References
+    ==========
+
+    .. [1] https://mathworld.wolfram.com/DeltaFunction.html
+
+    """
+
+    is_real = True
+
+    def fdiff(self, argindex=1):
+        """
+        Returns the first derivative of a DiracDelta Function.
+
+        Explanation
+        ===========
+
+        The difference between ``diff()`` and ``fdiff()`` is: ``diff()`` is the
+        user-level function and ``fdiff()`` is an object method. ``fdiff()`` is
+        a convenience method available in the ``Function`` class. It returns
+        the derivative of the function without considering the chain rule.
+        ``diff(function, x)`` calls ``Function._eval_derivative`` which in turn
+        calls ``fdiff()`` internally to compute the derivative of the function.
+
+        Examples
+        ========
+
+        >>> from sympy import DiracDelta, diff
+        >>> from sympy.abc import x
+
+        >>> DiracDelta(x).fdiff()
+        DiracDelta(x, 1)
+
+        >>> DiracDelta(x, 1).fdiff()
+        DiracDelta(x, 2)
+
+        >>> DiracDelta(x**2 - 1).fdiff()
+        DiracDelta(x**2 - 1, 1)
+
+        >>> diff(DiracDelta(x, 1)).fdiff()
+        DiracDelta(x, 3)
+
+        Parameters
+        ==========
+
+        argindex : integer
+            degree of derivative
+
+        """
+        if argindex == 1:
+            #I didn't know if there is a better way to handle default arguments
+            k = 0
+            if len(self.args) > 1:
+                k = self.args[1]
+            return self.func(self.args[0], k + 1)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @classmethod
+    def eval(cls, arg, k=S.Zero):
+        """
+        Returns a simplified form or a value of DiracDelta depending on the
+        argument passed by the DiracDelta object.
+
+        Explanation
+        ===========
+
+        The ``eval()`` method is automatically called when the ``DiracDelta``
+        class is about to be instantiated and it returns either some simplified
+        instance or the unevaluated instance depending on the argument passed.
+        In other words, ``eval()`` method is not needed to be called explicitly,
+        it is being called and evaluated once the object is called.
+
+        Examples
+        ========
+
+        >>> from sympy import DiracDelta, S
+        >>> from sympy.abc import x
+
+        >>> DiracDelta(x)
+        DiracDelta(x)
+
+        >>> DiracDelta(-x, 1)
+        -DiracDelta(x, 1)
+
+        >>> DiracDelta(1)
+        0
+
+        >>> DiracDelta(5, 1)
+        0
+
+        >>> DiracDelta(0)
+        DiracDelta(0)
+
+        >>> DiracDelta(-1)
+        0
+
+        >>> DiracDelta(S.NaN)
+        nan
+
+        >>> DiracDelta(x - 100).subs(x, 5)
+        0
+
+        >>> DiracDelta(x - 100).subs(x, 100)
+        DiracDelta(0)
+
+        Parameters
+        ==========
+
+        k : integer
+            order of derivative
+
+        arg : argument passed to DiracDelta
+
+        """
+        if not k.is_Integer or k.is_negative:
+            raise ValueError("Error: the second argument of DiracDelta must be \
+            a non-negative integer, %s given instead." % (k,))
+        if arg is S.NaN:
+            return S.NaN
+        if arg.is_nonzero:
+            return S.Zero
+        if fuzzy_not(im(arg).is_zero):
+            raise ValueError(filldedent('''
+                Function defined only for Real Values.
+                Complex part: %s  found in %s .''' % (
+                repr(im(arg)), repr(arg))))
+        c, nc = arg.args_cnc()
+        if c and c[0] is S.NegativeOne:
+            # keep this fast and simple instead of using
+            # could_extract_minus_sign
+            if k.is_odd:
+                return -cls(-arg, k)
+            elif k.is_even:
+                return cls(-arg, k) if k else cls(-arg)
+        elif k.is_zero:
+            return cls(arg, evaluate=False)
+
+    def _eval_expand_diracdelta(self, **hints):
+        """
+        Compute a simplified representation of the function using
+        property number 4. Pass ``wrt`` as a hint to expand the expression
+        with respect to a particular variable.
+
+        Explanation
+        ===========
+
+        ``wrt`` is:
+
+        - a variable with respect to which a DiracDelta expression will
+        get expanded.
+
+        Examples
+        ========
+
+        >>> from sympy import DiracDelta
+        >>> from sympy.abc import x, y
+
+        >>> DiracDelta(x*y).expand(diracdelta=True, wrt=x)
+        DiracDelta(x)/Abs(y)
+        >>> DiracDelta(x*y).expand(diracdelta=True, wrt=y)
+        DiracDelta(y)/Abs(x)
+
+        >>> DiracDelta(x**2 + x - 2).expand(diracdelta=True, wrt=x)
+        DiracDelta(x - 1)/3 + DiracDelta(x + 2)/3
+
+        See Also
+        ========
+
+        is_simple, Diracdelta
+
+        """
+        wrt = hints.get('wrt', None)
+        if wrt is None:
+            free = self.free_symbols
+            if len(free) == 1:
+                wrt = free.pop()
+            else:
+                raise TypeError(filldedent('''
+            When there is more than 1 free symbol or variable in the expression,
+            the 'wrt' keyword is required as a hint to expand when using the
+            DiracDelta hint.'''))
+
+        if not self.args[0].has(wrt) or (len(self.args) > 1 and self.args[1] != 0 ):
+            return self
+        try:
+            argroots = roots(self.args[0], wrt)
+            result = 0
+            valid = True
+            darg = abs(diff(self.args[0], wrt))
+            for r, m in argroots.items():
+                if r.is_real is not False and m == 1:
+                    result += self.func(wrt - r)/darg.subs(wrt, r)
+                else:
+                    # don't handle non-real and if m != 1 then
+                    # a polynomial will have a zero in the derivative (darg)
+                    # at r
+                    valid = False
+                    break
+            if valid:
+                return result
+        except PolynomialError:
+            pass
+        return self
+
+    def is_simple(self, x):
+        """
+        Tells whether the argument(args[0]) of DiracDelta is a linear
+        expression in *x*.
+
+        Examples
+        ========
+
+        >>> from sympy import DiracDelta, cos
+        >>> from sympy.abc import x, y
+
+        >>> DiracDelta(x*y).is_simple(x)
+        True
+        >>> DiracDelta(x*y).is_simple(y)
+        True
+
+        >>> DiracDelta(x**2 + x - 2).is_simple(x)
+        False
+
+        >>> DiracDelta(cos(x)).is_simple(x)
+        False
+
+        Parameters
+        ==========
+
+        x : can be a symbol
+
+        See Also
+        ========
+
+        sympy.simplify.simplify.simplify, DiracDelta
+
+        """
+        p = self.args[0].as_poly(x)
+        if p:
+            return p.degree() == 1
+        return False
+
+    def _eval_rewrite_as_Piecewise(self, *args, **kwargs):
+        """
+        Represents DiracDelta in a piecewise form.
+
+        Examples
+        ========
+
+        >>> from sympy import DiracDelta, Piecewise, Symbol
+        >>> x = Symbol('x')
+
+        >>> DiracDelta(x).rewrite(Piecewise)
+        Piecewise((DiracDelta(0), Eq(x, 0)), (0, True))
+
+        >>> DiracDelta(x - 5).rewrite(Piecewise)
+        Piecewise((DiracDelta(0), Eq(x, 5)), (0, True))
+
+        >>> DiracDelta(x**2 - 5).rewrite(Piecewise)
+           Piecewise((DiracDelta(0), Eq(x**2, 5)), (0, True))
+
+        >>> DiracDelta(x - 5, 4).rewrite(Piecewise)
+        DiracDelta(x - 5, 4)
+
+        """
+        if len(args) == 1:
+            return Piecewise((DiracDelta(0), Eq(args[0], 0)), (0, True))
+
+    def _eval_rewrite_as_SingularityFunction(self, *args, **kwargs):
+        """
+        Returns the DiracDelta expression written in the form of Singularity
+        Functions.
+
+        """
+        from sympy.solvers import solve
+        from sympy.functions.special.singularity_functions import SingularityFunction
+        if self == DiracDelta(0):
+            return SingularityFunction(0, 0, -1)
+        if self == DiracDelta(0, 1):
+            return SingularityFunction(0, 0, -2)
+        free = self.free_symbols
+        if len(free) == 1:
+            x = (free.pop())
+            if len(args) == 1:
+                return SingularityFunction(x, solve(args[0], x)[0], -1)
+            return SingularityFunction(x, solve(args[0], x)[0], -args[1] - 1)
+        else:
+            # I don't know how to handle the case for DiracDelta expressions
+            # having arguments with more than one variable.
+            raise TypeError(filldedent('''
+                rewrite(SingularityFunction) does not support
+                arguments with more that one variable.'''))
+
+
+###############################################################################
+############################## HEAVISIDE FUNCTION #############################
+###############################################################################
+
+
+class Heaviside(Function):
+    r"""
+    Heaviside step function.
+
+    Explanation
+    ===========
+
+    The Heaviside step function has the following properties:
+
+    1) $\frac{d}{d x} \theta(x) = \delta(x)$
+    2) $\theta(x) = \begin{cases} 0 & \text{for}\: x < 0 \\ \frac{1}{2} &
+       \text{for}\: x = 0 \\1 & \text{for}\: x > 0 \end{cases}$
+    3) $\frac{d}{d x} \max(x, 0) = \theta(x)$
+
+    Heaviside(x) is printed as $\theta(x)$ with the SymPy LaTeX printer.
+
+    The value at 0 is set differently in different fields. SymPy uses 1/2,
+    which is a convention from electronics and signal processing, and is
+    consistent with solving improper integrals by Fourier transform and
+    convolution.
+
+    To specify a different value of Heaviside at ``x=0``, a second argument
+    can be given. Using ``Heaviside(x, nan)`` gives an expression that will
+    evaluate to nan for x=0.
+
+    .. versionchanged:: 1.9 ``Heaviside(0)`` now returns 1/2 (before: undefined)
+
+    Examples
+    ========
+
+    >>> from sympy import Heaviside, nan
+    >>> from sympy.abc import x
+    >>> Heaviside(9)
+    1
+    >>> Heaviside(-9)
+    0
+    >>> Heaviside(0)
+    1/2
+    >>> Heaviside(0, nan)
+    nan
+    >>> (Heaviside(x) + 1).replace(Heaviside(x), Heaviside(x, 1))
+    Heaviside(x, 1) + 1
+
+    See Also
+    ========
+
+    DiracDelta
+
+    References
+    ==========
+
+    .. [1] https://mathworld.wolfram.com/HeavisideStepFunction.html
+    .. [2] https://dlmf.nist.gov/1.16#iv
+
+    """
+
+    is_real = True
+
+    def fdiff(self, argindex=1):
+        """
+        Returns the first derivative of a Heaviside Function.
+
+        Examples
+        ========
+
+        >>> from sympy import Heaviside, diff
+        >>> from sympy.abc import x
+
+        >>> Heaviside(x).fdiff()
+        DiracDelta(x)
+
+        >>> Heaviside(x**2 - 1).fdiff()
+        DiracDelta(x**2 - 1)
+
+        >>> diff(Heaviside(x)).fdiff()
+        DiracDelta(x, 1)
+
+        Parameters
+        ==========
+
+        argindex : integer
+            order of derivative
+
+        """
+        if argindex == 1:
+            return DiracDelta(self.args[0])
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def __new__(cls, arg, H0=S.Half, **options):
+        if isinstance(H0, Heaviside) and len(H0.args) == 1:
+            H0 = S.Half
+        return super(cls, cls).__new__(cls, arg, H0, **options)
+
+    @property
+    def pargs(self):
+        """Args without default S.Half"""
+        args = self.args
+        if args[1] is S.Half:
+            args = args[:1]
+        return args
+
+    @classmethod
+    def eval(cls, arg, H0=S.Half):
+        """
+        Returns a simplified form or a value of Heaviside depending on the
+        argument passed by the Heaviside object.
+
+        Explanation
+        ===========
+
+        The ``eval()`` method is automatically called when the ``Heaviside``
+        class is about to be instantiated and it returns either some simplified
+        instance or the unevaluated instance depending on the argument passed.
+        In other words, ``eval()`` method is not needed to be called explicitly,
+        it is being called and evaluated once the object is called.
+
+        Examples
+        ========
+
+        >>> from sympy import Heaviside, S
+        >>> from sympy.abc import x
+
+        >>> Heaviside(x)
+        Heaviside(x)
+
+        >>> Heaviside(19)
+        1
+
+        >>> Heaviside(0)
+        1/2
+
+        >>> Heaviside(0, 1)
+        1
+
+        >>> Heaviside(-5)
+        0
+
+        >>> Heaviside(S.NaN)
+        nan
+
+        >>> Heaviside(x - 100).subs(x, 5)
+        0
+
+        >>> Heaviside(x - 100).subs(x, 105)
+        1
+
+        Parameters
+        ==========
+
+        arg : argument passed by Heaviside object
+
+        H0 : value of Heaviside(0)
+
+        """
+        if arg.is_extended_negative:
+            return S.Zero
+        elif arg.is_extended_positive:
+            return S.One
+        elif arg.is_zero:
+            return H0
+        elif arg is S.NaN:
+            return S.NaN
+        elif fuzzy_not(im(arg).is_zero):
+            raise ValueError("Function defined only for Real Values. Complex part: %s  found in %s ." % (repr(im(arg)), repr(arg)) )
+
+    def _eval_rewrite_as_Piecewise(self, arg, H0=None, **kwargs):
+        """
+        Represents Heaviside in a Piecewise form.
+
+        Examples
+        ========
+
+        >>> from sympy import Heaviside, Piecewise, Symbol, nan
+        >>> x = Symbol('x')
+
+        >>> Heaviside(x).rewrite(Piecewise)
+        Piecewise((0, x < 0), (1/2, Eq(x, 0)), (1, True))
+
+        >>> Heaviside(x,nan).rewrite(Piecewise)
+        Piecewise((0, x < 0), (nan, Eq(x, 0)), (1, True))
+
+        >>> Heaviside(x - 5).rewrite(Piecewise)
+        Piecewise((0, x < 5), (1/2, Eq(x, 5)), (1, True))
+
+        >>> Heaviside(x**2 - 1).rewrite(Piecewise)
+        Piecewise((0, x**2 < 1), (1/2, Eq(x**2, 1)), (1, True))
+
+        """
+        if H0 == 0:
+            return Piecewise((0, arg <= 0), (1, True))
+        if H0 == 1:
+            return Piecewise((0, arg < 0), (1, True))
+        return Piecewise((0, arg < 0), (H0, Eq(arg, 0)), (1, True))
+
+    def _eval_rewrite_as_sign(self, arg, H0=S.Half, **kwargs):
+        """
+        Represents the Heaviside function in the form of sign function.
+
+        Explanation
+        ===========
+
+        The value of Heaviside(0) must be 1/2 for rewriting as sign to be
+        strictly equivalent. For easier usage, we also allow this rewriting
+        when Heaviside(0) is undefined.
+
+        Examples
+        ========
+
+        >>> from sympy import Heaviside, Symbol, sign, nan
+        >>> x = Symbol('x', real=True)
+        >>> y = Symbol('y')
+
+        >>> Heaviside(x).rewrite(sign)
+        sign(x)/2 + 1/2
+
+        >>> Heaviside(x, 0).rewrite(sign)
+        Piecewise((sign(x)/2 + 1/2, Ne(x, 0)), (0, True))
+
+        >>> Heaviside(x, nan).rewrite(sign)
+        Piecewise((sign(x)/2 + 1/2, Ne(x, 0)), (nan, True))
+
+        >>> Heaviside(x - 2).rewrite(sign)
+        sign(x - 2)/2 + 1/2
+
+        >>> Heaviside(x**2 - 2*x + 1).rewrite(sign)
+        sign(x**2 - 2*x + 1)/2 + 1/2
+
+        >>> Heaviside(y).rewrite(sign)
+        Heaviside(y)
+
+        >>> Heaviside(y**2 - 2*y + 1).rewrite(sign)
+        Heaviside(y**2 - 2*y + 1)
+
+        See Also
+        ========
+
+        sign
+
+        """
+        if arg.is_extended_real:
+            pw1 = Piecewise(
+                ((sign(arg) + 1)/2, Ne(arg, 0)),
+                (Heaviside(0, H0=H0), True))
+            pw2 = Piecewise(
+                ((sign(arg) + 1)/2, Eq(Heaviside(0, H0=H0), S.Half)),
+                (pw1, True))
+            return pw2
+
+    def _eval_rewrite_as_SingularityFunction(self, args, H0=S.Half, **kwargs):
+        """
+        Returns the Heaviside expression written in the form of Singularity
+        Functions.
+
+        """
+        from sympy.solvers import solve
+        from sympy.functions.special.singularity_functions import SingularityFunction
+        if self == Heaviside(0):
+            return SingularityFunction(0, 0, 0)
+        free = self.free_symbols
+        if len(free) == 1:
+            x = (free.pop())
+            return SingularityFunction(x, solve(args, x)[0], 0)
+            # TODO
+            # ((x - 5)**3*Heaviside(x - 5)).rewrite(SingularityFunction) should output
+            # SingularityFunction(x, 5, 0) instead of (x - 5)**3*SingularityFunction(x, 5, 0)
+        else:
+            # I don't know how to handle the case for Heaviside expressions
+            # having arguments with more than one variable.
+            raise TypeError(filldedent('''
+                rewrite(SingularityFunction) does not
+                support arguments with more that one variable.'''))

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/elliptic_integrals.py

@@ -0,0 +1,445 @@
+""" Elliptic Integrals. """
+
+from sympy.core import S, pi, I, Rational
+from sympy.core.function import Function, ArgumentIndexError
+from sympy.core.symbol import Dummy
+from sympy.functions.elementary.complexes import sign
+from sympy.functions.elementary.hyperbolic import atanh
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.elementary.trigonometric import sin, tan
+from sympy.functions.special.gamma_functions import gamma
+from sympy.functions.special.hyper import hyper, meijerg
+
+class elliptic_k(Function):
+    r"""
+    The complete elliptic integral of the first kind, defined by
+
+    .. math:: K(m) = F\left(\tfrac{\pi}{2}\middle| m\right)
+
+    where $F\left(z\middle| m\right)$ is the Legendre incomplete
+    elliptic integral of the first kind.
+
+    Explanation
+    ===========
+
+    The function $K(m)$ is a single-valued function on the complex
+    plane with branch cut along the interval $(1, \infty)$.
+
+    Note that our notation defines the incomplete elliptic integral
+    in terms of the parameter $m$ instead of the elliptic modulus
+    (eccentricity) $k$.
+    In this case, the parameter $m$ is defined as $m=k^2$.
+
+    Examples
+    ========
+
+    >>> from sympy import elliptic_k, I
+    >>> from sympy.abc import m
+    >>> elliptic_k(0)
+    pi/2
+    >>> elliptic_k(1.0 + I)
+    1.50923695405127 + 0.625146415202697*I
+    >>> elliptic_k(m).series(n=3)
+    pi/2 + pi*m/8 + 9*pi*m**2/128 + O(m**3)
+
+    See Also
+    ========
+
+    elliptic_f
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Elliptic_integrals
+    .. [2] https://functions.wolfram.com/EllipticIntegrals/EllipticK
+
+    """
+
+    @classmethod
+    def eval(cls, m):
+        if m.is_zero:
+            return pi*S.Half
+        elif m is S.Half:
+            return 8*pi**Rational(3, 2)/gamma(Rational(-1, 4))**2
+        elif m is S.One:
+            return S.ComplexInfinity
+        elif m is S.NegativeOne:
+            return gamma(Rational(1, 4))**2/(4*sqrt(2*pi))
+        elif m in (S.Infinity, S.NegativeInfinity, I*S.Infinity,
+                   I*S.NegativeInfinity, S.ComplexInfinity):
+            return S.Zero
+
+    def fdiff(self, argindex=1):
+        m = self.args[0]
+        return (elliptic_e(m) - (1 - m)*elliptic_k(m))/(2*m*(1 - m))
+
+    def _eval_conjugate(self):
+        m = self.args[0]
+        if (m.is_real and (m - 1).is_positive) is False:
+            return self.func(m.conjugate())
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        from sympy.simplify import hyperexpand
+        return hyperexpand(self.rewrite(hyper)._eval_nseries(x, n=n, logx=logx))
+
+    def _eval_rewrite_as_hyper(self, m, **kwargs):
+        return pi*S.Half*hyper((S.Half, S.Half), (S.One,), m)
+
+    def _eval_rewrite_as_meijerg(self, m, **kwargs):
+        return meijerg(((S.Half, S.Half), []), ((S.Zero,), (S.Zero,)), -m)/2
+
+    def _eval_is_zero(self):
+        m = self.args[0]
+        if m.is_infinite:
+            return True
+
+    def _eval_rewrite_as_Integral(self, *args):
+        from sympy.integrals.integrals import Integral
+        t = Dummy('t')
+        m = self.args[0]
+        return Integral(1/sqrt(1 - m*sin(t)**2), (t, 0, pi/2))
+
+
+class elliptic_f(Function):
+    r"""
+    The Legendre incomplete elliptic integral of the first
+    kind, defined by
+
+    .. math:: F\left(z\middle| m\right) =
+              \int_0^z \frac{dt}{\sqrt{1 - m \sin^2 t}}
+
+    Explanation
+    ===========
+
+    This function reduces to a complete elliptic integral of
+    the first kind, $K(m)$, when $z = \pi/2$.
+
+    Note that our notation defines the incomplete elliptic integral
+    in terms of the parameter $m$ instead of the elliptic modulus
+    (eccentricity) $k$.
+    In this case, the parameter $m$ is defined as $m=k^2$.
+
+    Examples
+    ========
+
+    >>> from sympy import elliptic_f, I
+    >>> from sympy.abc import z, m
+    >>> elliptic_f(z, m).series(z)
+    z + z**5*(3*m**2/40 - m/30) + m*z**3/6 + O(z**6)
+    >>> elliptic_f(3.0 + I/2, 1.0 + I)
+    2.909449841483 + 1.74720545502474*I
+
+    See Also
+    ========
+
+    elliptic_k
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Elliptic_integrals
+    .. [2] https://functions.wolfram.com/EllipticIntegrals/EllipticF
+
+    """
+
+    @classmethod
+    def eval(cls, z, m):
+        if z.is_zero:
+            return S.Zero
+        if m.is_zero:
+            return z
+        k = 2*z/pi
+        if k.is_integer:
+            return k*elliptic_k(m)
+        elif m in (S.Infinity, S.NegativeInfinity):
+            return S.Zero
+        elif z.could_extract_minus_sign():
+            return -elliptic_f(-z, m)
+
+    def fdiff(self, argindex=1):
+        z, m = self.args
+        fm = sqrt(1 - m*sin(z)**2)
+        if argindex == 1:
+            return 1/fm
+        elif argindex == 2:
+            return (elliptic_e(z, m)/(2*m*(1 - m)) - elliptic_f(z, m)/(2*m) -
+                    sin(2*z)/(4*(1 - m)*fm))
+        raise ArgumentIndexError(self, argindex)
+
+    def _eval_conjugate(self):
+        z, m = self.args
+        if (m.is_real and (m - 1).is_positive) is False:
+            return self.func(z.conjugate(), m.conjugate())
+
+    def _eval_rewrite_as_Integral(self, *args):
+        from sympy.integrals.integrals import Integral
+        t = Dummy('t')
+        z, m = self.args[0], self.args[1]
+        return Integral(1/(sqrt(1 - m*sin(t)**2)), (t, 0, z))
+
+    def _eval_is_zero(self):
+        z, m = self.args
+        if z.is_zero:
+            return True
+        if m.is_extended_real and m.is_infinite:
+            return True
+
+
+class elliptic_e(Function):
+    r"""
+    Called with two arguments $z$ and $m$, evaluates the
+    incomplete elliptic integral of the second kind, defined by
+
+    .. math:: E\left(z\middle| m\right) = \int_0^z \sqrt{1 - m \sin^2 t} dt
+
+    Called with a single argument $m$, evaluates the Legendre complete
+    elliptic integral of the second kind
+
+    .. math:: E(m) = E\left(\tfrac{\pi}{2}\middle| m\right)
+
+    Explanation
+    ===========
+
+    The function $E(m)$ is a single-valued function on the complex
+    plane with branch cut along the interval $(1, \infty)$.
+
+    Note that our notation defines the incomplete elliptic integral
+    in terms of the parameter $m$ instead of the elliptic modulus
+    (eccentricity) $k$.
+    In this case, the parameter $m$ is defined as $m=k^2$.
+
+    Examples
+    ========
+
+    >>> from sympy import elliptic_e, I
+    >>> from sympy.abc import z, m
+    >>> elliptic_e(z, m).series(z)
+    z + z**5*(-m**2/40 + m/30) - m*z**3/6 + O(z**6)
+    >>> elliptic_e(m).series(n=4)
+    pi/2 - pi*m/8 - 3*pi*m**2/128 - 5*pi*m**3/512 + O(m**4)
+    >>> elliptic_e(1 + I, 2 - I/2).n()
+    1.55203744279187 + 0.290764986058437*I
+    >>> elliptic_e(0)
+    pi/2
+    >>> elliptic_e(2.0 - I)
+    0.991052601328069 + 0.81879421395609*I
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Elliptic_integrals
+    .. [2] https://functions.wolfram.com/EllipticIntegrals/EllipticE2
+    .. [3] https://functions.wolfram.com/EllipticIntegrals/EllipticE
+
+    """
+
+    @classmethod
+    def eval(cls, m, z=None):
+        if z is not None:
+            z, m = m, z
+            k = 2*z/pi
+            if m.is_zero:
+                return z
+            if z.is_zero:
+                return S.Zero
+            elif k.is_integer:
+                return k*elliptic_e(m)
+            elif m in (S.Infinity, S.NegativeInfinity):
+                return S.ComplexInfinity
+            elif z.could_extract_minus_sign():
+                return -elliptic_e(-z, m)
+        else:
+            if m.is_zero:
+                return pi/2
+            elif m is S.One:
+                return S.One
+            elif m is S.Infinity:
+                return I*S.Infinity
+            elif m is S.NegativeInfinity:
+                return S.Infinity
+            elif m is S.ComplexInfinity:
+                return S.ComplexInfinity
+
+    def fdiff(self, argindex=1):
+        if len(self.args) == 2:
+            z, m = self.args
+            if argindex == 1:
+                return sqrt(1 - m*sin(z)**2)
+            elif argindex == 2:
+                return (elliptic_e(z, m) - elliptic_f(z, m))/(2*m)
+        else:
+            m = self.args[0]
+            if argindex == 1:
+                return (elliptic_e(m) - elliptic_k(m))/(2*m)
+        raise ArgumentIndexError(self, argindex)
+
+    def _eval_conjugate(self):
+        if len(self.args) == 2:
+            z, m = self.args
+            if (m.is_real and (m - 1).is_positive) is False:
+                return self.func(z.conjugate(), m.conjugate())
+        else:
+            m = self.args[0]
+            if (m.is_real and (m - 1).is_positive) is False:
+                return self.func(m.conjugate())
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        from sympy.simplify import hyperexpand
+        if len(self.args) == 1:
+            return hyperexpand(self.rewrite(hyper)._eval_nseries(x, n=n, logx=logx))
+        return super()._eval_nseries(x, n=n, logx=logx)
+
+    def _eval_rewrite_as_hyper(self, *args, **kwargs):
+        if len(args) == 1:
+            m = args[0]
+            return (pi/2)*hyper((Rational(-1, 2), S.Half), (S.One,), m)
+
+    def _eval_rewrite_as_meijerg(self, *args, **kwargs):
+        if len(args) == 1:
+            m = args[0]
+            return -meijerg(((S.Half, Rational(3, 2)), []), \
+                            ((S.Zero,), (S.Zero,)), -m)/4
+
+    def _eval_rewrite_as_Integral(self, *args):
+        from sympy.integrals.integrals import Integral
+        z, m = (pi/2, self.args[0]) if len(self.args) == 1 else self.args
+        t = Dummy('t')
+        return Integral(sqrt(1 - m*sin(t)**2), (t, 0, z))
+
+
+class elliptic_pi(Function):
+    r"""
+    Called with three arguments $n$, $z$ and $m$, evaluates the
+    Legendre incomplete elliptic integral of the third kind, defined by
+
+    .. math:: \Pi\left(n; z\middle| m\right) = \int_0^z \frac{dt}
+              {\left(1 - n \sin^2 t\right) \sqrt{1 - m \sin^2 t}}
+
+    Called with two arguments $n$ and $m$, evaluates the complete
+    elliptic integral of the third kind:
+
+    .. math:: \Pi\left(n\middle| m\right) =
+              \Pi\left(n; \tfrac{\pi}{2}\middle| m\right)
+
+    Explanation
+    ===========
+
+    Note that our notation defines the incomplete elliptic integral
+    in terms of the parameter $m$ instead of the elliptic modulus
+    (eccentricity) $k$.
+    In this case, the parameter $m$ is defined as $m=k^2$.
+
+    Examples
+    ========
+
+    >>> from sympy import elliptic_pi, I
+    >>> from sympy.abc import z, n, m
+    >>> elliptic_pi(n, z, m).series(z, n=4)
+    z + z**3*(m/6 + n/3) + O(z**4)
+    >>> elliptic_pi(0.5 + I, 1.0 - I, 1.2)
+    2.50232379629182 - 0.760939574180767*I
+    >>> elliptic_pi(0, 0)
+    pi/2
+    >>> elliptic_pi(1.0 - I/3, 2.0 + I)
+    3.29136443417283 + 0.32555634906645*I
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Elliptic_integrals
+    .. [2] https://functions.wolfram.com/EllipticIntegrals/EllipticPi3
+    .. [3] https://functions.wolfram.com/EllipticIntegrals/EllipticPi
+
+    """
+
+    @classmethod
+    def eval(cls, n, m, z=None):
+        if z is not None:
+            n, z, m = n, m, z
+            if n.is_zero:
+                return elliptic_f(z, m)
+            elif n is S.One:
+                return (elliptic_f(z, m) +
+                        (sqrt(1 - m*sin(z)**2)*tan(z) -
+                         elliptic_e(z, m))/(1 - m))
+            k = 2*z/pi
+            if k.is_integer:
+                return k*elliptic_pi(n, m)
+            elif m.is_zero:
+                return atanh(sqrt(n - 1)*tan(z))/sqrt(n - 1)
+            elif n == m:
+                return (elliptic_f(z, n) - elliptic_pi(1, z, n) +
+                        tan(z)/sqrt(1 - n*sin(z)**2))
+            elif n in (S.Infinity, S.NegativeInfinity):
+                return S.Zero
+            elif m in (S.Infinity, S.NegativeInfinity):
+                return S.Zero
+            elif z.could_extract_minus_sign():
+                return -elliptic_pi(n, -z, m)
+            if n.is_zero:
+                return elliptic_f(z, m)
+            if m.is_extended_real and m.is_infinite or \
+                    n.is_extended_real and n.is_infinite:
+                return S.Zero
+        else:
+            if n.is_zero:
+                return elliptic_k(m)
+            elif n is S.One:
+                return S.ComplexInfinity
+            elif m.is_zero:
+                return pi/(2*sqrt(1 - n))
+            elif m == S.One:
+                return S.NegativeInfinity/sign(n - 1)
+            elif n == m:
+                return elliptic_e(n)/(1 - n)
+            elif n in (S.Infinity, S.NegativeInfinity):
+                return S.Zero
+            elif m in (S.Infinity, S.NegativeInfinity):
+                return S.Zero
+            if n.is_zero:
+                return elliptic_k(m)
+            if m.is_extended_real and m.is_infinite or \
+                    n.is_extended_real and n.is_infinite:
+                return S.Zero
+
+    def _eval_conjugate(self):
+        if len(self.args) == 3:
+            n, z, m = self.args
+            if (n.is_real and (n - 1).is_positive) is False and \
+               (m.is_real and (m - 1).is_positive) is False:
+                return self.func(n.conjugate(), z.conjugate(), m.conjugate())
+        else:
+            n, m = self.args
+            return self.func(n.conjugate(), m.conjugate())
+
+    def fdiff(self, argindex=1):
+        if len(self.args) == 3:
+            n, z, m = self.args
+            fm, fn = sqrt(1 - m*sin(z)**2), 1 - n*sin(z)**2
+            if argindex == 1:
+                return (elliptic_e(z, m) + (m - n)*elliptic_f(z, m)/n +
+                        (n**2 - m)*elliptic_pi(n, z, m)/n -
+                        n*fm*sin(2*z)/(2*fn))/(2*(m - n)*(n - 1))
+            elif argindex == 2:
+                return 1/(fm*fn)
+            elif argindex == 3:
+                return (elliptic_e(z, m)/(m - 1) +
+                        elliptic_pi(n, z, m) -
+                        m*sin(2*z)/(2*(m - 1)*fm))/(2*(n - m))
+        else:
+            n, m = self.args
+            if argindex == 1:
+                return (elliptic_e(m) + (m - n)*elliptic_k(m)/n +
+                        (n**2 - m)*elliptic_pi(n, m)/n)/(2*(m - n)*(n - 1))
+            elif argindex == 2:
+                return (elliptic_e(m)/(m - 1) + elliptic_pi(n, m))/(2*(n - m))
+        raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_Integral(self, *args):
+        from sympy.integrals.integrals import Integral
+        if len(self.args) == 2:
+            n, m, z = self.args[0], self.args[1], pi/2
+        else:
+            n, z, m = self.args
+        t = Dummy('t')
+        return Integral(1/((1 - n*sin(t)**2)*sqrt(1 - m*sin(t)**2)), (t, 0, z))

