Add files using upload-large-folder tool

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

@@ -0,0 +1,25 @@
+"""Calculus-related methods."""
+
+from .euler import euler_equations
+from .singularities import (singularities, is_increasing,
+                            is_strictly_increasing, is_decreasing,
+                            is_strictly_decreasing, is_monotonic)
+from .finite_diff import finite_diff_weights, apply_finite_diff, differentiate_finite
+from .util import (periodicity, not_empty_in, is_convex,
+                   stationary_points, minimum, maximum)
+from .accumulationbounds import AccumBounds
+
+__all__ = [
+'euler_equations',
+
+'singularities', 'is_increasing',
+'is_strictly_increasing', 'is_decreasing',
+'is_strictly_decreasing', 'is_monotonic',
+
+'finite_diff_weights', 'apply_finite_diff', 'differentiate_finite',
+
+'periodicity', 'not_empty_in', 'is_convex', 'stationary_points',
+'minimum', 'maximum',
+
+'AccumBounds'
+]

llmeval-env/lib/python3.10/site-packages/sympy/calculus/accumulationbounds.py

@@ -0,0 +1,805 @@
+from sympy.core import Add, Mul, Pow, S
+from sympy.core.basic import Basic
+from sympy.core.expr import Expr
+from sympy.core.numbers import _sympifyit, oo, zoo
+from sympy.core.relational import is_le, is_lt, is_ge, is_gt
+from sympy.core.sympify import _sympify
+from sympy.functions.elementary.miscellaneous import Min, Max
+from sympy.logic.boolalg import And
+from sympy.multipledispatch import dispatch
+from sympy.series.order import Order
+from sympy.sets.sets import FiniteSet
+
+
+class AccumulationBounds(Expr):
+    r"""An accumulation bounds.
+
+    # Note AccumulationBounds has an alias: AccumBounds
+
+    AccumulationBounds represent an interval `[a, b]`, which is always closed
+    at the ends. Here `a` and `b` can be any value from extended real numbers.
+
+    The intended meaning of AccummulationBounds is to give an approximate
+    location of the accumulation points of a real function at a limit point.
+
+    Let `a` and `b` be reals such that `a \le b`.
+
+    `\left\langle a, b\right\rangle = \{x \in \mathbb{R} \mid a \le x \le b\}`
+
+    `\left\langle -\infty, b\right\rangle = \{x \in \mathbb{R} \mid x \le b\} \cup \{-\infty, \infty\}`
+
+    `\left\langle a, \infty \right\rangle = \{x \in \mathbb{R} \mid a \le x\} \cup \{-\infty, \infty\}`
+
+    `\left\langle -\infty, \infty \right\rangle = \mathbb{R} \cup \{-\infty, \infty\}`
+
+    ``oo`` and ``-oo`` are added to the second and third definition respectively,
+    since if either ``-oo`` or ``oo`` is an argument, then the other one should
+    be included (though not as an end point). This is forced, since we have,
+    for example, ``1/AccumBounds(0, 1) = AccumBounds(1, oo)``, and the limit at
+    `0` is not one-sided. As `x` tends to `0-`, then `1/x \rightarrow -\infty`, so `-\infty`
+    should be interpreted as belonging to ``AccumBounds(1, oo)`` though it need
+    not appear explicitly.
+
+    In many cases it suffices to know that the limit set is bounded.
+    However, in some other cases more exact information could be useful.
+    For example, all accumulation values of `\cos(x) + 1` are non-negative.
+    (``AccumBounds(-1, 1) + 1 = AccumBounds(0, 2)``)
+
+    A AccumulationBounds object is defined to be real AccumulationBounds,
+    if its end points are finite reals.
+
+    Let `X`, `Y` be real AccumulationBounds, then their sum, difference,
+    product are defined to be the following sets:
+
+    `X + Y = \{ x+y \mid x \in X \cap y \in Y\}`
+
+    `X - Y = \{ x-y \mid x \in X \cap y \in Y\}`
+
+    `X \times Y = \{ x \times y \mid x \in X \cap y \in Y\}`
+
+    When an AccumBounds is raised to a negative power, if 0 is contained
+    between the bounds then an infinite range is returned, otherwise if an
+    endpoint is 0 then a semi-infinite range with consistent sign will be returned.
+
+    AccumBounds in expressions behave a lot like Intervals but the
+    semantics are not necessarily the same. Division (or exponentiation
+    to a negative integer power) could be handled with *intervals* by
+    returning a union of the results obtained after splitting the
+    bounds between negatives and positives, but that is not done with
+    AccumBounds. In addition, bounds are assumed to be independent of
+    each other; if the same bound is used in more than one place in an
+    expression, the result may not be the supremum or infimum of the
+    expression (see below). Finally, when a boundary is ``1``,
+    exponentiation to the power of ``oo`` yields ``oo``, neither
+    ``1`` nor ``nan``.
+
+    Examples
+    ========
+
+    >>> from sympy import AccumBounds, sin, exp, log, pi, E, S, oo
+    >>> from sympy.abc import x
+
+    >>> AccumBounds(0, 1) + AccumBounds(1, 2)
+    AccumBounds(1, 3)
+
+    >>> AccumBounds(0, 1) - AccumBounds(0, 2)
+    AccumBounds(-2, 1)
+
+    >>> AccumBounds(-2, 3)*AccumBounds(-1, 1)
+    AccumBounds(-3, 3)
+
+    >>> AccumBounds(1, 2)*AccumBounds(3, 5)
+    AccumBounds(3, 10)
+
+    The exponentiation of AccumulationBounds is defined
+    as follows:
+
+    If 0 does not belong to `X` or `n > 0` then
+
+    `X^n = \{ x^n \mid x \in X\}`
+
+    >>> AccumBounds(1, 4)**(S(1)/2)
+    AccumBounds(1, 2)
+
+    otherwise, an infinite or semi-infinite result is obtained:
+
+    >>> 1/AccumBounds(-1, 1)
+    AccumBounds(-oo, oo)
+    >>> 1/AccumBounds(0, 2)
+    AccumBounds(1/2, oo)
+    >>> 1/AccumBounds(-oo, 0)
+    AccumBounds(-oo, 0)
+
+    A boundary of 1 will always generate all nonnegatives:
+
+    >>> AccumBounds(1, 2)**oo
+    AccumBounds(0, oo)
+    >>> AccumBounds(0, 1)**oo
+    AccumBounds(0, oo)
+
+    If the exponent is itself an AccumulationBounds or is not an
+    integer then unevaluated results will be returned unless the base
+    values are positive:
+
+    >>> AccumBounds(2, 3)**AccumBounds(-1, 2)
+    AccumBounds(1/3, 9)
+    >>> AccumBounds(-2, 3)**AccumBounds(-1, 2)
+    AccumBounds(-2, 3)**AccumBounds(-1, 2)
+
+    >>> AccumBounds(-2, -1)**(S(1)/2)
+    sqrt(AccumBounds(-2, -1))
+
+    Note: `\left\langle a, b\right\rangle^2` is not same as `\left\langle a, b\right\rangle \times \left\langle a, b\right\rangle`
+
+    >>> AccumBounds(-1, 1)**2
+    AccumBounds(0, 1)
+
+    >>> AccumBounds(1, 3) < 4
+    True
+
+    >>> AccumBounds(1, 3) < -1
+    False
+
+    Some elementary functions can also take AccumulationBounds as input.
+    A function `f` evaluated for some real AccumulationBounds `\left\langle a, b \right\rangle`
+    is defined as `f(\left\langle a, b\right\rangle) = \{ f(x) \mid a \le x \le b \}`
+
+    >>> sin(AccumBounds(pi/6, pi/3))
+    AccumBounds(1/2, sqrt(3)/2)
+
+    >>> exp(AccumBounds(0, 1))
+    AccumBounds(1, E)
+
+    >>> log(AccumBounds(1, E))
+    AccumBounds(0, 1)
+
+    Some symbol in an expression can be substituted for a AccumulationBounds
+    object. But it does not necessarily evaluate the AccumulationBounds for
+    that expression.
+
+    The same expression can be evaluated to different values depending upon
+    the form it is used for substitution since each instance of an
+    AccumulationBounds is considered independent. For example:
+
+    >>> (x**2 + 2*x + 1).subs(x, AccumBounds(-1, 1))
+    AccumBounds(-1, 4)
+
+    >>> ((x + 1)**2).subs(x, AccumBounds(-1, 1))
+    AccumBounds(0, 4)
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Interval_arithmetic
+
+    .. [2] https://fab.cba.mit.edu/classes/S62.12/docs/Hickey_interval.pdf
+
+    Notes
+    =====
+
+    Do not use ``AccumulationBounds`` for floating point interval arithmetic
+    calculations, use ``mpmath.iv`` instead.
+    """
+
+    is_extended_real = True
+    is_number = False
+
+    def __new__(cls, min, max):
+
+        min = _sympify(min)
+        max = _sympify(max)
+
+        # Only allow real intervals (use symbols with 'is_extended_real=True').
+        if not min.is_extended_real or not max.is_extended_real:
+            raise ValueError("Only real AccumulationBounds are supported")
+
+        if max == min:
+            return max
+
+        # Make sure that the created AccumBounds object will be valid.
+        if max.is_number and min.is_number:
+            bad = max.is_comparable and min.is_comparable and max < min
+        else:
+            bad = (max - min).is_extended_negative
+        if bad:
+            raise ValueError(
+                "Lower limit should be smaller than upper limit")
+
+        return Basic.__new__(cls, min, max)
+
+    # setting the operation priority
+    _op_priority = 11.0
+
+    def _eval_is_real(self):
+        if self.min.is_real and self.max.is_real:
+            return True
+
+    @property
+    def min(self):
+        """
+        Returns the minimum possible value attained by AccumulationBounds
+        object.
+
+        Examples
+        ========
+
+        >>> from sympy import AccumBounds
+        >>> AccumBounds(1, 3).min
+        1
+
+        """
+        return self.args[0]
+
+    @property
+    def max(self):
+        """
+        Returns the maximum possible value attained by AccumulationBounds
+        object.
+
+        Examples
+        ========
+
+        >>> from sympy import AccumBounds
+        >>> AccumBounds(1, 3).max
+        3
+
+        """
+        return self.args[1]
+
+    @property
+    def delta(self):
+        """
+        Returns the difference of maximum possible value attained by
+        AccumulationBounds object and minimum possible value attained
+        by AccumulationBounds object.
+
+        Examples
+        ========
+
+        >>> from sympy import AccumBounds
+        >>> AccumBounds(1, 3).delta
+        2
+
+        """
+        return self.max - self.min
+
+    @property
+    def mid(self):
+        """
+        Returns the mean of maximum possible value attained by
+        AccumulationBounds object and minimum possible value
+        attained by AccumulationBounds object.
+
+        Examples
+        ========
+
+        >>> from sympy import AccumBounds
+        >>> AccumBounds(1, 3).mid
+        2
+
+        """
+        return (self.min + self.max) / 2
+
+    @_sympifyit('other', NotImplemented)
+    def _eval_power(self, other):
+        return self.__pow__(other)
+
+    @_sympifyit('other', NotImplemented)
+    def __add__(self, other):
+        if isinstance(other, Expr):
+            if isinstance(other, AccumBounds):
+                return AccumBounds(
+                    Add(self.min, other.min),
+                    Add(self.max, other.max))
+            if other is S.Infinity and self.min is S.NegativeInfinity or \
+                    other is S.NegativeInfinity and self.max is S.Infinity:
+                return AccumBounds(-oo, oo)
+            elif other.is_extended_real:
+                if self.min is S.NegativeInfinity and self.max is S.Infinity:
+                    return AccumBounds(-oo, oo)
+                elif self.min is S.NegativeInfinity:
+                    return AccumBounds(-oo, self.max + other)
+                elif self.max is S.Infinity:
+                    return AccumBounds(self.min + other, oo)
+                else:
+                    return AccumBounds(Add(self.min, other), Add(self.max, other))
+            return Add(self, other, evaluate=False)
+        return NotImplemented
+
+    __radd__ = __add__
+
+    def __neg__(self):
+        return AccumBounds(-self.max, -self.min)
+
+    @_sympifyit('other', NotImplemented)
+    def __sub__(self, other):
+        if isinstance(other, Expr):
+            if isinstance(other, AccumBounds):
+                return AccumBounds(
+                    Add(self.min, -other.max),
+                    Add(self.max, -other.min))
+            if other is S.NegativeInfinity and self.min is S.NegativeInfinity or \
+                    other is S.Infinity and self.max is S.Infinity:
+                return AccumBounds(-oo, oo)
+            elif other.is_extended_real:
+                if self.min is S.NegativeInfinity and self.max is S.Infinity:
+                    return AccumBounds(-oo, oo)
+                elif self.min is S.NegativeInfinity:
+                    return AccumBounds(-oo, self.max - other)
+                elif self.max is S.Infinity:
+                    return AccumBounds(self.min - other, oo)
+                else:
+                    return AccumBounds(
+                        Add(self.min, -other),
+                        Add(self.max, -other))
+            return Add(self, -other, evaluate=False)
+        return NotImplemented
+
+    @_sympifyit('other', NotImplemented)
+    def __rsub__(self, other):
+        return self.__neg__() + other
+
+    @_sympifyit('other', NotImplemented)
+    def __mul__(self, other):
+        if self.args == (-oo, oo):
+            return self
+        if isinstance(other, Expr):
+            if isinstance(other, AccumBounds):
+                if other.args == (-oo, oo):
+                    return other
+                v = set()
+                for a in self.args:
+                    vi = other*a
+                    for i in vi.args or (vi,):
+                        v.add(i)
+                return AccumBounds(Min(*v), Max(*v))
+            if other is S.Infinity:
+                if self.min.is_zero:
+                    return AccumBounds(0, oo)
+                if self.max.is_zero:
+                    return AccumBounds(-oo, 0)
+            if other is S.NegativeInfinity:
+                if self.min.is_zero:
+                    return AccumBounds(-oo, 0)
+                if self.max.is_zero:
+                    return AccumBounds(0, oo)
+            if other.is_extended_real:
+                if other.is_zero:
+                    if self.max is S.Infinity:
+                        return AccumBounds(0, oo)
+                    if self.min is S.NegativeInfinity:
+                        return AccumBounds(-oo, 0)
+                    return S.Zero
+                if other.is_extended_positive:
+                    return AccumBounds(
+                        Mul(self.min, other),
+                        Mul(self.max, other))
+                elif other.is_extended_negative:
+                    return AccumBounds(
+                        Mul(self.max, other),
+                        Mul(self.min, other))
+            if isinstance(other, Order):
+                return other
+            return Mul(self, other, evaluate=False)
+        return NotImplemented
+
+    __rmul__ = __mul__
+
+    @_sympifyit('other', NotImplemented)
+    def __truediv__(self, other):
+        if isinstance(other, Expr):
+            if isinstance(other, AccumBounds):
+                if other.min.is_positive or other.max.is_negative:
+                    return self * AccumBounds(1/other.max, 1/other.min)
+
+                if (self.min.is_extended_nonpositive and self.max.is_extended_nonnegative and
+                    other.min.is_extended_nonpositive and other.max.is_extended_nonnegative):
+                    if self.min.is_zero and other.min.is_zero:
+                        return AccumBounds(0, oo)
+                    if self.max.is_zero and other.min.is_zero:
+                        return AccumBounds(-oo, 0)
+                    return AccumBounds(-oo, oo)
+
+                if self.max.is_extended_negative:
+                    if other.min.is_extended_negative:
+                        if other.max.is_zero:
+                            return AccumBounds(self.max / other.min, oo)
+                        if other.max.is_extended_positive:
+                            # if we were dealing with intervals we would return
+                            # Union(Interval(-oo, self.max/other.max),
+                            #       Interval(self.max/other.min, oo))
+                            return AccumBounds(-oo, oo)
+
+                    if other.min.is_zero and other.max.is_extended_positive:
+                        return AccumBounds(-oo, self.max / other.max)
+
+                if self.min.is_extended_positive:
+                    if other.min.is_extended_negative:
+                        if other.max.is_zero:
+                            return AccumBounds(-oo, self.min / other.min)
+                        if other.max.is_extended_positive:
+                            # if we were dealing with intervals we would return
+                            # Union(Interval(-oo, self.min/other.min),
+                            #       Interval(self.min/other.max, oo))
+                            return AccumBounds(-oo, oo)
+
+                    if other.min.is_zero and other.max.is_extended_positive:
+                        return AccumBounds(self.min / other.max, oo)
+
+            elif other.is_extended_real:
+                if other in (S.Infinity, S.NegativeInfinity):
+                    if self == AccumBounds(-oo, oo):
+                        return AccumBounds(-oo, oo)
+                    if self.max is S.Infinity:
+                        return AccumBounds(Min(0, other), Max(0, other))
+                    if self.min is S.NegativeInfinity:
+                        return AccumBounds(Min(0, -other), Max(0, -other))
+                if other.is_extended_positive:
+                    return AccumBounds(self.min / other, self.max / other)
+                elif other.is_extended_negative:
+                    return AccumBounds(self.max / other, self.min / other)
+            if (1 / other) is S.ComplexInfinity:
+                return Mul(self, 1 / other, evaluate=False)
+            else:
+                return Mul(self, 1 / other)
+
+        return NotImplemented
+
+    @_sympifyit('other', NotImplemented)
+    def __rtruediv__(self, other):
+        if isinstance(other, Expr):
+            if other.is_extended_real:
+                if other.is_zero:
+                    return S.Zero
+                if (self.min.is_extended_nonpositive and self.max.is_extended_nonnegative):
+                    if self.min.is_zero:
+                        if other.is_extended_positive:
+                            return AccumBounds(Mul(other, 1 / self.max), oo)
+                        if other.is_extended_negative:
+                            return AccumBounds(-oo, Mul(other, 1 / self.max))
+                    if self.max.is_zero:
+                        if other.is_extended_positive:
+                            return AccumBounds(-oo, Mul(other, 1 / self.min))
+                        if other.is_extended_negative:
+                            return AccumBounds(Mul(other, 1 / self.min), oo)
+                    return AccumBounds(-oo, oo)
+                else:
+                    return AccumBounds(Min(other / self.min, other / self.max),
+                                       Max(other / self.min, other / self.max))
+            return Mul(other, 1 / self, evaluate=False)
+        else:
+            return NotImplemented
+
+    @_sympifyit('other', NotImplemented)
+    def __pow__(self, other):
+        if isinstance(other, Expr):
+            if other is S.Infinity:
+                if self.min.is_extended_nonnegative:
+                    if self.max < 1:
+                        return S.Zero
+                    if self.min > 1:
+                        return S.Infinity
+                    return AccumBounds(0, oo)
+                elif self.max.is_extended_negative:
+                    if self.min > -1:
+                        return S.Zero
+                    if self.max < -1:
+                        return zoo
+                    return S.NaN
+                else:
+                    if self.min > -1:
+                        if self.max < 1:
+                            return S.Zero
+                        return AccumBounds(0, oo)
+                    return AccumBounds(-oo, oo)
+
+            if other is S.NegativeInfinity:
+                return (1/self)**oo
+
+            # generically true
+            if (self.max - self.min).is_nonnegative:
+                # well defined
+                if self.min.is_nonnegative:
+                    # no 0 to worry about
+                    if other.is_nonnegative:
+                        # no infinity to worry about
+                        return self.func(self.min**other, self.max**other)
+
+            if other.is_zero:
+                return S.One  # x**0 = 1
+
+            if other.is_Integer or other.is_integer:
+                if self.min.is_extended_positive:
+                    return AccumBounds(
+                        Min(self.min**other, self.max**other),
+                        Max(self.min**other, self.max**other))
+                elif self.max.is_extended_negative:
+                    return AccumBounds(
+                        Min(self.max**other, self.min**other),
+                        Max(self.max**other, self.min**other))
+
+                if other % 2 == 0:
+                    if other.is_extended_negative:
+                        if self.min.is_zero:
+                            return AccumBounds(self.max**other, oo)
+                        if self.max.is_zero:
+                            return AccumBounds(self.min**other, oo)
+                        return (1/self)**(-other)
+                    return AccumBounds(
+                        S.Zero, Max(self.min**other, self.max**other))
+                elif other % 2 == 1:
+                    if other.is_extended_negative:
+                        if self.min.is_zero:
+                            return AccumBounds(self.max**other, oo)
+                        if self.max.is_zero:
+                            return AccumBounds(-oo, self.min**other)
+                        return (1/self)**(-other)
+                    return AccumBounds(self.min**other, self.max**other)
+
+            # non-integer exponent
+            # 0**neg or neg**frac yields complex
+            if (other.is_number or other.is_rational) and (
+                    self.min.is_extended_nonnegative or (
+                    other.is_extended_nonnegative and
+                    self.min.is_extended_nonnegative)):
+                num, den = other.as_numer_denom()
+                if num is S.One:
+                    return AccumBounds(*[i**(1/den) for i in self.args])
+
+                elif den is not S.One:  # e.g. if other is not Float
+                    return (self**num)**(1/den)  # ok for non-negative base
+
+            if isinstance(other, AccumBounds):
+                if (self.min.is_extended_positive or
+                        self.min.is_extended_nonnegative and
+                        other.min.is_extended_nonnegative):
+                    p = [self**i for i in other.args]
+                    if not any(i.is_Pow for i in p):
+                        a = [j for i in p for j in i.args or (i,)]
+                        try:
+                            return self.func(min(a), max(a))
+                        except TypeError:  # can't sort
+                            pass
+
+            return Pow(self, other, evaluate=False)
+
+        return NotImplemented
+
+    @_sympifyit('other', NotImplemented)
+    def __rpow__(self, other):
+        if other.is_real and other.is_extended_nonnegative and (
+                self.max - self.min).is_extended_positive:
+            if other is S.One:
+                return S.One
+            if other.is_extended_positive:
+                a, b = [other**i for i in self.args]
+                if min(a, b) != a:
+                    a, b = b, a
+                return self.func(a, b)
+            if other.is_zero:
+                if self.min.is_zero:
+                    return self.func(0, 1)
+                if self.min.is_extended_positive:
+                    return S.Zero
+
+        return Pow(other, self, evaluate=False)
+
+    def __abs__(self):
+        if self.max.is_extended_negative:
+            return self.__neg__()
+        elif self.min.is_extended_negative:
+            return AccumBounds(S.Zero, Max(abs(self.min), self.max))
+        else:
+            return self
+
+
+    def __contains__(self, other):
+        """
+        Returns ``True`` if other is contained in self, where other
+        belongs to extended real numbers, ``False`` if not contained,
+        otherwise TypeError is raised.
+
+        Examples
+        ========
+
+        >>> from sympy import AccumBounds, oo
+        >>> 1 in AccumBounds(-1, 3)
+        True
+
+        -oo and oo go together as limits (in AccumulationBounds).
+
+        >>> -oo in AccumBounds(1, oo)
+        True
+
+        >>> oo in AccumBounds(-oo, 0)
+        True
+
+        """
+        other = _sympify(other)
+
+        if other in (S.Infinity, S.NegativeInfinity):
+            if self.min is S.NegativeInfinity or self.max is S.Infinity:
+                return True
+            return False
+
+        rv = And(self.min <= other, self.max >= other)
+        if rv not in (True, False):
+            raise TypeError("input failed to evaluate")
+        return rv
+
+    def intersection(self, other):
+        """
+        Returns the intersection of 'self' and 'other'.
+        Here other can be an instance of :py:class:`~.FiniteSet` or AccumulationBounds.
+
+        Parameters
+        ==========
+
+        other : AccumulationBounds
+            Another AccumulationBounds object with which the intersection
+            has to be computed.
+
+        Returns
+        =======
+
+        AccumulationBounds
+            Intersection of ``self`` and ``other``.
+
+        Examples
+        ========
+
+        >>> from sympy import AccumBounds, FiniteSet
+        >>> AccumBounds(1, 3).intersection(AccumBounds(2, 4))
+        AccumBounds(2, 3)
+
+        >>> AccumBounds(1, 3).intersection(AccumBounds(4, 6))
+        EmptySet
+
+        >>> AccumBounds(1, 4).intersection(FiniteSet(1, 2, 5))
+        {1, 2}
+
+        """
+        if not isinstance(other, (AccumBounds, FiniteSet)):
+            raise TypeError(
+                "Input must be AccumulationBounds or FiniteSet object")
+
+        if isinstance(other, FiniteSet):
+            fin_set = S.EmptySet
+            for i in other:
+                if i in self:
+                    fin_set = fin_set + FiniteSet(i)
+            return fin_set
+
+        if self.max < other.min or self.min > other.max:
+            return S.EmptySet
+
+        if self.min <= other.min:
+            if self.max <= other.max:
+                return AccumBounds(other.min, self.max)
+            if self.max > other.max:
+                return other
+
+        if other.min <= self.min:
+            if other.max < self.max:
+                return AccumBounds(self.min, other.max)
+            if other.max > self.max:
+                return self
+
+    def union(self, other):
+        # TODO : Devise a better method for Union of AccumBounds
+        # this method is not actually correct and
+        # can be made better
+        if not isinstance(other, AccumBounds):
+            raise TypeError(
+                "Input must be AccumulationBounds or FiniteSet object")
+
+        if self.min <= other.min and self.max >= other.min:
+            return AccumBounds(self.min, Max(self.max, other.max))
+
+        if other.min <= self.min and other.max >= self.min:
+            return AccumBounds(other.min, Max(self.max, other.max))
+
+
+@dispatch(AccumulationBounds, AccumulationBounds) # type: ignore # noqa:F811
+def _eval_is_le(lhs, rhs): # noqa:F811
+    if is_le(lhs.max, rhs.min):
+        return True
+    if is_gt(lhs.min, rhs.max):
+        return False
+
+
+@dispatch(AccumulationBounds, Basic) # type: ignore # noqa:F811
+def _eval_is_le(lhs, rhs): # noqa: F811
+
+    """
+    Returns ``True `` if range of values attained by ``lhs`` AccumulationBounds
+    object is greater than the range of values attained by ``rhs``,
+    where ``rhs`` may be any value of type AccumulationBounds object or
+    extended real number value, ``False`` if ``rhs`` satisfies
+    the same property, else an unevaluated :py:class:`~.Relational`.
+
+    Examples
+    ========
+
+    >>> from sympy import AccumBounds, oo
+    >>> AccumBounds(1, 3) > AccumBounds(4, oo)
+    False
+    >>> AccumBounds(1, 4) > AccumBounds(3, 4)
+    AccumBounds(1, 4) > AccumBounds(3, 4)
+    >>> AccumBounds(1, oo) > -1
+    True
+
+    """
+    if not rhs.is_extended_real:
+            raise TypeError(
+                "Invalid comparison of %s %s" %
+                (type(rhs), rhs))
+    elif rhs.is_comparable:
+        if is_le(lhs.max, rhs):
+            return True
+        if is_gt(lhs.min, rhs):
+            return False
+
+
+@dispatch(AccumulationBounds, AccumulationBounds)
+def _eval_is_ge(lhs, rhs): # noqa:F811
+    if is_ge(lhs.min, rhs.max):
+        return True
+    if is_lt(lhs.max, rhs.min):
+        return False
+
+
+@dispatch(AccumulationBounds, Expr)  # type:ignore
+def _eval_is_ge(lhs, rhs): # noqa: F811
+    """
+    Returns ``True`` if range of values attained by ``lhs`` AccumulationBounds
+    object is less that the range of values attained by ``rhs``, where
+    other may be any value of type AccumulationBounds object or extended
+    real number value, ``False`` if ``rhs`` satisfies the same
+    property, else an unevaluated :py:class:`~.Relational`.
+
+    Examples
+    ========
+
+    >>> from sympy import AccumBounds, oo
+    >>> AccumBounds(1, 3) >= AccumBounds(4, oo)
+    False
+    >>> AccumBounds(1, 4) >= AccumBounds(3, 4)
+    AccumBounds(1, 4) >= AccumBounds(3, 4)
+    >>> AccumBounds(1, oo) >= 1
+    True
+    """
+
+    if not rhs.is_extended_real:
+        raise TypeError(
+            "Invalid comparison of %s %s" %
+            (type(rhs), rhs))
+    elif rhs.is_comparable:
+        if is_ge(lhs.min, rhs):
+            return True
+        if is_lt(lhs.max, rhs):
+            return False
+
+
+@dispatch(Expr, AccumulationBounds)  # type:ignore
+def _eval_is_ge(lhs, rhs): # noqa:F811
+    if not lhs.is_extended_real:
+        raise TypeError(
+            "Invalid comparison of %s %s" %
+            (type(lhs), lhs))
+    elif lhs.is_comparable:
+        if is_le(rhs.max, lhs):
+            return True
+        if is_gt(rhs.min, lhs):
+            return False
+
+
+@dispatch(AccumulationBounds, AccumulationBounds)  # type:ignore
+def _eval_is_ge(lhs, rhs): # noqa:F811
+    if is_ge(lhs.min, rhs.max):
+        return True
+    if is_lt(lhs.max, rhs.min):
+        return False
+
+# setting an alias for AccumulationBounds
+AccumBounds = AccumulationBounds