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/error_functions.py

@@ -0,0 +1,2741 @@
+""" This module contains various functions that are special cases
+    of incomplete gamma functions. It should probably be renamed. """
+
+from sympy.core import EulerGamma  # Must be imported from core, not core.numbers
+from sympy.core.add import Add
+from sympy.core.cache import cacheit
+from sympy.core.function import Function, ArgumentIndexError, expand_mul
+from sympy.core.numbers import I, pi, Rational
+from sympy.core.relational import is_eq
+from sympy.core.power import Pow
+from sympy.core.singleton import S
+from sympy.core.symbol import Symbol
+from sympy.core.sympify import sympify
+from sympy.functions.combinatorial.factorials import factorial, factorial2, RisingFactorial
+from sympy.functions.elementary.complexes import  polar_lift, re, unpolarify
+from sympy.functions.elementary.integers import ceiling, floor
+from sympy.functions.elementary.miscellaneous import sqrt, root
+from sympy.functions.elementary.exponential import exp, log, exp_polar
+from sympy.functions.elementary.hyperbolic import cosh, sinh
+from sympy.functions.elementary.trigonometric import cos, sin, sinc
+from sympy.functions.special.hyper import hyper, meijerg
+
+# TODO series expansions
+# TODO see the "Note:" in Ei
+
+# Helper function
+def real_to_real_as_real_imag(self, deep=True, **hints):
+    if self.args[0].is_extended_real:
+        if deep:
+            hints['complex'] = False
+            return (self.expand(deep, **hints), S.Zero)
+        else:
+            return (self, S.Zero)
+    if deep:
+        x, y = self.args[0].expand(deep, **hints).as_real_imag()
+    else:
+        x, y = self.args[0].as_real_imag()
+    re = (self.func(x + I*y) + self.func(x - I*y))/2
+    im = (self.func(x + I*y) - self.func(x - I*y))/(2*I)
+    return (re, im)
+
+
+###############################################################################
+################################ ERROR FUNCTION ###############################
+###############################################################################
+
+
+class erf(Function):
+    r"""
+    The Gauss error function.
+
+    Explanation
+    ===========
+
+    This function is defined as:
+
+    .. math ::
+        \mathrm{erf}(x) = \frac{2}{\sqrt{\pi}} \int_0^x e^{-t^2} \mathrm{d}t.
+
+    Examples
+    ========
+
+    >>> from sympy import I, oo, erf
+    >>> from sympy.abc import z
+
+    Several special values are known:
+
+    >>> erf(0)
+    0
+    >>> erf(oo)
+    1
+    >>> erf(-oo)
+    -1
+    >>> erf(I*oo)
+    oo*I
+    >>> erf(-I*oo)
+    -oo*I
+
+    In general one can pull out factors of -1 and $I$ from the argument:
+
+    >>> erf(-z)
+    -erf(z)
+
+    The error function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(erf(z))
+    erf(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erf(z), z)
+    2*exp(-z**2)/sqrt(pi)
+
+    We can numerically evaluate the error function to arbitrary precision
+    on the whole complex plane:
+
+    >>> erf(4).evalf(30)
+    0.999999984582742099719981147840
+
+    >>> erf(-4*I).evalf(30)
+    -1296959.73071763923152794095062*I
+
+    See Also
+    ========
+
+    erfc: Complementary error function.
+    erfi: Imaginary error function.
+    erf2: Two-argument error function.
+    erfinv: Inverse error function.
+    erfcinv: Inverse Complementary error function.
+    erf2inv: Inverse two-argument error function.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Error_function
+    .. [2] https://dlmf.nist.gov/7
+    .. [3] https://mathworld.wolfram.com/Erf.html
+    .. [4] https://functions.wolfram.com/GammaBetaErf/Erf
+
+    """
+
+    unbranched = True
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return 2*exp(-self.args[0]**2)/sqrt(pi)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+
+    def inverse(self, argindex=1):
+        """
+        Returns the inverse of this function.
+
+        """
+        return erfinv
+
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_Number:
+            if arg is S.NaN:
+                return S.NaN
+            elif arg is S.Infinity:
+                return S.One
+            elif arg is S.NegativeInfinity:
+                return S.NegativeOne
+            elif arg.is_zero:
+                return S.Zero
+
+        if isinstance(arg, erfinv):
+             return arg.args[0]
+
+        if isinstance(arg, erfcinv):
+            return S.One - arg.args[0]
+
+        if arg.is_zero:
+            return S.Zero
+
+        # Only happens with unevaluated erf2inv
+        if isinstance(arg, erf2inv) and arg.args[0].is_zero:
+            return arg.args[1]
+
+        # Try to pull out factors of I
+        t = arg.extract_multiplicatively(I)
+        if t in (S.Infinity, S.NegativeInfinity):
+            return arg
+
+        # Try to pull out factors of -1
+        if arg.could_extract_minus_sign():
+            return -cls(-arg)
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n < 0 or n % 2 == 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            k = floor((n - 1)/S(2))
+            if len(previous_terms) > 2:
+                return -previous_terms[-2] * x**2 * (n - 2)/(n*k)
+            else:
+                return 2*S.NegativeOne**k * x**n/(n*factorial(k)*sqrt(pi))
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate())
+
+    def _eval_is_real(self):
+        return self.args[0].is_extended_real
+
+    def _eval_is_finite(self):
+        if self.args[0].is_finite:
+            return True
+        else:
+            return self.args[0].is_extended_real
+
+    def _eval_is_zero(self):
+        return self.args[0].is_zero
+
+    def _eval_rewrite_as_uppergamma(self, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return sqrt(z**2)/z*(S.One - uppergamma(S.Half, z**2)/sqrt(pi))
+
+    def _eval_rewrite_as_fresnels(self, z, **kwargs):
+        arg = (S.One - I)*z/sqrt(pi)
+        return (S.One + I)*(fresnelc(arg) - I*fresnels(arg))
+
+    def _eval_rewrite_as_fresnelc(self, z, **kwargs):
+        arg = (S.One - I)*z/sqrt(pi)
+        return (S.One + I)*(fresnelc(arg) - I*fresnels(arg))
+
+    def _eval_rewrite_as_meijerg(self, z, **kwargs):
+        return z/sqrt(pi)*meijerg([S.Half], [], [0], [Rational(-1, 2)], z**2)
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        return 2*z/sqrt(pi)*hyper([S.Half], [3*S.Half], -z**2)
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        return sqrt(z**2)/z - z*expint(S.Half, z**2)/sqrt(pi)
+
+    def _eval_rewrite_as_tractable(self, z, limitvar=None, **kwargs):
+        from sympy.series.limits import limit
+        if limitvar:
+            lim = limit(z, limitvar, S.Infinity)
+            if lim is S.NegativeInfinity:
+                return S.NegativeOne + _erfs(-z)*exp(-z**2)
+        return S.One - _erfs(z)*exp(-z**2)
+
+    def _eval_rewrite_as_erfc(self, z, **kwargs):
+        return S.One - erfc(z)
+
+    def _eval_rewrite_as_erfi(self, z, **kwargs):
+        return -I*erfi(I*z)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.ComplexInfinity:
+            arg0 = arg.limit(x, 0, dir='-' if cdir == -1 else '+')
+        if x in arg.free_symbols and arg0.is_zero:
+            return 2*arg/sqrt(pi)
+        else:
+            return self.func(arg0)
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        if point in [S.Infinity, S.NegativeInfinity]:
+            z = self.args[0]
+
+            try:
+                _, ex = z.leadterm(x)
+            except (ValueError, NotImplementedError):
+                return self
+
+            ex = -ex # as x->1/x for aseries
+            if ex.is_positive:
+                newn = ceiling(n/ex)
+                s = [S.NegativeOne**k * factorial2(2*k - 1) / (z**(2*k + 1) * 2**k)
+                     for k in range(newn)] + [Order(1/z**newn, x)]
+                return S.One - (exp(-z**2)/sqrt(pi)) * Add(*s)
+
+        return super(erf, self)._eval_aseries(n, args0, x, logx)
+
+    as_real_imag = real_to_real_as_real_imag
+
+
+class erfc(Function):
+    r"""
+    Complementary Error Function.
+
+    Explanation
+    ===========
+
+    The function is defined as:
+
+    .. math ::
+        \mathrm{erfc}(x) = \frac{2}{\sqrt{\pi}} \int_x^\infty e^{-t^2} \mathrm{d}t
+
+    Examples
+    ========
+
+    >>> from sympy import I, oo, erfc
+    >>> from sympy.abc import z
+
+    Several special values are known:
+
+    >>> erfc(0)
+    1
+    >>> erfc(oo)
+    0
+    >>> erfc(-oo)
+    2
+    >>> erfc(I*oo)
+    -oo*I
+    >>> erfc(-I*oo)
+    oo*I
+
+    The error function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(erfc(z))
+    erfc(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erfc(z), z)
+    -2*exp(-z**2)/sqrt(pi)
+
+    It also follows
+
+    >>> erfc(-z)
+    2 - erfc(z)
+
+    We can numerically evaluate the complementary error function to arbitrary
+    precision on the whole complex plane:
+
+    >>> erfc(4).evalf(30)
+    0.0000000154172579002800188521596734869
+
+    >>> erfc(4*I).evalf(30)
+    1.0 - 1296959.73071763923152794095062*I
+
+    See Also
+    ========
+
+    erf: Gaussian error function.
+    erfi: Imaginary error function.
+    erf2: Two-argument error function.
+    erfinv: Inverse error function.
+    erfcinv: Inverse Complementary error function.
+    erf2inv: Inverse two-argument error function.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Error_function
+    .. [2] https://dlmf.nist.gov/7
+    .. [3] https://mathworld.wolfram.com/Erfc.html
+    .. [4] https://functions.wolfram.com/GammaBetaErf/Erfc
+
+    """
+
+    unbranched = True
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return -2*exp(-self.args[0]**2)/sqrt(pi)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def inverse(self, argindex=1):
+        """
+        Returns the inverse of this function.
+
+        """
+        return erfcinv
+
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_Number:
+            if arg is S.NaN:
+                return S.NaN
+            elif arg is S.Infinity:
+                return S.Zero
+            elif arg.is_zero:
+                return S.One
+
+        if isinstance(arg, erfinv):
+            return S.One - arg.args[0]
+
+        if isinstance(arg, erfcinv):
+            return arg.args[0]
+
+        if arg.is_zero:
+            return S.One
+
+        # Try to pull out factors of I
+        t = arg.extract_multiplicatively(I)
+        if t in (S.Infinity, S.NegativeInfinity):
+            return -arg
+
+        # Try to pull out factors of -1
+        if arg.could_extract_minus_sign():
+            return 2 - cls(-arg)
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n == 0:
+            return S.One
+        elif n < 0 or n % 2 == 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            k = floor((n - 1)/S(2))
+            if len(previous_terms) > 2:
+                return -previous_terms[-2] * x**2 * (n - 2)/(n*k)
+            else:
+                return -2*S.NegativeOne**k * x**n/(n*factorial(k)*sqrt(pi))
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate())
+
+    def _eval_is_real(self):
+        return self.args[0].is_extended_real
+
+    def _eval_rewrite_as_tractable(self, z, limitvar=None, **kwargs):
+        return self.rewrite(erf).rewrite("tractable", deep=True, limitvar=limitvar)
+
+    def _eval_rewrite_as_erf(self, z, **kwargs):
+        return S.One - erf(z)
+
+    def _eval_rewrite_as_erfi(self, z, **kwargs):
+        return S.One + I*erfi(I*z)
+
+    def _eval_rewrite_as_fresnels(self, z, **kwargs):
+        arg = (S.One - I)*z/sqrt(pi)
+        return S.One - (S.One + I)*(fresnelc(arg) - I*fresnels(arg))
+
+    def _eval_rewrite_as_fresnelc(self, z, **kwargs):
+        arg = (S.One-I)*z/sqrt(pi)
+        return S.One - (S.One + I)*(fresnelc(arg) - I*fresnels(arg))
+
+    def _eval_rewrite_as_meijerg(self, z, **kwargs):
+        return S.One - z/sqrt(pi)*meijerg([S.Half], [], [0], [Rational(-1, 2)], z**2)
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        return S.One - 2*z/sqrt(pi)*hyper([S.Half], [3*S.Half], -z**2)
+
+    def _eval_rewrite_as_uppergamma(self, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return S.One - sqrt(z**2)/z*(S.One - uppergamma(S.Half, z**2)/sqrt(pi))
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        return S.One - sqrt(z**2)/z + z*expint(S.Half, z**2)/sqrt(pi)
+
+    def _eval_expand_func(self, **hints):
+        return self.rewrite(erf)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.ComplexInfinity:
+            arg0 = arg.limit(x, 0, dir='-' if cdir == -1 else '+')
+        if arg0.is_zero:
+            return S.One
+        else:
+            return self.func(arg0)
+
+    as_real_imag = real_to_real_as_real_imag
+
+    def _eval_aseries(self, n, args0, x, logx):
+        return S.One - erf(*self.args)._eval_aseries(n, args0, x, logx)
+
+
+class erfi(Function):
+    r"""
+    Imaginary error function.
+
+    Explanation
+    ===========
+
+    The function erfi is defined as:
+
+    .. math ::
+        \mathrm{erfi}(x) = \frac{2}{\sqrt{\pi}} \int_0^x e^{t^2} \mathrm{d}t
+
+    Examples
+    ========
+
+    >>> from sympy import I, oo, erfi
+    >>> from sympy.abc import z
+
+    Several special values are known:
+
+    >>> erfi(0)
+    0
+    >>> erfi(oo)
+    oo
+    >>> erfi(-oo)
+    -oo
+    >>> erfi(I*oo)
+    I
+    >>> erfi(-I*oo)
+    -I
+
+    In general one can pull out factors of -1 and $I$ from the argument:
+
+    >>> erfi(-z)
+    -erfi(z)
+
+    >>> from sympy import conjugate
+    >>> conjugate(erfi(z))
+    erfi(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erfi(z), z)
+    2*exp(z**2)/sqrt(pi)
+
+    We can numerically evaluate the imaginary error function to arbitrary
+    precision on the whole complex plane:
+
+    >>> erfi(2).evalf(30)
+    18.5648024145755525987042919132
+
+    >>> erfi(-2*I).evalf(30)
+    -0.995322265018952734162069256367*I
+
+    See Also
+    ========
+
+    erf: Gaussian error function.
+    erfc: Complementary error function.
+    erf2: Two-argument error function.
+    erfinv: Inverse error function.
+    erfcinv: Inverse Complementary error function.
+    erf2inv: Inverse two-argument error function.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Error_function
+    .. [2] https://mathworld.wolfram.com/Erfi.html
+    .. [3] https://functions.wolfram.com/GammaBetaErf/Erfi
+
+    """
+
+    unbranched = True
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return 2*exp(self.args[0]**2)/sqrt(pi)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @classmethod
+    def eval(cls, z):
+        if z.is_Number:
+            if z is S.NaN:
+                return S.NaN
+            elif z.is_zero:
+                return S.Zero
+            elif z is S.Infinity:
+                return S.Infinity
+
+        if z.is_zero:
+            return S.Zero
+
+        # Try to pull out factors of -1
+        if z.could_extract_minus_sign():
+            return -cls(-z)
+
+        # Try to pull out factors of I
+        nz = z.extract_multiplicatively(I)
+        if nz is not None:
+            if nz is S.Infinity:
+                return I
+            if isinstance(nz, erfinv):
+                return I*nz.args[0]
+            if isinstance(nz, erfcinv):
+                return I*(S.One - nz.args[0])
+            # Only happens with unevaluated erf2inv
+            if isinstance(nz, erf2inv) and nz.args[0].is_zero:
+                return I*nz.args[1]
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n < 0 or n % 2 == 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            k = floor((n - 1)/S(2))
+            if len(previous_terms) > 2:
+                return previous_terms[-2] * x**2 * (n - 2)/(n*k)
+            else:
+                return 2 * x**n/(n*factorial(k)*sqrt(pi))
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate())
+
+    def _eval_is_extended_real(self):
+        return self.args[0].is_extended_real
+
+    def _eval_is_zero(self):
+        return self.args[0].is_zero
+
+    def _eval_rewrite_as_tractable(self, z, limitvar=None, **kwargs):
+        return self.rewrite(erf).rewrite("tractable", deep=True, limitvar=limitvar)
+
+    def _eval_rewrite_as_erf(self, z, **kwargs):
+        return -I*erf(I*z)
+
+    def _eval_rewrite_as_erfc(self, z, **kwargs):
+        return I*erfc(I*z) - I
+
+    def _eval_rewrite_as_fresnels(self, z, **kwargs):
+        arg = (S.One + I)*z/sqrt(pi)
+        return (S.One - I)*(fresnelc(arg) - I*fresnels(arg))
+
+    def _eval_rewrite_as_fresnelc(self, z, **kwargs):
+        arg = (S.One + I)*z/sqrt(pi)
+        return (S.One - I)*(fresnelc(arg) - I*fresnels(arg))
+
+    def _eval_rewrite_as_meijerg(self, z, **kwargs):
+        return z/sqrt(pi)*meijerg([S.Half], [], [0], [Rational(-1, 2)], -z**2)
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        return 2*z/sqrt(pi)*hyper([S.Half], [3*S.Half], z**2)
+
+    def _eval_rewrite_as_uppergamma(self, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return sqrt(-z**2)/z*(uppergamma(S.Half, -z**2)/sqrt(pi) - S.One)
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        return sqrt(-z**2)/z - z*expint(S.Half, -z**2)/sqrt(pi)
+
+    def _eval_expand_func(self, **hints):
+        return self.rewrite(erf)
+
+    as_real_imag = real_to_real_as_real_imag
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if x in arg.free_symbols and arg0.is_zero:
+            return 2*arg/sqrt(pi)
+        elif arg0.is_finite:
+            return self.func(arg0)
+        return self.func(arg)
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        if point is S.Infinity:
+            z = self.args[0]
+            s = [factorial2(2*k - 1) / (2**k * z**(2*k + 1))
+                    for k in range(n)] + [Order(1/z**n, x)]
+            return -I + (exp(z**2)/sqrt(pi)) * Add(*s)
+
+        return super(erfi, self)._eval_aseries(n, args0, x, logx)
+
+
+class erf2(Function):
+    r"""
+    Two-argument error function.
+
+    Explanation
+    ===========
+
+    This function is defined as:
+
+    .. math ::
+        \mathrm{erf2}(x, y) = \frac{2}{\sqrt{\pi}} \int_x^y e^{-t^2} \mathrm{d}t
+
+    Examples
+    ========
+
+    >>> from sympy import oo, erf2
+    >>> from sympy.abc import x, y
+
+    Several special values are known:
+
+    >>> erf2(0, 0)
+    0
+    >>> erf2(x, x)
+    0
+    >>> erf2(x, oo)
+    1 - erf(x)
+    >>> erf2(x, -oo)
+    -erf(x) - 1
+    >>> erf2(oo, y)
+    erf(y) - 1
+    >>> erf2(-oo, y)
+    erf(y) + 1
+
+    In general one can pull out factors of -1:
+
+    >>> erf2(-x, -y)
+    -erf2(x, y)
+
+    The error function obeys the mirror symmetry:
+
+    >>> from sympy import conjugate
+    >>> conjugate(erf2(x, y))
+    erf2(conjugate(x), conjugate(y))
+
+    Differentiation with respect to $x$, $y$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erf2(x, y), x)
+    -2*exp(-x**2)/sqrt(pi)
+    >>> diff(erf2(x, y), y)
+    2*exp(-y**2)/sqrt(pi)
+
+    See Also
+    ========
+
+    erf: Gaussian error function.
+    erfc: Complementary error function.
+    erfi: Imaginary error function.
+    erfinv: Inverse error function.
+    erfcinv: Inverse Complementary error function.
+    erf2inv: Inverse two-argument error function.
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/GammaBetaErf/Erf2/
+
+    """
+
+
+    def fdiff(self, argindex):
+        x, y = self.args
+        if argindex == 1:
+            return -2*exp(-x**2)/sqrt(pi)
+        elif argindex == 2:
+            return 2*exp(-y**2)/sqrt(pi)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @classmethod
+    def eval(cls, x, y):
+        chk = (S.Infinity, S.NegativeInfinity, S.Zero)
+        if x is S.NaN or y is S.NaN:
+            return S.NaN
+        elif x == y:
+            return S.Zero
+        elif x in chk or y in chk:
+            return erf(y) - erf(x)
+
+        if isinstance(y, erf2inv) and y.args[0] == x:
+            return y.args[1]
+
+        if x.is_zero or y.is_zero or x.is_extended_real and x.is_infinite or \
+                y.is_extended_real and y.is_infinite:
+            return erf(y) - erf(x)
+
+        #Try to pull out -1 factor
+        sign_x = x.could_extract_minus_sign()
+        sign_y = y.could_extract_minus_sign()
+        if (sign_x and sign_y):
+            return -cls(-x, -y)
+        elif (sign_x or sign_y):
+            return erf(y)-erf(x)
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate(), self.args[1].conjugate())
+
+    def _eval_is_extended_real(self):
+        return self.args[0].is_extended_real and self.args[1].is_extended_real
+
+    def _eval_rewrite_as_erf(self, x, y, **kwargs):
+        return erf(y) - erf(x)
+
+    def _eval_rewrite_as_erfc(self, x, y, **kwargs):
+        return erfc(x) - erfc(y)
+
+    def _eval_rewrite_as_erfi(self, x, y, **kwargs):
+        return I*(erfi(I*x)-erfi(I*y))
+
+    def _eval_rewrite_as_fresnels(self, x, y, **kwargs):
+        return erf(y).rewrite(fresnels) - erf(x).rewrite(fresnels)
+
+    def _eval_rewrite_as_fresnelc(self, x, y, **kwargs):
+        return erf(y).rewrite(fresnelc) - erf(x).rewrite(fresnelc)
+
+    def _eval_rewrite_as_meijerg(self, x, y, **kwargs):
+        return erf(y).rewrite(meijerg) - erf(x).rewrite(meijerg)
+
+    def _eval_rewrite_as_hyper(self, x, y, **kwargs):
+        return erf(y).rewrite(hyper) - erf(x).rewrite(hyper)
+
+    def _eval_rewrite_as_uppergamma(self, x, y, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return (sqrt(y**2)/y*(S.One - uppergamma(S.Half, y**2)/sqrt(pi)) -
+            sqrt(x**2)/x*(S.One - uppergamma(S.Half, x**2)/sqrt(pi)))
+
+    def _eval_rewrite_as_expint(self, x, y, **kwargs):
+        return erf(y).rewrite(expint) - erf(x).rewrite(expint)
+
+    def _eval_expand_func(self, **hints):
+        return self.rewrite(erf)
+
+    def _eval_is_zero(self):
+        return is_eq(*self.args)
+
+class erfinv(Function):
+    r"""
+    Inverse Error Function. The erfinv function is defined as:
+
+    .. math ::
+        \mathrm{erf}(x) = y \quad \Rightarrow \quad \mathrm{erfinv}(y) = x
+
+    Examples
+    ========
+
+    >>> from sympy import erfinv
+    >>> from sympy.abc import x
+
+    Several special values are known:
+
+    >>> erfinv(0)
+    0
+    >>> erfinv(1)
+    oo
+
+    Differentiation with respect to $x$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erfinv(x), x)
+    sqrt(pi)*exp(erfinv(x)**2)/2
+
+    We can numerically evaluate the inverse error function to arbitrary
+    precision on [-1, 1]:
+
+    >>> erfinv(0.2).evalf(30)
+    0.179143454621291692285822705344
+
+    See Also
+    ========
+
+    erf: Gaussian error function.
+    erfc: Complementary error function.
+    erfi: Imaginary error function.
+    erf2: Two-argument error function.
+    erfcinv: Inverse Complementary error function.
+    erf2inv: Inverse two-argument error function.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Error_function#Inverse_functions
+    .. [2] https://functions.wolfram.com/GammaBetaErf/InverseErf/
+
+    """
+
+
+    def fdiff(self, argindex =1):
+        if argindex == 1:
+            return sqrt(pi)*exp(self.func(self.args[0])**2)*S.Half
+        else :
+            raise ArgumentIndexError(self, argindex)
+
+    def inverse(self, argindex=1):
+        """
+        Returns the inverse of this function.
+
+        """
+        return erf
+
+    @classmethod
+    def eval(cls, z):
+        if z is S.NaN:
+            return S.NaN
+        elif z is S.NegativeOne:
+            return S.NegativeInfinity
+        elif z.is_zero:
+            return S.Zero
+        elif z is S.One:
+            return S.Infinity
+
+        if isinstance(z, erf) and z.args[0].is_extended_real:
+            return z.args[0]
+
+        if z.is_zero:
+            return S.Zero
+
+        # Try to pull out factors of -1
+        nz = z.extract_multiplicatively(-1)
+        if nz is not None and (isinstance(nz, erf) and (nz.args[0]).is_extended_real):
+            return -nz.args[0]
+
+    def _eval_rewrite_as_erfcinv(self, z, **kwargs):
+       return erfcinv(1-z)
+
+    def _eval_is_zero(self):
+        return self.args[0].is_zero
+
+
+class erfcinv (Function):
+    r"""
+    Inverse Complementary Error Function. The erfcinv function is defined as:
+
+    .. math ::
+        \mathrm{erfc}(x) = y \quad \Rightarrow \quad \mathrm{erfcinv}(y) = x
+
+    Examples
+    ========
+
+    >>> from sympy import erfcinv
+    >>> from sympy.abc import x
+
+    Several special values are known:
+
+    >>> erfcinv(1)
+    0
+    >>> erfcinv(0)
+    oo
+
+    Differentiation with respect to $x$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erfcinv(x), x)
+    -sqrt(pi)*exp(erfcinv(x)**2)/2
+
+    See Also
+    ========
+
+    erf: Gaussian error function.
+    erfc: Complementary error function.
+    erfi: Imaginary error function.
+    erf2: Two-argument error function.
+    erfinv: Inverse error function.
+    erf2inv: Inverse two-argument error function.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Error_function#Inverse_functions