llmeval-env/lib/python3.10/site-packages/sympy/calculus/euler.py

@@ -0,0 +1,108 @@
+"""
+This module implements a method to find
+Euler-Lagrange Equations for given Lagrangian.
+"""
+from itertools import combinations_with_replacement
+from sympy.core.function import (Derivative, Function, diff)
+from sympy.core.relational import Eq
+from sympy.core.singleton import S
+from sympy.core.symbol import Symbol
+from sympy.core.sympify import sympify
+from sympy.utilities.iterables import iterable
+
+
+def euler_equations(L, funcs=(), vars=()):
+    r"""
+    Find the Euler-Lagrange equations [1]_ for a given Lagrangian.
+
+    Parameters
+    ==========
+
+    L : Expr
+        The Lagrangian that should be a function of the functions listed
+        in the second argument and their derivatives.
+
+        For example, in the case of two functions $f(x,y)$, $g(x,y)$ and
+        two independent variables $x$, $y$ the Lagrangian has the form:
+
+            .. math:: L\left(f(x,y),g(x,y),\frac{\partial f(x,y)}{\partial x},
+                      \frac{\partial f(x,y)}{\partial y},
+                      \frac{\partial g(x,y)}{\partial x},
+                      \frac{\partial g(x,y)}{\partial y},x,y\right)
+
+        In many cases it is not necessary to provide anything, except the
+        Lagrangian, it will be auto-detected (and an error raised if this
+        cannot be done).
+
+    funcs : Function or an iterable of Functions
+        The functions that the Lagrangian depends on. The Euler equations
+        are differential equations for each of these functions.
+
+    vars : Symbol or an iterable of Symbols
+        The Symbols that are the independent variables of the functions.
+
+    Returns
+    =======
+
+    eqns : list of Eq
+        The list of differential equations, one for each function.
+
+    Examples
+    ========
+
+    >>> from sympy import euler_equations, Symbol, Function
+    >>> x = Function('x')
+    >>> t = Symbol('t')
+    >>> L = (x(t).diff(t))**2/2 - x(t)**2/2
+    >>> euler_equations(L, x(t), t)
+    [Eq(-x(t) - Derivative(x(t), (t, 2)), 0)]
+    >>> u = Function('u')
+    >>> x = Symbol('x')
+    >>> L = (u(t, x).diff(t))**2/2 - (u(t, x).diff(x))**2/2
+    >>> euler_equations(L, u(t, x), [t, x])
+    [Eq(-Derivative(u(t, x), (t, 2)) + Derivative(u(t, x), (x, 2)), 0)]
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Euler%E2%80%93Lagrange_equation
+
+    """
+
+    funcs = tuple(funcs) if iterable(funcs) else (funcs,)
+
+    if not funcs:
+        funcs = tuple(L.atoms(Function))
+    else:
+        for f in funcs:
+            if not isinstance(f, Function):
+                raise TypeError('Function expected, got: %s' % f)
+
+    vars = tuple(vars) if iterable(vars) else (vars,)
+
+    if not vars:
+        vars = funcs[0].args
+    else:
+        vars = tuple(sympify(var) for var in vars)
+
+    if not all(isinstance(v, Symbol) for v in vars):
+        raise TypeError('Variables are not symbols, got %s' % vars)
+
+    for f in funcs:
+        if not vars == f.args:
+            raise ValueError("Variables %s do not match args: %s" % (vars, f))
+
+    order = max([len(d.variables) for d in L.atoms(Derivative)
+                        if d.expr in funcs] + [0])
+
+    eqns = []
+    for f in funcs:
+        eq = diff(L, f)
+        for i in range(1, order + 1):
+            for p in combinations_with_replacement(vars, i):
+                eq = eq + S.NegativeOne**i*diff(L, diff(f, *p), *p)
+        new_eq = Eq(eq, 0)
+        if isinstance(new_eq, Eq):
+            eqns.append(new_eq)
+
+    return eqns

llmeval-env/lib/python3.10/site-packages/sympy/calculus/finite_diff.py

@@ -0,0 +1,476 @@
+"""
+Finite difference weights
+=========================
+
+This module implements an algorithm for efficient generation of finite
+difference weights for ordinary differentials of functions for
+derivatives from 0 (interpolation) up to arbitrary order.
+
+The core algorithm is provided in the finite difference weight generating
+function (``finite_diff_weights``), and two convenience functions are provided
+for:
+
+- estimating a derivative (or interpolate) directly from a series of points
+    is also provided (``apply_finite_diff``).
+- differentiating by using finite difference approximations
+    (``differentiate_finite``).
+
+"""
+
+from sympy.core.function import Derivative
+from sympy.core.singleton import S
+from sympy.core.function import Subs
+from sympy.core.traversal import preorder_traversal
+from sympy.utilities.exceptions import sympy_deprecation_warning
+from sympy.utilities.iterables import iterable
+
+
+
+def finite_diff_weights(order, x_list, x0=S.One):
+    """
+    Calculates the finite difference weights for an arbitrarily spaced
+    one-dimensional grid (``x_list``) for derivatives at ``x0`` of order
+    0, 1, ..., up to ``order`` using a recursive formula. Order of accuracy
+    is at least ``len(x_list) - order``, if ``x_list`` is defined correctly.
+
+    Parameters
+    ==========
+
+    order: int
+        Up to what derivative order weights should be calculated.
+        0 corresponds to interpolation.
+    x_list: sequence
+        Sequence of (unique) values for the independent variable.
+        It is useful (but not necessary) to order ``x_list`` from
+        nearest to furthest from ``x0``; see examples below.
+    x0: Number or Symbol
+        Root or value of the independent variable for which the finite
+        difference weights should be generated. Default is ``S.One``.
+
+    Returns
+    =======
+
+    list
+        A list of sublists, each corresponding to coefficients for
+        increasing derivative order, and each containing lists of
+        coefficients for increasing subsets of x_list.
+
+    Examples
+    ========
+
+    >>> from sympy import finite_diff_weights, S
+    >>> res = finite_diff_weights(1, [-S(1)/2, S(1)/2, S(3)/2, S(5)/2], 0)
+    >>> res
+    [[[1, 0, 0, 0],
+      [1/2, 1/2, 0, 0],
+      [3/8, 3/4, -1/8, 0],
+      [5/16, 15/16, -5/16, 1/16]],
+     [[0, 0, 0, 0],
+      [-1, 1, 0, 0],
+      [-1, 1, 0, 0],
+      [-23/24, 7/8, 1/8, -1/24]]]
+    >>> res[0][-1]  # FD weights for 0th derivative, using full x_list
+    [5/16, 15/16, -5/16, 1/16]
+    >>> res[1][-1]  # FD weights for 1st derivative
+    [-23/24, 7/8, 1/8, -1/24]
+    >>> res[1][-2]  # FD weights for 1st derivative, using x_list[:-1]
+    [-1, 1, 0, 0]
+    >>> res[1][-1][0]  # FD weight for 1st deriv. for x_list[0]
+    -23/24
+    >>> res[1][-1][1]  # FD weight for 1st deriv. for x_list[1], etc.
+    7/8
+
+    Each sublist contains the most accurate formula at the end.
+    Note, that in the above example ``res[1][1]`` is the same as ``res[1][2]``.
+    Since res[1][2] has an order of accuracy of
+    ``len(x_list[:3]) - order = 3 - 1 = 2``, the same is true for ``res[1][1]``!
+
+    >>> res = finite_diff_weights(1, [S(0), S(1), -S(1), S(2), -S(2)], 0)[1]
+    >>> res
+    [[0, 0, 0, 0, 0],
+     [-1, 1, 0, 0, 0],
+     [0, 1/2, -1/2, 0, 0],
+     [-1/2, 1, -1/3, -1/6, 0],
+     [0, 2/3, -2/3, -1/12, 1/12]]
+    >>> res[0]  # no approximation possible, using x_list[0] only
+    [0, 0, 0, 0, 0]
+    >>> res[1]  # classic forward step approximation
+    [-1, 1, 0, 0, 0]
+    >>> res[2]  # classic centered approximation
+    [0, 1/2, -1/2, 0, 0]
+    >>> res[3:]  # higher order approximations
+    [[-1/2, 1, -1/3, -1/6, 0], [0, 2/3, -2/3, -1/12, 1/12]]
+
+    Let us compare this to a differently defined ``x_list``. Pay attention to
+    ``foo[i][k]`` corresponding to the gridpoint defined by ``x_list[k]``.
+
+    >>> foo = finite_diff_weights(1, [-S(2), -S(1), S(0), S(1), S(2)], 0)[1]
+    >>> foo
+    [[0, 0, 0, 0, 0],
+     [-1, 1, 0, 0, 0],
+     [1/2, -2, 3/2, 0, 0],
+     [1/6, -1, 1/2, 1/3, 0],
+     [1/12, -2/3, 0, 2/3, -1/12]]
+    >>> foo[1]  # not the same and of lower accuracy as res[1]!
+    [-1, 1, 0, 0, 0]
+    >>> foo[2]  # classic double backward step approximation
+    [1/2, -2, 3/2, 0, 0]
+    >>> foo[4]  # the same as res[4]
+    [1/12, -2/3, 0, 2/3, -1/12]
+
+    Note that, unless you plan on using approximations based on subsets of
+    ``x_list``, the order of gridpoints does not matter.
+
+    The capability to generate weights at arbitrary points can be
+    used e.g. to minimize Runge's phenomenon by using Chebyshev nodes:
+
+    >>> from sympy import cos, symbols, pi, simplify
+    >>> N, (h, x) = 4, symbols('h x')
+    >>> x_list = [x+h*cos(i*pi/(N)) for i in range(N,-1,-1)] # chebyshev nodes
+    >>> print(x_list)
+    [-h + x, -sqrt(2)*h/2 + x, x, sqrt(2)*h/2 + x, h + x]
+    >>> mycoeffs = finite_diff_weights(1, x_list, 0)[1][4]
+    >>> [simplify(c) for c in  mycoeffs] #doctest: +NORMALIZE_WHITESPACE
+    [(h**3/2 + h**2*x - 3*h*x**2 - 4*x**3)/h**4,
+    (-sqrt(2)*h**3 - 4*h**2*x + 3*sqrt(2)*h*x**2 + 8*x**3)/h**4,
+    (6*h**2*x - 8*x**3)/h**4,
+    (sqrt(2)*h**3 - 4*h**2*x - 3*sqrt(2)*h*x**2 + 8*x**3)/h**4,
+    (-h**3/2 + h**2*x + 3*h*x**2 - 4*x**3)/h**4]
+
+    Notes
+    =====
+
+    If weights for a finite difference approximation of 3rd order
+    derivative is wanted, weights for 0th, 1st and 2nd order are
+    calculated "for free", so are formulae using subsets of ``x_list``.
+    This is something one can take advantage of to save computational cost.
+    Be aware that one should define ``x_list`` from nearest to furthest from
+    ``x0``. If not, subsets of ``x_list`` will yield poorer approximations,
+    which might not grand an order of accuracy of ``len(x_list) - order``.
+
+    See also
+    ========
+
+    sympy.calculus.finite_diff.apply_finite_diff
+
+    References
+    ==========
+
+    .. [1] Generation of Finite Difference Formulas on Arbitrarily Spaced
+            Grids, Bengt Fornberg; Mathematics of computation; 51; 184;
+            (1988); 699-706; doi:10.1090/S0025-5718-1988-0935077-0
+
+    """
+    # The notation below closely corresponds to the one used in the paper.
+    order = S(order)
+    if not order.is_number:
+        raise ValueError("Cannot handle symbolic order.")
+    if order < 0:
+        raise ValueError("Negative derivative order illegal.")
+    if int(order) != order:
+        raise ValueError("Non-integer order illegal")
+    M = order
+    N = len(x_list) - 1
+    delta = [[[0 for nu in range(N+1)] for n in range(N+1)] for
+             m in range(M+1)]
+    delta[0][0][0] = S.One
+    c1 = S.One
+    for n in range(1, N+1):
+        c2 = S.One
+        for nu in range(n):
+            c3 = x_list[n] - x_list[nu]
+            c2 = c2 * c3
+            if n <= M:
+                delta[n][n-1][nu] = 0
+            for m in range(min(n, M)+1):
+                delta[m][n][nu] = (x_list[n]-x0)*delta[m][n-1][nu] -\
+                    m*delta[m-1][n-1][nu]
+                delta[m][n][nu] /= c3
+        for m in range(min(n, M)+1):
+            delta[m][n][n] = c1/c2*(m*delta[m-1][n-1][n-1] -
+                                    (x_list[n-1]-x0)*delta[m][n-1][n-1])
+        c1 = c2
+    return delta
+
+
+def apply_finite_diff(order, x_list, y_list, x0=S.Zero):
+    """
+    Calculates the finite difference approximation of
+    the derivative of requested order at ``x0`` from points
+    provided in ``x_list`` and ``y_list``.
+
+    Parameters
+    ==========
+
+    order: int
+        order of derivative to approximate. 0 corresponds to interpolation.
+    x_list: sequence
+        Sequence of (unique) values for the independent variable.
+    y_list: sequence
+        The function value at corresponding values for the independent
+        variable in x_list.
+    x0: Number or Symbol
+        At what value of the independent variable the derivative should be
+        evaluated. Defaults to 0.
+
+    Returns
+    =======
+
+    sympy.core.add.Add or sympy.core.numbers.Number
+        The finite difference expression approximating the requested
+        derivative order at ``x0``.
+
+    Examples
+    ========
+
+    >>> from sympy import apply_finite_diff
+    >>> cube = lambda arg: (1.0*arg)**3
+    >>> xlist = range(-3,3+1)
+    >>> apply_finite_diff(2, xlist, map(cube, xlist), 2) - 12 # doctest: +SKIP
+    -3.55271367880050e-15
+
+    we see that the example above only contain rounding errors.
+    apply_finite_diff can also be used on more abstract objects:
+
+    >>> from sympy import IndexedBase, Idx
+    >>> x, y = map(IndexedBase, 'xy')