+    .. [2] https://functions.wolfram.com/GammaBetaErf/InverseErfc/
+
+    """
+
+
+    def fdiff(self, argindex =1):
+        if argindex == 1:
+            return -sqrt(pi)*exp(self.func(self.args[0])**2)*S.Half
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def inverse(self, argindex=1):
+        """
+        Returns the inverse of this function.
+
+        """
+        return erfc
+
+    @classmethod
+    def eval(cls, z):
+        if z is S.NaN:
+            return S.NaN
+        elif z.is_zero:
+            return S.Infinity
+        elif z is S.One:
+            return S.Zero
+        elif z == 2:
+            return S.NegativeInfinity
+
+        if z.is_zero:
+            return S.Infinity
+
+    def _eval_rewrite_as_erfinv(self, z, **kwargs):
+        return erfinv(1-z)
+
+    def _eval_is_zero(self):
+        return (self.args[0] - 1).is_zero
+
+    def _eval_is_infinite(self):
+        return self.args[0].is_zero
+
+
+class erf2inv(Function):
+    r"""
+    Two-argument Inverse error function. The erf2inv function is defined as:
+
+    .. math ::
+        \mathrm{erf2}(x, w) = y \quad \Rightarrow \quad \mathrm{erf2inv}(x, y) = w
+
+    Examples
+    ========
+
+    >>> from sympy import erf2inv, oo
+    >>> from sympy.abc import x, y
+
+    Several special values are known:
+
+    >>> erf2inv(0, 0)
+    0
+    >>> erf2inv(1, 0)
+    1
+    >>> erf2inv(0, 1)
+    oo
+    >>> erf2inv(0, y)
+    erfinv(y)
+    >>> erf2inv(oo, y)
+    erfcinv(-y)
+
+    Differentiation with respect to $x$ and $y$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(erf2inv(x, y), x)
+    exp(-x**2 + erf2inv(x, y)**2)
+    >>> diff(erf2inv(x, y), y)
+    sqrt(pi)*exp(erf2inv(x, y)**2)/2
+
+    See Also
+    ========
+
+    erf: Gaussian error function.
+    erfc: Complementary error function.
+    erfi: Imaginary error function.
+    erf2: Two-argument error function.
+    erfinv: Inverse error function.
+    erfcinv: Inverse complementary error function.
+
+    References
+    ==========
+
+    .. [1] https://functions.wolfram.com/GammaBetaErf/InverseErf2/
+
+    """
+
+
+    def fdiff(self, argindex):
+        x, y = self.args
+        if argindex == 1:
+            return exp(self.func(x,y)**2-x**2)
+        elif argindex == 2:
+            return sqrt(pi)*S.Half*exp(self.func(x,y)**2)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @classmethod
+    def eval(cls, x, y):
+        if x is S.NaN or y is S.NaN:
+            return S.NaN
+        elif x.is_zero and y.is_zero:
+            return S.Zero
+        elif x.is_zero and y is S.One:
+            return S.Infinity
+        elif x is S.One and y.is_zero:
+            return S.One
+        elif x.is_zero:
+            return erfinv(y)
+        elif x is S.Infinity:
+            return erfcinv(-y)
+        elif y.is_zero:
+            return x
+        elif y is S.Infinity:
+            return erfinv(x)
+
+        if x.is_zero:
+            if y.is_zero:
+                return S.Zero
+            else:
+                return erfinv(y)
+        if y.is_zero:
+            return x
+
+    def _eval_is_zero(self):
+        x, y = self.args
+        if x.is_zero and y.is_zero:
+            return True
+
+###############################################################################
+#################### EXPONENTIAL INTEGRALS ####################################
+###############################################################################
+
+class Ei(Function):
+    r"""
+    The classical exponential integral.
+
+    Explanation
+    ===========
+
+    For use in SymPy, this function is defined as
+
+    .. math:: \operatorname{Ei}(x) = \sum_{n=1}^\infty \frac{x^n}{n\, n!}
+                                     + \log(x) + \gamma,
+
+    where $\gamma$ is the Euler-Mascheroni constant.
+
+    If $x$ is a polar number, this defines an analytic function on the
+    Riemann surface of the logarithm. Otherwise this defines an analytic
+    function in the cut plane $\mathbb{C} \setminus (-\infty, 0]$.
+
+    **Background**
+
+    The name exponential integral comes from the following statement:
+
+    .. math:: \operatorname{Ei}(x) = \int_{-\infty}^x \frac{e^t}{t} \mathrm{d}t
+
+    If the integral is interpreted as a Cauchy principal value, this statement
+    holds for $x > 0$ and $\operatorname{Ei}(x)$ as defined above.
+
+    Examples
+    ========
+
+    >>> from sympy import Ei, polar_lift, exp_polar, I, pi
+    >>> from sympy.abc import x
+
+    >>> Ei(-1)
+    Ei(-1)
+
+    This yields a real value:
+
+    >>> Ei(-1).n(chop=True)
+    -0.219383934395520
+
+    On the other hand the analytic continuation is not real:
+
+    >>> Ei(polar_lift(-1)).n(chop=True)
+    -0.21938393439552 + 3.14159265358979*I
+
+    The exponential integral has a logarithmic branch point at the origin:
+
+    >>> Ei(x*exp_polar(2*I*pi))
+    Ei(x) + 2*I*pi
+
+    Differentiation is supported:
+
+    >>> Ei(x).diff(x)
+    exp(x)/x
+
+    The exponential integral is related to many other special functions.
+    For example:
+
+    >>> from sympy import expint, Shi
+    >>> Ei(x).rewrite(expint)
+    -expint(1, x*exp_polar(I*pi)) - I*pi
+    >>> Ei(x).rewrite(Shi)
+    Chi(x) + Shi(x)
+
+    See Also
+    ========
+
+    expint: Generalised exponential integral.
+    E1: Special case of the generalised exponential integral.
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+    uppergamma: Upper incomplete gamma function.
+
+    References
+    ==========
+
+    .. [1] https://dlmf.nist.gov/6.6
+    .. [2] https://en.wikipedia.org/wiki/Exponential_integral
+    .. [3] Abramowitz & Stegun, section 5: https://web.archive.org/web/20201128173312/http://people.math.sfu.ca/~cbm/aands/page_228.htm
+
+    """
+
+
+    @classmethod
+    def eval(cls, z):
+        if z.is_zero:
+            return S.NegativeInfinity
+        elif z is S.Infinity:
+            return S.Infinity
+        elif z is S.NegativeInfinity:
+            return S.Zero
+
+        if z.is_zero:
+            return S.NegativeInfinity
+
+        nz, n = z.extract_branch_factor()
+        if n:
+            return Ei(nz) + 2*I*pi*n
+
+    def fdiff(self, argindex=1):
+        arg = unpolarify(self.args[0])
+        if argindex == 1:
+            return exp(arg)/arg
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_evalf(self, prec):
+        if (self.args[0]/polar_lift(-1)).is_positive:
+            return Function._eval_evalf(self, prec) + (I*pi)._eval_evalf(prec)
+        return Function._eval_evalf(self, prec)
+
+    def _eval_rewrite_as_uppergamma(self, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        # XXX this does not currently work usefully because uppergamma
+        #     immediately turns into expint
+        return -uppergamma(0, polar_lift(-1)*z) - I*pi
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        return -expint(1, polar_lift(-1)*z) - I*pi
+
+    def _eval_rewrite_as_li(self, z, **kwargs):
+        if isinstance(z, log):
+            return li(z.args[0])
+        # TODO:
+        # Actually it only holds that:
+        #  Ei(z) = li(exp(z))
+        # for -pi < imag(z) <= pi
+        return li(exp(z))
+
+    def _eval_rewrite_as_Si(self, z, **kwargs):
+        if z.is_negative:
+            return Shi(z) + Chi(z) - I*pi
+        else:
+            return Shi(z) + Chi(z)
+    _eval_rewrite_as_Ci = _eval_rewrite_as_Si
+    _eval_rewrite_as_Chi = _eval_rewrite_as_Si
+    _eval_rewrite_as_Shi = _eval_rewrite_as_Si
+
+    def _eval_rewrite_as_tractable(self, z, limitvar=None, **kwargs):
+        return exp(z) * _eis(z)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        from sympy import re
+        x0 = self.args[0].limit(x, 0)
+        arg = self.args[0].as_leading_term(x, cdir=cdir)
+        cdir = arg.dir(x, cdir)
+        if x0.is_zero:
+            c, e = arg.as_coeff_exponent(x)
+            logx = log(x) if logx is None else logx
+            return log(c) + e*logx + EulerGamma - (
+                I*pi if re(cdir).is_negative else S.Zero)
+        return super()._eval_as_leading_term(x, logx=logx, cdir=cdir)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        x0 = self.args[0].limit(x, 0)
+        if x0.is_zero:
+            f = self._eval_rewrite_as_Si(*self.args)
+            return f._eval_nseries(x, n, logx)
+        return super()._eval_nseries(x, n, logx)
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        if point is S.Infinity:
+            z = self.args[0]
+            s = [factorial(k) / (z)**k for k in range(n)] + \
+                    [Order(1/z**n, x)]
+            return (exp(z)/z) * Add(*s)
+
+        return super(Ei, self)._eval_aseries(n, args0, x, logx)
+
+
+class expint(Function):
+    r"""
+    Generalized exponential integral.
+
+    Explanation
+    ===========
+
+    This function is defined as
+
+    .. math:: \operatorname{E}_\nu(z) = z^{\nu - 1} \Gamma(1 - \nu, z),
+
+    where $\Gamma(1 - \nu, z)$ is the upper incomplete gamma function
+    (``uppergamma``).
+
+    Hence for $z$ with positive real part we have
+
+    .. math:: \operatorname{E}_\nu(z)
+              =   \int_1^\infty \frac{e^{-zt}}{t^\nu} \mathrm{d}t,
+
+    which explains the name.
+
+    The representation as an incomplete gamma function provides an analytic
+    continuation for $\operatorname{E}_\nu(z)$. If $\nu$ is a
+    non-positive integer, the exponential integral is thus an unbranched
+    function of $z$, otherwise there is a branch point at the origin.
+    Refer to the incomplete gamma function documentation for details of the
+    branching behavior.
+
+    Examples
+    ========
+
+    >>> from sympy import expint, S
+    >>> from sympy.abc import nu, z
+
+    Differentiation is supported. Differentiation with respect to $z$ further
+    explains the name: for integral orders, the exponential integral is an
+    iterated integral of the exponential function.
+
+    >>> expint(nu, z).diff(z)
+    -expint(nu - 1, z)
+
+    Differentiation with respect to $\nu$ has no classical expression:
+
+    >>> expint(nu, z).diff(nu)
+    -z**(nu - 1)*meijerg(((), (1, 1)), ((0, 0, 1 - nu), ()), z)
+
+    At non-postive integer orders, the exponential integral reduces to the
+    exponential function:
+
+    >>> expint(0, z)
+    exp(-z)/z
+    >>> expint(-1, z)
+    exp(-z)/z + exp(-z)/z**2
+
+    At half-integers it reduces to error functions:
+
+    >>> expint(S(1)/2, z)
+    sqrt(pi)*erfc(sqrt(z))/sqrt(z)
+
+    At positive integer orders it can be rewritten in terms of exponentials
+    and ``expint(1, z)``. Use ``expand_func()`` to do this:
+
+    >>> from sympy import expand_func
+    >>> expand_func(expint(5, z))
+    z**4*expint(1, z)/24 + (-z**3 + z**2 - 2*z + 6)*exp(-z)/24
+
+    The generalised exponential integral is essentially equivalent to the
+    incomplete gamma function:
+
+    >>> from sympy import uppergamma
+    >>> expint(nu, z).rewrite(uppergamma)
+    z**(nu - 1)*uppergamma(1 - nu, z)
+
+    As such it is branched at the origin:
+
+    >>> from sympy import exp_polar, pi, I
+    >>> expint(4, z*exp_polar(2*pi*I))
+    I*pi*z**3/3 + expint(4, z)
+    >>> expint(nu, z*exp_polar(2*pi*I))
+    z**(nu - 1)*(exp(2*I*pi*nu) - 1)*gamma(1 - nu) + expint(nu, z)
+
+    See Also
+    ========
+
+    Ei: Another related function called exponential integral.
+    E1: The classical case, returns expint(1, z).
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+    uppergamma
+
+    References
+    ==========
+
+    .. [1] https://dlmf.nist.gov/8.19
+    .. [2] https://functions.wolfram.com/GammaBetaErf/ExpIntegralE/
+    .. [3] https://en.wikipedia.org/wiki/Exponential_integral
+
+    """
+
+
+    @classmethod
+    def eval(cls, nu, z):
+        from sympy.functions.special.gamma_functions import (gamma, uppergamma)
+        nu2 = unpolarify(nu)
+        if nu != nu2:
+            return expint(nu2, z)
+        if nu.is_Integer and nu <= 0 or (not nu.is_Integer and (2*nu).is_Integer):
+            return unpolarify(expand_mul(z**(nu - 1)*uppergamma(1 - nu, z)))
+
+        # Extract branching information. This can be deduced from what is
+        # explained in lowergamma.eval().
+        z, n = z.extract_branch_factor()
+        if n is S.Zero:
+            return
+        if nu.is_integer:
+            if not nu > 0:
+                return
+            return expint(nu, z) \
+                - 2*pi*I*n*S.NegativeOne**(nu - 1)/factorial(nu - 1)*unpolarify(z)**(nu - 1)
+        else:
+            return (exp(2*I*pi*nu*n) - 1)*z**(nu - 1)*gamma(1 - nu) + expint(nu, z)
+
+    def fdiff(self, argindex):
+        nu, z = self.args
+        if argindex == 1:
+            return -z**(nu - 1)*meijerg([], [1, 1], [0, 0, 1 - nu], [], z)
+        elif argindex == 2:
+            return -expint(nu - 1, z)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_uppergamma(self, nu, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return z**(nu - 1)*uppergamma(1 - nu, z)
+
+    def _eval_rewrite_as_Ei(self, nu, z, **kwargs):
+        if nu == 1:
+            return -Ei(z*exp_polar(-I*pi)) - I*pi
+        elif nu.is_Integer and nu > 1:
+            # DLMF, 8.19.7
+            x = -unpolarify(z)
+            return x**(nu - 1)/factorial(nu - 1)*E1(z).rewrite(Ei) + \
+                exp(x)/factorial(nu - 1) * \
+                Add(*[factorial(nu - k - 2)*x**k for k in range(nu - 1)])
+        else:
+            return self
+
+    def _eval_expand_func(self, **hints):
+        return self.rewrite(Ei).rewrite(expint, **hints)
+
+    def _eval_rewrite_as_Si(self, nu, z, **kwargs):
+        if nu != 1:
+            return self
+        return Shi(z) - Chi(z)
+    _eval_rewrite_as_Ci = _eval_rewrite_as_Si
+    _eval_rewrite_as_Chi = _eval_rewrite_as_Si
+    _eval_rewrite_as_Shi = _eval_rewrite_as_Si
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        if not self.args[0].has(x):
+            nu = self.args[0]
+            if nu == 1:
+                f = self._eval_rewrite_as_Si(*self.args)
+                return f._eval_nseries(x, n, logx)
+            elif nu.is_Integer and nu > 1:
+                f = self._eval_rewrite_as_Ei(*self.args)
+                return f._eval_nseries(x, n, logx)
+        return super()._eval_nseries(x, n, logx)
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[1]
+        nu = self.args[0]
+
+        if point is S.Infinity:
+            z = self.args[1]
+            s = [S.NegativeOne**k * RisingFactorial(nu, k) / z**k for k in range(n)] + [Order(1/z**n, x)]
+            return (exp(-z)/z) * Add(*s)
+
+        return super(expint, self)._eval_aseries(n, args0, x, logx)
+
+
+def E1(z):
+    """
+    Classical case of the generalized exponential integral.
+
+    Explanation
+    ===========
+
+    This is equivalent to ``expint(1, z)``.
+
+    Examples
+    ========
+
+    >>> from sympy import E1
+    >>> E1(0)
+    expint(1, 0)
+
+    >>> E1(5)
+    expint(1, 5)
+
+    See Also
+    ========
+
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+
+    """
+    return expint(1, z)
+
+
+class li(Function):
+    r"""
+    The classical logarithmic integral.
+
+    Explanation
+    ===========
+
+    For use in SymPy, this function is defined as
+
+    .. math:: \operatorname{li}(x) = \int_0^x \frac{1}{\log(t)} \mathrm{d}t \,.
+
+    Examples
+    ========
+
+    >>> from sympy import I, oo, li
+    >>> from sympy.abc import z
+
+    Several special values are known:
+
+    >>> li(0)
+    0
+    >>> li(1)
+    -oo
+    >>> li(oo)
+    oo
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(li(z), z)
+    1/log(z)
+
+    Defining the ``li`` function via an integral:
+    >>> from sympy import integrate
+    >>> integrate(li(z))
+    z*li(z) - Ei(2*log(z))
+
+    >>> integrate(li(z),z)
+    z*li(z) - Ei(2*log(z))
+
+
+    The logarithmic integral can also be defined in terms of ``Ei``:
+
+    >>> from sympy import Ei
+    >>> li(z).rewrite(Ei)
+    Ei(log(z))
+    >>> diff(li(z).rewrite(Ei), z)
+    1/log(z)
+
+    We can numerically evaluate the logarithmic integral to arbitrary precision
+    on the whole complex plane (except the singular points):
+
+    >>> li(2).evalf(30)
+    1.04516378011749278484458888919
+
+    >>> li(2*I).evalf(30)
+    1.0652795784357498247001125598 + 3.08346052231061726610939702133*I
+
+    We can even compute Soldner's constant by the help of mpmath:
+
+    >>> from mpmath import findroot
+    >>> findroot(li, 2)
+    1.45136923488338
+
+    Further transformations include rewriting ``li`` in terms of
+    the trigonometric integrals ``Si``, ``Ci``, ``Shi`` and ``Chi``:
+
+    >>> from sympy import Si, Ci, Shi, Chi
+    >>> li(z).rewrite(Si)
+    -log(I*log(z)) - log(1/log(z))/2 + log(log(z))/2 + Ci(I*log(z)) + Shi(log(z))
+    >>> li(z).rewrite(Ci)
+    -log(I*log(z)) - log(1/log(z))/2 + log(log(z))/2 + Ci(I*log(z)) + Shi(log(z))
+    >>> li(z).rewrite(Shi)
+    -log(1/log(z))/2 + log(log(z))/2 + Chi(log(z)) - Shi(log(z))
+    >>> li(z).rewrite(Chi)
+    -log(1/log(z))/2 + log(log(z))/2 + Chi(log(z)) - Shi(log(z))
+
+    See Also
+    ========
+
+    Li: Offset logarithmic integral.
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    E1: Special case of the generalised exponential integral.
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Logarithmic_integral
+    .. [2] https://mathworld.wolfram.com/LogarithmicIntegral.html
+    .. [3] https://dlmf.nist.gov/6
+    .. [4] https://mathworld.wolfram.com/SoldnersConstant.html
+
+    """
+
+
+    @classmethod
+    def eval(cls, z):
+        if z.is_zero:
+            return S.Zero
+        elif z is S.One:
+            return S.NegativeInfinity
+        elif z is S.Infinity:
+            return S.Infinity
+        if z.is_zero:
+            return S.Zero
+
+    def fdiff(self, argindex=1):
+        arg = self.args[0]
+        if argindex == 1:
+            return S.One / log(arg)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_conjugate(self):
+        z = self.args[0]
+        # Exclude values on the branch cut (-oo, 0)
+        if not z.is_extended_negative:
+            return self.func(z.conjugate())
+
+    def _eval_rewrite_as_Li(self, z, **kwargs):
+        return Li(z) + li(2)
+
+    def _eval_rewrite_as_Ei(self, z, **kwargs):
+        return Ei(log(z))
+
+    def _eval_rewrite_as_uppergamma(self, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return (-uppergamma(0, -log(z)) +
+                S.Half*(log(log(z)) - log(S.One/log(z))) - log(-log(z)))
+
+    def _eval_rewrite_as_Si(self, z, **kwargs):
+        return (Ci(I*log(z)) - I*Si(I*log(z)) -
+                S.Half*(log(S.One/log(z)) - log(log(z))) - log(I*log(z)))
+
+    _eval_rewrite_as_Ci = _eval_rewrite_as_Si
+
+    def _eval_rewrite_as_Shi(self, z, **kwargs):
+        return (Chi(log(z)) - Shi(log(z)) - S.Half*(log(S.One/log(z)) - log(log(z))))
+
+    _eval_rewrite_as_Chi = _eval_rewrite_as_Shi
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        return (log(z)*hyper((1, 1), (2, 2), log(z)) +
+                S.Half*(log(log(z)) - log(S.One/log(z))) + EulerGamma)
+
+    def _eval_rewrite_as_meijerg(self, z, **kwargs):
+        return (-log(-log(z)) - S.Half*(log(S.One/log(z)) - log(log(z)))
+                - meijerg(((), (1,)), ((0, 0), ()), -log(z)))
+
+    def _eval_rewrite_as_tractable(self, z, limitvar=None, **kwargs):
+        return z * _eis(log(z))
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        z = self.args[0]
+        s = [(log(z))**k / (factorial(k) * k) for k in range(1, n)]
+        return EulerGamma + log(log(z)) + Add(*s)
+
+    def _eval_is_zero(self):
+        z = self.args[0]
+        if z.is_zero:
+            return True
+
+class Li(Function):
+    r"""
+    The offset logarithmic integral.
+
+    Explanation
+    ===========
+
+    For use in SymPy, this function is defined as
+
+    .. math:: \operatorname{Li}(x) = \operatorname{li}(x) - \operatorname{li}(2)
+
+    Examples
+    ========
+
+    >>> from sympy import Li
+    >>> from sympy.abc import z
+
+    The following special value is known:
+
+    >>> Li(2)
+    0
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(Li(z), z)
+    1/log(z)
+
+    The shifted logarithmic integral can be written in terms of $li(z)$:
+
+    >>> from sympy import li
+    >>> Li(z).rewrite(li)
+    li(z) - li(2)
+
+    We can numerically evaluate the logarithmic integral to arbitrary precision
+    on the whole complex plane (except the singular points):
+
+    >>> Li(2).evalf(30)
+    0
+
+    >>> Li(4).evalf(30)
+    1.92242131492155809316615998938
+
+    See Also
+    ========
+
+    li: Logarithmic integral.
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    E1: Special case of the generalised exponential integral.
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Logarithmic_integral
+    .. [2] https://mathworld.wolfram.com/LogarithmicIntegral.html
+    .. [3] https://dlmf.nist.gov/6
+
+    """
+
+
+    @classmethod
+    def eval(cls, z):
+        if z is S.Infinity:
+            return S.Infinity
+        elif z == S(2):
+            return S.Zero
+
+    def fdiff(self, argindex=1):
+        arg = self.args[0]
+        if argindex == 1:
+            return S.One / log(arg)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_evalf(self, prec):
+        return self.rewrite(li).evalf(prec)
+
+    def _eval_rewrite_as_li(self, z, **kwargs):
+        return li(z) - li(2)
+
+    def _eval_rewrite_as_tractable(self, z, limitvar=None, **kwargs):
+        return self.rewrite(li).rewrite("tractable", deep=True)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        f = self._eval_rewrite_as_li(*self.args)
+        return f._eval_nseries(x, n, logx)
+
+###############################################################################
+#################### TRIGONOMETRIC INTEGRALS ##################################
+###############################################################################
+
+class TrigonometricIntegral(Function):
+    """ Base class for trigonometric integrals. """
+
+
+    @classmethod
+    def eval(cls, z):
+        if z is S.Zero:
+            return cls._atzero
+        elif z is S.Infinity:
+            return cls._atinf()
+        elif z is S.NegativeInfinity:
+            return cls._atneginf()
+
+        if z.is_zero:
+            return cls._atzero
+
+        nz = z.extract_multiplicatively(polar_lift(I))
+        if nz is None and cls._trigfunc(0) == 0:
+            nz = z.extract_multiplicatively(I)
+        if nz is not None:
+            return cls._Ifactor(nz, 1)
+        nz = z.extract_multiplicatively(polar_lift(-I))
+        if nz is not None:
+            return cls._Ifactor(nz, -1)
+
+        nz = z.extract_multiplicatively(polar_lift(-1))
+        if nz is None and cls._trigfunc(0) == 0:
+            nz = z.extract_multiplicatively(-1)
+        if nz is not None:
+            return cls._minusfactor(nz)
+
+        nz, n = z.extract_branch_factor()
+        if n == 0 and nz == z:
+            return
+        return 2*pi*I*n*cls._trigfunc(0) + cls(nz)
+
+    def fdiff(self, argindex=1):
+        arg = unpolarify(self.args[0])
+        if argindex == 1:
+            return self._trigfunc(arg)/arg
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_Ei(self, z, **kwargs):
+        return self._eval_rewrite_as_expint(z).rewrite(Ei)
+
+    def _eval_rewrite_as_uppergamma(self, z, **kwargs):
+        from sympy.functions.special.gamma_functions import uppergamma
+        return self._eval_rewrite_as_expint(z).rewrite(uppergamma)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        # NOTE this is fairly inefficient
+        n += 1
+        if self.args[0].subs(x, 0) != 0:
+            return super()._eval_nseries(x, n, logx)
+        baseseries = self._trigfunc(x)._eval_nseries(x, n, logx)
+        if self._trigfunc(0) != 0:
+            baseseries -= 1
+        baseseries = baseseries.replace(Pow, lambda t, n: t**n/n, simultaneous=False)
+        if self._trigfunc(0) != 0:
+            baseseries += EulerGamma + log(x)
+        return baseseries.subs(x, self.args[0])._eval_nseries(x, n, logx)
+
+
+class Si(TrigonometricIntegral):
+    r"""
+    Sine integral.
+
+    Explanation
+    ===========
+
+    This function is defined by
+
+    .. math:: \operatorname{Si}(z) = \int_0^z \frac{\sin{t}}{t} \mathrm{d}t.
+
+    It is an entire function.
+
+    Examples
+    ========
+
+    >>> from sympy import Si
+    >>> from sympy.abc import z
+
+    The sine integral is an antiderivative of $sin(z)/z$:
+
+    >>> Si(z).diff(z)
+    sin(z)/z
+
+    It is unbranched:
+
+    >>> from sympy import exp_polar, I, pi
+    >>> Si(z*exp_polar(2*I*pi))
+    Si(z)
+
+    Sine integral behaves much like ordinary sine under multiplication by ``I``:
+
+    >>> Si(I*z)
+    I*Shi(z)
+    >>> Si(-z)
+    -Si(z)
+
+    It can also be expressed in terms of exponential integrals, but beware
+    that the latter is branched:
+
+    >>> from sympy import expint
+    >>> Si(z).rewrite(expint)