+    >>> i = Idx('i')
+    >>> x_list, y_list = zip(*[(x[i+j], y[i+j]) for j in range(-1,2)])
+    >>> apply_finite_diff(1, x_list, y_list, x[i])
+    ((x[i + 1] - x[i])/(-x[i - 1] + x[i]) - 1)*y[i]/(x[i + 1] - x[i]) -
+    (x[i + 1] - x[i])*y[i - 1]/((x[i + 1] - x[i - 1])*(-x[i - 1] + x[i])) +
+    (-x[i - 1] + x[i])*y[i + 1]/((x[i + 1] - x[i - 1])*(x[i + 1] - x[i]))
+
+    Notes
+    =====
+
+    Order = 0 corresponds to interpolation.
+    Only supply so many points you think makes sense
+    to around x0 when extracting the derivative (the function
+    need to be well behaved within that region). Also beware
+    of Runge's phenomenon.
+
+    See also
+    ========
+
+    sympy.calculus.finite_diff.finite_diff_weights
+
+    References
+    ==========
+
+    Fortran 90 implementation with Python interface for numerics: finitediff_
+
+    .. _finitediff: https://github.com/bjodah/finitediff
+
+    """
+
+    # In the original paper the following holds for the notation:
+    # M = order
+    # N = len(x_list) - 1
+
+    N = len(x_list) - 1
+    if len(x_list) != len(y_list):
+        raise ValueError("x_list and y_list not equal in length.")
+
+    delta = finite_diff_weights(order, x_list, x0)
+
+    derivative = 0
+    for nu in range(len(x_list)):
+        derivative += delta[order][N][nu]*y_list[nu]
+    return derivative
+
+
+def _as_finite_diff(derivative, points=1, x0=None, wrt=None):
+    """
+    Returns an approximation of a derivative of a function in
+    the form of a finite difference formula. The expression is a
+    weighted sum of the function at a number of discrete values of
+    (one of) the independent variable(s).
+
+    Parameters
+    ==========
+
+    derivative: a Derivative instance
+
+    points: sequence or coefficient, optional
+        If sequence: discrete values (length >= order+1) of the
+        independent variable used for generating the finite
+        difference weights.
+        If it is a coefficient, it will be used as the step-size
+        for generating an equidistant sequence of length order+1
+        centered around ``x0``. default: 1 (step-size 1)
+
+    x0: number or Symbol, optional
+        the value of the independent variable (``wrt``) at which the
+        derivative is to be approximated. Default: same as ``wrt``.
+
+    wrt: Symbol, optional
+        "with respect to" the variable for which the (partial)
+        derivative is to be approximated for. If not provided it
+        is required that the Derivative is ordinary. Default: ``None``.
+
+    Examples
+    ========
+
+    >>> from sympy import symbols, Function, exp, sqrt, Symbol
+    >>> from sympy.calculus.finite_diff import _as_finite_diff
+    >>> x, h = symbols('x h')
+    >>> f = Function('f')
+    >>> _as_finite_diff(f(x).diff(x))
+    -f(x - 1/2) + f(x + 1/2)
+
+    The default step size and number of points are 1 and ``order + 1``
+    respectively. We can change the step size by passing a symbol
+    as a parameter:
+
+    >>> _as_finite_diff(f(x).diff(x), h)
+    -f(-h/2 + x)/h + f(h/2 + x)/h
+
+    We can also specify the discretized values to be used in a sequence:
+
+    >>> _as_finite_diff(f(x).diff(x), [x, x+h, x+2*h])
+    -3*f(x)/(2*h) + 2*f(h + x)/h - f(2*h + x)/(2*h)
+
+    The algorithm is not restricted to use equidistant spacing, nor
+    do we need to make the approximation around ``x0``, but we can get
+    an expression estimating the derivative at an offset:
+
+    >>> e, sq2 = exp(1), sqrt(2)
+    >>> xl = [x-h, x+h, x+e*h]
+    >>> _as_finite_diff(f(x).diff(x, 1), xl, x+h*sq2)
+    2*h*((h + sqrt(2)*h)/(2*h) - (-sqrt(2)*h + h)/(2*h))*f(E*h + x)/((-h + E*h)*(h + E*h)) +
+    (-(-sqrt(2)*h + h)/(2*h) - (-sqrt(2)*h + E*h)/(2*h))*f(-h + x)/(h + E*h) +
+    (-(h + sqrt(2)*h)/(2*h) + (-sqrt(2)*h + E*h)/(2*h))*f(h + x)/(-h + E*h)
+
+    Partial derivatives are also supported:
+
+    >>> y = Symbol('y')
+    >>> d2fdxdy=f(x,y).diff(x,y)
+    >>> _as_finite_diff(d2fdxdy, wrt=x)
+    -Derivative(f(x - 1/2, y), y) + Derivative(f(x + 1/2, y), y)
+
+    See also
+    ========
+
+    sympy.calculus.finite_diff.apply_finite_diff
+    sympy.calculus.finite_diff.finite_diff_weights
+
+    """
+    if derivative.is_Derivative:
+        pass
+    elif derivative.is_Atom:
+        return derivative
+    else:
+        return derivative.fromiter(
+            [_as_finite_diff(ar, points, x0, wrt) for ar
+             in derivative.args], **derivative.assumptions0)
+
+    if wrt is None:
+        old = None
+        for v in derivative.variables:
+            if old is v:
+                continue
+            derivative = _as_finite_diff(derivative, points, x0, v)
+            old = v
+        return derivative
+
+    order = derivative.variables.count(wrt)
+
+    if x0 is None:
+        x0 = wrt
+
+    if not iterable(points):
+        if getattr(points, 'is_Function', False) and wrt in points.args:
+            points = points.subs(wrt, x0)
+        # points is simply the step-size, let's make it a
+        # equidistant sequence centered around x0
+        if order % 2 == 0:
+            # even order => odd number of points, grid point included
+            points = [x0 + points*i for i
+                      in range(-order//2, order//2 + 1)]
+        else:
+            # odd order => even number of points, half-way wrt grid point
+            points = [x0 + points*S(i)/2 for i
+                      in range(-order, order + 1, 2)]
+    others = [wrt, 0]
+    for v in set(derivative.variables):
+        if v == wrt:
+            continue
+        others += [v, derivative.variables.count(v)]
+    if len(points) < order+1:
+        raise ValueError("Too few points for order %d" % order)
+    return apply_finite_diff(order, points, [
+        Derivative(derivative.expr.subs({wrt: x}), *others) for
+        x in points], x0)
+
+
+def differentiate_finite(expr, *symbols,
+                         points=1, x0=None, wrt=None, evaluate=False):
+    r""" Differentiate expr and replace Derivatives with finite differences.
+
+    Parameters
+    ==========
+
+    expr : expression
+    \*symbols : differentiate with respect to symbols
+    points: sequence, coefficient or undefined function, optional
+        see ``Derivative.as_finite_difference``
+    x0: number or Symbol, optional
+        see ``Derivative.as_finite_difference``
+    wrt: Symbol, optional
+        see ``Derivative.as_finite_difference``
+
+    Examples
+    ========
+
+    >>> from sympy import sin, Function, differentiate_finite
+    >>> from sympy.abc import x, y, h
+    >>> f, g = Function('f'), Function('g')
+    >>> differentiate_finite(f(x)*g(x), x, points=[x-h, x+h])
+    -f(-h + x)*g(-h + x)/(2*h) + f(h + x)*g(h + x)/(2*h)
+
+    ``differentiate_finite`` works on any expression, including the expressions
+    with embedded derivatives:
+
+    >>> differentiate_finite(f(x) + sin(x), x, 2)
+    -2*f(x) + f(x - 1) + f(x + 1) - 2*sin(x) + sin(x - 1) + sin(x + 1)
+    >>> differentiate_finite(f(x, y), x, y)
+    f(x - 1/2, y - 1/2) - f(x - 1/2, y + 1/2) - f(x + 1/2, y - 1/2) + f(x + 1/2, y + 1/2)
+    >>> differentiate_finite(f(x)*g(x).diff(x), x)
+    (-g(x) + g(x + 1))*f(x + 1/2) - (g(x) - g(x - 1))*f(x - 1/2)
+
+    To make finite difference with non-constant discretization step use
+    undefined functions:
+
+    >>> dx = Function('dx')
+    >>> differentiate_finite(f(x)*g(x).diff(x), points=dx(x))
+    -(-g(x - dx(x)/2 - dx(x - dx(x)/2)/2)/dx(x - dx(x)/2) +
+    g(x - dx(x)/2 + dx(x - dx(x)/2)/2)/dx(x - dx(x)/2))*f(x - dx(x)/2)/dx(x) +
+    (-g(x + dx(x)/2 - dx(x + dx(x)/2)/2)/dx(x + dx(x)/2) +
+    g(x + dx(x)/2 + dx(x + dx(x)/2)/2)/dx(x + dx(x)/2))*f(x + dx(x)/2)/dx(x)
+
+    """
+    if any(term.is_Derivative for term in list(preorder_traversal(expr))):
+        evaluate = False
+
+    Dexpr = expr.diff(*symbols, evaluate=evaluate)
+    if evaluate:
+        sympy_deprecation_warning("""
+        The evaluate flag to differentiate_finite() is deprecated.
+
+        evaluate=True expands the intermediate derivatives before computing
+        differences, but this usually not what you want, as it does not
+        satisfy the product rule.
+        """,
+            deprecated_since_version="1.5",
+             active_deprecations_target="deprecated-differentiate_finite-evaluate",
+        )
+        return Dexpr.replace(
+            lambda arg: arg.is_Derivative,
+            lambda arg: arg.as_finite_difference(points=points, x0=x0, wrt=wrt))
+    else:
+        DFexpr = Dexpr.as_finite_difference(points=points, x0=x0, wrt=wrt)
+        return DFexpr.replace(
+            lambda arg: isinstance(arg, Subs),
+            lambda arg: arg.expr.as_finite_difference(
+                    points=points, x0=arg.point[0], wrt=arg.variables[0]))

llmeval-env/lib/python3.10/site-packages/sympy/calculus/singularities.py

@@ -0,0 +1,398 @@
+"""
+Singularities
+=============
+
+This module implements algorithms for finding singularities for a function
+and identifying types of functions.
+
+The differential calculus methods in this module include methods to identify
+the following function types in the given ``Interval``:
+- Increasing
+- Strictly Increasing
+- Decreasing
+- Strictly Decreasing
+- Monotonic
+
+"""
+
+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.elementary.exponential import log
+from sympy.functions.elementary.trigonometric import sec, csc, cot, tan, cos
+from sympy.utilities.misc import filldedent
+
+
+def singularities(expression, symbol, domain=None):
+    """
+    Find singularities of a given function.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function in which singularities need to be found.
+    symbol : Symbol
+        The symbol over the values of which the singularity in
+        expression in being searched for.
+
+    Returns
+    =======
+
+    Set
+        A set of values for ``symbol`` for which ``expression`` has a
+        singularity. An ``EmptySet`` is returned if ``expression`` has no
+        singularities for any given value of ``Symbol``.
+
+    Raises
+    ======
+
+    NotImplementedError
+        Methods for determining the singularities of this function have
+        not been developed.
+
+    Notes
+    =====
+
+    This function does not find non-isolated singularities
+    nor does it find branch points of the expression.
+
+    Currently supported functions are:
+        - univariate continuous (real or complex) functions
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Mathematical_singularity
+
+    Examples
+    ========
+
+    >>> from sympy import singularities, Symbol, log
+    >>> x = Symbol('x', real=True)
+    >>> y = Symbol('y', real=False)
+    >>> singularities(x**2 + x + 1, x)
+    EmptySet
+    >>> singularities(1/(x + 1), x)
+    {-1}
+    >>> singularities(1/(y**2 + 1), y)
+    {-I, I}
+    >>> singularities(1/(y**3 + 1), y)
+    {-1, 1/2 - sqrt(3)*I/2, 1/2 + sqrt(3)*I/2}
+    >>> singularities(log(x), x)
+    {0}
+
+    """
+    from sympy.solvers.solveset import solveset
+
+    if domain is None:
+        domain = S.Reals if symbol.is_real else S.Complexes
+    try:
+        sings = S.EmptySet
+        for i in expression.rewrite([sec, csc, cot, tan], cos).atoms(Pow):
+            if i.exp.is_infinite:
+                raise NotImplementedError
+            if i.exp.is_negative:
+                sings += solveset(i.base, symbol, domain)
+        for i in expression.atoms(log):
+            sings += solveset(i.args[0], symbol, domain)
+        return sings
+    except NotImplementedError:
+        raise NotImplementedError(filldedent('''
+            Methods for determining the singularities
+            of this function have not been developed.'''))
+
+
+###########################################################################
+#                      DIFFERENTIAL CALCULUS METHODS                      #
+###########################################################################
+
+
+def monotonicity_helper(expression, predicate, interval=S.Reals, symbol=None):
+    """
+    Helper function for functions checking function monotonicity.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function which is being checked
+    predicate : function
+        The property being tested for. The function takes in an integer
+        and returns a boolean. The integer input is the derivative and
+        the boolean result should be true if the property is being held,
+        and false otherwise.
+    interval : Set, optional
+        The range of values in which we are testing, defaults to all reals.
+    symbol : Symbol, optional
+        The symbol present in expression which gets varied over the given range.
+
+    It returns a boolean indicating whether the interval in which
+    the function's derivative satisfies given predicate is a superset
+    of the given interval.
+
+    Returns
+    =======
+
+    Boolean
+        True if ``predicate`` is true for all the derivatives when ``symbol``
+        is varied in ``range``, False otherwise.
+
+    """
+    from sympy.solvers.solveset import solveset
+
+    expression = sympify(expression)
+    free = expression.free_symbols
+
+    if symbol is None:
+        if len(free) > 1:
+            raise NotImplementedError(
+                'The function has not yet been implemented'
+                ' for all multivariate expressions.'
+            )
+
+    variable = symbol or (free.pop() if free else Symbol('x'))
+    derivative = expression.diff(variable)
+    predicate_interval = solveset(predicate(derivative), variable, S.Reals)
+    return interval.is_subset(predicate_interval)
+
+
+def is_increasing(expression, interval=S.Reals, symbol=None):
+    """
+    Return whether the function is increasing in the given interval.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function which is being checked.
+    interval : Set, optional
+        The range of values in which we are testing (defaults to set of
+        all real numbers).
+    symbol : Symbol, optional
+        The symbol present in expression which gets varied over the given range.
+
+    Returns
+    =======
+
+    Boolean
+        True if ``expression`` is increasing (either strictly increasing or
+        constant) in the given ``interval``, False otherwise.
+
+    Examples
+    ========
+
+    >>> from sympy import is_increasing
+    >>> from sympy.abc import x, y
+    >>> from sympy import S, Interval, oo
+    >>> is_increasing(x**3 - 3*x**2 + 4*x, S.Reals)
+    True
+    >>> is_increasing(-x**2, Interval(-oo, 0))
+    True
+    >>> is_increasing(-x**2, Interval(0, oo))
+    False
+    >>> is_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval(-2, 3))
+    False
+    >>> is_increasing(x**2 + y, Interval(1, 2), x)
+    True
+
+    """
+    return monotonicity_helper(expression, lambda x: x >= 0, interval, symbol)
+
+
+def is_strictly_increasing(expression, interval=S.Reals, symbol=None):
+    """
+    Return whether the function is strictly increasing in the given interval.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function which is being checked.
+    interval : Set, optional
+        The range of values in which we are testing (defaults to set of
+        all real numbers).
+    symbol : Symbol, optional
+        The symbol present in expression which gets varied over the given range.
+
+    Returns
+    =======
+
+    Boolean
+        True if ``expression`` is strictly increasing in the given ``interval``,
+        False otherwise.
+
+    Examples
+    ========
+
+    >>> from sympy import is_strictly_increasing
+    >>> from sympy.abc import x, y
+    >>> from sympy import Interval, oo
+    >>> is_strictly_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval.Ropen(-oo, -2))
+    True
+    >>> is_strictly_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval.Lopen(3, oo))
+    True
+    >>> is_strictly_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval.open(-2, 3))
+    False
+    >>> is_strictly_increasing(-x**2, Interval(0, oo))
+    False
+    >>> is_strictly_increasing(-x**2 + y, Interval(-oo, 0), x)
+    False
+
+    """
+    return monotonicity_helper(expression, lambda x: x > 0, interval, symbol)
+
+
+def is_decreasing(expression, interval=S.Reals, symbol=None):
+    """
+    Return whether the function is decreasing in the given interval.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function which is being checked.
+    interval : Set, optional
+        The range of values in which we are testing (defaults to set of
+        all real numbers).
+    symbol : Symbol, optional
+        The symbol present in expression which gets varied over the given range.
+
+    Returns
+    =======
+
+    Boolean
+        True if ``expression`` is decreasing (either strictly decreasing or
+        constant) in the given ``interval``, False otherwise.
+
+    Examples
+    ========
+
+    >>> from sympy import is_decreasing
+    >>> from sympy.abc import x, y
+    >>> from sympy import S, Interval, oo
+    >>> is_decreasing(1/(x**2 - 3*x), Interval.open(S(3)/2, 3))
+    True
+    >>> is_decreasing(1/(x**2 - 3*x), Interval.open(1.5, 3))
+    True
+    >>> is_decreasing(1/(x**2 - 3*x), Interval.Lopen(3, oo))
+    True
+    >>> is_decreasing(1/(x**2 - 3*x), Interval.Ropen(-oo, S(3)/2))
+    False
+    >>> is_decreasing(1/(x**2 - 3*x), Interval.Ropen(-oo, 1.5))
+    False
+    >>> is_decreasing(-x**2, Interval(-oo, 0))
+    False
+    >>> is_decreasing(-x**2 + y, Interval(-oo, 0), x)
+    False
+
+    """
+    return monotonicity_helper(expression, lambda x: x <= 0, interval, symbol)
+
+
+def is_strictly_decreasing(expression, interval=S.Reals, symbol=None):
+    """
+    Return whether the function is strictly decreasing in the given interval.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function which is being checked.
+    interval : Set, optional
+        The range of values in which we are testing (defaults to set of
+        all real numbers).
+    symbol : Symbol, optional
+        The symbol present in expression which gets varied over the given range.
+
+    Returns
+    =======
+
+    Boolean
+        True if ``expression`` is strictly decreasing in the given ``interval``,
+        False otherwise.
+
+    Examples
+    ========
+
+    >>> from sympy import is_strictly_decreasing
+    >>> from sympy.abc import x, y
+    >>> from sympy import S, Interval, oo
+    >>> is_strictly_decreasing(1/(x**2 - 3*x), Interval.Lopen(3, oo))
+    True
+    >>> is_strictly_decreasing(1/(x**2 - 3*x), Interval.Ropen(-oo, S(3)/2))
+    False
+    >>> is_strictly_decreasing(1/(x**2 - 3*x), Interval.Ropen(-oo, 1.5))
+    False
+    >>> is_strictly_decreasing(-x**2, Interval(-oo, 0))
+    False
+    >>> is_strictly_decreasing(-x**2 + y, Interval(-oo, 0), x)
+    False
+
+    """
+    return monotonicity_helper(expression, lambda x: x < 0, interval, symbol)
+
+
+def is_monotonic(expression, interval=S.Reals, symbol=None):
+    """
+    Return whether the function is monotonic in the given interval.
+
+    Parameters
+    ==========
+
+    expression : Expr
+        The target function which is being checked.
+    interval : Set, optional
+        The range of values in which we are testing (defaults to set of
+        all real numbers).
+    symbol : Symbol, optional
+        The symbol present in expression which gets varied over the given range.
+
+    Returns
+    =======
+
+    Boolean
+        True if ``expression`` is monotonic in the given ``interval``,
+        False otherwise.
+
+    Raises
+    ======
+
+    NotImplementedError
+        Monotonicity check has not been implemented for the queried function.
+
+    Examples
+    ========
+
+    >>> from sympy import is_monotonic
+    >>> from sympy.abc import x, y
+    >>> from sympy import S, Interval, oo
+    >>> is_monotonic(1/(x**2 - 3*x), Interval.open(S(3)/2, 3))
+    True
+    >>> is_monotonic(1/(x**2 - 3*x), Interval.open(1.5, 3))
+    True
+    >>> is_monotonic(1/(x**2 - 3*x), Interval.Lopen(3, oo))
+    True
+    >>> is_monotonic(x**3 - 3*x**2 + 4*x, S.Reals)
+    True
+    >>> is_monotonic(-x**2, S.Reals)
+    False
+    >>> is_monotonic(x**2 + y + 1, Interval(1, 2), x)
+    True
+
+    """
+    from sympy.solvers.solveset import solveset
+
+    expression = sympify(expression)
+
+    free = expression.free_symbols
+    if symbol is None and len(free) > 1:
+        raise NotImplementedError(
+            'is_monotonic has not yet been implemented'
+            ' for all multivariate expressions.'
+        )
+
+    variable = symbol or (free.pop() if free else Symbol('x'))
+    turning_points = solveset(expression.diff(variable), variable, interval)
+    return interval.intersection(turning_points) is S.EmptySet

llmeval-env/lib/python3.10/site-packages/sympy/calculus/tests/test_accumulationbounds.py