+    -I*(-expint(1, z*exp_polar(-I*pi/2))/2 +
+         expint(1, z*exp_polar(I*pi/2))/2) + pi/2
+
+    It can be rewritten in the form of sinc function (by definition):
+
+    >>> from sympy import sinc
+    >>> Si(z).rewrite(sinc)
+    Integral(sinc(t), (t, 0, z))
+
+    See Also
+    ========
+
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    sinc: unnormalized sinc function
+    E1: Special case of the generalised exponential integral.
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Trigonometric_integral
+
+    """
+
+    _trigfunc = sin
+    _atzero = S.Zero
+
+    @classmethod
+    def _atinf(cls):
+        return pi*S.Half
+
+    @classmethod
+    def _atneginf(cls):
+        return -pi*S.Half
+
+    @classmethod
+    def _minusfactor(cls, z):
+        return -Si(z)
+
+    @classmethod
+    def _Ifactor(cls, z, sign):
+        return I*Shi(z)*sign
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        # XXX should we polarify z?
+        return pi/2 + (E1(polar_lift(I)*z) - E1(polar_lift(-I)*z))/2/I
+
+    def _eval_rewrite_as_sinc(self, z, **kwargs):
+        from sympy.integrals.integrals import Integral
+        t = Symbol('t', Dummy=True)
+        return Integral(sinc(t), (t, 0, z))
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        # Expansion at oo
+        if point is S.Infinity:
+            z = self.args[0]
+            p = [S.NegativeOne**k * factorial(2*k) / z**(2*k)
+                    for k in range(int((n - 1)/2))] + [Order(1/z**n, x)]
+            q = [S.NegativeOne**k * factorial(2*k + 1) / z**(2*k + 1)
+                    for k in range(int(n/2) - 1)] + [Order(1/z**n, x)]
+            return pi/2 - (cos(z)/z)*Add(*p) - (sin(z)/z)*Add(*q)
+
+        # All other points are not handled
+        return super(Si, self)._eval_aseries(n, args0, x, logx)
+
+    def _eval_is_zero(self):
+        z = self.args[0]
+        if z.is_zero:
+            return True
+
+
+class Ci(TrigonometricIntegral):
+    r"""
+    Cosine integral.
+
+    Explanation
+    ===========
+
+    This function is defined for positive $x$ by
+
+    .. math:: \operatorname{Ci}(x) = \gamma + \log{x}
+                         + \int_0^x \frac{\cos{t} - 1}{t} \mathrm{d}t
+           = -\int_x^\infty \frac{\cos{t}}{t} \mathrm{d}t,
+
+    where $\gamma$ is the Euler-Mascheroni constant.
+
+    We have
+
+    .. math:: \operatorname{Ci}(z) =
+        -\frac{\operatorname{E}_1\left(e^{i\pi/2} z\right)
+               + \operatorname{E}_1\left(e^{-i \pi/2} z\right)}{2}
+
+    which holds for all polar $z$ and thus provides an analytic
+    continuation to the Riemann surface of the logarithm.
+
+    The formula also holds as stated
+    for $z \in \mathbb{C}$ with $\Re(z) > 0$.
+    By lifting to the principal branch, we obtain an analytic function on the
+    cut complex plane.
+
+    Examples
+    ========
+
+    >>> from sympy import Ci
+    >>> from sympy.abc import z
+
+    The cosine integral is a primitive of $\cos(z)/z$:
+
+    >>> Ci(z).diff(z)
+    cos(z)/z
+
+    It has a logarithmic branch point at the origin:
+
+    >>> from sympy import exp_polar, I, pi
+    >>> Ci(z*exp_polar(2*I*pi))
+    Ci(z) + 2*I*pi
+
+    The cosine integral behaves somewhat like ordinary $\cos$ under
+    multiplication by $i$:
+
+    >>> from sympy import polar_lift
+    >>> Ci(polar_lift(I)*z)
+    Chi(z) + I*pi/2
+    >>> Ci(polar_lift(-1)*z)
+    Ci(z) + I*pi
+
+    It can also be expressed in terms of exponential integrals:
+
+    >>> from sympy import expint
+    >>> Ci(z).rewrite(expint)
+    -expint(1, z*exp_polar(-I*pi/2))/2 - expint(1, z*exp_polar(I*pi/2))/2
+
+    See Also
+    ========
+
+    Si: Sine integral.
+    Shi: Hyperbolic sine integral.
+    Chi: Hyperbolic cosine integral.
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    E1: Special case of the generalised exponential integral.
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Trigonometric_integral
+
+    """
+
+    _trigfunc = cos
+    _atzero = S.ComplexInfinity
+
+    @classmethod
+    def _atinf(cls):
+        return S.Zero
+
+    @classmethod
+    def _atneginf(cls):
+        return I*pi
+
+    @classmethod
+    def _minusfactor(cls, z):
+        return Ci(z) + I*pi
+
+    @classmethod
+    def _Ifactor(cls, z, sign):
+        return Chi(z) + I*pi/2*sign
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        return -(E1(polar_lift(I)*z) + E1(polar_lift(-I)*z))/2
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.NaN:
+            arg0 = arg.limit(x, 0, dir='-' if re(cdir).is_negative else '+')
+        if arg0.is_zero:
+            c, e = arg.as_coeff_exponent(x)
+            logx = log(x) if logx is None else logx
+            return log(c) + e*logx + EulerGamma
+        elif arg0.is_finite:
+            return self.func(arg0)
+        else:
+            return self
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        # Expansion at oo
+        if point is S.Infinity:
+            z = self.args[0]
+            p = [S.NegativeOne**k * factorial(2*k) / z**(2*k)
+                    for k in range(int((n - 1)/2))] + [Order(1/z**n, x)]
+            q = [S.NegativeOne**k * factorial(2*k + 1) / z**(2*k + 1)
+                    for k in range(int(n/2) - 1)] + [Order(1/z**n, x)]
+            return (sin(z)/z)*Add(*p) - (cos(z)/z)*Add(*q)
+
+        # All other points are not handled
+        return super(Ci, self)._eval_aseries(n, args0, x, logx)
+
+
+class Shi(TrigonometricIntegral):
+    r"""
+    Sinh integral.
+
+    Explanation
+    ===========
+
+    This function is defined by
+
+    .. math:: \operatorname{Shi}(z) = \int_0^z \frac{\sinh{t}}{t} \mathrm{d}t.
+
+    It is an entire function.
+
+    Examples
+    ========
+
+    >>> from sympy import Shi
+    >>> from sympy.abc import z
+
+    The Sinh integral is a primitive of $\sinh(z)/z$:
+
+    >>> Shi(z).diff(z)
+    sinh(z)/z
+
+    It is unbranched:
+
+    >>> from sympy import exp_polar, I, pi
+    >>> Shi(z*exp_polar(2*I*pi))
+    Shi(z)
+
+    The $\sinh$ integral behaves much like ordinary $\sinh$ under
+    multiplication by $i$:
+
+    >>> Shi(I*z)
+    I*Si(z)
+    >>> Shi(-z)
+    -Shi(z)
+
+    It can also be expressed in terms of exponential integrals, but beware
+    that the latter is branched:
+
+    >>> from sympy import expint
+    >>> Shi(z).rewrite(expint)
+    expint(1, z)/2 - expint(1, z*exp_polar(I*pi))/2 - I*pi/2
+
+    See Also
+    ========
+
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Chi: Hyperbolic cosine integral.
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    E1: Special case of the generalised exponential integral.
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Trigonometric_integral
+
+    """
+
+    _trigfunc = sinh
+    _atzero = S.Zero
+
+    @classmethod
+    def _atinf(cls):
+        return S.Infinity
+
+    @classmethod
+    def _atneginf(cls):
+        return S.NegativeInfinity
+
+    @classmethod
+    def _minusfactor(cls, z):
+        return -Shi(z)
+
+    @classmethod
+    def _Ifactor(cls, z, sign):
+        return I*Si(z)*sign
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        # XXX should we polarify z?
+        return (E1(z) - E1(exp_polar(I*pi)*z))/2 - I*pi/2
+
+    def _eval_is_zero(self):
+        z = self.args[0]
+        if z.is_zero:
+            return True
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[0].as_leading_term(x)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.NaN:
+            arg0 = arg.limit(x, 0, dir='-' if re(cdir).is_negative else '+')
+        if arg0.is_zero:
+            return arg
+        elif not arg0.is_infinite:
+            return self.func(arg0)
+        else:
+            return self
+
+
+class Chi(TrigonometricIntegral):
+    r"""
+    Cosh integral.
+
+    Explanation
+    ===========
+
+    This function is defined for positive $x$ by
+
+    .. math:: \operatorname{Chi}(x) = \gamma + \log{x}
+                         + \int_0^x \frac{\cosh{t} - 1}{t} \mathrm{d}t,
+
+    where $\gamma$ is the Euler-Mascheroni constant.
+
+    We have
+
+    .. math:: \operatorname{Chi}(z) = \operatorname{Ci}\left(e^{i \pi/2}z\right)
+                         - i\frac{\pi}{2},
+
+    which holds for all polar $z$ and thus provides an analytic
+    continuation to the Riemann surface of the logarithm.
+    By lifting to the principal branch we obtain an analytic function on the
+    cut complex plane.
+
+    Examples
+    ========
+
+    >>> from sympy import Chi
+    >>> from sympy.abc import z
+
+    The $\cosh$ integral is a primitive of $\cosh(z)/z$:
+
+    >>> Chi(z).diff(z)
+    cosh(z)/z
+
+    It has a logarithmic branch point at the origin:
+
+    >>> from sympy import exp_polar, I, pi
+    >>> Chi(z*exp_polar(2*I*pi))
+    Chi(z) + 2*I*pi
+
+    The $\cosh$ integral behaves somewhat like ordinary $\cosh$ under
+    multiplication by $i$:
+
+    >>> from sympy import polar_lift
+    >>> Chi(polar_lift(I)*z)
+    Ci(z) + I*pi/2
+    >>> Chi(polar_lift(-1)*z)
+    Chi(z) + I*pi
+
+    It can also be expressed in terms of exponential integrals:
+
+    >>> from sympy import expint
+    >>> Chi(z).rewrite(expint)
+    -expint(1, z)/2 - expint(1, z*exp_polar(I*pi))/2 - I*pi/2
+
+    See Also
+    ========
+
+    Si: Sine integral.
+    Ci: Cosine integral.
+    Shi: Hyperbolic sine integral.
+    Ei: Exponential integral.
+    expint: Generalised exponential integral.
+    E1: Special case of the generalised exponential integral.
+    li: Logarithmic integral.
+    Li: Offset logarithmic integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Trigonometric_integral
+
+    """
+
+    _trigfunc = cosh
+    _atzero = S.ComplexInfinity
+
+    @classmethod
+    def _atinf(cls):
+        return S.Infinity
+
+    @classmethod
+    def _atneginf(cls):
+        return S.Infinity
+
+    @classmethod
+    def _minusfactor(cls, z):
+        return Chi(z) + I*pi
+
+    @classmethod
+    def _Ifactor(cls, z, sign):
+        return Ci(z) + I*pi/2*sign
+
+    def _eval_rewrite_as_expint(self, z, **kwargs):
+        return -I*pi/2 - (E1(z) + E1(exp_polar(I*pi)*z))/2
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.NaN:
+            arg0 = arg.limit(x, 0, dir='-' if re(cdir).is_negative else '+')
+        if arg0.is_zero:
+            c, e = arg.as_coeff_exponent(x)
+            logx = log(x) if logx is None else logx
+            return log(c) + e*logx + EulerGamma
+        elif arg0.is_finite:
+            return self.func(arg0)
+        else:
+            return self
+
+
+###############################################################################
+#################### FRESNEL INTEGRALS ########################################
+###############################################################################
+
+class FresnelIntegral(Function):
+    """ Base class for the Fresnel integrals."""
+
+    unbranched = True
+
+    @classmethod
+    def eval(cls, z):
+        # Values at positive infinities signs
+        # if any were extracted automatically
+        if z is S.Infinity:
+            return S.Half
+
+        # Value at zero
+        if z.is_zero:
+            return S.Zero
+
+        # Try to pull out factors of -1 and I
+        prefact = S.One
+        newarg = z
+        changed = False
+
+        nz = newarg.extract_multiplicatively(-1)
+        if nz is not None:
+            prefact = -prefact
+            newarg = nz
+            changed = True
+
+        nz = newarg.extract_multiplicatively(I)
+        if nz is not None:
+            prefact = cls._sign*I*prefact
+            newarg = nz
+            changed = True
+
+        if changed:
+            return prefact*cls(newarg)
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            return self._trigfunc(S.Half*pi*self.args[0]**2)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_is_extended_real(self):
+        return self.args[0].is_extended_real
+
+    _eval_is_finite = _eval_is_extended_real
+
+    def _eval_is_zero(self):
+        return self.args[0].is_zero
+
+    def _eval_conjugate(self):
+        return self.func(self.args[0].conjugate())
+
+    as_real_imag = real_to_real_as_real_imag
+
+
+class fresnels(FresnelIntegral):
+    r"""
+    Fresnel integral S.
+
+    Explanation
+    ===========
+
+    This function is defined by
+
+    .. math:: \operatorname{S}(z) = \int_0^z \sin{\frac{\pi}{2} t^2} \mathrm{d}t.
+
+    It is an entire function.
+
+    Examples
+    ========
+
+    >>> from sympy import I, oo, fresnels
+    >>> from sympy.abc import z
+
+    Several special values are known:
+
+    >>> fresnels(0)
+    0
+    >>> fresnels(oo)
+    1/2
+    >>> fresnels(-oo)
+    -1/2
+    >>> fresnels(I*oo)
+    -I/2
+    >>> fresnels(-I*oo)
+    I/2
+
+    In general one can pull out factors of -1 and $i$ from the argument:
+
+    >>> fresnels(-z)
+    -fresnels(z)
+    >>> fresnels(I*z)
+    -I*fresnels(z)
+
+    The Fresnel S integral obeys the mirror symmetry
+    $\overline{S(z)} = S(\bar{z})$:
+
+    >>> from sympy import conjugate
+    >>> conjugate(fresnels(z))
+    fresnels(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(fresnels(z), z)
+    sin(pi*z**2/2)
+
+    Defining the Fresnel functions via an integral:
+
+    >>> from sympy import integrate, pi, sin, expand_func
+    >>> integrate(sin(pi*z**2/2), z)
+    3*fresnels(z)*gamma(3/4)/(4*gamma(7/4))
+    >>> expand_func(integrate(sin(pi*z**2/2), z))
+    fresnels(z)
+
+    We can numerically evaluate the Fresnel integral to arbitrary precision
+    on the whole complex plane:
+
+    >>> fresnels(2).evalf(30)
+    0.343415678363698242195300815958
+
+    >>> fresnels(-2*I).evalf(30)
+    0.343415678363698242195300815958*I
+
+    See Also
+    ========
+
+    fresnelc: Fresnel cosine integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Fresnel_integral
+    .. [2] https://dlmf.nist.gov/7
+    .. [3] https://mathworld.wolfram.com/FresnelIntegrals.html
+    .. [4] https://functions.wolfram.com/GammaBetaErf/FresnelS
+    .. [5] The converging factors for the fresnel integrals
+            by John W. Wrench Jr. and Vicki Alley
+
+    """
+    _trigfunc = sin
+    _sign = -S.One
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n < 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            if len(previous_terms) > 1:
+                p = previous_terms[-1]
+                return (-pi**2*x**4*(4*n - 1)/(8*n*(2*n + 1)*(4*n + 3))) * p
+            else:
+                return x**3 * (-x**4)**n * (S(2)**(-2*n - 1)*pi**(2*n + 1)) / ((4*n + 3)*factorial(2*n + 1))
+
+    def _eval_rewrite_as_erf(self, z, **kwargs):
+        return (S.One + I)/4 * (erf((S.One + I)/2*sqrt(pi)*z) - I*erf((S.One - I)/2*sqrt(pi)*z))
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        return pi*z**3/6 * hyper([Rational(3, 4)], [Rational(3, 2), Rational(7, 4)], -pi**2*z**4/16)
+
+    def _eval_rewrite_as_meijerg(self, z, **kwargs):
+        return (pi*z**Rational(9, 4) / (sqrt(2)*(z**2)**Rational(3, 4)*(-z)**Rational(3, 4))
+                * meijerg([], [1], [Rational(3, 4)], [Rational(1, 4), 0], -pi**2*z**4/16))
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        from sympy.series.order import Order
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.ComplexInfinity:
+            arg0 = arg.limit(x, 0, dir='-' if re(cdir).is_negative else '+')
+        if arg0.is_zero:
+            return pi*arg**3/6
+        elif arg0 in [S.Infinity, S.NegativeInfinity]:
+            s = 1 if arg0 is S.Infinity else -1
+            return s*S.Half + Order(x, x)
+        else:
+            return self.func(arg0)
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        # Expansion at oo and -oo
+        if point in [S.Infinity, -S.Infinity]:
+            z = self.args[0]
+
+            # expansion of S(x) = S1(x*sqrt(pi/2)), see reference[5] page 1-8
+            # as only real infinities are dealt with, sin and cos are O(1)
+            p = [S.NegativeOne**k * factorial(4*k + 1) /
+                 (2**(2*k + 2) * z**(4*k + 3) * 2**(2*k)*factorial(2*k))
+                 for k in range(0, n) if 4*k + 3 < n]
+            q = [1/(2*z)] + [S.NegativeOne**k * factorial(4*k - 1) /
+                 (2**(2*k + 1) * z**(4*k + 1) * 2**(2*k - 1)*factorial(2*k - 1))
+                 for k in range(1, n) if 4*k + 1 < n]
+
+            p = [-sqrt(2/pi)*t for t in p]
+            q = [-sqrt(2/pi)*t for t in q]
+            s = 1 if point is S.Infinity else -1
+            # The expansion at oo is 1/2 + some odd powers of z
+            # To get the expansion at -oo, replace z by -z and flip the sign
+            # The result -1/2 + the same odd powers of z as before.
+            return s*S.Half + (sin(z**2)*Add(*p) + cos(z**2)*Add(*q)
+                ).subs(x, sqrt(2/pi)*x) + Order(1/z**n, x)
+
+        # All other points are not handled
+        return super()._eval_aseries(n, args0, x, logx)
+
+
+class fresnelc(FresnelIntegral):
+    r"""
+    Fresnel integral C.
+
+    Explanation
+    ===========
+
+    This function is defined by
+
+    .. math:: \operatorname{C}(z) = \int_0^z \cos{\frac{\pi}{2} t^2} \mathrm{d}t.
+
+    It is an entire function.
+
+    Examples
+    ========
+
+    >>> from sympy import I, oo, fresnelc
+    >>> from sympy.abc import z
+
+    Several special values are known:
+
+    >>> fresnelc(0)
+    0
+    >>> fresnelc(oo)
+    1/2
+    >>> fresnelc(-oo)
+    -1/2
+    >>> fresnelc(I*oo)
+    I/2
+    >>> fresnelc(-I*oo)
+    -I/2
+
+    In general one can pull out factors of -1 and $i$ from the argument:
+
+    >>> fresnelc(-z)
+    -fresnelc(z)
+    >>> fresnelc(I*z)
+    I*fresnelc(z)
+
+    The Fresnel C integral obeys the mirror symmetry
+    $\overline{C(z)} = C(\bar{z})$:
+
+    >>> from sympy import conjugate
+    >>> conjugate(fresnelc(z))
+    fresnelc(conjugate(z))
+
+    Differentiation with respect to $z$ is supported:
+
+    >>> from sympy import diff
+    >>> diff(fresnelc(z), z)
+    cos(pi*z**2/2)
+
+    Defining the Fresnel functions via an integral:
+
+    >>> from sympy import integrate, pi, cos, expand_func
+    >>> integrate(cos(pi*z**2/2), z)
+    fresnelc(z)*gamma(1/4)/(4*gamma(5/4))
+    >>> expand_func(integrate(cos(pi*z**2/2), z))
+    fresnelc(z)
+
+    We can numerically evaluate the Fresnel integral to arbitrary precision
+    on the whole complex plane:
+
+    >>> fresnelc(2).evalf(30)
+    0.488253406075340754500223503357
+
+    >>> fresnelc(-2*I).evalf(30)
+    -0.488253406075340754500223503357*I
+
+    See Also
+    ========
+
+    fresnels: Fresnel sine integral.
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Fresnel_integral
+    .. [2] https://dlmf.nist.gov/7
+    .. [3] https://mathworld.wolfram.com/FresnelIntegrals.html
+    .. [4] https://functions.wolfram.com/GammaBetaErf/FresnelC
+    .. [5] The converging factors for the fresnel integrals
+            by John W. Wrench Jr. and Vicki Alley
+
+    """
+    _trigfunc = cos
+    _sign = S.One
+
+    @staticmethod
+    @cacheit
+    def taylor_term(n, x, *previous_terms):
+        if n < 0:
+            return S.Zero
+        else:
+            x = sympify(x)
+            if len(previous_terms) > 1:
+                p = previous_terms[-1]
+                return (-pi**2*x**4*(4*n - 3)/(8*n*(2*n - 1)*(4*n + 1))) * p
+            else:
+                return x * (-x**4)**n * (S(2)**(-2*n)*pi**(2*n)) / ((4*n + 1)*factorial(2*n))
+
+    def _eval_rewrite_as_erf(self, z, **kwargs):
+        return (S.One - I)/4 * (erf((S.One + I)/2*sqrt(pi)*z) + I*erf((S.One - I)/2*sqrt(pi)*z))
+
+    def _eval_rewrite_as_hyper(self, z, **kwargs):
+        return z * hyper([Rational(1, 4)], [S.Half, Rational(5, 4)], -pi**2*z**4/16)
+
+    def _eval_rewrite_as_meijerg(self, z, **kwargs):
+        return (pi*z**Rational(3, 4) / (sqrt(2)*root(z**2, 4)*root(-z, 4))
+                * meijerg([], [1], [Rational(1, 4)], [Rational(3, 4), 0], -pi**2*z**4/16))
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        from sympy.series.order import Order
+        arg = self.args[0].as_leading_term(x, logx=logx, cdir=cdir)
+        arg0 = arg.subs(x, 0)
+
+        if arg0 is S.ComplexInfinity:
+            arg0 = arg.limit(x, 0, dir='-' if re(cdir).is_negative else '+')
+        if arg0.is_zero:
+            return arg
+        elif arg0 in [S.Infinity, S.NegativeInfinity]:
+            s = 1 if arg0 is S.Infinity else -1
+            return s*S.Half + Order(x, x)
+        else:
+            return self.func(arg0)
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        # Expansion at oo
+        if point in [S.Infinity, -S.Infinity]:
+            z = self.args[0]
+
+            # expansion of C(x) = C1(x*sqrt(pi/2)), see reference[5] page 1-8
+            # as only real infinities are dealt with, sin and cos are O(1)
+            p = [S.NegativeOne**k * factorial(4*k + 1) /
+                 (2**(2*k + 2) * z**(4*k + 3) * 2**(2*k)*factorial(2*k))
+                 for k in range(n) if 4*k + 3 < n]
+            q = [1/(2*z)] + [S.NegativeOne**k * factorial(4*k - 1) /
+                 (2**(2*k + 1) * z**(4*k + 1) * 2**(2*k - 1)*factorial(2*k - 1))
+                 for k in range(1, n) if 4*k + 1 < n]
+
+            p = [-sqrt(2/pi)*t for t in p]
+            q = [ sqrt(2/pi)*t for t in q]
+            s = 1 if point is S.Infinity else -1
+            # The expansion at oo is 1/2 + some odd powers of z
+            # To get the expansion at -oo, replace z by -z and flip the sign
+            # The result -1/2 + the same odd powers of z as before.
+            return s*S.Half + (cos(z**2)*Add(*p) + sin(z**2)*Add(*q)
+                ).subs(x, sqrt(2/pi)*x) + Order(1/z**n, x)
+
+        # All other points are not handled
+        return super()._eval_aseries(n, args0, x, logx)
+
+
+###############################################################################
+#################### HELPER FUNCTIONS #########################################
+###############################################################################
+
+
+class _erfs(Function):
+    """
+    Helper function to make the $\\mathrm{erf}(z)$ function
+    tractable for the Gruntz algorithm.
+
+    """
+    @classmethod
+    def eval(cls, arg):
+        if arg.is_zero:
+            return S.One
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        point = args0[0]
+
+        # Expansion at oo
+        if point is S.Infinity:
+            z = self.args[0]
+            l = [1/sqrt(pi) * factorial(2*k)*(-S(
+                 4))**(-k)/factorial(k) * (1/z)**(2*k + 1) for k in range(n)]
+            o = Order(1/z**(2*n + 1), x)
+            # It is very inefficient to first add the order and then do the nseries
+            return (Add(*l))._eval_nseries(x, n, logx) + o
+
+        # Expansion at I*oo
+        t = point.extract_multiplicatively(I)
+        if t is S.Infinity:
+            z = self.args[0]
+            # TODO: is the series really correct?
+            l = [1/sqrt(pi) * factorial(2*k)*(-S(
+                 4))**(-k)/factorial(k) * (1/z)**(2*k + 1) for k in range(n)]
+            o = Order(1/z**(2*n + 1), x)
+            # It is very inefficient to first add the order and then do the nseries
+            return (Add(*l))._eval_nseries(x, n, logx) + o
+
+        # All other points are not handled
+        return super()._eval_aseries(n, args0, x, logx)
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            z = self.args[0]
+            return -2/sqrt(pi) + 2*z*_erfs(z)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_intractable(self, z, **kwargs):
+        return (S.One - erf(z))*exp(z**2)
+
+
+class _eis(Function):
+    """
+    Helper function to make the $\\mathrm{Ei}(z)$ and $\\mathrm{li}(z)$
+    functions tractable for the Gruntz algorithm.
+
+    """
+
+
+    def _eval_aseries(self, n, args0, x, logx):
+        from sympy.series.order import Order
+        if args0[0] != S.Infinity:
+            return super(_erfs, self)._eval_aseries(n, args0, x, logx)
+
+        z = self.args[0]
+        l = [factorial(k) * (1/z)**(k + 1) for k in range(n)]
+        o = Order(1/z**(n + 1), x)
+        # It is very inefficient to first add the order and then do the nseries
+        return (Add(*l))._eval_nseries(x, n, logx) + o
+
+
+    def fdiff(self, argindex=1):
+        if argindex == 1:
+            z = self.args[0]
+            return S.One / z - _eis(z)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_intractable(self, z, **kwargs):
+        return exp(-z)*Ei(z)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        x0 = self.args[0].limit(x, 0)
+        if x0.is_zero:
+            f = self._eval_rewrite_as_intractable(*self.args)
+            return f._eval_as_leading_term(x, logx=logx, cdir=cdir)
+        return super()._eval_as_leading_term(x, logx=logx, cdir=cdir)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+        x0 = self.args[0].limit(x, 0)
+        if x0.is_zero:
+            f = self._eval_rewrite_as_intractable(*self.args)
+            return f._eval_nseries(x, n, logx)
+        return super()._eval_nseries(x, n, logx)

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/hyper.py

@@ -0,0 +1,1152 @@
+"""Hypergeometric and Meijer G-functions"""
+from functools import reduce
+
+from sympy.core import S, ilcm, Mod
+from sympy.core.add import Add
+from sympy.core.expr import Expr
+from sympy.core.function import Function, Derivative, ArgumentIndexError
+
+from sympy.core.containers import Tuple
+from sympy.core.mul import Mul
+from sympy.core.numbers import I, pi, oo, zoo
+from sympy.core.relational import Ne
+from sympy.core.sorting import default_sort_key
+from sympy.core.symbol import Dummy
+
+from sympy.functions import (sqrt, exp, log, sin, cos, asin, atan,
+        sinh, cosh, asinh, acosh, atanh, acoth)
+from sympy.functions import factorial, RisingFactorial
+from sympy.functions.elementary.complexes import Abs, re, unpolarify
+from sympy.functions.elementary.exponential import exp_polar
+from sympy.functions.elementary.integers import ceiling
+from sympy.functions.elementary.piecewise import Piecewise
+from sympy.logic.boolalg import (And, Or)
+
+class TupleArg(Tuple):
+    def limit(self, x, xlim, dir='+'):
+        """ Compute limit x->xlim.
+        """
+        from sympy.series.limits import limit
+        return TupleArg(*[limit(f, x, xlim, dir) for f in self.args])
+
+
+# TODO should __new__ accept **options?
+# TODO should constructors should check if parameters are sensible?
+
+
+def _prep_tuple(v):
+    """
+    Turn an iterable argument *v* into a tuple and unpolarify, since both
+    hypergeometric and meijer g-functions are unbranched in their parameters.
+
+    Examples
+    ========
+
+    >>> from sympy.functions.special.hyper import _prep_tuple
+    >>> _prep_tuple([1, 2, 3])
+    (1, 2, 3)
+    >>> _prep_tuple((4, 5))
+    (4, 5)
+    >>> _prep_tuple((7, 8, 9))
+    (7, 8, 9)
+
+    """
+    return TupleArg(*[unpolarify(x) for x in v])
+
+
+class TupleParametersBase(Function):
+    """ Base class that takes care of differentiation, when some of
+        the arguments are actually tuples. """
+    # This is not deduced automatically since there are Tuples as arguments.
+    is_commutative = True
+
+    def _eval_derivative(self, s):
+        try:
+            res = 0
+            if self.args[0].has(s) or self.args[1].has(s):
+                for i, p in enumerate(self._diffargs):
+                    m = self._diffargs[i].diff(s)
+                    if m != 0:
+                        res += self.fdiff((1, i))*m
+            return res + self.fdiff(3)*self.args[2].diff(s)
+        except (ArgumentIndexError, NotImplementedError):
+            return Derivative(self, s)
+
+
+class hyper(TupleParametersBase):
+    r"""
+    The generalized hypergeometric function is defined by a series where
+    the ratios of successive terms are a rational function of the summation
+    index. When convergent, it is continued analytically to the largest
+    possible domain.
+
+    Explanation
+    ===========
+
+    The hypergeometric function depends on two vectors of parameters, called
+    the numerator parameters $a_p$, and the denominator parameters
+    $b_q$. It also has an argument $z$. The series definition is
+
+    .. math ::
+        {}_pF_q\left(\begin{matrix} a_1, \cdots, a_p \\ b_1, \cdots, b_q \end{matrix}
+                     \middle| z \right)
+        = \sum_{n=0}^\infty \frac{(a_1)_n \cdots (a_p)_n}{(b_1)_n \cdots (b_q)_n}
+                            \frac{z^n}{n!},
+
+    where $(a)_n = (a)(a+1)\cdots(a+n-1)$ denotes the rising factorial.
+
+    If one of the $b_q$ is a non-positive integer then the series is
+    undefined unless one of the $a_p$ is a larger (i.e., smaller in
+    magnitude) non-positive integer. If none of the $b_q$ is a
+    non-positive integer and one of the $a_p$ is a non-positive
+    integer, then the series reduces to a polynomial. To simplify the
+    following discussion, we assume that none of the $a_p$ or
+    $b_q$ is a non-positive integer. For more details, see the
+    references.
+
+    The series converges for all $z$ if $p \le q$, and thus
+    defines an entire single-valued function in this case. If $p =
+    q+1$ the series converges for $|z| < 1$, and can be continued
+    analytically into a half-plane. If $p > q+1$ the series is
+    divergent for all $z$.
+
+    Please note the hypergeometric function constructor currently does *not*
+    check if the parameters actually yield a well-defined function.
+
+    Examples
+    ========
+
+    The parameters $a_p$ and $b_q$ can be passed as arbitrary
+    iterables, for example:
+
+    >>> from sympy import hyper
+    >>> from sympy.abc import x, n, a
+    >>> hyper((1, 2, 3), [3, 4], x)
+    hyper((1, 2, 3), (3, 4), x)
+
+    There is also pretty printing (it looks better using Unicode):
+
+    >>> from sympy import pprint
+    >>> pprint(hyper((1, 2, 3), [3, 4], x), use_unicode=False)
+      _
+     |_  /1, 2, 3 |  \
+     |   |        | x|
+    3  2 \  3, 4  |  /
+
+    The parameters must always be iterables, even if they are vectors of
+    length one or zero:
+
+    >>> hyper((1, ), [], x)
+    hyper((1,), (), x)
+
+    But of course they may be variables (but if they depend on $x$ then you
+    should not expect much implemented functionality):
+
+    >>> hyper((n, a), (n**2,), x)
+    hyper((n, a), (n**2,), x)
+
+    The hypergeometric function generalizes many named special functions.
+    The function ``hyperexpand()`` tries to express a hypergeometric function
+    using named special functions. For example:
+
+    >>> from sympy import hyperexpand
+    >>> hyperexpand(hyper([], [], x))
+    exp(x)
+
+    You can also use ``expand_func()``:
+
+    >>> from sympy import expand_func
+    >>> expand_func(x*hyper([1, 1], [2], -x))
+    log(x + 1)
+
+    More examples:
+
+    >>> from sympy import S
+    >>> hyperexpand(hyper([], [S(1)/2], -x**2/4))
+    cos(x)
+    >>> hyperexpand(x*hyper([S(1)/2, S(1)/2], [S(3)/2], x**2))
+    asin(x)
+
+    We can also sometimes ``hyperexpand()`` parametric functions:
+
+    >>> from sympy.abc import a
+    >>> hyperexpand(hyper([-a], [], x))
+    (1 - x)**a
+
+    See Also
+    ========
+
+    sympy.simplify.hyperexpand
+    gamma
+    meijerg
+
+    References
+    ==========
+
+    .. [1] Luke, Y. L. (1969), The Special Functions and Their Approximations,
+           Volume 1
+    .. [2] https://en.wikipedia.org/wiki/Generalized_hypergeometric_function
+
+    """
+
+
+    def __new__(cls, ap, bq, z, **kwargs):
+        # TODO should we check convergence conditions?
+        return Function.__new__(cls, _prep_tuple(ap), _prep_tuple(bq), z, **kwargs)
+
+    @classmethod
+    def eval(cls, ap, bq, z):
+        if len(ap) <= len(bq) or (len(ap) == len(bq) + 1 and (Abs(z) <= 1) == True):
+            nz = unpolarify(z)
+            if z != nz:
+                return hyper(ap, bq, nz)
+
+    def fdiff(self, argindex=3):
+        if argindex != 3:
+            raise ArgumentIndexError(self, argindex)
+        nap = Tuple(*[a + 1 for a in self.ap])
+        nbq = Tuple(*[b + 1 for b in self.bq])
+        fac = Mul(*self.ap)/Mul(*self.bq)
+        return fac*hyper(nap, nbq, self.argument)
+
+    def _eval_expand_func(self, **hints):
+        from sympy.functions.special.gamma_functions import gamma
+        from sympy.simplify.hyperexpand import hyperexpand
+        if len(self.ap) == 2 and len(self.bq) == 1 and self.argument == 1:
+            a, b = self.ap
+            c = self.bq[0]
+            return gamma(c)*gamma(c - a - b)/gamma(c - a)/gamma(c - b)
+        return hyperexpand(self)
+
+    def _eval_rewrite_as_Sum(self, ap, bq, z, **kwargs):
+        from sympy.concrete.summations import Sum
+        n = Dummy("n", integer=True)
+        rfap = [RisingFactorial(a, n) for a in ap]
+        rfbq = [RisingFactorial(b, n) for b in bq]
+        coeff = Mul(*rfap) / Mul(*rfbq)
+        return Piecewise((Sum(coeff * z**n / factorial(n), (n, 0, oo)),
+                         self.convergence_statement), (self, True))
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        arg = self.args[2]
+        x0 = arg.subs(x, 0)
+        if x0 is S.NaN:
+            x0 = arg.limit(x, 0, dir='-' if re(cdir).is_negative else '+')
+
+        if x0 is S.Zero:
+            return S.One
+        return super()._eval_as_leading_term(x, logx=logx, cdir=cdir)
+
+    def _eval_nseries(self, x, n, logx, cdir=0):
+
+        from sympy.series.order import Order
+
+        arg = self.args[2]
+        x0 = arg.limit(x, 0)
+        ap = self.args[0]
+        bq = self.args[1]
+
+        if x0 != 0:
+            return super()._eval_nseries(x, n, logx)
+
+        terms = []
+
+        for i in range(n):
+            num = Mul(*[RisingFactorial(a, i) for a in ap])
+            den = Mul(*[RisingFactorial(b, i) for b in bq])
+            terms.append(((num/den) * (arg**i)) / factorial(i))
+
+        return (Add(*terms) + Order(x**n,x))
+
+    @property
+    def argument(self):
+        """ Argument of the hypergeometric function. """
+        return self.args[2]
+
+    @property
+    def ap(self):
+        """ Numerator parameters of the hypergeometric function. """
+        return Tuple(*self.args[0])
+
+    @property
+    def bq(self):
+        """ Denominator parameters of the hypergeometric function. """
+        return Tuple(*self.args[1])
+
+    @property
+    def _diffargs(self):
+        return self.ap + self.bq
+
+    @property
+    def eta(self):
+        """ A quantity related to the convergence of the series. """
+        return sum(self.ap) - sum(self.bq)
+
+    @property
+    def radius_of_convergence(self):
+        """
+        Compute the radius of convergence of the defining series.
+
+        Explanation
+        ===========
+
+        Note that even if this is not ``oo``, the function may still be
+        evaluated outside of the radius of convergence by analytic
+        continuation. But if this is zero, then the function is not actually
+        defined anywhere else.
+
+        Examples
+        ========
+
+        >>> from sympy import hyper
+        >>> from sympy.abc import z
+        >>> hyper((1, 2), [3], z).radius_of_convergence
+        1
+        >>> hyper((1, 2, 3), [4], z).radius_of_convergence
+        0
+        >>> hyper((1, 2), (3, 4), z).radius_of_convergence
+        oo
+
+        """
+        if any(a.is_integer and (a <= 0) == True for a in self.ap + self.bq):
+            aints = [a for a in self.ap if a.is_Integer and (a <= 0) == True]
+            bints = [a for a in self.bq if a.is_Integer and (a <= 0) == True]
+            if len(aints) < len(bints):
+                return S.Zero
+            popped = False
+            for b in bints:
+                cancelled = False
+                while aints:
+                    a = aints.pop()
+                    if a >= b:
+                        cancelled = True
+                        break
+                    popped = True
+                if not cancelled:
+                    return S.Zero
+            if aints or popped:
+                # There are still non-positive numerator parameters.
+                # This is a polynomial.
+                return oo
+        if len(self.ap) == len(self.bq) + 1:
+            return S.One
+        elif len(self.ap) <= len(self.bq):
+            return oo
+        else:
+            return S.Zero
+
+    @property
+    def convergence_statement(self):
+        """ Return a condition on z under which the series converges. """
+        R = self.radius_of_convergence
+        if R == 0:
+            return False
+        if R == oo:
+            return True
+        # The special functions and their approximations, page 44
+        e = self.eta
+        z = self.argument
+        c1 = And(re(e) < 0, abs(z) <= 1)
+        c2 = And(0 <= re(e), re(e) < 1, abs(z) <= 1, Ne(z, 1))
+        c3 = And(re(e) >= 1, abs(z) < 1)
+        return Or(c1, c2, c3)
+
+    def _eval_simplify(self, **kwargs):
+        from sympy.simplify.hyperexpand import hyperexpand
+        return hyperexpand(self)
+
+
+class meijerg(TupleParametersBase):
+    r"""
+    The Meijer G-function is defined by a Mellin-Barnes type integral that
+    resembles an inverse Mellin transform. It generalizes the hypergeometric
+    functions.
+
+    Explanation
+    ===========
+
+    The Meijer G-function depends on four sets of parameters. There are
+    "*numerator parameters*"
+    $a_1, \ldots, a_n$ and $a_{n+1}, \ldots, a_p$, and there are
+    "*denominator parameters*"
+    $b_1, \ldots, b_m$ and $b_{m+1}, \ldots, b_q$.
+    Confusingly, it is traditionally denoted as follows (note the position
+    of $m$, $n$, $p$, $q$, and how they relate to the lengths of the four
+    parameter vectors):
+
+    .. math ::
+        G_{p,q}^{m,n} \left(\begin{matrix}a_1, \cdots, a_n & a_{n+1}, \cdots, a_p \\
+                                        b_1, \cdots, b_m & b_{m+1}, \cdots, b_q
+                          \end{matrix} \middle| z \right).
+
+    However, in SymPy the four parameter vectors are always available
+    separately (see examples), so that there is no need to keep track of the
+    decorating sub- and super-scripts on the G symbol.
+
+    The G function is defined as the following integral:
+
+    .. math ::
+         \frac{1}{2 \pi i} \int_L \frac{\prod_{j=1}^m \Gamma(b_j - s)
+         \prod_{j=1}^n \Gamma(1 - a_j + s)}{\prod_{j=m+1}^q \Gamma(1- b_j +s)
+         \prod_{j=n+1}^p \Gamma(a_j - s)} z^s \mathrm{d}s,
+
+    where $\Gamma(z)$ is the gamma function. There are three possible
+    contours which we will not describe in detail here (see the references).
+    If the integral converges along more than one of them, the definitions
+    agree. The contours all separate the poles of $\Gamma(1-a_j+s)$
+    from the poles of $\Gamma(b_k-s)$, so in particular the G function
+    is undefined if $a_j - b_k \in \mathbb{Z}_{>0}$ for some
+    $j \le n$ and $k \le m$.
+
+    The conditions under which one of the contours yields a convergent integral
+    are complicated and we do not state them here, see the references.
+
+    Please note currently the Meijer G-function constructor does *not* check any
+    convergence conditions.
+
+    Examples
+    ========
+
+    You can pass the parameters either as four separate vectors:
+
+    >>> from sympy import meijerg, Tuple, pprint
+    >>> from sympy.abc import x, a
+    >>> pprint(meijerg((1, 2), (a, 4), (5,), [], x), use_unicode=False)
+     __1, 2 /1, 2  a, 4 |  \
+    /__     |           | x|
+    \_|4, 1 \ 5         |  /
+
+    Or as two nested vectors:
+
+    >>> pprint(meijerg([(1, 2), (3, 4)], ([5], Tuple()), x), use_unicode=False)
+     __1, 2 /1, 2  3, 4 |  \
+    /__     |           | x|
+    \_|4, 1 \ 5         |  /
+
+    As with the hypergeometric function, the parameters may be passed as
+    arbitrary iterables. Vectors of length zero and one also have to be
+    passed as iterables. The parameters need not be constants, but if they
+    depend on the argument then not much implemented functionality should be
+    expected.
+
+    All the subvectors of parameters are available:
+
+    >>> from sympy import pprint
+    >>> g = meijerg([1], [2], [3], [4], x)
+    >>> pprint(g, use_unicode=False)
+     __1, 1 /1  2 |  \
+    /__     |     | x|
+    \_|2, 2 \3  4 |  /
+    >>> g.an
+    (1,)
+    >>> g.ap
+    (1, 2)
+    >>> g.aother
+    (2,)
+    >>> g.bm
+    (3,)
+    >>> g.bq
+    (3, 4)
+    >>> g.bother
+    (4,)
+
+    The Meijer G-function generalizes the hypergeometric functions.
+    In some cases it can be expressed in terms of hypergeometric functions,
+    using Slater's theorem. For example:
+
+    >>> from sympy import hyperexpand
+    >>> from sympy.abc import a, b, c
+    >>> hyperexpand(meijerg([a], [], [c], [b], x), allow_hyper=True)
+    x**c*gamma(-a + c + 1)*hyper((-a + c + 1,),
+                                 (-b + c + 1,), -x)/gamma(-b + c + 1)
+
+    Thus the Meijer G-function also subsumes many named functions as special
+    cases. You can use ``expand_func()`` or ``hyperexpand()`` to (try to)
+    rewrite a Meijer G-function in terms of named special functions. For
+    example:
+
+    >>> from sympy import expand_func, S
+    >>> expand_func(meijerg([[],[]], [[0],[]], -x))
+    exp(x)
+    >>> hyperexpand(meijerg([[],[]], [[S(1)/2],[0]], (x/2)**2))
+    sin(x)/sqrt(pi)
+
+    See Also
+    ========
+
+    hyper
+    sympy.simplify.hyperexpand
+
+    References
+    ==========
+
+    .. [1] Luke, Y. L. (1969), The Special Functions and Their Approximations,
+           Volume 1
+    .. [2] https://en.wikipedia.org/wiki/Meijer_G-function
+
+    """
+
+
+    def __new__(cls, *args, **kwargs):
+        if len(args) == 5:
+            args = [(args[0], args[1]), (args[2], args[3]), args[4]]
+        if len(args) != 3:
+            raise TypeError("args must be either as, as', bs, bs', z or "
+                            "as, bs, z")
+
+        def tr(p):
+            if len(p) != 2:
+                raise TypeError("wrong argument")
+            return TupleArg(_prep_tuple(p[0]), _prep_tuple(p[1]))
+
+        arg0, arg1 = tr(args[0]), tr(args[1])
+        if Tuple(arg0, arg1).has(oo, zoo, -oo):
+            raise ValueError("G-function parameters must be finite")
+        if any((a - b).is_Integer and a - b > 0
+               for a in arg0[0] for b in arg1[0]):
+            raise ValueError("no parameter a1, ..., an may differ from "
+                         "any b1, ..., bm by a positive integer")
+
+        # TODO should we check convergence conditions?
+        return Function.__new__(cls, arg0, arg1, args[2], **kwargs)
+
+    def fdiff(self, argindex=3):
+        if argindex != 3:
+            return self._diff_wrt_parameter(argindex[1])
+        if len(self.an) >= 1:
+            a = list(self.an)
+            a[0] -= 1
+            G = meijerg(a, self.aother, self.bm, self.bother, self.argument)
+            return 1/self.argument * ((self.an[0] - 1)*self + G)
+        elif len(self.bm) >= 1:
+            b = list(self.bm)
+            b[0] += 1
+            G = meijerg(self.an, self.aother, b, self.bother, self.argument)
+            return 1/self.argument * (self.bm[0]*self - G)
+        else:
+            return S.Zero
+
+    def _diff_wrt_parameter(self, idx):
+        # Differentiation wrt a parameter can only be done in very special
+        # cases. In particular, if we want to differentiate with respect to
+        # `a`, all other gamma factors have to reduce to rational functions.
+        #
+        # Let MT denote mellin transform. Suppose T(-s) is the gamma factor
+        # appearing in the definition of G. Then
+        #
+        #   MT(log(z)G(z)) = d/ds T(s) = d/da T(s) + ...
+        #
+        # Thus d/da G(z) = log(z)G(z) - ...
+        # The ... can be evaluated as a G function under the above conditions,
+        # the formula being most easily derived by using
+        #
+        # d  Gamma(s + n)    Gamma(s + n) / 1    1                1     \
+        # -- ------------ =  ------------ | - + ----  + ... + --------- |
+        # ds Gamma(s)        Gamma(s)     \ s   s + 1         s + n - 1 /
+        #
+        # which follows from the difference equation of the digamma function.
+        # (There is a similar equation for -n instead of +n).
+
+        # We first figure out how to pair the parameters.
+        an = list(self.an)
+        ap = list(self.aother)
+        bm = list(self.bm)
+        bq = list(self.bother)
+        if idx < len(an):
+            an.pop(idx)
+        else:
+            idx -= len(an)
+            if idx < len(ap):
+                ap.pop(idx)
+            else:
+                idx -= len(ap)
+                if idx < len(bm):
+                    bm.pop(idx)
+                else:
+                    bq.pop(idx - len(bm))
+        pairs1 = []
+        pairs2 = []
+        for l1, l2, pairs in [(an, bq, pairs1), (ap, bm, pairs2)]:
+            while l1:
+                x = l1.pop()
+                found = None
+                for i, y in enumerate(l2):
+                    if not Mod((x - y).simplify(), 1):
+                        found = i
+                        break
+                if found is None:
+                    raise NotImplementedError('Derivative not expressible '
+                                              'as G-function?')
+                y = l2[i]
+                l2.pop(i)
+                pairs.append((x, y))
+
+        # Now build the result.
+        res = log(self.argument)*self
+
+        for a, b in pairs1:
+            sign = 1
+            n = a - b
+            base = b
+            if n < 0:
+                sign = -1
+                n = b - a
+                base = a
+            for k in range(n):
+                res -= sign*meijerg(self.an + (base + k + 1,), self.aother,
+                                    self.bm, self.bother + (base + k + 0,),
+                                    self.argument)
+
+        for a, b in pairs2:
+            sign = 1
+            n = b - a
+            base = a
+            if n < 0:
+                sign = -1
+                n = a - b
+                base = b
+            for k in range(n):
+                res -= sign*meijerg(self.an, self.aother + (base + k + 1,),
+                                    self.bm + (base + k + 0,), self.bother,
+                                    self.argument)
+
+        return res
+
+    def get_period(self):
+        """
+        Return a number $P$ such that $G(x*exp(I*P)) == G(x)$.
+
+        Examples
+        ========
+
+        >>> from sympy import meijerg, pi, S
+        >>> from sympy.abc import z
+
+        >>> meijerg([1], [], [], [], z).get_period()
+        2*pi
+        >>> meijerg([pi], [], [], [], z).get_period()
+        oo
+        >>> meijerg([1, 2], [], [], [], z).get_period()
+        oo
+        >>> meijerg([1,1], [2], [1, S(1)/2, S(1)/3], [1], z).get_period()
+        12*pi
+
+        """
+        # This follows from slater's theorem.
+        def compute(l):
+            # first check that no two differ by an integer
+            for i, b in enumerate(l):
+                if not b.is_Rational:
+                    return oo
+                for j in range(i + 1, len(l)):
+                    if not Mod((b - l[j]).simplify(), 1):
+                        return oo
+            return reduce(ilcm, (x.q for x in l), 1)
+        beta = compute(self.bm)
+        alpha = compute(self.an)
+        p, q = len(self.ap), len(self.bq)
+        if p == q:
+            if oo in (alpha, beta):
+                return oo
+            return 2*pi*ilcm(alpha, beta)
+        elif p < q:
+            return 2*pi*beta
+        else:
+            return 2*pi*alpha
+
+    def _eval_expand_func(self, **hints):
+        from sympy.simplify.hyperexpand import hyperexpand
+        return hyperexpand(self)
+
+    def _eval_evalf(self, prec):
+        # The default code is insufficient for polar arguments.
+        # mpmath provides an optional argument "r", which evaluates
+        # G(z**(1/r)). I am not sure what its intended use is, but we hijack it
+        # here in the following way: to evaluate at a number z of |argument|
+        # less than (say) n*pi, we put r=1/n, compute z' = root(z, n)
+        # (carefully so as not to loose the branch information), and evaluate
+        # G(z'**(1/r)) = G(z'**n) = G(z).
+        import mpmath
+        znum = self.argument._eval_evalf(prec)
+        if znum.has(exp_polar):
+            znum, branch = znum.as_coeff_mul(exp_polar)
+            if len(branch) != 1:
+                return
+            branch = branch[0].args[0]/I
+        else:
+            branch = S.Zero
+        n = ceiling(abs(branch/pi)) + 1
+        znum = znum**(S.One/n)*exp(I*branch / n)
+
+        # Convert all args to mpf or mpc
+        try:
+            [z, r, ap, bq] = [arg._to_mpmath(prec)
+                    for arg in [znum, 1/n, self.args[0], self.args[1]]]
+        except ValueError:
+            return
+
+        with mpmath.workprec(prec):
+            v = mpmath.meijerg(ap, bq, z, r)
+
+        return Expr._from_mpmath(v, prec)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        from sympy.simplify.hyperexpand import hyperexpand
+        return hyperexpand(self).as_leading_term(x, logx=logx, cdir=cdir)
+
+    def integrand(self, s):
+        """ Get the defining integrand D(s). """
+        from sympy.functions.special.gamma_functions import gamma
+        return self.argument**s \
+            * Mul(*(gamma(b - s) for b in self.bm)) \
+            * Mul(*(gamma(1 - a + s) for a in self.an)) \
+            / Mul(*(gamma(1 - b + s) for b in self.bother)) \
+            / Mul(*(gamma(a - s) for a in self.aother))
+
+    @property
+    def argument(self):
+        """ Argument of the Meijer G-function. """
+        return self.args[2]
+
+    @property
+    def an(self):
+        """ First set of numerator parameters. """
+        return Tuple(*self.args[0][0])
+
+    @property
+    def ap(self):
+        """ Combined numerator parameters. """
+        return Tuple(*(self.args[0][0] + self.args[0][1]))
+
+    @property
+    def aother(self):
+        """ Second set of numerator parameters. """
+        return Tuple(*self.args[0][1])
+
+    @property
+    def bm(self):
+        """ First set of denominator parameters. """
+        return Tuple(*self.args[1][0])
+
+    @property
+    def bq(self):
+        """ Combined denominator parameters. """
+        return Tuple(*(self.args[1][0] + self.args[1][1]))
+
+    @property
+    def bother(self):
+        """ Second set of denominator parameters. """
+        return Tuple(*self.args[1][1])
+
+    @property
+    def _diffargs(self):
+        return self.ap + self.bq
+
+    @property
+    def nu(self):
+        """ A quantity related to the convergence region of the integral,
+            c.f. references. """
+        return sum(self.bq) - sum(self.ap)
+
+    @property
+    def delta(self):
+        """ A quantity related to the convergence region of the integral,
+            c.f. references. """
+        return len(self.bm) + len(self.an) - S(len(self.ap) + len(self.bq))/2
+
+    @property
+    def is_number(self):
+        """ Returns true if expression has numeric data only. """
+        return not self.free_symbols
+
+
+class HyperRep(Function):
+    """
+    A base class for "hyper representation functions".
+
+    This is used exclusively in ``hyperexpand()``, but fits more logically here.
+
+    pFq is branched at 1 if p == q+1. For use with slater-expansion, we want
+    define an "analytic continuation" to all polar numbers, which is
+    continuous on circles and on the ray t*exp_polar(I*pi). Moreover, we want
+    a "nice" expression for the various cases.
+
+    This base class contains the core logic, concrete derived classes only
+    supply the actual functions.
+
+    """
+
+
+    @classmethod
+    def eval(cls, *args):
+        newargs = tuple(map(unpolarify, args[:-1])) + args[-1:]
+        if args != newargs:
+            return cls(*newargs)
+
+    @classmethod
+    def _expr_small(cls, x):
+        """ An expression for F(x) which holds for |x| < 1. """
+        raise NotImplementedError
+
+    @classmethod
+    def _expr_small_minus(cls, x):
+        """ An expression for F(-x) which holds for |x| < 1. """
+        raise NotImplementedError
+
+    @classmethod
+    def _expr_big(cls, x, n):
+        """ An expression for F(exp_polar(2*I*pi*n)*x), |x| > 1. """
+        raise NotImplementedError
+
+    @classmethod
+    def _expr_big_minus(cls, x, n):
+        """ An expression for F(exp_polar(2*I*pi*n + pi*I)*x), |x| > 1. """
+        raise NotImplementedError
+
+    def _eval_rewrite_as_nonrep(self, *args, **kwargs):
+        x, n = self.args[-1].extract_branch_factor(allow_half=True)
+        minus = False
+        newargs = self.args[:-1] + (x,)
+        if not n.is_Integer:
+            minus = True
+            n -= S.Half
+        newerargs = newargs + (n,)
+        if minus:
+            small = self._expr_small_minus(*newargs)
+            big = self._expr_big_minus(*newerargs)
+        else:
+            small = self._expr_small(*newargs)
+            big = self._expr_big(*newerargs)
+
+        if big == small:
+            return small
+        return Piecewise((big, abs(x) > 1), (small, True))
+
+    def _eval_rewrite_as_nonrepsmall(self, *args, **kwargs):
+        x, n = self.args[-1].extract_branch_factor(allow_half=True)
+        args = self.args[:-1] + (x,)
+        if not n.is_Integer:
+            return self._expr_small_minus(*args)
+        return self._expr_small(*args)
+
+
+class HyperRep_power1(HyperRep):
+    """ Return a representative for hyper([-a], [], z) == (1 - z)**a. """
+
+    @classmethod
+    def _expr_small(cls, a, x):
+        return (1 - x)**a
+
+    @classmethod
+    def _expr_small_minus(cls, a, x):
+        return (1 + x)**a
+
+    @classmethod
+    def _expr_big(cls, a, x, n):
+        if a.is_integer:
+            return cls._expr_small(a, x)
+        return (x - 1)**a*exp((2*n - 1)*pi*I*a)
+
+    @classmethod
+    def _expr_big_minus(cls, a, x, n):
+        if a.is_integer:
+            return cls._expr_small_minus(a, x)
+        return (1 + x)**a*exp(2*n*pi*I*a)
+
+
+class HyperRep_power2(HyperRep):
+    """ Return a representative for hyper([a, a - 1/2], [2*a], z). """
+
+    @classmethod
+    def _expr_small(cls, a, x):
+        return 2**(2*a - 1)*(1 + sqrt(1 - x))**(1 - 2*a)
+
+    @classmethod
+    def _expr_small_minus(cls, a, x):
+        return 2**(2*a - 1)*(1 + sqrt(1 + x))**(1 - 2*a)
+
+    @classmethod
+    def _expr_big(cls, a, x, n):
+        sgn = -1
+        if n.is_odd:
+            sgn = 1
+            n -= 1
+        return 2**(2*a - 1)*(1 + sgn*I*sqrt(x - 1))**(1 - 2*a) \
+            *exp(-2*n*pi*I*a)
+
+    @classmethod
+    def _expr_big_minus(cls, a, x, n):
+        sgn = 1
+        if n.is_odd:
+            sgn = -1
+        return sgn*2**(2*a - 1)*(sqrt(1 + x) + sgn)**(1 - 2*a)*exp(-2*pi*I*a*n)
+
+
+class HyperRep_log1(HyperRep):
+    """ Represent -z*hyper([1, 1], [2], z) == log(1 - z). """
+    @classmethod
+    def _expr_small(cls, x):
+        return log(1 - x)
+
+    @classmethod
+    def _expr_small_minus(cls, x):
+        return log(1 + x)
+
+    @classmethod
+    def _expr_big(cls, x, n):
+        return log(x - 1) + (2*n - 1)*pi*I
+
+    @classmethod
+    def _expr_big_minus(cls, x, n):
+        return log(1 + x) + 2*n*pi*I
+
+
+class HyperRep_atanh(HyperRep):
+    """ Represent hyper([1/2, 1], [3/2], z) == atanh(sqrt(z))/sqrt(z). """
+    @classmethod
+    def _expr_small(cls, x):
+        return atanh(sqrt(x))/sqrt(x)
+
+    def _expr_small_minus(cls, x):
+        return atan(sqrt(x))/sqrt(x)
+
+    def _expr_big(cls, x, n):
+        if n.is_even:
+            return (acoth(sqrt(x)) + I*pi/2)/sqrt(x)
+        else:
+            return (acoth(sqrt(x)) - I*pi/2)/sqrt(x)
+
+    def _expr_big_minus(cls, x, n):
+        if n.is_even:
+            return atan(sqrt(x))/sqrt(x)
+        else:
+            return (atan(sqrt(x)) - pi)/sqrt(x)
+
+
+class HyperRep_asin1(HyperRep):
+    """ Represent hyper([1/2, 1/2], [3/2], z) == asin(sqrt(z))/sqrt(z). """
+    @classmethod
+    def _expr_small(cls, z):
+        return asin(sqrt(z))/sqrt(z)
+
+    @classmethod
+    def _expr_small_minus(cls, z):
+        return asinh(sqrt(z))/sqrt(z)
+
+    @classmethod
+    def _expr_big(cls, z, n):
+        return S.NegativeOne**n*((S.Half - n)*pi/sqrt(z) + I*acosh(sqrt(z))/sqrt(z))
+
+    @classmethod
+    def _expr_big_minus(cls, z, n):
+        return S.NegativeOne**n*(asinh(sqrt(z))/sqrt(z) + n*pi*I/sqrt(z))
+
+
+class HyperRep_asin2(HyperRep):
+    """ Represent hyper([1, 1], [3/2], z) == asin(sqrt(z))/sqrt(z)/sqrt(1-z). """
+    # TODO this can be nicer
+    @classmethod
+    def _expr_small(cls, z):
+        return HyperRep_asin1._expr_small(z) \
+            /HyperRep_power1._expr_small(S.Half, z)
+
+    @classmethod
+    def _expr_small_minus(cls, z):
+        return HyperRep_asin1._expr_small_minus(z) \
+            /HyperRep_power1._expr_small_minus(S.Half, z)
+
+    @classmethod
+    def _expr_big(cls, z, n):
+        return HyperRep_asin1._expr_big(z, n) \
+            /HyperRep_power1._expr_big(S.Half, z, n)
+
+    @classmethod
+    def _expr_big_minus(cls, z, n):
+        return HyperRep_asin1._expr_big_minus(z, n) \
+            /HyperRep_power1._expr_big_minus(S.Half, z, n)
+
+
+class HyperRep_sqrts1(HyperRep):
+    """ Return a representative for hyper([-a, 1/2 - a], [1/2], z). """
+
+    @classmethod
+    def _expr_small(cls, a, z):
+        return ((1 - sqrt(z))**(2*a) + (1 + sqrt(z))**(2*a))/2
+
+    @classmethod
+    def _expr_small_minus(cls, a, z):
+        return (1 + z)**a*cos(2*a*atan(sqrt(z)))
+
+    @classmethod
+    def _expr_big(cls, a, z, n):
+        if n.is_even:
+            return ((sqrt(z) + 1)**(2*a)*exp(2*pi*I*n*a) +
+                    (sqrt(z) - 1)**(2*a)*exp(2*pi*I*(n - 1)*a))/2
+        else:
+            n -= 1
+            return ((sqrt(z) - 1)**(2*a)*exp(2*pi*I*a*(n + 1)) +
+                    (sqrt(z) + 1)**(2*a)*exp(2*pi*I*a*n))/2
+
+    @classmethod
+    def _expr_big_minus(cls, a, z, n):
+        if n.is_even:
+            return (1 + z)**a*exp(2*pi*I*n*a)*cos(2*a*atan(sqrt(z)))
+        else:
+            return (1 + z)**a*exp(2*pi*I*n*a)*cos(2*a*atan(sqrt(z)) - 2*pi*a)
+
+
+class HyperRep_sqrts2(HyperRep):
+    """ Return a representative for
+          sqrt(z)/2*[(1-sqrt(z))**2a - (1 + sqrt(z))**2a]
+          == -2*z/(2*a+1) d/dz hyper([-a - 1/2, -a], [1/2], z)"""
+
+    @classmethod
+    def _expr_small(cls, a, z):
+        return sqrt(z)*((1 - sqrt(z))**(2*a) - (1 + sqrt(z))**(2*a))/2
+
+    @classmethod
+    def _expr_small_minus(cls, a, z):
+        return sqrt(z)*(1 + z)**a*sin(2*a*atan(sqrt(z)))
+
+    @classmethod
+    def _expr_big(cls, a, z, n):
+        if n.is_even:
+            return sqrt(z)/2*((sqrt(z) - 1)**(2*a)*exp(2*pi*I*a*(n - 1)) -
+                              (sqrt(z) + 1)**(2*a)*exp(2*pi*I*a*n))
+        else:
+            n -= 1
+            return sqrt(z)/2*((sqrt(z) - 1)**(2*a)*exp(2*pi*I*a*(n + 1)) -
+                              (sqrt(z) + 1)**(2*a)*exp(2*pi*I*a*n))
+
+    def _expr_big_minus(cls, a, z, n):
+        if n.is_even:
+            return (1 + z)**a*exp(2*pi*I*n*a)*sqrt(z)*sin(2*a*atan(sqrt(z)))
+        else:
+            return (1 + z)**a*exp(2*pi*I*n*a)*sqrt(z) \
+                *sin(2*a*atan(sqrt(z)) - 2*pi*a)
+
+
+class HyperRep_log2(HyperRep):
+    """ Represent log(1/2 + sqrt(1 - z)/2) == -z/4*hyper([3/2, 1, 1], [2, 2], z) """
+
+    @classmethod
+    def _expr_small(cls, z):
+        return log(S.Half + sqrt(1 - z)/2)
+
+    @classmethod
+    def _expr_small_minus(cls, z):
+        return log(S.Half + sqrt(1 + z)/2)
+
+    @classmethod
+    def _expr_big(cls, z, n):
+        if n.is_even:
+            return (n - S.Half)*pi*I + log(sqrt(z)/2) + I*asin(1/sqrt(z))
+        else:
+            return (n - S.Half)*pi*I + log(sqrt(z)/2) - I*asin(1/sqrt(z))
+
+    def _expr_big_minus(cls, z, n):
+        if n.is_even:
+            return pi*I*n + log(S.Half + sqrt(1 + z)/2)
+        else:
+            return pi*I*n + log(sqrt(1 + z)/2 - S.Half)
+
+
+class HyperRep_cosasin(HyperRep):
+    """ Represent hyper([a, -a], [1/2], z) == cos(2*a*asin(sqrt(z))). """
+    # Note there are many alternative expressions, e.g. as powers of a sum of
+    # square roots.
+
+    @classmethod
+    def _expr_small(cls, a, z):
+        return cos(2*a*asin(sqrt(z)))
+
+    @classmethod
+    def _expr_small_minus(cls, a, z):
+        return cosh(2*a*asinh(sqrt(z)))
+
+    @classmethod
+    def _expr_big(cls, a, z, n):
+        return cosh(2*a*acosh(sqrt(z)) + a*pi*I*(2*n - 1))
+
+    @classmethod
+    def _expr_big_minus(cls, a, z, n):
+        return cosh(2*a*asinh(sqrt(z)) + 2*a*pi*I*n)
+
+
+class HyperRep_sinasin(HyperRep):
+    """ Represent 2*a*z*hyper([1 - a, 1 + a], [3/2], z)
+        == sqrt(z)/sqrt(1-z)*sin(2*a*asin(sqrt(z))) """
+
+    @classmethod
+    def _expr_small(cls, a, z):
+        return sqrt(z)/sqrt(1 - z)*sin(2*a*asin(sqrt(z)))
+
+    @classmethod
+    def _expr_small_minus(cls, a, z):
+        return -sqrt(z)/sqrt(1 + z)*sinh(2*a*asinh(sqrt(z)))
+
+    @classmethod
+    def _expr_big(cls, a, z, n):
+        return -1/sqrt(1 - 1/z)*sinh(2*a*acosh(sqrt(z)) + a*pi*I*(2*n - 1))
+
+    @classmethod
+    def _expr_big_minus(cls, a, z, n):
+        return -1/sqrt(1 + 1/z)*sinh(2*a*asinh(sqrt(z)) + 2*a*pi*I*n)
+
+class appellf1(Function):
+    r"""
+    This is the Appell hypergeometric function of two variables as:
+
+    .. math ::
+        F_1(a,b_1,b_2,c,x,y) = \sum_{m=0}^{\infty} \sum_{n=0}^{\infty}
+        \frac{(a)_{m+n} (b_1)_m (b_2)_n}{(c)_{m+n}}
+        \frac{x^m y^n}{m! n!}.
+
+    Examples
+    ========
+
+    >>> from sympy import appellf1, symbols
+    >>> x, y, a, b1, b2, c = symbols('x y a b1 b2 c')
+    >>> appellf1(2., 1., 6., 4., 5., 6.)
+    0.0063339426292673
+    >>> appellf1(12., 12., 6., 4., 0.5, 0.12)
+    172870711.659936
+    >>> appellf1(40, 2, 6, 4, 15, 60)
+    appellf1(40, 2, 6, 4, 15, 60)
+    >>> appellf1(20., 12., 10., 3., 0.5, 0.12)
+    15605338197184.4
+    >>> appellf1(40, 2, 6, 4, x, y)
+    appellf1(40, 2, 6, 4, x, y)
+    >>> appellf1(a, b1, b2, c, x, y)
+    appellf1(a, b1, b2, c, x, y)
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Appell_series
+    .. [2] https://functions.wolfram.com/HypergeometricFunctions/AppellF1/
+
+    """
+
+    @classmethod
+    def eval(cls, a, b1, b2, c, x, y):
+        if default_sort_key(b1) > default_sort_key(b2):
+            b1, b2 = b2, b1
+            x, y = y, x
+            return cls(a, b1, b2, c, x, y)
+        elif b1 == b2 and default_sort_key(x) > default_sort_key(y):
+            x, y = y, x
+            return cls(a, b1, b2, c, x, y)
+        if x == 0 and y == 0:
+            return S.One
+
+    def fdiff(self, argindex=5):
+        a, b1, b2, c, x, y = self.args
+        if argindex == 5:
+            return (a*b1/c)*appellf1(a + 1, b1 + 1, b2, c + 1, x, y)
+        elif argindex == 6:
+            return (a*b2/c)*appellf1(a + 1, b1, b2 + 1, c + 1, x, y)
+        elif argindex in (1, 2, 3, 4):
+            return Derivative(self, self.args[argindex-1])
+        else:
+            raise ArgumentIndexError(self, argindex)