@@ -0,0 +1,336 @@
+from sympy.core.numbers import (E, Rational, oo, pi, zoo)
+from sympy.core.singleton import S
+from sympy.core.symbol import Symbol
+from sympy.functions.elementary.exponential import (exp, log)
+from sympy.functions.elementary.miscellaneous import (Max, Min, sqrt)
+from sympy.functions.elementary.trigonometric import (cos, sin, tan)
+from sympy.calculus.accumulationbounds import AccumBounds
+from sympy.core import Add, Mul, Pow
+from sympy.core.expr import unchanged
+from sympy.testing.pytest import raises, XFAIL
+from sympy.abc import x
+
+a = Symbol('a', real=True)
+B = AccumBounds
+
+
+def test_AccumBounds():
+    assert B(1, 2).args == (1, 2)
+    assert B(1, 2).delta is S.One
+    assert B(1, 2).mid == Rational(3, 2)
+    assert B(1, 3).is_real == True
+
+    assert B(1, 1) is S.One
+
+    assert B(1, 2) + 1 == B(2, 3)
+    assert 1 + B(1, 2) == B(2, 3)
+    assert B(1, 2) + B(2, 3) == B(3, 5)
+
+    assert -B(1, 2) == B(-2, -1)
+
+    assert B(1, 2) - 1 == B(0, 1)
+    assert 1 - B(1, 2) == B(-1, 0)
+    assert B(2, 3) - B(1, 2) == B(0, 2)
+
+    assert x + B(1, 2) == Add(B(1, 2), x)
+    assert a + B(1, 2) == B(1 + a, 2 + a)
+    assert B(1, 2) - x == Add(B(1, 2), -x)
+
+    assert B(-oo, 1) + oo == B(-oo, oo)
+    assert B(1, oo) + oo is oo
+    assert B(1, oo) - oo == B(-oo, oo)
+    assert (-oo - B(-1, oo)) is -oo
+    assert B(-oo, 1) - oo is -oo
+
+    assert B(1, oo) - oo == B(-oo, oo)
+    assert B(-oo, 1) - (-oo) == B(-oo, oo)
+    assert (oo - B(1, oo)) == B(-oo, oo)
+    assert (-oo - B(1, oo)) is -oo
+
+    assert B(1, 2)/2 == B(S.Half, 1)
+    assert 2/B(2, 3) == B(Rational(2, 3), 1)
+    assert 1/B(-1, 1) == B(-oo, oo)
+
+    assert abs(B(1, 2)) == B(1, 2)
+    assert abs(B(-2, -1)) == B(1, 2)
+    assert abs(B(-2, 1)) == B(0, 2)
+    assert abs(B(-1, 2)) == B(0, 2)
+    c = Symbol('c')
+    raises(ValueError, lambda: B(0, c))
+    raises(ValueError, lambda: B(1, -1))
+    r = Symbol('r', real=True)
+    raises(ValueError, lambda: B(r, r - 1))
+
+
+def test_AccumBounds_mul():
+    assert B(1, 2)*2 == B(2, 4)
+    assert 2*B(1, 2) == B(2, 4)
+    assert B(1, 2)*B(2, 3) == B(2, 6)
+    assert B(0, 2)*B(2, oo) == B(0, oo)
+    l, r = B(-oo, oo), B(-a, a)
+    assert l*r == B(-oo, oo)
+    assert r*l == B(-oo, oo)
+    l, r = B(1, oo), B(-3, -2)
+    assert l*r == B(-oo, -2)
+    assert r*l == B(-oo, -2)
+    assert B(1, 2)*0 == 0
+    assert B(1, oo)*0 == B(0, oo)
+    assert B(-oo, 1)*0 == B(-oo, 0)
+    assert B(-oo, oo)*0 == B(-oo, oo)
+
+    assert B(1, 2)*x == Mul(B(1, 2), x, evaluate=False)
+
+    assert B(0, 2)*oo == B(0, oo)
+    assert B(-2, 0)*oo == B(-oo, 0)
+    assert B(0, 2)*(-oo) == B(-oo, 0)
+    assert B(-2, 0)*(-oo) == B(0, oo)
+    assert B(-1, 1)*oo == B(-oo, oo)
+    assert B(-1, 1)*(-oo) == B(-oo, oo)
+    assert B(-oo, oo)*oo == B(-oo, oo)
+
+
+def test_AccumBounds_div():
+    assert B(-1, 3)/B(3, 4) == B(Rational(-1, 3), 1)
+    assert B(-2, 4)/B(-3, 4) == B(-oo, oo)
+    assert B(-3, -2)/B(-4, 0) == B(S.Half, oo)
+
+    # these two tests can have a better answer
+    # after Union of B is improved
+    assert B(-3, -2)/B(-2, 1) == B(-oo, oo)
+    assert B(2, 3)/B(-2, 2) == B(-oo, oo)
+
+    assert B(-3, -2)/B(0, 4) == B(-oo, Rational(-1, 2))
+    assert B(2, 4)/B(-3, 0) == B(-oo, Rational(-2, 3))
+    assert B(2, 4)/B(0, 3) == B(Rational(2, 3), oo)
+
+    assert B(0, 1)/B(0, 1) == B(0, oo)
+    assert B(-1, 0)/B(0, 1) == B(-oo, 0)
+    assert B(-1, 2)/B(-2, 2) == B(-oo, oo)
+
+    assert 1/B(-1, 2) == B(-oo, oo)
+    assert 1/B(0, 2) == B(S.Half, oo)
+    assert (-1)/B(0, 2) == B(-oo, Rational(-1, 2))
+    assert 1/B(-oo, 0) == B(-oo, 0)
+    assert 1/B(-1, 0) == B(-oo, -1)
+    assert (-2)/B(-oo, 0) == B(0, oo)
+    assert 1/B(-oo, -1) == B(-1, 0)
+
+    assert B(1, 2)/a == Mul(B(1, 2), 1/a, evaluate=False)
+
+    assert B(1, 2)/0 == B(1, 2)*zoo
+    assert B(1, oo)/oo == B(0, oo)
+    assert B(1, oo)/(-oo) == B(-oo, 0)
+    assert B(-oo, -1)/oo == B(-oo, 0)
+    assert B(-oo, -1)/(-oo) == B(0, oo)
+    assert B(-oo, oo)/oo == B(-oo, oo)
+    assert B(-oo, oo)/(-oo) == B(-oo, oo)
+    assert B(-1, oo)/oo == B(0, oo)
+    assert B(-1, oo)/(-oo) == B(-oo, 0)
+    assert B(-oo, 1)/oo == B(-oo, 0)
+    assert B(-oo, 1)/(-oo) == B(0, oo)
+
+
+def test_issue_18795():
+    r = Symbol('r', real=True)
+    a = B(-1,1)
+    c = B(7, oo)
+    b = B(-oo, oo)
+    assert c - tan(r) == B(7-tan(r), oo)
+    assert b + tan(r) == B(-oo, oo)
+    assert (a + r)/a == B(-oo, oo)*B(r - 1, r + 1)
+    assert (b + a)/a == B(-oo, oo)
+
+
+def test_AccumBounds_func():
+    assert (x**2 + 2*x + 1).subs(x, B(-1, 1)) == B(-1, 4)
+    assert exp(B(0, 1)) == B(1, E)
+    assert exp(B(-oo, oo)) == B(0, oo)
+    assert log(B(3, 6)) == B(log(3), log(6))
+
+
+@XFAIL
+def test_AccumBounds_powf():
+    nn = Symbol('nn', nonnegative=True)
+    assert B(1 + nn, 2 + nn)**B(1, 2) == B(1 + nn, (2 + nn)**2)
+    i = Symbol('i', integer=True, negative=True)
+    assert B(1, 2)**i == B(2**i, 1)
+
+
+def test_AccumBounds_pow():
+    assert B(0, 2)**2 == B(0, 4)
+    assert B(-1, 1)**2 == B(0, 1)
+    assert B(1, 2)**2 == B(1, 4)
+    assert B(-1, 2)**3 == B(-1, 8)
+    assert B(-1, 1)**0 == 1
+
+    assert B(1, 2)**Rational(5, 2) == B(1, 4*sqrt(2))
+    assert B(0, 2)**S.Half == B(0, sqrt(2))
+
+    neg = Symbol('neg', negative=True)
+    assert unchanged(Pow, B(neg, 1), S.Half)
+    nn = Symbol('nn', nonnegative=True)
+    assert B(nn, nn + 1)**S.Half == B(sqrt(nn), sqrt(nn + 1))
+    assert B(nn, nn + 1)**nn == B(nn**nn, (nn + 1)**nn)
+    assert unchanged(Pow, B(nn, nn + 1), x)
+    i = Symbol('i', integer=True)
+    assert B(1, 2)**i == B(Min(1, 2**i), Max(1, 2**i))
+    i = Symbol('i', integer=True, nonnegative=True)
+    assert B(1, 2)**i == B(1, 2**i)
+    assert B(0, 1)**i == B(0**i, 1)
+
+    assert B(1, 5)**(-2) == B(Rational(1, 25), 1)
+    assert B(-1, 3)**(-2) == B(0, oo)
+    assert B(0, 2)**(-3) == B(Rational(1, 8), oo)
+    assert B(-2, 0)**(-3) == B(-oo, -Rational(1, 8))
+    assert B(0, 2)**(-2) == B(Rational(1, 4), oo)
+    assert B(-1, 2)**(-3) == B(-oo, oo)
+    assert B(-3, -2)**(-3) == B(Rational(-1, 8), Rational(-1, 27))
+    assert B(-3, -2)**(-2) == B(Rational(1, 9), Rational(1, 4))
+    assert B(0, oo)**S.Half == B(0, oo)
+    assert B(-oo, 0)**(-2) == B(0, oo)
+    assert B(-2, 0)**(-2) == B(Rational(1, 4), oo)
+
+    assert B(Rational(1, 3), S.Half)**oo is S.Zero
+    assert B(0, S.Half)**oo is S.Zero
+    assert B(S.Half, 1)**oo == B(0, oo)
+    assert B(0, 1)**oo == B(0, oo)
+    assert B(2, 3)**oo is oo
+    assert B(1, 2)**oo == B(0, oo)
+    assert B(S.Half, 3)**oo == B(0, oo)
+    assert B(Rational(-1, 3), Rational(-1, 4))**oo is S.Zero
+    assert B(-1, Rational(-1, 2))**oo is S.NaN
+    assert B(-3, -2)**oo is zoo
+    assert B(-2, -1)**oo is S.NaN
+    assert B(-2, Rational(-1, 2))**oo is S.NaN
+    assert B(Rational(-1, 2), S.Half)**oo is S.Zero
+    assert B(Rational(-1, 2), 1)**oo == B(0, oo)
+    assert B(Rational(-2, 3), 2)**oo == B(0, oo)
+    assert B(-1, 1)**oo == B(-oo, oo)
+    assert B(-1, S.Half)**oo == B(-oo, oo)
+    assert B(-1, 2)**oo == B(-oo, oo)
+    assert B(-2, S.Half)**oo == B(-oo, oo)
+
+    assert B(1, 2)**x == Pow(B(1, 2), x, evaluate=False)
+
+    assert B(2, 3)**(-oo) is S.Zero
+    assert B(0, 2)**(-oo) == B(0, oo)
+    assert B(-1, 2)**(-oo) == B(-oo, oo)
+
+    assert (tan(x)**sin(2*x)).subs(x, B(0, pi/2)) == \
+        Pow(B(-oo, oo), B(0, 1))
+
+
+def test_AccumBounds_exponent():
+    # base is 0
+    z = 0**B(a, a + S.Half)
+    assert z.subs(a, 0) == B(0, 1)
+    assert z.subs(a, 1) == 0
+    p = z.subs(a, -1)
+    assert p.is_Pow and p.args == (0, B(-1, -S.Half))
+    # base > 0
+    #   when base is 1 the type of bounds does not matter
+    assert 1**B(a, a + 1) == 1
+    #  otherwise we need to know if 0 is in the bounds
+    assert S.Half**B(-2, 2) == B(S(1)/4, 4)
+    assert 2**B(-2, 2) == B(S(1)/4, 4)
+
+    # +eps may introduce +oo
+    # if there is a negative integer exponent
+    assert B(0, 1)**B(S(1)/2, 1) == B(0, 1)
+    assert B(0, 1)**B(0, 1) == B(0, 1)
+
+    # positive bases have positive bounds
+    assert B(2, 3)**B(-3, -2) == B(S(1)/27, S(1)/4)
+    assert B(2, 3)**B(-3, 2) == B(S(1)/27, 9)
+
+    # bounds generating imaginary parts unevaluated
+    assert unchanged(Pow, B(-1, 1), B(1, 2))
+    assert B(0, S(1)/2)**B(1, oo) == B(0, S(1)/2)
+    assert B(0, 1)**B(1, oo) == B(0, oo)
+    assert B(0, 2)**B(1, oo) == B(0, oo)
+    assert B(0, oo)**B(1, oo) == B(0, oo)
+    assert B(S(1)/2, 1)**B(1, oo) == B(0, oo)
+    assert B(S(1)/2, 1)**B(-oo, -1) == B(0, oo)
+    assert B(S(1)/2, 1)**B(-oo, oo) == B(0, oo)
+    assert B(S(1)/2, 2)**B(1, oo) == B(0, oo)
+    assert B(S(1)/2, 2)**B(-oo, -1) == B(0, oo)
+    assert B(S(1)/2, 2)**B(-oo, oo) == B(0, oo)
+    assert B(S(1)/2, oo)**B(1, oo) == B(0, oo)
+    assert B(S(1)/2, oo)**B(-oo, -1) == B(0, oo)
+    assert B(S(1)/2, oo)**B(-oo, oo) == B(0, oo)
+    assert B(1, 2)**B(1, oo) == B(0, oo)
+    assert B(1, 2)**B(-oo, -1) == B(0, oo)
+    assert B(1, 2)**B(-oo, oo) == B(0, oo)
+    assert B(1, oo)**B(1, oo) == B(0, oo)
+    assert B(1, oo)**B(-oo, -1) == B(0, oo)
+    assert B(1, oo)**B(-oo, oo) == B(0, oo)
+    assert B(2, oo)**B(1, oo) == B(2, oo)
+    assert B(2, oo)**B(-oo, -1) == B(0, S(1)/2)
+    assert B(2, oo)**B(-oo, oo) == B(0, oo)
+
+
+def test_comparison_AccumBounds():
+    assert (B(1, 3) < 4) == S.true
+    assert (B(1, 3) < -1) == S.false
+    assert (B(1, 3) < 2).rel_op == '<'
+    assert (B(1, 3) <= 2).rel_op == '<='
+
+    assert (B(1, 3) > 4) == S.false
+    assert (B(1, 3) > -1) == S.true
+    assert (B(1, 3) > 2).rel_op == '>'
+    assert (B(1, 3) >= 2).rel_op == '>='
+
+    assert (B(1, 3) < B(4, 6)) == S.true
+    assert (B(1, 3) < B(2, 4)).rel_op == '<'
+    assert (B(1, 3) < B(-2, 0)) == S.false
+
+    assert (B(1, 3) <= B(4, 6)) == S.true
+    assert (B(1, 3) <= B(-2, 0)) == S.false
+
+    assert (B(1, 3) > B(4, 6)) == S.false
+    assert (B(1, 3) > B(-2, 0)) == S.true
+
+    assert (B(1, 3) >= B(4, 6)) == S.false
+    assert (B(1, 3) >= B(-2, 0)) == S.true
+
+    # issue 13499
+    assert (cos(x) > 0).subs(x, oo) == (B(-1, 1) > 0)
+
+    c = Symbol('c')
+    raises(TypeError, lambda: (B(0, 1) < c))
+    raises(TypeError, lambda: (B(0, 1) <= c))
+    raises(TypeError, lambda: (B(0, 1) > c))
+    raises(TypeError, lambda: (B(0, 1) >= c))
+
+
+def test_contains_AccumBounds():
+    assert (1 in B(1, 2)) == S.true
+    raises(TypeError, lambda: a in B(1, 2))
+    assert 0 in B(-1, 0)
+    raises(TypeError, lambda:
+        (cos(1)**2 + sin(1)**2 - 1) in B(-1, 0))
+    assert (-oo in B(1, oo)) == S.true
+    assert (oo in B(-oo, 0)) == S.true
+
+    # issue 13159
+    assert Mul(0, B(-1, 1)) == Mul(B(-1, 1), 0) == 0
+    import itertools
+    for perm in itertools.permutations([0, B(-1, 1), x]):
+        assert Mul(*perm) == 0
+
+
+def test_intersection_AccumBounds():
+    assert B(0, 3).intersection(B(1, 2)) == B(1, 2)
+    assert B(0, 3).intersection(B(1, 4)) == B(1, 3)
+    assert B(0, 3).intersection(B(-1, 2)) == B(0, 2)
+    assert B(0, 3).intersection(B(-1, 4)) == B(0, 3)
+    assert B(0, 1).intersection(B(2, 3)) == S.EmptySet
+    raises(TypeError, lambda: B(0, 3).intersection(1))
+
+
+def test_union_AccumBounds():
+    assert B(0, 3).union(B(1, 2)) == B(0, 3)
+    assert B(0, 3).union(B(1, 4)) == B(0, 4)
+    assert B(0, 3).union(B(-1, 2)) == B(-1, 3)
+    assert B(0, 3).union(B(-1, 4)) == B(-1, 4)
+    raises(TypeError, lambda: B(0, 3).union(1))