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/singularity_functions.py

@@ -0,0 +1,228 @@
+from sympy.core import S, oo, diff
+from sympy.core.function import Function, ArgumentIndexError
+from sympy.core.logic import fuzzy_not
+from sympy.core.relational import Eq
+from sympy.functions.elementary.complexes import im
+from sympy.functions.elementary.piecewise import Piecewise
+from sympy.functions.special.delta_functions import Heaviside
+
+###############################################################################
+############################# SINGULARITY FUNCTION ############################
+###############################################################################
+
+
+class SingularityFunction(Function):
+    r"""
+    Singularity functions are a class of discontinuous functions.
+
+    Explanation
+    ===========
+
+    Singularity functions take a variable, an offset, and an exponent as
+    arguments. These functions are represented using Macaulay brackets as:
+
+    SingularityFunction(x, a, n) := <x - a>^n
+
+    The singularity function will automatically evaluate to
+    ``Derivative(DiracDelta(x - a), x, -n - 1)`` if ``n < 0``
+    and ``(x - a)**n*Heaviside(x - a)`` if ``n >= 0``.
+
+    Examples
+    ========
+
+    >>> from sympy import SingularityFunction, diff, Piecewise, DiracDelta, Heaviside, Symbol
+    >>> from sympy.abc import x, a, n
+    >>> SingularityFunction(x, a, n)
+    SingularityFunction(x, a, n)
+    >>> y = Symbol('y', positive=True)
+    >>> n = Symbol('n', nonnegative=True)
+    >>> SingularityFunction(y, -10, n)
+    (y + 10)**n
+    >>> y = Symbol('y', negative=True)
+    >>> SingularityFunction(y, 10, n)
+    0
+    >>> SingularityFunction(x, 4, -1).subs(x, 4)
+    oo
+    >>> SingularityFunction(x, 10, -2).subs(x, 10)
+    oo
+    >>> SingularityFunction(4, 1, 5)
+    243
+    >>> diff(SingularityFunction(x, 1, 5) + SingularityFunction(x, 1, 4), x)
+    4*SingularityFunction(x, 1, 3) + 5*SingularityFunction(x, 1, 4)
+    >>> diff(SingularityFunction(x, 4, 0), x, 2)
+    SingularityFunction(x, 4, -2)
+    >>> SingularityFunction(x, 4, 5).rewrite(Piecewise)
+    Piecewise(((x - 4)**5, x > 4), (0, True))
+    >>> expr = SingularityFunction(x, a, n)
+    >>> y = Symbol('y', positive=True)
+    >>> n = Symbol('n', nonnegative=True)
+    >>> expr.subs({x: y, a: -10, n: n})
+    (y + 10)**n
+
+    The methods ``rewrite(DiracDelta)``, ``rewrite(Heaviside)``, and
+    ``rewrite('HeavisideDiracDelta')`` returns the same output. One can use any
+    of these methods according to their choice.
+
+    >>> expr = SingularityFunction(x, 4, 5) + SingularityFunction(x, -3, -1) - SingularityFunction(x, 0, -2)
+    >>> expr.rewrite(Heaviside)
+    (x - 4)**5*Heaviside(x - 4) + DiracDelta(x + 3) - DiracDelta(x, 1)
+    >>> expr.rewrite(DiracDelta)
+    (x - 4)**5*Heaviside(x - 4) + DiracDelta(x + 3) - DiracDelta(x, 1)
+    >>> expr.rewrite('HeavisideDiracDelta')
+    (x - 4)**5*Heaviside(x - 4) + DiracDelta(x + 3) - DiracDelta(x, 1)
+
+    See Also
+    ========
+
+    DiracDelta, Heaviside
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Singularity_function
+
+    """
+
+    is_real = True
+
+    def fdiff(self, argindex=1):
+        """
+        Returns the first derivative of a DiracDelta Function.
+
+        Explanation
+        ===========
+
+        The difference between ``diff()`` and ``fdiff()`` is: ``diff()`` is the
+        user-level function and ``fdiff()`` is an object method. ``fdiff()`` is
+        a convenience method available in the ``Function`` class. It returns
+        the derivative of the function without considering the chain rule.
+        ``diff(function, x)`` calls ``Function._eval_derivative`` which in turn
+        calls ``fdiff()`` internally to compute the derivative of the function.
+
+        """
+
+        if argindex == 1:
+            x, a, n = self.args
+            if n in (S.Zero, S.NegativeOne):
+                return self.func(x, a, n-1)
+            elif n.is_positive:
+                return n*self.func(x, a, n-1)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    @classmethod
+    def eval(cls, variable, offset, exponent):
+        """
+        Returns a simplified form or a value of Singularity Function depending
+        on the argument passed by the object.
+
+        Explanation
+        ===========
+
+        The ``eval()`` method is automatically called when the
+        ``SingularityFunction`` class is about to be instantiated and it
+        returns either some simplified instance or the unevaluated instance
+        depending on the argument passed. In other words, ``eval()`` method is
+        not needed to be called explicitly, it is being called and evaluated
+        once the object is called.
+
+        Examples
+        ========
+
+        >>> from sympy import SingularityFunction, Symbol, nan
+        >>> from sympy.abc import x, a, n
+        >>> SingularityFunction(x, a, n)
+        SingularityFunction(x, a, n)
+        >>> SingularityFunction(5, 3, 2)
+        4
+        >>> SingularityFunction(x, a, nan)
+        nan
+        >>> SingularityFunction(x, 3, 0).subs(x, 3)
+        1
+        >>> SingularityFunction(4, 1, 5)
+        243
+        >>> x = Symbol('x', positive = True)
+        >>> a = Symbol('a', negative = True)
+        >>> n = Symbol('n', nonnegative = True)
+        >>> SingularityFunction(x, a, n)
+        (-a + x)**n
+        >>> x = Symbol('x', negative = True)
+        >>> a = Symbol('a', positive = True)
+        >>> SingularityFunction(x, a, n)
+        0
+
+        """
+
+        x = variable
+        a = offset
+        n = exponent
+        shift = (x - a)
+
+        if fuzzy_not(im(shift).is_zero):
+            raise ValueError("Singularity Functions are defined only for Real Numbers.")
+        if fuzzy_not(im(n).is_zero):
+            raise ValueError("Singularity Functions are not defined for imaginary exponents.")
+        if shift is S.NaN or n is S.NaN:
+            return S.NaN
+        if (n + 2).is_negative:
+            raise ValueError("Singularity Functions are not defined for exponents less than -2.")
+        if shift.is_extended_negative:
+            return S.Zero
+        if n.is_nonnegative and shift.is_extended_nonnegative:
+            return (x - a)**n
+        if n in (S.NegativeOne, -2):
+            if shift.is_negative or shift.is_extended_positive:
+                return S.Zero
+            if shift.is_zero:
+                return oo
+
+    def _eval_rewrite_as_Piecewise(self, *args, **kwargs):
+        '''
+        Converts a Singularity Function expression into its Piecewise form.
+
+        '''
+        x, a, n = self.args
+
+        if n in (S.NegativeOne, S(-2)):
+            return Piecewise((oo, Eq((x - a), 0)), (0, True))
+        elif n.is_nonnegative:
+            return Piecewise(((x - a)**n, (x - a) > 0), (0, True))
+
+    def _eval_rewrite_as_Heaviside(self, *args, **kwargs):
+        '''
+        Rewrites a Singularity Function expression using Heavisides and DiracDeltas.
+
+        '''
+        x, a, n = self.args
+
+        if n == -2:
+            return diff(Heaviside(x - a), x.free_symbols.pop(), 2)
+        if n == -1:
+            return diff(Heaviside(x - a), x.free_symbols.pop(), 1)
+        if n.is_nonnegative:
+            return (x - a)**n*Heaviside(x - a)
+
+    def _eval_as_leading_term(self, x, logx=None, cdir=0):
+        z, a, n = self.args
+        shift = (z - a).subs(x, 0)
+        if n < 0:
+            return S.Zero
+        elif n.is_zero and shift.is_zero:
+            return S.Zero if cdir == -1 else S.One
+        elif shift.is_positive:
+            return shift**n
+        return S.Zero
+
+    def _eval_nseries(self, x, n, logx=None, cdir=0):
+        z, a, n = self.args
+        shift = (z - a).subs(x, 0)
+        if n < 0:
+            return S.Zero
+        elif n.is_zero and shift.is_zero:
+            return S.Zero if cdir == -1 else S.One
+        elif shift.is_positive:
+            return ((z - a)**n)._eval_nseries(x, n, logx=logx, cdir=cdir)
+        return S.Zero
+
+    _eval_rewrite_as_DiracDelta = _eval_rewrite_as_Heaviside
+    _eval_rewrite_as_HeavisideDiracDelta = _eval_rewrite_as_Heaviside

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/spherical_harmonics.py

@@ -0,0 +1,334 @@
+from sympy.core.expr import Expr
+from sympy.core.function import Function, ArgumentIndexError
+from sympy.core.numbers import I, pi
+from sympy.core.singleton import S
+from sympy.core.symbol import Dummy
+from sympy.functions import assoc_legendre
+from sympy.functions.combinatorial.factorials import factorial
+from sympy.functions.elementary.complexes import Abs, conjugate
+from sympy.functions.elementary.exponential import exp
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.elementary.trigonometric import sin, cos, cot
+
+_x = Dummy("x")
+
+class Ynm(Function):
+    r"""
+    Spherical harmonics defined as
+
+    .. math::
+        Y_n^m(\theta, \varphi) := \sqrt{\frac{(2n+1)(n-m)!}{4\pi(n+m)!}}
+                                  \exp(i m \varphi)
+                                  \mathrm{P}_n^m\left(\cos(\theta)\right)
+
+    Explanation
+    ===========
+
+    ``Ynm()`` gives the spherical harmonic function of order $n$ and $m$
+    in $\theta$ and $\varphi$, $Y_n^m(\theta, \varphi)$. The four
+    parameters are as follows: $n \geq 0$ an integer and $m$ an integer
+    such that $-n \leq m \leq n$ holds. The two angles are real-valued
+    with $\theta \in [0, \pi]$ and $\varphi \in [0, 2\pi]$.
+
+    Examples
+    ========
+
+    >>> from sympy import Ynm, Symbol, simplify
+    >>> from sympy.abc import n,m
+    >>> theta = Symbol("theta")
+    >>> phi = Symbol("phi")
+
+    >>> Ynm(n, m, theta, phi)
+    Ynm(n, m, theta, phi)
+
+    Several symmetries are known, for the order:
+
+    >>> Ynm(n, -m, theta, phi)
+    (-1)**m*exp(-2*I*m*phi)*Ynm(n, m, theta, phi)
+
+    As well as for the angles:
+
+    >>> Ynm(n, m, -theta, phi)
+    Ynm(n, m, theta, phi)
+
+    >>> Ynm(n, m, theta, -phi)
+    exp(-2*I*m*phi)*Ynm(n, m, theta, phi)
+
+    For specific integers $n$ and $m$ we can evaluate the harmonics
+    to more useful expressions:
+
+    >>> simplify(Ynm(0, 0, theta, phi).expand(func=True))
+    1/(2*sqrt(pi))
+
+    >>> simplify(Ynm(1, -1, theta, phi).expand(func=True))
+    sqrt(6)*exp(-I*phi)*sin(theta)/(4*sqrt(pi))
+
+    >>> simplify(Ynm(1, 0, theta, phi).expand(func=True))
+    sqrt(3)*cos(theta)/(2*sqrt(pi))
+
+    >>> simplify(Ynm(1, 1, theta, phi).expand(func=True))
+    -sqrt(6)*exp(I*phi)*sin(theta)/(4*sqrt(pi))
+
+    >>> simplify(Ynm(2, -2, theta, phi).expand(func=True))
+    sqrt(30)*exp(-2*I*phi)*sin(theta)**2/(8*sqrt(pi))
+
+    >>> simplify(Ynm(2, -1, theta, phi).expand(func=True))
+    sqrt(30)*exp(-I*phi)*sin(2*theta)/(8*sqrt(pi))
+
+    >>> simplify(Ynm(2, 0, theta, phi).expand(func=True))
+    sqrt(5)*(3*cos(theta)**2 - 1)/(4*sqrt(pi))
+
+    >>> simplify(Ynm(2, 1, theta, phi).expand(func=True))
+    -sqrt(30)*exp(I*phi)*sin(2*theta)/(8*sqrt(pi))
+
+    >>> simplify(Ynm(2, 2, theta, phi).expand(func=True))
+    sqrt(30)*exp(2*I*phi)*sin(theta)**2/(8*sqrt(pi))
+
+    We can differentiate the functions with respect
+    to both angles:
+
+    >>> from sympy import Ynm, Symbol, diff
+    >>> from sympy.abc import n,m
+    >>> theta = Symbol("theta")
+    >>> phi = Symbol("phi")
+
+    >>> diff(Ynm(n, m, theta, phi), theta)
+    m*cot(theta)*Ynm(n, m, theta, phi) + sqrt((-m + n)*(m + n + 1))*exp(-I*phi)*Ynm(n, m + 1, theta, phi)
+
+    >>> diff(Ynm(n, m, theta, phi), phi)
+    I*m*Ynm(n, m, theta, phi)
+
+    Further we can compute the complex conjugation:
+
+    >>> from sympy import Ynm, Symbol, conjugate
+    >>> from sympy.abc import n,m
+    >>> theta = Symbol("theta")
+    >>> phi = Symbol("phi")
+
+    >>> conjugate(Ynm(n, m, theta, phi))
+    (-1)**(2*m)*exp(-2*I*m*phi)*Ynm(n, m, theta, phi)
+
+    To get back the well known expressions in spherical
+    coordinates, we use full expansion:
+
+    >>> from sympy import Ynm, Symbol, expand_func
+    >>> from sympy.abc import n,m
+    >>> theta = Symbol("theta")
+    >>> phi = Symbol("phi")
+
+    >>> expand_func(Ynm(n, m, theta, phi))
+    sqrt((2*n + 1)*factorial(-m + n)/factorial(m + n))*exp(I*m*phi)*assoc_legendre(n, m, cos(theta))/(2*sqrt(pi))
+
+    See Also
+    ========
+
+    Ynm_c, Znm
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Spherical_harmonics
+    .. [2] https://mathworld.wolfram.com/SphericalHarmonic.html
+    .. [3] https://functions.wolfram.com/Polynomials/SphericalHarmonicY/
+    .. [4] https://dlmf.nist.gov/14.30
+
+    """
+
+    @classmethod
+    def eval(cls, n, m, theta, phi):
+        # Handle negative index m and arguments theta, phi
+        if m.could_extract_minus_sign():
+            m = -m
+            return S.NegativeOne**m * exp(-2*I*m*phi) * Ynm(n, m, theta, phi)
+        if theta.could_extract_minus_sign():
+            theta = -theta
+            return Ynm(n, m, theta, phi)
+        if phi.could_extract_minus_sign():
+            phi = -phi
+            return exp(-2*I*m*phi) * Ynm(n, m, theta, phi)
+
+        # TODO Add more simplififcation here
+
+    def _eval_expand_func(self, **hints):
+        n, m, theta, phi = self.args
+        rv = (sqrt((2*n + 1)/(4*pi) * factorial(n - m)/factorial(n + m)) *
+                exp(I*m*phi) * assoc_legendre(n, m, cos(theta)))
+        # We can do this because of the range of theta
+        return rv.subs(sqrt(-cos(theta)**2 + 1), sin(theta))
+
+    def fdiff(self, argindex=4):
+        if argindex == 1:
+            # Diff wrt n
+            raise ArgumentIndexError(self, argindex)
+        elif argindex == 2:
+            # Diff wrt m
+            raise ArgumentIndexError(self, argindex)
+        elif argindex == 3:
+            # Diff wrt theta
+            n, m, theta, phi = self.args
+            return (m * cot(theta) * Ynm(n, m, theta, phi) +
+                    sqrt((n - m)*(n + m + 1)) * exp(-I*phi) * Ynm(n, m + 1, theta, phi))
+        elif argindex == 4:
+            # Diff wrt phi
+            n, m, theta, phi = self.args
+            return I * m * Ynm(n, m, theta, phi)
+        else:
+            raise ArgumentIndexError(self, argindex)
+
+    def _eval_rewrite_as_polynomial(self, n, m, theta, phi, **kwargs):
+        # TODO: Make sure n \in N
+        # TODO: Assert |m| <= n ortherwise we should return 0
+        return self.expand(func=True)
+
+    def _eval_rewrite_as_sin(self, n, m, theta, phi, **kwargs):
+        return self.rewrite(cos)
+
+    def _eval_rewrite_as_cos(self, n, m, theta, phi, **kwargs):
+        # This method can be expensive due to extensive use of simplification!
+        from sympy.simplify import simplify, trigsimp
+        # TODO: Make sure n \in N
+        # TODO: Assert |m| <= n ortherwise we should return 0
+        term = simplify(self.expand(func=True))
+        # We can do this because of the range of theta
+        term = term.xreplace({Abs(sin(theta)):sin(theta)})
+        return simplify(trigsimp(term))
+
+    def _eval_conjugate(self):
+        # TODO: Make sure theta \in R and phi \in R
+        n, m, theta, phi = self.args
+        return S.NegativeOne**m * self.func(n, -m, theta, phi)
+
+    def as_real_imag(self, deep=True, **hints):
+        # TODO: Handle deep and hints
+        n, m, theta, phi = self.args
+        re = (sqrt((2*n + 1)/(4*pi) * factorial(n - m)/factorial(n + m)) *
+              cos(m*phi) * assoc_legendre(n, m, cos(theta)))
+        im = (sqrt((2*n + 1)/(4*pi) * factorial(n - m)/factorial(n + m)) *
+              sin(m*phi) * assoc_legendre(n, m, cos(theta)))
+        return (re, im)
+
+    def _eval_evalf(self, prec):
+        # Note: works without this function by just calling
+        #       mpmath for Legendre polynomials. But using
+        #       the dedicated function directly is cleaner.
+        from mpmath import mp, workprec
+        n = self.args[0]._to_mpmath(prec)
+        m = self.args[1]._to_mpmath(prec)
+        theta = self.args[2]._to_mpmath(prec)
+        phi = self.args[3]._to_mpmath(prec)
+        with workprec(prec):
+            res = mp.spherharm(n, m, theta, phi)
+        return Expr._from_mpmath(res, prec)
+
+
+def Ynm_c(n, m, theta, phi):
+    r"""
+    Conjugate spherical harmonics defined as
+
+    .. math::
+        \overline{Y_n^m(\theta, \varphi)} := (-1)^m Y_n^{-m}(\theta, \varphi).
+
+    Examples
+    ========
+
+    >>> from sympy import Ynm_c, Symbol, simplify
+    >>> from sympy.abc import n,m
+    >>> theta = Symbol("theta")
+    >>> phi = Symbol("phi")
+    >>> Ynm_c(n, m, theta, phi)
+    (-1)**(2*m)*exp(-2*I*m*phi)*Ynm(n, m, theta, phi)
+    >>> Ynm_c(n, m, -theta, phi)
+    (-1)**(2*m)*exp(-2*I*m*phi)*Ynm(n, m, theta, phi)
+
+    For specific integers $n$ and $m$ we can evaluate the harmonics
+    to more useful expressions:
+
+    >>> simplify(Ynm_c(0, 0, theta, phi).expand(func=True))
+    1/(2*sqrt(pi))
+    >>> simplify(Ynm_c(1, -1, theta, phi).expand(func=True))
+    sqrt(6)*exp(I*(-phi + 2*conjugate(phi)))*sin(theta)/(4*sqrt(pi))
+
+    See Also
+    ========
+
+    Ynm, Znm
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Spherical_harmonics
+    .. [2] https://mathworld.wolfram.com/SphericalHarmonic.html
+    .. [3] https://functions.wolfram.com/Polynomials/SphericalHarmonicY/
+
+    """
+    return conjugate(Ynm(n, m, theta, phi))
+
+
+class Znm(Function):
+    r"""
+    Real spherical harmonics defined as
+
+    .. math::
+
+        Z_n^m(\theta, \varphi) :=
+        \begin{cases}
+          \frac{Y_n^m(\theta, \varphi) + \overline{Y_n^m(\theta, \varphi)}}{\sqrt{2}} &\quad m > 0 \\
+          Y_n^m(\theta, \varphi) &\quad m = 0 \\
+          \frac{Y_n^m(\theta, \varphi) - \overline{Y_n^m(\theta, \varphi)}}{i \sqrt{2}} &\quad m < 0 \\
+        \end{cases}
+
+    which gives in simplified form
+
+    .. math::
+
+        Z_n^m(\theta, \varphi) =
+        \begin{cases}
+          \frac{Y_n^m(\theta, \varphi) + (-1)^m Y_n^{-m}(\theta, \varphi)}{\sqrt{2}} &\quad m > 0 \\
+          Y_n^m(\theta, \varphi) &\quad m = 0 \\
+          \frac{Y_n^m(\theta, \varphi) - (-1)^m Y_n^{-m}(\theta, \varphi)}{i \sqrt{2}} &\quad m < 0 \\
+        \end{cases}
+
+    Examples
+    ========
+
+    >>> from sympy import Znm, Symbol, simplify
+    >>> from sympy.abc import n, m
+    >>> theta = Symbol("theta")
+    >>> phi = Symbol("phi")
+    >>> Znm(n, m, theta, phi)
+    Znm(n, m, theta, phi)
+
+    For specific integers n and m we can evaluate the harmonics
+    to more useful expressions:
+
+    >>> simplify(Znm(0, 0, theta, phi).expand(func=True))
+    1/(2*sqrt(pi))
+    >>> simplify(Znm(1, 1, theta, phi).expand(func=True))
+    -sqrt(3)*sin(theta)*cos(phi)/(2*sqrt(pi))
+    >>> simplify(Znm(2, 1, theta, phi).expand(func=True))
+    -sqrt(15)*sin(2*theta)*cos(phi)/(4*sqrt(pi))
+
+    See Also
+    ========
+
+    Ynm, Ynm_c
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Spherical_harmonics
+    .. [2] https://mathworld.wolfram.com/SphericalHarmonic.html
+    .. [3] https://functions.wolfram.com/Polynomials/SphericalHarmonicY/
+
+    """
+
+    @classmethod
+    def eval(cls, n, m, theta, phi):
+        if m.is_positive:
+            zz = (Ynm(n, m, theta, phi) + Ynm_c(n, m, theta, phi)) / sqrt(2)
+            return zz
+        elif m.is_zero:
+            return Ynm(n, m, theta, phi)
+        elif m.is_negative:
+            zz = (Ynm(n, m, theta, phi) - Ynm_c(n, m, theta, phi)) / (sqrt(2)*I)
+            return zz

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/tensor_functions.py

@@ -0,0 +1,474 @@
+from math import prod
+
+from sympy.core import S, Integer
+from sympy.core.function import Function
+from sympy.core.logic import fuzzy_not
+from sympy.core.relational import Ne
+from sympy.core.sorting import default_sort_key
+from sympy.external.gmpy import SYMPY_INTS
+from sympy.functions.combinatorial.factorials import factorial
+from sympy.functions.elementary.piecewise import Piecewise
+from sympy.utilities.iterables import has_dups
+
+###############################################################################
+###################### Kronecker Delta, Levi-Civita etc. ######################
+###############################################################################
+
+
+def Eijk(*args, **kwargs):
+    """
+    Represent the Levi-Civita symbol.
+
+    This is a compatibility wrapper to ``LeviCivita()``.
+
+    See Also
+    ========
+
+    LeviCivita
+
+    """
+    return LeviCivita(*args, **kwargs)
+
+
+def eval_levicivita(*args):
+    """Evaluate Levi-Civita symbol."""
+    n = len(args)
+    return prod(
+        prod(args[j] - args[i] for j in range(i + 1, n))
+        / factorial(i) for i in range(n))
+    # converting factorial(i) to int is slightly faster
+
+
+class LeviCivita(Function):
+    """
+    Represent the Levi-Civita symbol.
+
+    Explanation
+    ===========
+
+    For even permutations of indices it returns 1, for odd permutations -1, and
+    for everything else (a repeated index) it returns 0.
+
+    Thus it represents an alternating pseudotensor.
+
+    Examples
+    ========
+
+    >>> from sympy import LeviCivita
+    >>> from sympy.abc import i, j, k
+    >>> LeviCivita(1, 2, 3)
+    1
+    >>> LeviCivita(1, 3, 2)
+    -1
+    >>> LeviCivita(1, 2, 2)
+    0
+    >>> LeviCivita(i, j, k)
+    LeviCivita(i, j, k)
+    >>> LeviCivita(i, j, i)
+    0
+
+    See Also
+    ========
+
+    Eijk
+
+    """
+
+    is_integer = True
+
+    @classmethod
+    def eval(cls, *args):
+        if all(isinstance(a, (SYMPY_INTS, Integer)) for a in args):
+            return eval_levicivita(*args)
+        if has_dups(args):
+            return S.Zero
+
+    def doit(self, **hints):
+        return eval_levicivita(*self.args)
+
+
+class KroneckerDelta(Function):
+    """
+    The discrete, or Kronecker, delta function.
+
+    Explanation
+    ===========
+
+    A function that takes in two integers $i$ and $j$. It returns $0$ if $i$
+    and $j$ are not equal, or it returns $1$ if $i$ and $j$ are equal.
+
+    Examples
+    ========
+
+    An example with integer indices:
+
+        >>> from sympy import KroneckerDelta
+        >>> KroneckerDelta(1, 2)
+        0
+        >>> KroneckerDelta(3, 3)
+        1
+
+    Symbolic indices:
+
+        >>> from sympy.abc import i, j, k
+        >>> KroneckerDelta(i, j)
+        KroneckerDelta(i, j)
+        >>> KroneckerDelta(i, i)
+        1
+        >>> KroneckerDelta(i, i + 1)
+        0
+        >>> KroneckerDelta(i, i + 1 + k)
+        KroneckerDelta(i, i + k + 1)
+
+    Parameters
+    ==========
+
+    i : Number, Symbol
+        The first index of the delta function.
+    j : Number, Symbol
+        The second index of the delta function.
+
+    See Also
+    ========
+
+    eval
+    DiracDelta
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Kronecker_delta
+
+    """
+
+    is_integer = True
+
+    @classmethod
+    def eval(cls, i, j, delta_range=None):
+        """
+        Evaluates the discrete delta function.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta
+        >>> from sympy.abc import i, j, k
+
+        >>> KroneckerDelta(i, j)
+        KroneckerDelta(i, j)
+        >>> KroneckerDelta(i, i)
+        1
+        >>> KroneckerDelta(i, i + 1)
+        0
+        >>> KroneckerDelta(i, i + 1 + k)
+        KroneckerDelta(i, i + k + 1)
+
+        # indirect doctest
+
+        """
+
+        if delta_range is not None:
+            dinf, dsup = delta_range
+            if (dinf - i > 0) == True:
+                return S.Zero
+            if (dinf - j > 0) == True:
+                return S.Zero
+            if (dsup - i < 0) == True:
+                return S.Zero
+            if (dsup - j < 0) == True:
+                return S.Zero
+
+        diff = i - j
+        if diff.is_zero:
+            return S.One
+        elif fuzzy_not(diff.is_zero):
+            return S.Zero
+
+        if i.assumptions0.get("below_fermi") and \
+                j.assumptions0.get("above_fermi"):
+            return S.Zero
+        if j.assumptions0.get("below_fermi") and \
+                i.assumptions0.get("above_fermi"):
+            return S.Zero
+        # to make KroneckerDelta canonical
+        # following lines will check if inputs are in order
+        # if not, will return KroneckerDelta with correct order
+        if i != min(i, j, key=default_sort_key):
+            if delta_range:
+                return cls(j, i, delta_range)
+            else:
+                return cls(j, i)
+
+    @property
+    def delta_range(self):
+        if len(self.args) > 2:
+            return self.args[2]
+
+    def _eval_power(self, expt):
+        if expt.is_positive:
+            return self
+        if expt.is_negative and expt is not S.NegativeOne:
+            return 1/self
+
+    @property
+    def is_above_fermi(self):
+        """
+        True if Delta can be non-zero above fermi.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> q = Symbol('q')
+        >>> KroneckerDelta(p, a).is_above_fermi
+        True
+        >>> KroneckerDelta(p, i).is_above_fermi
+        False
+        >>> KroneckerDelta(p, q).is_above_fermi
+        True
+
+        See Also
+        ========
+
+        is_below_fermi, is_only_below_fermi, is_only_above_fermi
+
+        """
+        if self.args[0].assumptions0.get("below_fermi"):
+            return False
+        if self.args[1].assumptions0.get("below_fermi"):
+            return False
+        return True
+
+    @property
+    def is_below_fermi(self):
+        """
+        True if Delta can be non-zero below fermi.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> q = Symbol('q')
+        >>> KroneckerDelta(p, a).is_below_fermi
+        False
+        >>> KroneckerDelta(p, i).is_below_fermi
+        True
+        >>> KroneckerDelta(p, q).is_below_fermi
+        True
+
+        See Also
+        ========
+
+        is_above_fermi, is_only_above_fermi, is_only_below_fermi
+
+        """
+        if self.args[0].assumptions0.get("above_fermi"):
+            return False
+        if self.args[1].assumptions0.get("above_fermi"):
+            return False
+        return True
+
+    @property
+    def is_only_above_fermi(self):
+        """
+        True if Delta is restricted to above fermi.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> q = Symbol('q')
+        >>> KroneckerDelta(p, a).is_only_above_fermi
+        True
+        >>> KroneckerDelta(p, q).is_only_above_fermi
+        False
+        >>> KroneckerDelta(p, i).is_only_above_fermi
+        False
+
+        See Also
+        ========
+
+        is_above_fermi, is_below_fermi, is_only_below_fermi
+
+        """
+        return ( self.args[0].assumptions0.get("above_fermi")
+                or
+                self.args[1].assumptions0.get("above_fermi")
+                ) or False
+
+    @property
+    def is_only_below_fermi(self):
+        """
+        True if Delta is restricted to below fermi.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> q = Symbol('q')
+        >>> KroneckerDelta(p, i).is_only_below_fermi
+        True
+        >>> KroneckerDelta(p, q).is_only_below_fermi
+        False
+        >>> KroneckerDelta(p, a).is_only_below_fermi
+        False
+
+        See Also
+        ========
+
+        is_above_fermi, is_below_fermi, is_only_above_fermi
+
+        """
+        return ( self.args[0].assumptions0.get("below_fermi")
+                or
+                self.args[1].assumptions0.get("below_fermi")
+                ) or False
+
+    @property
+    def indices_contain_equal_information(self):
+        """
+        Returns True if indices are either both above or below fermi.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> q = Symbol('q')
+        >>> KroneckerDelta(p, q).indices_contain_equal_information
+        True
+        >>> KroneckerDelta(p, q+1).indices_contain_equal_information
+        True
+        >>> KroneckerDelta(i, p).indices_contain_equal_information
+        False
+
+        """
+        if (self.args[0].assumptions0.get("below_fermi") and
+                self.args[1].assumptions0.get("below_fermi")):
+            return True
+        if (self.args[0].assumptions0.get("above_fermi")
+                and self.args[1].assumptions0.get("above_fermi")):
+            return True
+
+        # if both indices are general we are True, else false
+        return self.is_below_fermi and self.is_above_fermi
+
+    @property
+    def preferred_index(self):
+        """
+        Returns the index which is preferred to keep in the final expression.
+
+        Explanation
+        ===========
+
+        The preferred index is the index with more information regarding fermi
+        level. If indices contain the same information, 'a' is preferred before
+        'b'.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> j = Symbol('j', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> KroneckerDelta(p, i).preferred_index
+        i
+        >>> KroneckerDelta(p, a).preferred_index
+        a
+        >>> KroneckerDelta(i, j).preferred_index
+        i
+
+        See Also
+        ========
+
+        killable_index
+
+        """
+        if self._get_preferred_index():
+            return self.args[1]
+        else:
+            return self.args[0]
+
+    @property
+    def killable_index(self):
+        """
+        Returns the index which is preferred to substitute in the final
+        expression.
+
+        Explanation
+        ===========
+
+        The index to substitute is the index with less information regarding
+        fermi level. If indices contain the same information, 'a' is preferred
+        before 'b'.
+
+        Examples
+        ========
+
+        >>> from sympy import KroneckerDelta, Symbol
+        >>> a = Symbol('a', above_fermi=True)
+        >>> i = Symbol('i', below_fermi=True)
+        >>> j = Symbol('j', below_fermi=True)
+        >>> p = Symbol('p')
+        >>> KroneckerDelta(p, i).killable_index
+        p
+        >>> KroneckerDelta(p, a).killable_index
+        p
+        >>> KroneckerDelta(i, j).killable_index
+        j
+
+        See Also
+        ========
+
+        preferred_index
+
+        """
+        if self._get_preferred_index():
+            return self.args[0]
+        else:
+            return self.args[1]
+
+    def _get_preferred_index(self):
+        """
+        Returns the index which is preferred to keep in the final expression.
+
+        The preferred index is the index with more information regarding fermi
+        level. If indices contain the same information, index 0 is returned.
+
+        """
+        if not self.is_above_fermi:
+            if self.args[0].assumptions0.get("below_fermi"):
+                return 0
+            else:
+                return 1
+        elif not self.is_below_fermi:
+            if self.args[0].assumptions0.get("above_fermi"):
+                return 0
+            else:
+                return 1
+        else:
+            return 0
+
+    @property
+    def indices(self):
+        return self.args[0:2]
+
+    def _eval_rewrite_as_Piecewise(self, *args, **kwargs):
+        i, j = args
+        return Piecewise((0, Ne(i, j)), (1, True))

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/tests/test_beta_functions.py

@@ -0,0 +1,89 @@
+from sympy.core.function import (diff, expand_func)
+from sympy.core.numbers import I, Rational, pi
+from sympy.core.singleton import S
+from sympy.core.symbol import (Dummy, symbols)
+from sympy.functions.combinatorial.numbers import catalan
+from sympy.functions.elementary.complexes import conjugate
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.special.beta_functions import (beta, betainc, betainc_regularized)
+from sympy.functions.special.gamma_functions import gamma, polygamma
+from sympy.functions.special.hyper import hyper
+from sympy.integrals.integrals import Integral
+from sympy.core.function import ArgumentIndexError
+from sympy.core.expr import unchanged
+from sympy.testing.pytest import raises
+
+
+def test_beta():
+    x, y = symbols('x y')
+    t = Dummy('t')
+
+    assert unchanged(beta, x, y)
+    assert unchanged(beta, x, x)
+
+    assert beta(5, -3).is_real == True
+    assert beta(3, y).is_real is None
+
+    assert expand_func(beta(x, y)) == gamma(x)*gamma(y)/gamma(x + y)
+    assert expand_func(beta(x, y) - beta(y, x)) == 0  # Symmetric
+    assert expand_func(beta(x, y)) == expand_func(beta(x, y + 1) + beta(x + 1, y)).simplify()
+
+    assert diff(beta(x, y), x) == beta(x, y)*(polygamma(0, x) - polygamma(0, x + y))
+    assert diff(beta(x, y), y) == beta(x, y)*(polygamma(0, y) - polygamma(0, x + y))
+
+    assert conjugate(beta(x, y)) == beta(conjugate(x), conjugate(y))
+
+    raises(ArgumentIndexError, lambda: beta(x, y).fdiff(3))
+
+    assert beta(x, y).rewrite(gamma) == gamma(x)*gamma(y)/gamma(x + y)
+    assert beta(x).rewrite(gamma) == gamma(x)**2/gamma(2*x)
+    assert beta(x, y).rewrite(Integral).dummy_eq(Integral(t**(x - 1) * (1 - t)**(y - 1), (t, 0, 1)))
+    assert beta(Rational(-19, 10), Rational(-1, 10)) == S.Zero
+    assert beta(Rational(-19, 10), Rational(-9, 10)) == \
+        800*2**(S(4)/5)*sqrt(pi)*gamma(S.One/10)/(171*gamma(-S(7)/5))
+    assert beta(Rational(19, 10), Rational(29, 10)) == 100/(551*catalan(Rational(19, 10)))
+    assert beta(1, 0) == S.ComplexInfinity
+    assert beta(0, 1) == S.ComplexInfinity
+    assert beta(2, 3) == S.One/12
+    assert unchanged(beta, x, x + 1)
+    assert unchanged(beta, x, 1)
+    assert unchanged(beta, 1, y)
+    assert beta(x, x + 1).doit() == 1/(x*(x+1)*catalan(x))
+    assert beta(1, y).doit() == 1/y
+    assert beta(x, 1).doit() == 1/x
+    assert beta(Rational(-19, 10), Rational(-1, 10), evaluate=False).doit() == S.Zero
+    assert beta(2) == beta(2, 2)
+    assert beta(x, evaluate=False) != beta(x, x)
+    assert beta(x, evaluate=False).doit() == beta(x, x)
+
+
+def test_betainc():
+    a, b, x1, x2 = symbols('a b x1 x2')
+
+    assert unchanged(betainc, a, b, x1, x2)
+    assert unchanged(betainc, a, b, 0, x1)
+
+    assert betainc(1, 2, 0, -5).is_real == True
+    assert betainc(1, 2, 0, x2).is_real is None
+    assert conjugate(betainc(I, 2, 3 - I, 1 + 4*I)) == betainc(-I, 2, 3 + I, 1 - 4*I)
+
+    assert betainc(a, b, 0, 1).rewrite(Integral).dummy_eq(beta(a, b).rewrite(Integral))
+    assert betainc(1, 2, 0, x2).rewrite(hyper) == x2*hyper((1, -1), (2,), x2)
+
+    assert betainc(1, 2, 3, 3).evalf() == 0
+
+
+def test_betainc_regularized():
+    a, b, x1, x2 = symbols('a b x1 x2')
+
+    assert unchanged(betainc_regularized, a, b, x1, x2)
+    assert unchanged(betainc_regularized, a, b, 0, x1)
+
+    assert betainc_regularized(3, 5, 0, -1).is_real == True
+    assert betainc_regularized(3, 5, 0, x2).is_real is None
+    assert conjugate(betainc_regularized(3*I, 1, 2 + I, 1 + 2*I)) == betainc_regularized(-3*I, 1, 2 - I, 1 - 2*I)
+
+    assert betainc_regularized(a, b, 0, 1).rewrite(Integral) == 1
+    assert betainc_regularized(1, 2, x1, x2).rewrite(hyper) == 2*x2*hyper((1, -1), (2,), x2) - 2*x1*hyper((1, -1), (2,), x1)
+
+    assert betainc_regularized(4, 1, 5, 5).evalf() == 0

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/tests/test_elliptic_integrals.py

@@ -0,0 +1,179 @@
+from sympy.core.numbers import (I, Rational, oo, pi, zoo)
+from sympy.core.singleton import S
+from sympy.core.symbol import (Dummy, Symbol)
+from sympy.functions.elementary.hyperbolic import atanh
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.elementary.trigonometric import (sin, tan)
+from sympy.functions.special.gamma_functions import gamma
+from sympy.functions.special.hyper import (hyper, meijerg)
+from sympy.integrals.integrals import Integral
+from sympy.series.order import O
+from sympy.functions.special.elliptic_integrals import (elliptic_k as K,
+    elliptic_f as F, elliptic_e as E, elliptic_pi as P)
+from sympy.core.random import (test_derivative_numerically as td,
+                                      random_complex_number as randcplx,
+                                      verify_numerically as tn)
+from sympy.abc import z, m, n
+
+i = Symbol('i', integer=True)
+j = Symbol('k', integer=True, positive=True)
+t = Dummy('t')
+
+def test_K():
+    assert K(0) == pi/2
+    assert K(S.Half) == 8*pi**Rational(3, 2)/gamma(Rational(-1, 4))**2
+    assert K(1) is zoo
+    assert K(-1) == gamma(Rational(1, 4))**2/(4*sqrt(2*pi))
+    assert K(oo) == 0
+    assert K(-oo) == 0
+    assert K(I*oo) == 0
+    assert K(-I*oo) == 0
+    assert K(zoo) == 0
+
+    assert K(z).diff(z) == (E(z) - (1 - z)*K(z))/(2*z*(1 - z))
+    assert td(K(z), z)
+
+    zi = Symbol('z', real=False)
+    assert K(zi).conjugate() == K(zi.conjugate())
+    zr = Symbol('z', negative=True)
+    assert K(zr).conjugate() == K(zr)
+
+    assert K(z).rewrite(hyper) == \
+        (pi/2)*hyper((S.Half, S.Half), (S.One,), z)
+    assert tn(K(z), (pi/2)*hyper((S.Half, S.Half), (S.One,), z))
+    assert K(z).rewrite(meijerg) == \
+        meijerg(((S.Half, S.Half), []), ((S.Zero,), (S.Zero,)), -z)/2
+    assert tn(K(z), meijerg(((S.Half, S.Half), []), ((S.Zero,), (S.Zero,)), -z)/2)
+
+    assert K(z).series(z) == pi/2 + pi*z/8 + 9*pi*z**2/128 + \
+        25*pi*z**3/512 + 1225*pi*z**4/32768 + 3969*pi*z**5/131072 + O(z**6)
+
+    assert K(m).rewrite(Integral).dummy_eq(
+        Integral(1/sqrt(1 - m*sin(t)**2), (t, 0, pi/2)))
+
+def test_F():
+    assert F(z, 0) == z
+    assert F(0, m) == 0
+    assert F(pi*i/2, m) == i*K(m)
+    assert F(z, oo) == 0
+    assert F(z, -oo) == 0
+
+    assert F(-z, m) == -F(z, m)
+
+    assert F(z, m).diff(z) == 1/sqrt(1 - m*sin(z)**2)
+    assert F(z, m).diff(m) == E(z, m)/(2*m*(1 - m)) - F(z, m)/(2*m) - \
+        sin(2*z)/(4*(1 - m)*sqrt(1 - m*sin(z)**2))
+    r = randcplx()
+    assert td(F(z, r), z)
+    assert td(F(r, m), m)
+
+    mi = Symbol('m', real=False)
+    assert F(z, mi).conjugate() == F(z.conjugate(), mi.conjugate())
+    mr = Symbol('m', negative=True)
+    assert F(z, mr).conjugate() == F(z.conjugate(), mr)
+
+    assert F(z, m).series(z) == \
+        z + z**5*(3*m**2/40 - m/30) + m*z**3/6 + O(z**6)
+
+    assert F(z, m).rewrite(Integral).dummy_eq(
+        Integral(1/sqrt(1 - m*sin(t)**2), (t, 0, z)))
+
+def test_E():
+    assert E(z, 0) == z
+    assert E(0, m) == 0
+    assert E(i*pi/2, m) == i*E(m)
+    assert E(z, oo) is zoo
+    assert E(z, -oo) is zoo
+    assert E(0) == pi/2
+    assert E(1) == 1
+    assert E(oo) == I*oo
+    assert E(-oo) is oo
+    assert E(zoo) is zoo
+
+    assert E(-z, m) == -E(z, m)
+
+    assert E(z, m).diff(z) == sqrt(1 - m*sin(z)**2)
+    assert E(z, m).diff(m) == (E(z, m) - F(z, m))/(2*m)
+    assert E(z).diff(z) == (E(z) - K(z))/(2*z)
+    r = randcplx()
+    assert td(E(r, m), m)
+    assert td(E(z, r), z)
+    assert td(E(z), z)
+
+    mi = Symbol('m', real=False)
+    assert E(z, mi).conjugate() == E(z.conjugate(), mi.conjugate())
+    assert E(mi).conjugate() == E(mi.conjugate())
+    mr = Symbol('m', negative=True)
+    assert E(z, mr).conjugate() == E(z.conjugate(), mr)
+    assert E(mr).conjugate() == E(mr)
+
+    assert E(z).rewrite(hyper) == (pi/2)*hyper((Rational(-1, 2), S.Half), (S.One,), z)
+    assert tn(E(z), (pi/2)*hyper((Rational(-1, 2), S.Half), (S.One,), z))
+    assert E(z).rewrite(meijerg) == \
+        -meijerg(((S.Half, Rational(3, 2)), []), ((S.Zero,), (S.Zero,)), -z)/4
+    assert tn(E(z), -meijerg(((S.Half, Rational(3, 2)), []), ((S.Zero,), (S.Zero,)), -z)/4)
+
+    assert E(z, m).series(z) == \
+        z + z**5*(-m**2/40 + m/30) - m*z**3/6 + O(z**6)
+    assert E(z).series(z) == pi/2 - pi*z/8 - 3*pi*z**2/128 - \
+        5*pi*z**3/512 - 175*pi*z**4/32768 - 441*pi*z**5/131072 + O(z**6)
+
+    assert E(z, m).rewrite(Integral).dummy_eq(
+        Integral(sqrt(1 - m*sin(t)**2), (t, 0, z)))
+    assert E(m).rewrite(Integral).dummy_eq(
+        Integral(sqrt(1 - m*sin(t)**2), (t, 0, pi/2)))
+
+def test_P():
+    assert P(0, z, m) == F(z, m)
+    assert P(1, z, m) == F(z, m) + \
+        (sqrt(1 - m*sin(z)**2)*tan(z) - E(z, m))/(1 - m)
+    assert P(n, i*pi/2, m) == i*P(n, m)
+    assert P(n, z, 0) == atanh(sqrt(n - 1)*tan(z))/sqrt(n - 1)
+    assert P(n, z, n) == F(z, n) - P(1, z, n) + tan(z)/sqrt(1 - n*sin(z)**2)
+    assert P(oo, z, m) == 0
+    assert P(-oo, z, m) == 0
+    assert P(n, z, oo) == 0
+    assert P(n, z, -oo) == 0
+    assert P(0, m) == K(m)
+    assert P(1, m) is zoo
+    assert P(n, 0) == pi/(2*sqrt(1 - n))
+    assert P(2, 1) is -oo
+    assert P(-1, 1) is oo
+    assert P(n, n) == E(n)/(1 - n)
+
+    assert P(n, -z, m) == -P(n, z, m)
+
+    ni, mi = Symbol('n', real=False), Symbol('m', real=False)
+    assert P(ni, z, mi).conjugate() == \
+        P(ni.conjugate(), z.conjugate(), mi.conjugate())
+    nr, mr = Symbol('n', negative=True), \
+        Symbol('m', negative=True)
+    assert P(nr, z, mr).conjugate() == P(nr, z.conjugate(), mr)
+    assert P(n, m).conjugate() == P(n.conjugate(), m.conjugate())
+
+    assert P(n, z, m).diff(n) == (E(z, m) + (m - n)*F(z, m)/n +
+        (n**2 - m)*P(n, z, m)/n - n*sqrt(1 -
+            m*sin(z)**2)*sin(2*z)/(2*(1 - n*sin(z)**2)))/(2*(m - n)*(n - 1))
+    assert P(n, z, m).diff(z) == 1/(sqrt(1 - m*sin(z)**2)*(1 - n*sin(z)**2))
+    assert P(n, z, m).diff(m) == (E(z, m)/(m - 1) + P(n, z, m) -
+        m*sin(2*z)/(2*(m - 1)*sqrt(1 - m*sin(z)**2)))/(2*(n - m))
+    assert P(n, m).diff(n) == (E(m) + (m - n)*K(m)/n +
+        (n**2 - m)*P(n, m)/n)/(2*(m - n)*(n - 1))
+    assert P(n, m).diff(m) == (E(m)/(m - 1) + P(n, m))/(2*(n - m))
+
+    # These tests fail due to
+    # https://github.com/fredrik-johansson/mpmath/issues/571#issuecomment-777201962
+    # https://github.com/sympy/sympy/issues/20933#issuecomment-777080385
+    #
+    # rx, ry = randcplx(), randcplx()
+    # assert td(P(n, rx, ry), n)
+    # assert td(P(rx, z, ry), z)
+    # assert td(P(rx, ry, m), m)
+
+    assert P(n, z, m).series(z) == z + z**3*(m/6 + n/3) + \
+        z**5*(3*m**2/40 + m*n/10 - m/30 + n**2/5 - n/15) + O(z**6)
+
+    assert P(n, z, m).rewrite(Integral).dummy_eq(
+        Integral(1/((1 - n*sin(t)**2)*sqrt(1 - m*sin(t)**2)), (t, 0, z)))
+    assert P(n, m).rewrite(Integral).dummy_eq(
+        Integral(1/((1 - n*sin(t)**2)*sqrt(1 - m*sin(t)**2)), (t, 0, pi/2)))

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/tests/test_spherical_harmonics.py

@@ -0,0 +1,66 @@
+from sympy.core.function import diff
+from sympy.core.numbers import (I, pi)
+from sympy.core.symbol import Symbol
+from sympy.functions.elementary.complexes import conjugate
+from sympy.functions.elementary.exponential import exp
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.elementary.trigonometric import (cos, cot, sin)
+from sympy.functions.special.spherical_harmonics import Ynm, Znm, Ynm_c
+
+
+def test_Ynm():
+    # https://en.wikipedia.org/wiki/Spherical_harmonics
+    th, ph = Symbol("theta", real=True), Symbol("phi", real=True)
+    from sympy.abc import n,m
+
+    assert Ynm(0, 0, th, ph).expand(func=True) == 1/(2*sqrt(pi))
+    assert Ynm(1, -1, th, ph) == -exp(-2*I*ph)*Ynm(1, 1, th, ph)
+    assert Ynm(1, -1, th, ph).expand(func=True) == sqrt(6)*sin(th)*exp(-I*ph)/(4*sqrt(pi))
+    assert Ynm(1, 0, th, ph).expand(func=True) == sqrt(3)*cos(th)/(2*sqrt(pi))
+    assert Ynm(1, 1, th, ph).expand(func=True) == -sqrt(6)*sin(th)*exp(I*ph)/(4*sqrt(pi))
+    assert Ynm(2, 0, th, ph).expand(func=True) == 3*sqrt(5)*cos(th)**2/(4*sqrt(pi)) - sqrt(5)/(4*sqrt(pi))
+    assert Ynm(2, 1, th, ph).expand(func=True) == -sqrt(30)*sin(th)*exp(I*ph)*cos(th)/(4*sqrt(pi))
+    assert Ynm(2, -2, th, ph).expand(func=True) == (-sqrt(30)*exp(-2*I*ph)*cos(th)**2/(8*sqrt(pi))
+                                                    + sqrt(30)*exp(-2*I*ph)/(8*sqrt(pi)))
+    assert Ynm(2, 2, th, ph).expand(func=True) == (-sqrt(30)*exp(2*I*ph)*cos(th)**2/(8*sqrt(pi))
+                                                   + sqrt(30)*exp(2*I*ph)/(8*sqrt(pi)))
+
+    assert diff(Ynm(n, m, th, ph), th) == (m*cot(th)*Ynm(n, m, th, ph)
+                                           + sqrt((-m + n)*(m + n + 1))*exp(-I*ph)*Ynm(n, m + 1, th, ph))
+    assert diff(Ynm(n, m, th, ph), ph) == I*m*Ynm(n, m, th, ph)
+
+    assert conjugate(Ynm(n, m, th, ph)) == (-1)**(2*m)*exp(-2*I*m*ph)*Ynm(n, m, th, ph)
+
+    assert Ynm(n, m, -th, ph) == Ynm(n, m, th, ph)
+    assert Ynm(n, m, th, -ph) == exp(-2*I*m*ph)*Ynm(n, m, th, ph)
+    assert Ynm(n, -m, th, ph) == (-1)**m*exp(-2*I*m*ph)*Ynm(n, m, th, ph)
+
+
+def test_Ynm_c():
+    th, ph = Symbol("theta", real=True), Symbol("phi", real=True)
+    from sympy.abc import n,m
+
+    assert Ynm_c(n, m, th, ph) == (-1)**(2*m)*exp(-2*I*m*ph)*Ynm(n, m, th, ph)
+
+
+def test_Znm():
+    # https://en.wikipedia.org/wiki/Solid_harmonics#List_of_lowest_functions
+    th, ph = Symbol("theta", real=True), Symbol("phi", real=True)
+
+    assert Znm(0, 0, th, ph) == Ynm(0, 0, th, ph)
+    assert Znm(1, -1, th, ph) == (-sqrt(2)*I*(Ynm(1, 1, th, ph)
+                                  - exp(-2*I*ph)*Ynm(1, 1, th, ph))/2)
+    assert Znm(1, 0, th, ph) == Ynm(1, 0, th, ph)
+    assert Znm(1, 1, th, ph) == (sqrt(2)*(Ynm(1, 1, th, ph)
+                                 + exp(-2*I*ph)*Ynm(1, 1, th, ph))/2)
+    assert Znm(0, 0, th, ph).expand(func=True) == 1/(2*sqrt(pi))
+    assert Znm(1, -1, th, ph).expand(func=True) == (sqrt(3)*I*sin(th)*exp(I*ph)/(4*sqrt(pi))
+                                                    - sqrt(3)*I*sin(th)*exp(-I*ph)/(4*sqrt(pi)))
+    assert Znm(1, 0, th, ph).expand(func=True) == sqrt(3)*cos(th)/(2*sqrt(pi))
+    assert Znm(1, 1, th, ph).expand(func=True) == (-sqrt(3)*sin(th)*exp(I*ph)/(4*sqrt(pi))
+                                                   - sqrt(3)*sin(th)*exp(-I*ph)/(4*sqrt(pi)))
+    assert Znm(2, -1, th, ph).expand(func=True) == (sqrt(15)*I*sin(th)*exp(I*ph)*cos(th)/(4*sqrt(pi))
+                                                    - sqrt(15)*I*sin(th)*exp(-I*ph)*cos(th)/(4*sqrt(pi)))
+    assert Znm(2, 0, th, ph).expand(func=True) == 3*sqrt(5)*cos(th)**2/(4*sqrt(pi)) - sqrt(5)/(4*sqrt(pi))
+    assert Znm(2, 1, th, ph).expand(func=True) == (-sqrt(15)*sin(th)*exp(I*ph)*cos(th)/(4*sqrt(pi))
+                                                   - sqrt(15)*sin(th)*exp(-I*ph)*cos(th)/(4*sqrt(pi)))

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/tests/test_tensor_functions.py

@@ -0,0 +1,145 @@
+from sympy.core.relational import Ne
+from sympy.core.symbol import (Dummy, Symbol, symbols)
+from sympy.functions.elementary.complexes import (adjoint, conjugate, transpose)
+from sympy.functions.elementary.piecewise import Piecewise
+from sympy.functions.special.tensor_functions import (Eijk, KroneckerDelta, LeviCivita)
+
+from sympy.physics.secondquant import evaluate_deltas, F
+
+x, y = symbols('x y')
+
+
+def test_levicivita():
+    assert Eijk(1, 2, 3) == LeviCivita(1, 2, 3)
+    assert LeviCivita(1, 2, 3) == 1
+    assert LeviCivita(int(1), int(2), int(3)) == 1
+    assert LeviCivita(1, 3, 2) == -1
+    assert LeviCivita(1, 2, 2) == 0
+    i, j, k = symbols('i j k')
+    assert LeviCivita(i, j, k) == LeviCivita(i, j, k, evaluate=False)
+    assert LeviCivita(i, j, i) == 0
+    assert LeviCivita(1, i, i) == 0
+    assert LeviCivita(i, j, k).doit() == (j - i)*(k - i)*(k - j)/2
+    assert LeviCivita(1, 2, 3, 1) == 0
+    assert LeviCivita(4, 5, 1, 2, 3) == 1
+    assert LeviCivita(4, 5, 2, 1, 3) == -1
+
+    assert LeviCivita(i, j, k).is_integer is True
+
+    assert adjoint(LeviCivita(i, j, k)) == LeviCivita(i, j, k)
+    assert conjugate(LeviCivita(i, j, k)) == LeviCivita(i, j, k)
+    assert transpose(LeviCivita(i, j, k)) == LeviCivita(i, j, k)
+
+
+def test_kronecker_delta():
+    i, j = symbols('i j')
+    k = Symbol('k', nonzero=True)
+    assert KroneckerDelta(1, 1) == 1
+    assert KroneckerDelta(1, 2) == 0
+    assert KroneckerDelta(k, 0) == 0
+    assert KroneckerDelta(x, x) == 1
+    assert KroneckerDelta(x**2 - y**2, x**2 - y**2) == 1
+    assert KroneckerDelta(i, i) == 1
+    assert KroneckerDelta(i, i + 1) == 0
+    assert KroneckerDelta(0, 0) == 1
+    assert KroneckerDelta(0, 1) == 0
+    assert KroneckerDelta(i + k, i) == 0
+    assert KroneckerDelta(i + k, i + k) == 1
+    assert KroneckerDelta(i + k, i + 1 + k) == 0
+    assert KroneckerDelta(i, j).subs({"i": 1, "j": 0}) == 0
+    assert KroneckerDelta(i, j).subs({"i": 3, "j": 3}) == 1
+
+    assert KroneckerDelta(i, j)**0 == 1
+    for n in range(1, 10):
+        assert KroneckerDelta(i, j)**n == KroneckerDelta(i, j)
+        assert KroneckerDelta(i, j)**-n == 1/KroneckerDelta(i, j)
+
+    assert KroneckerDelta(i, j).is_integer is True
+
+    assert adjoint(KroneckerDelta(i, j)) == KroneckerDelta(i, j)
+    assert conjugate(KroneckerDelta(i, j)) == KroneckerDelta(i, j)
+    assert transpose(KroneckerDelta(i, j)) == KroneckerDelta(i, j)
+    # to test if canonical
+    assert (KroneckerDelta(i, j) == KroneckerDelta(j, i)) == True
+
+    assert KroneckerDelta(i, j).rewrite(Piecewise) == Piecewise((0, Ne(i, j)), (1, True))
+
+    # Tests with range:
+    assert KroneckerDelta(i, j, (0, i)).args == (i, j, (0, i))
+    assert KroneckerDelta(i, j, (-j, i)).delta_range == (-j, i)
+
+    # If index is out of range, return zero:
+    assert KroneckerDelta(i, j, (0, i-1)) == 0
+    assert KroneckerDelta(-1, j, (0, i-1)) == 0
+    assert KroneckerDelta(j, -1, (0, i-1)) == 0
+    assert KroneckerDelta(j, i, (0, i-1)) == 0
+
+
+def test_kronecker_delta_secondquant():
+    """secondquant-specific methods"""
+    D = KroneckerDelta
+    i, j, v, w = symbols('i j v w', below_fermi=True, cls=Dummy)
+    a, b, t, u = symbols('a b t u', above_fermi=True, cls=Dummy)
+    p, q, r, s = symbols('p q r s', cls=Dummy)
+
+    assert D(i, a) == 0
+    assert D(i, t) == 0
+
+    assert D(i, j).is_above_fermi is False
+    assert D(a, b).is_above_fermi is True
+    assert D(p, q).is_above_fermi is True
+    assert D(i, q).is_above_fermi is False
+    assert D(q, i).is_above_fermi is False
+    assert D(q, v).is_above_fermi is False
+    assert D(a, q).is_above_fermi is True
+
+    assert D(i, j).is_below_fermi is True
+    assert D(a, b).is_below_fermi is False
+    assert D(p, q).is_below_fermi is True
+    assert D(p, j).is_below_fermi is True
+    assert D(q, b).is_below_fermi is False
+
+    assert D(i, j).is_only_above_fermi is False
+    assert D(a, b).is_only_above_fermi is True
+    assert D(p, q).is_only_above_fermi is False
+    assert D(i, q).is_only_above_fermi is False
+    assert D(q, i).is_only_above_fermi is False
+    assert D(a, q).is_only_above_fermi is True
+
+    assert D(i, j).is_only_below_fermi is True
+    assert D(a, b).is_only_below_fermi is False
+    assert D(p, q).is_only_below_fermi is False
+    assert D(p, j).is_only_below_fermi is True
+    assert D(q, b).is_only_below_fermi is False
+
+    assert not D(i, q).indices_contain_equal_information
+    assert not D(a, q).indices_contain_equal_information
+    assert D(p, q).indices_contain_equal_information
+    assert D(a, b).indices_contain_equal_information
+    assert D(i, j).indices_contain_equal_information
+
+    assert D(q, b).preferred_index == b
+    assert D(q, b).killable_index == q
+    assert D(q, t).preferred_index == t
+    assert D(q, t).killable_index == q
+    assert D(q, i).preferred_index == i
+    assert D(q, i).killable_index == q
+    assert D(q, v).preferred_index == v
+    assert D(q, v).killable_index == q
+    assert D(q, p).preferred_index == p
+    assert D(q, p).killable_index == q
+
+    EV = evaluate_deltas
+    assert EV(D(a, q)*F(q)) == F(a)
+    assert EV(D(i, q)*F(q)) == F(i)
+    assert EV(D(a, q)*F(a)) == D(a, q)*F(a)
+    assert EV(D(i, q)*F(i)) == D(i, q)*F(i)
+    assert EV(D(a, b)*F(a)) == F(b)
+    assert EV(D(a, b)*F(b)) == F(a)
+    assert EV(D(i, j)*F(i)) == F(j)
+    assert EV(D(i, j)*F(j)) == F(i)
+    assert EV(D(p, q)*F(q)) == F(p)
+    assert EV(D(p, q)*F(p)) == F(q)
+    assert EV(D(p, j)*D(p, i)*F(i)) == F(j)
+    assert EV(D(p, j)*D(p, i)*F(j)) == F(i)
+    assert EV(D(p, q)*D(p, i))*F(i) == D(q, i)*F(i)

env-llmeval/lib/python3.10/site-packages/sympy/functions/special/tests/test_zeta_functions.py

@@ -0,0 +1,286 @@
+from sympy.concrete.summations import Sum
+from sympy.core.function import expand_func
+from sympy.core.numbers import (Float, I, Rational, nan, oo, pi, zoo)
+from sympy.core.singleton import S
+from sympy.core.symbol import Symbol
+from sympy.functions.elementary.complexes import (Abs, polar_lift)
+from sympy.functions.elementary.exponential import (exp, exp_polar, log)
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.special.zeta_functions import (dirichlet_eta, lerchphi, polylog, riemann_xi, stieltjes, zeta)
+from sympy.series.order import O
+from sympy.core.function import ArgumentIndexError
+from sympy.functions.combinatorial.numbers import bernoulli, factorial, genocchi, harmonic
+from sympy.testing.pytest import raises
+from sympy.core.random import (test_derivative_numerically as td,
+                      random_complex_number as randcplx, verify_numerically)
+
+x = Symbol('x')
+a = Symbol('a')
+b = Symbol('b', negative=True)
+z = Symbol('z')
+s = Symbol('s')
+
+
+def test_zeta_eval():
+
+    assert zeta(nan) is nan
+    assert zeta(x, nan) is nan
+
+    assert zeta(0) == Rational(-1, 2)
+    assert zeta(0, x) == S.Half - x
+    assert zeta(0, b) == S.Half - b
+
+    assert zeta(1) is zoo
+    assert zeta(1, 2) is zoo
+    assert zeta(1, -7) is zoo
+    assert zeta(1, x) is zoo
+
+    assert zeta(2, 1) == pi**2/6
+    assert zeta(3, 1) == zeta(3)
+
+    assert zeta(2) == pi**2/6
+    assert zeta(4) == pi**4/90
+    assert zeta(6) == pi**6/945
+
+    assert zeta(4, 3) == pi**4/90 - Rational(17, 16)
+    assert zeta(7, 4) == zeta(7) - Rational(282251, 279936)
+    assert zeta(S.Half, 2).func == zeta
+    assert expand_func(zeta(S.Half, 2)) == zeta(S.Half) - 1
+    assert zeta(x, 3).func == zeta
+    assert expand_func(zeta(x, 3)) == zeta(x) - 1 - 1/2**x
+
+    assert zeta(2, 0) is nan
+    assert zeta(3, -1) is nan
+    assert zeta(4, -2) is nan
+
+    assert zeta(oo) == 1
+
+    assert zeta(-1) == Rational(-1, 12)
+    assert zeta(-2) == 0
+    assert zeta(-3) == Rational(1, 120)
+    assert zeta(-4) == 0
+    assert zeta(-5) == Rational(-1, 252)
+
+    assert zeta(-1, 3) == Rational(-37, 12)
+    assert zeta(-1, 7) == Rational(-253, 12)
+    assert zeta(-1, -4) == Rational(-121, 12)
+    assert zeta(-1, -9) == Rational(-541, 12)
+
+    assert zeta(-4, 3) == -17
+    assert zeta(-4, -8) == 8772
+
+    assert zeta(0, 1) == Rational(-1, 2)
+    assert zeta(0, -1) == Rational(3, 2)
+
+    assert zeta(0, 2) == Rational(-3, 2)
+    assert zeta(0, -2) == Rational(5, 2)
+
+    assert zeta(
+        3).evalf(20).epsilon_eq(Float("1.2020569031595942854", 20), 1e-19)
+
+
+def test_zeta_series():
+    assert zeta(x, a).series(a, z, 2) == \
+        zeta(x, z) - x*(a-z)*zeta(x+1, z) + O((a-z)**2, (a, z))
+
+
+def test_dirichlet_eta_eval():
+    assert dirichlet_eta(0) == S.Half
+    assert dirichlet_eta(-1) == Rational(1, 4)
+    assert dirichlet_eta(1) == log(2)
+    assert dirichlet_eta(1, S.Half).simplify() == pi/2
+    assert dirichlet_eta(1, 2) == 1 - log(2)
+    assert dirichlet_eta(2) == pi**2/12
+    assert dirichlet_eta(4) == pi**4*Rational(7, 720)
+    assert str(dirichlet_eta(I).evalf(n=10)) == '0.5325931818 + 0.2293848577*I'
+    assert str(dirichlet_eta(I, I).evalf(n=10)) == '3.462349253 + 0.220285771*I'
+
+
+def test_riemann_xi_eval():
+    assert riemann_xi(2) == pi/6
+    assert riemann_xi(0) == Rational(1, 2)
+    assert riemann_xi(1) == Rational(1, 2)
+    assert riemann_xi(3).rewrite(zeta) == 3*zeta(3)/(2*pi)
+    assert riemann_xi(4) == pi**2/15
+
+
+def test_rewriting():
+    from sympy.functions.elementary.piecewise import Piecewise
+    assert isinstance(dirichlet_eta(x).rewrite(zeta), Piecewise)
+    assert isinstance(dirichlet_eta(x).rewrite(genocchi), Piecewise)
+    assert zeta(x).rewrite(dirichlet_eta) == dirichlet_eta(x)/(1 - 2**(1 - x))
+    assert zeta(x).rewrite(dirichlet_eta, a=2) == zeta(x)
+    assert verify_numerically(dirichlet_eta(x), dirichlet_eta(x).rewrite(zeta), x)
+    assert verify_numerically(dirichlet_eta(x), dirichlet_eta(x).rewrite(genocchi), x)
+    assert verify_numerically(zeta(x), zeta(x).rewrite(dirichlet_eta), x)
+
+    assert zeta(x, a).rewrite(lerchphi) == lerchphi(1, x, a)
+    assert polylog(s, z).rewrite(lerchphi) == lerchphi(z, s, 1)*z
+
+    assert lerchphi(1, x, a).rewrite(zeta) == zeta(x, a)
+    assert z*lerchphi(z, s, 1).rewrite(polylog) == polylog(s, z)
+
+
+def test_derivatives():
+    from sympy.core.function import Derivative
+    assert zeta(x, a).diff(x) == Derivative(zeta(x, a), x)
+    assert zeta(x, a).diff(a) == -x*zeta(x + 1, a)
+    assert lerchphi(
+        z, s, a).diff(z) == (lerchphi(z, s - 1, a) - a*lerchphi(z, s, a))/z
+    assert lerchphi(z, s, a).diff(a) == -s*lerchphi(z, s + 1, a)
+    assert polylog(s, z).diff(z) == polylog(s - 1, z)/z
+
+    b = randcplx()
+    c = randcplx()
+    assert td(zeta(b, x), x)
+    assert td(polylog(b, z), z)
+    assert td(lerchphi(c, b, x), x)
+    assert td(lerchphi(x, b, c), x)
+    raises(ArgumentIndexError, lambda: lerchphi(c, b, x).fdiff(2))
+    raises(ArgumentIndexError, lambda: lerchphi(c, b, x).fdiff(4))
+    raises(ArgumentIndexError, lambda: polylog(b, z).fdiff(1))
+    raises(ArgumentIndexError, lambda: polylog(b, z).fdiff(3))
+
+
+def myexpand(func, target):
+    expanded = expand_func(func)
+    if target is not None:
+        return expanded == target
+    if expanded == func:  # it didn't expand
+        return False
+
+    # check to see that the expanded and original evaluate to the same value
+    subs = {}
+    for a in func.free_symbols:
+        subs[a] = randcplx()
+    return abs(func.subs(subs).n()
+               - expanded.replace(exp_polar, exp).subs(subs).n()) < 1e-10
+
+
+def test_polylog_expansion():
+    assert polylog(s, 0) == 0
+    assert polylog(s, 1) == zeta(s)
+    assert polylog(s, -1) == -dirichlet_eta(s)
+    assert polylog(s, exp_polar(I*pi*Rational(4, 3))) == polylog(s, exp(I*pi*Rational(4, 3)))
+    assert polylog(s, exp_polar(I*pi)/3) == polylog(s, exp(I*pi)/3)
+
+    assert myexpand(polylog(1, z), -log(1 - z))
+    assert myexpand(polylog(0, z), z/(1 - z))
+    assert myexpand(polylog(-1, z), z/(1 - z)**2)
+    assert ((1-z)**3 * expand_func(polylog(-2, z))).simplify() == z*(1 + z)
+    assert myexpand(polylog(-5, z), None)
+
+
+def test_polylog_series():
+    assert polylog(1, z).series(z, n=5) == z + z**2/2 + z**3/3 + z**4/4 + O(z**5)
+    assert polylog(1, sqrt(z)).series(z, n=3) == z/2 + z**2/4 + sqrt(z)\
+        + z**(S(3)/2)/3 + z**(S(5)/2)/5 + O(z**3)
+
+    # https://github.com/sympy/sympy/issues/9497
+    assert polylog(S(3)/2, -z).series(z, 0, 5) == -z + sqrt(2)*z**2/4\
+        - sqrt(3)*z**3/9 + z**4/8 + O(z**5)
+
+
+def test_issue_8404():
+    i = Symbol('i', integer=True)
+    assert Abs(Sum(1/(3*i + 1)**2, (i, 0, S.Infinity)).doit().n(4)
+        - 1.122) < 0.001
+
+
+def test_polylog_values():
+    assert polylog(2, 2) == pi**2/4 - I*pi*log(2)
+    assert polylog(2, S.Half) == pi**2/12 - log(2)**2/2
+    for z in [S.Half, 2, (sqrt(5)-1)/2, -(sqrt(5)-1)/2, -(sqrt(5)+1)/2, (3-sqrt(5))/2]:
+        assert Abs(polylog(2, z).evalf() - polylog(2, z, evaluate=False).evalf()) < 1e-15
+    z = Symbol("z")
+    for s in [-1, 0]:
+        for _ in range(10):
+            assert verify_numerically(polylog(s, z), polylog(s, z, evaluate=False),
+                                      z, a=-3, b=-2, c=S.Half, d=2)
+            assert verify_numerically(polylog(s, z), polylog(s, z, evaluate=False),
+                                      z, a=2, b=-2, c=5, d=2)
+
+    from sympy.integrals.integrals import Integral
+    assert polylog(0, Integral(1, (x, 0, 1))) == -S.Half
+
+
+def test_lerchphi_expansion():
+    assert myexpand(lerchphi(1, s, a), zeta(s, a))
+    assert myexpand(lerchphi(z, s, 1), polylog(s, z)/z)
+
+    # direct summation
+    assert myexpand(lerchphi(z, -1, a), a/(1 - z) + z/(1 - z)**2)
+    assert myexpand(lerchphi(z, -3, a), None)
+    # polylog reduction
+    assert myexpand(lerchphi(z, s, S.Half),
+                    2**(s - 1)*(polylog(s, sqrt(z))/sqrt(z)
+                              - polylog(s, polar_lift(-1)*sqrt(z))/sqrt(z)))
+    assert myexpand(lerchphi(z, s, 2), -1/z + polylog(s, z)/z**2)
+    assert myexpand(lerchphi(z, s, Rational(3, 2)), None)
+    assert myexpand(lerchphi(z, s, Rational(7, 3)), None)
+    assert myexpand(lerchphi(z, s, Rational(-1, 3)), None)
+    assert myexpand(lerchphi(z, s, Rational(-5, 2)), None)
+
+    # hurwitz zeta reduction
+    assert myexpand(lerchphi(-1, s, a),
+                    2**(-s)*zeta(s, a/2) - 2**(-s)*zeta(s, (a + 1)/2))
+    assert myexpand(lerchphi(I, s, a), None)
+    assert myexpand(lerchphi(-I, s, a), None)
+    assert myexpand(lerchphi(exp(I*pi*Rational(2, 5)), s, a), None)
+
+
+def test_stieltjes():
+    assert isinstance(stieltjes(x), stieltjes)
+    assert isinstance(stieltjes(x, a), stieltjes)
+
+    # Zero'th constant EulerGamma
+    assert stieltjes(0) == S.EulerGamma
+    assert stieltjes(0, 1) == S.EulerGamma
+
+    # Not defined
+    assert stieltjes(nan) is nan
+    assert stieltjes(0, nan) is nan
+    assert stieltjes(-1) is S.ComplexInfinity
+    assert stieltjes(1.5) is S.ComplexInfinity
+    assert stieltjes(z, 0) is S.ComplexInfinity
+    assert stieltjes(z, -1) is S.ComplexInfinity
+
+
+def test_stieltjes_evalf():
+    assert abs(stieltjes(0).evalf() - 0.577215664) < 1E-9
+    assert abs(stieltjes(0, 0.5).evalf() - 1.963510026) < 1E-9
+    assert abs(stieltjes(1, 2).evalf() + 0.072815845) < 1E-9
+
+
+def test_issue_10475():
+    a = Symbol('a', extended_real=True)
+    b = Symbol('b', extended_positive=True)
+    s = Symbol('s', zero=False)
+
+    assert zeta(2 + I).is_finite
+    assert zeta(1).is_finite is False
+    assert zeta(x).is_finite is None
+    assert zeta(x + I).is_finite is None
+    assert zeta(a).is_finite is None
+    assert zeta(b).is_finite is None
+    assert zeta(-b).is_finite is True
+    assert zeta(b**2 - 2*b + 1).is_finite is None
+    assert zeta(a + I).is_finite is True
+    assert zeta(b + 1).is_finite is True
+    assert zeta(s + 1).is_finite is True
+
+
+def test_issue_14177():
+    n = Symbol('n', nonnegative=True, integer=True)
+
+    assert zeta(-n).rewrite(bernoulli) == bernoulli(n+1) / (-n-1)
+    assert zeta(-n, a).rewrite(bernoulli) == bernoulli(n+1, a) / (-n-1)
+    z2n = -(2*I*pi)**(2*n)*bernoulli(2*n) / (2*factorial(2*n))
+    assert zeta(2*n).rewrite(bernoulli) == z2n
+    assert expand_func(zeta(s, n+1)) == zeta(s) - harmonic(n, s)
+    assert expand_func(zeta(-b, -n)) is nan
+    assert expand_func(zeta(-b, n)) == zeta(-b, n)
+
+    n = Symbol('n')
+
+    assert zeta(2*n) == zeta(2*n) # As sign of z (= 2*n) is not determined

env-llmeval/lib/python3.10/site-packages/sympy/logic/__init__.py

@@ -0,0 +1,12 @@
+from .boolalg import (to_cnf, to_dnf, to_nnf, And, Or, Not, Xor, Nand, Nor, Implies,
+    Equivalent, ITE, POSform, SOPform, simplify_logic, bool_map, true, false,
+    gateinputcount)
+from .inference import satisfiable
+
+__all__ = [
+    'to_cnf', 'to_dnf', 'to_nnf', 'And', 'Or', 'Not', 'Xor', 'Nand', 'Nor',
+    'Implies', 'Equivalent', 'ITE', 'POSform', 'SOPform', 'simplify_logic',
+    'bool_map', 'true', 'false', 'gateinputcount',
+
+    'satisfiable',
+]

env-llmeval/lib/python3.10/site-packages/sympy/logic/algorithms/dpll.py

@@ -0,0 +1,308 @@
+"""Implementation of DPLL algorithm
+
+Further improvements: eliminate calls to pl_true, implement branching rules,
+efficient unit propagation.
+
+References:
+  - https://en.wikipedia.org/wiki/DPLL_algorithm
+  - https://www.researchgate.net/publication/242384772_Implementations_of_the_DPLL_Algorithm
+"""
+
+from sympy.core.sorting import default_sort_key
+from sympy.logic.boolalg import Or, Not, conjuncts, disjuncts, to_cnf, \
+    to_int_repr, _find_predicates
+from sympy.assumptions.cnf import CNF
+from sympy.logic.inference import pl_true, literal_symbol
+
+
+def dpll_satisfiable(expr):
+    """
+    Check satisfiability of a propositional sentence.
+    It returns a model rather than True when it succeeds
+
+    >>> from sympy.abc import A, B
+    >>> from sympy.logic.algorithms.dpll import dpll_satisfiable
+    >>> dpll_satisfiable(A & ~B)
+    {A: True, B: False}
+    >>> dpll_satisfiable(A & ~A)
+    False
+
+    """
+    if not isinstance(expr, CNF):
+        clauses = conjuncts(to_cnf(expr))
+    else:
+        clauses = expr.clauses
+    if False in clauses:
+        return False
+    symbols = sorted(_find_predicates(expr), key=default_sort_key)
+    symbols_int_repr = set(range(1, len(symbols) + 1))
+    clauses_int_repr = to_int_repr(clauses, symbols)
+    result = dpll_int_repr(clauses_int_repr, symbols_int_repr, {})
+    if not result:
+        return result
+    output = {}
+    for key in result:
+        output.update({symbols[key - 1]: result[key]})
+    return output
+
+
+def dpll(clauses, symbols, model):
+    """
+    Compute satisfiability in a partial model.
+    Clauses is an array of conjuncts.
+
+    >>> from sympy.abc import A, B, D
+    >>> from sympy.logic.algorithms.dpll import dpll
+    >>> dpll([A, B, D], [A, B], {D: False})
+    False
+
+    """
+    # compute DP kernel
+    P, value = find_unit_clause(clauses, model)
+    while P:
+        model.update({P: value})
+        symbols.remove(P)
+        if not value:
+            P = ~P
+        clauses = unit_propagate(clauses, P)
+        P, value = find_unit_clause(clauses, model)
+    P, value = find_pure_symbol(symbols, clauses)
+    while P:
+        model.update({P: value})
+        symbols.remove(P)
+        if not value:
+            P = ~P
+        clauses = unit_propagate(clauses, P)
+        P, value = find_pure_symbol(symbols, clauses)
+    # end DP kernel
+    unknown_clauses = []
+    for c in clauses:
+        val = pl_true(c, model)
+        if val is False:
+            return False
+        if val is not True:
+            unknown_clauses.append(c)
+    if not unknown_clauses:
+        return model
+    if not clauses:
+        return model
+    P = symbols.pop()
+    model_copy = model.copy()
+    model.update({P: True})
+    model_copy.update({P: False})
+    symbols_copy = symbols[:]
+    return (dpll(unit_propagate(unknown_clauses, P), symbols, model) or
+            dpll(unit_propagate(unknown_clauses, Not(P)), symbols_copy, model_copy))
+
+
+def dpll_int_repr(clauses, symbols, model):
+    """
+    Compute satisfiability in a partial model.
+    Arguments are expected to be in integer representation
+
+    >>> from sympy.logic.algorithms.dpll import dpll_int_repr
+    >>> dpll_int_repr([{1}, {2}, {3}], {1, 2}, {3: False})
+    False
+
+    """
+    # compute DP kernel
+    P, value = find_unit_clause_int_repr(clauses, model)
+    while P:
+        model.update({P: value})
+        symbols.remove(P)
+        if not value:
+            P = -P
+        clauses = unit_propagate_int_repr(clauses, P)
+        P, value = find_unit_clause_int_repr(clauses, model)
+    P, value = find_pure_symbol_int_repr(symbols, clauses)
+    while P:
+        model.update({P: value})
+        symbols.remove(P)
+        if not value:
+            P = -P
+        clauses = unit_propagate_int_repr(clauses, P)
+        P, value = find_pure_symbol_int_repr(symbols, clauses)
+    # end DP kernel
+    unknown_clauses = []
+    for c in clauses:
+        val = pl_true_int_repr(c, model)
+        if val is False:
+            return False
+        if val is not True:
+            unknown_clauses.append(c)
+    if not unknown_clauses:
+        return model
+    P = symbols.pop()
+    model_copy = model.copy()
+    model.update({P: True})
+    model_copy.update({P: False})
+    symbols_copy = symbols.copy()
+    return (dpll_int_repr(unit_propagate_int_repr(unknown_clauses, P), symbols, model) or
+            dpll_int_repr(unit_propagate_int_repr(unknown_clauses, -P), symbols_copy, model_copy))
+
+### helper methods for DPLL
+
+
+def pl_true_int_repr(clause, model={}):
+    """
+    Lightweight version of pl_true.
+    Argument clause represents the set of args of an Or clause. This is used
+    inside dpll_int_repr, it is not meant to be used directly.
+
+    >>> from sympy.logic.algorithms.dpll import pl_true_int_repr
+    >>> pl_true_int_repr({1, 2}, {1: False})
+    >>> pl_true_int_repr({1, 2}, {1: False, 2: False})
+    False
+
+    """
+    result = False
+    for lit in clause:
+        if lit < 0:
+            p = model.get(-lit)
+            if p is not None:
+                p = not p
+        else:
+            p = model.get(lit)
+        if p is True:
+            return True
+        elif p is None:
+            result = None
+    return result
+
+
+def unit_propagate(clauses, symbol):
+    """
+    Returns an equivalent set of clauses
+    If a set of clauses contains the unit clause l, the other clauses are
+    simplified by the application of the two following rules:
+
+      1. every clause containing l is removed
+      2. in every clause that contains ~l this literal is deleted
+
+    Arguments are expected to be in CNF.
+
+    >>> from sympy.abc import A, B, D
+    >>> from sympy.logic.algorithms.dpll import unit_propagate
+    >>> unit_propagate([A | B, D | ~B, B], B)
+    [D, B]
+
+    """
+    output = []
+    for c in clauses:
+        if c.func != Or:
+            output.append(c)
+            continue
+        for arg in c.args:
+            if arg == ~symbol:
+                output.append(Or(*[x for x in c.args if x != ~symbol]))
+                break
+            if arg == symbol:
+                break
+        else:
+            output.append(c)
+    return output
+
+
+def unit_propagate_int_repr(clauses, s):
+    """
+    Same as unit_propagate, but arguments are expected to be in integer
+    representation
+
+    >>> from sympy.logic.algorithms.dpll import unit_propagate_int_repr
+    >>> unit_propagate_int_repr([{1, 2}, {3, -2}, {2}], 2)
+    [{3}]
+
+    """
+    negated = {-s}
+    return [clause - negated for clause in clauses if s not in clause]
+
+
+def find_pure_symbol(symbols, unknown_clauses):
+    """
+    Find a symbol and its value if it appears only as a positive literal
+    (or only as a negative) in clauses.
+
+    >>> from sympy.abc import A, B, D
+    >>> from sympy.logic.algorithms.dpll import find_pure_symbol
+    >>> find_pure_symbol([A, B, D], [A|~B,~B|~D,D|A])
+    (A, True)
+
+    """
+    for sym in symbols:
+        found_pos, found_neg = False, False
+        for c in unknown_clauses:
+            if not found_pos and sym in disjuncts(c):
+                found_pos = True
+            if not found_neg and Not(sym) in disjuncts(c):
+                found_neg = True
+        if found_pos != found_neg:
+            return sym, found_pos
+    return None, None
+
+
+def find_pure_symbol_int_repr(symbols, unknown_clauses):
+    """
+    Same as find_pure_symbol, but arguments are expected
+    to be in integer representation
+
+    >>> from sympy.logic.algorithms.dpll import find_pure_symbol_int_repr
+    >>> find_pure_symbol_int_repr({1,2,3},
+    ...     [{1, -2}, {-2, -3}, {3, 1}])
+    (1, True)
+
+    """
+    all_symbols = set().union(*unknown_clauses)
+    found_pos = all_symbols.intersection(symbols)
+    found_neg = all_symbols.intersection([-s for s in symbols])
+    for p in found_pos:
+        if -p not in found_neg:
+            return p, True
+    for p in found_neg:
+        if -p not in found_pos:
+            return -p, False
+    return None, None
+
+
+def find_unit_clause(clauses, model):
+    """
+    A unit clause has only 1 variable that is not bound in the model.
+
+    >>> from sympy.abc import A, B, D
+    >>> from sympy.logic.algorithms.dpll import find_unit_clause
+    >>> find_unit_clause([A | B | D, B | ~D, A | ~B], {A:True})
+    (B, False)
+
+    """
+    for clause in clauses:
+        num_not_in_model = 0
+        for literal in disjuncts(clause):
+            sym = literal_symbol(literal)
+            if sym not in model:
+                num_not_in_model += 1
+                P, value = sym, not isinstance(literal, Not)
+        if num_not_in_model == 1:
+            return P, value
+    return None, None
+
+
+def find_unit_clause_int_repr(clauses, model):
+    """
+    Same as find_unit_clause, but arguments are expected to be in
+    integer representation.
+
+    >>> from sympy.logic.algorithms.dpll import find_unit_clause_int_repr
+    >>> find_unit_clause_int_repr([{1, 2, 3},
+    ...     {2, -3}, {1, -2}], {1: True})
+    (2, False)
+
+    """
+    bound = set(model) | {-sym for sym in model}
+    for clause in clauses:
+        unbound = clause - bound
+        if len(unbound) == 1:
+            p = unbound.pop()
+            if p < 0:
+                return -p, False
+            else:
+                return p, True
+    return None, None