llmeval-env/lib/python3.10/site-packages/sympy/calculus/tests/test_euler.py

@@ -0,0 +1,74 @@
+from sympy.core.function import (Derivative as D, Function)
+from sympy.core.relational import Eq
+from sympy.core.symbol import (Symbol, symbols)
+from sympy.functions.elementary.trigonometric import (cos, sin)
+from sympy.testing.pytest import raises
+from sympy.calculus.euler import euler_equations as euler
+
+
+def test_euler_interface():
+    x = Function('x')
+    y = Symbol('y')
+    t = Symbol('t')
+    raises(TypeError, lambda: euler())
+    raises(TypeError, lambda: euler(D(x(t), t)*y(t), [x(t), y]))
+    raises(ValueError, lambda: euler(D(x(t), t)*x(y), [x(t), x(y)]))
+    raises(TypeError, lambda: euler(D(x(t), t)**2, x(0)))
+    raises(TypeError, lambda: euler(D(x(t), t)*y(t), [t]))
+    assert euler(D(x(t), t)**2/2, {x(t)}) == [Eq(-D(x(t), t, t), 0)]
+    assert euler(D(x(t), t)**2/2, x(t), {t}) == [Eq(-D(x(t), t, t), 0)]
+
+
+def test_euler_pendulum():
+    x = Function('x')
+    t = Symbol('t')
+    L = D(x(t), t)**2/2 + cos(x(t))
+    assert euler(L, x(t), t) == [Eq(-sin(x(t)) - D(x(t), t, t), 0)]
+
+
+def test_euler_henonheiles():
+    x = Function('x')
+    y = Function('y')
+    t = Symbol('t')
+    L = sum(D(z(t), t)**2/2 - z(t)**2/2 for z in [x, y])
+    L += -x(t)**2*y(t) + y(t)**3/3
+    assert euler(L, [x(t), y(t)], t) == [Eq(-2*x(t)*y(t) - x(t) -
+                                            D(x(t), t, t), 0),
+                                         Eq(-x(t)**2 + y(t)**2 -
+                                            y(t) - D(y(t), t, t), 0)]
+
+
+def test_euler_sineg():
+    psi = Function('psi')
+    t = Symbol('t')
+    x = Symbol('x')
+    L = D(psi(t, x), t)**2/2 - D(psi(t, x), x)**2/2 + cos(psi(t, x))
+    assert euler(L, psi(t, x), [t, x]) == [Eq(-sin(psi(t, x)) -
+                                              D(psi(t, x), t, t) +
+                                              D(psi(t, x), x, x), 0)]
+
+
+def test_euler_high_order():
+    # an example from hep-th/0309038
+    m = Symbol('m')
+    k = Symbol('k')
+    x = Function('x')
+    y = Function('y')
+    t = Symbol('t')
+    L = (m*D(x(t), t)**2/2 + m*D(y(t), t)**2/2 -
+         k*D(x(t), t)*D(y(t), t, t) + k*D(y(t), t)*D(x(t), t, t))
+    assert euler(L, [x(t), y(t)]) == [Eq(2*k*D(y(t), t, t, t) -
+                                         m*D(x(t), t, t), 0),
+                                      Eq(-2*k*D(x(t), t, t, t) -
+                                         m*D(y(t), t, t), 0)]
+
+    w = Symbol('w')
+    L = D(x(t, w), t, w)**2/2
+    assert euler(L) == [Eq(D(x(t, w), t, t, w, w), 0)]
+
+def test_issue_18653():
+    x, y, z = symbols("x y z")
+    f, g, h = symbols("f g h", cls=Function, args=(x, y))
+    f, g, h = f(), g(), h()
+    expr2 = f.diff(x)*h.diff(z)
+    assert euler(expr2, (f,), (x, y)) == []

llmeval-env/lib/python3.10/site-packages/sympy/calculus/tests/test_singularities.py

@@ -0,0 +1,103 @@
+from sympy.core.numbers import (I, Rational, oo)
+from sympy.core.singleton import S
+from sympy.core.symbol import Symbol
+from sympy.functions.elementary.exponential import (exp, log)
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.calculus.singularities import (
+    singularities,
+    is_increasing,
+    is_strictly_increasing,
+    is_decreasing,
+    is_strictly_decreasing,
+    is_monotonic
+)
+from sympy.sets import Interval, FiniteSet
+from sympy.testing.pytest import raises
+from sympy.abc import x, y
+
+
+def test_singularities():
+    x = Symbol('x')
+    assert singularities(x**2, x) == S.EmptySet
+    assert singularities(x/(x**2 + 3*x + 2), x) == FiniteSet(-2, -1)
+    assert singularities(1/(x**2 + 1), x) == FiniteSet(I, -I)
+    assert singularities(x/(x**3 + 1), x) == \
+        FiniteSet(-1, (1 - sqrt(3) * I) / 2, (1 + sqrt(3) * I) / 2)
+    assert singularities(1/(y**2 + 2*I*y + 1), y) == \
+        FiniteSet(-I + sqrt(2)*I, -I - sqrt(2)*I)
+
+    x = Symbol('x', real=True)
+    assert singularities(1/(x**2 + 1), x) == S.EmptySet
+    assert singularities(exp(1/x), x, S.Reals) == FiniteSet(0)
+    assert singularities(exp(1/x), x, Interval(1, 2)) == S.EmptySet
+    assert singularities(log((x - 2)**2), x, Interval(1, 3)) == FiniteSet(2)
+    raises(NotImplementedError, lambda: singularities(x**-oo, x))
+
+
+def test_is_increasing():
+    """Test whether is_increasing returns correct value."""
+    a = Symbol('a', negative=True)
+
+    assert is_increasing(x**3 - 3*x**2 + 4*x, S.Reals)
+    assert is_increasing(-x**2, Interval(-oo, 0))
+    assert not is_increasing(-x**2, Interval(0, oo))
+    assert not is_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval(-2, 3))
+    assert is_increasing(x**2 + y, Interval(1, oo), x)
+    assert is_increasing(-x**2*a, Interval(1, oo), x)
+    assert is_increasing(1)
+
+    assert is_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval(-2, 3)) is False
+
+
+def test_is_strictly_increasing():
+    """Test whether is_strictly_increasing returns correct value."""
+    assert is_strictly_increasing(
+        4*x**3 - 6*x**2 - 72*x + 30, Interval.Ropen(-oo, -2))
+    assert is_strictly_increasing(
+        4*x**3 - 6*x**2 - 72*x + 30, Interval.Lopen(3, oo))
+    assert not is_strictly_increasing(
+        4*x**3 - 6*x**2 - 72*x + 30, Interval.open(-2, 3))
+    assert not is_strictly_increasing(-x**2, Interval(0, oo))
+    assert not is_strictly_decreasing(1)
+
+    assert is_strictly_increasing(4*x**3 - 6*x**2 - 72*x + 30, Interval.open(-2, 3)) is False
+
+
+def test_is_decreasing():
+    """Test whether is_decreasing returns correct value."""
+    b = Symbol('b', positive=True)
+
+    assert is_decreasing(1/(x**2 - 3*x), Interval.open(Rational(3,2), 3))
+    assert is_decreasing(1/(x**2 - 3*x), Interval.open(1.5, 3))
+    assert is_decreasing(1/(x**2 - 3*x), Interval.Lopen(3, oo))
+    assert not is_decreasing(1/(x**2 - 3*x), Interval.Ropen(-oo, Rational(3, 2)))
+    assert not is_decreasing(-x**2, Interval(-oo, 0))
+    assert not is_decreasing(-x**2*b, Interval(-oo, 0), x)
+
+
+def test_is_strictly_decreasing():
+    """Test whether is_strictly_decreasing returns correct value."""
+    assert is_strictly_decreasing(1/(x**2 - 3*x), Interval.Lopen(3, oo))
+    assert not is_strictly_decreasing(
+        1/(x**2 - 3*x), Interval.Ropen(-oo, Rational(3, 2)))
+    assert not is_strictly_decreasing(-x**2, Interval(-oo, 0))
+    assert not is_strictly_decreasing(1)
+    assert is_strictly_decreasing(1/(x**2 - 3*x), Interval.open(Rational(3,2), 3))
+    assert is_strictly_decreasing(1/(x**2 - 3*x), Interval.open(1.5, 3))
+
+
+def test_is_monotonic():
+    """Test whether is_monotonic returns correct value."""
+    assert is_monotonic(1/(x**2 - 3*x), Interval.open(Rational(3,2), 3))
+    assert is_monotonic(1/(x**2 - 3*x), Interval.open(1.5, 3))
+    assert is_monotonic(1/(x**2 - 3*x), Interval.Lopen(3, oo))
+    assert is_monotonic(x**3 - 3*x**2 + 4*x, S.Reals)
+    assert not is_monotonic(-x**2, S.Reals)
+    assert is_monotonic(x**2 + y + 1, Interval(1, 2), x)
+    raises(NotImplementedError, lambda: is_monotonic(x**2 + y + 1))
+
+
+def test_issue_23401():
+    x = Symbol('x')
+    expr = (x + 1)/(-1.0e-3*x**2 + 0.1*x + 0.1)
+    assert is_increasing(expr, Interval(1,2), x)

llmeval-env/lib/python3.10/site-packages/sympy/calculus/util.py

@@ -0,0 +1,841 @@
+from .accumulationbounds import AccumBounds, AccumulationBounds # noqa: F401
+from .singularities import singularities
+from sympy.core import Pow, S
+from sympy.core.function import diff, expand_mul
+from sympy.core.kind import NumberKind
+from sympy.core.mod import Mod
+from sympy.core.numbers import equal_valued
+from sympy.core.relational import Relational
+from sympy.core.symbol import Symbol, Dummy
+from sympy.core.sympify import _sympify
+from sympy.functions.elementary.complexes import Abs, im, re
+from sympy.functions.elementary.exponential import exp, log
+from sympy.functions.elementary.piecewise import Piecewise
+from sympy.functions.elementary.trigonometric import (
+    TrigonometricFunction, sin, cos, csc, sec)
+from sympy.polys.polytools import degree, lcm_list
+from sympy.sets.sets import (Interval, Intersection, FiniteSet, Union,
+                             Complement)
+from sympy.sets.fancysets import ImageSet
+from sympy.utilities import filldedent
+from sympy.utilities.iterables import iterable
+
+
+def continuous_domain(f, symbol, domain):
+    """
+    Returns the intervals in the given domain for which the function
+    is continuous.
+    This method is limited by the ability to determine the various
+    singularities and discontinuities of the given function.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    symbol : :py:class:`~.Symbol`
+        The variable for which the intervals are to be determined.
+    domain : :py:class:`~.Interval`
+        The domain over which the continuity of the symbol has to be checked.
+
+    Examples
+    ========
+
+    >>> from sympy import Interval, Symbol, S, tan, log, pi, sqrt
+    >>> from sympy.calculus.util import continuous_domain
+    >>> x = Symbol('x')
+    >>> continuous_domain(1/x, x, S.Reals)
+    Union(Interval.open(-oo, 0), Interval.open(0, oo))
+    >>> continuous_domain(tan(x), x, Interval(0, pi))
+    Union(Interval.Ropen(0, pi/2), Interval.Lopen(pi/2, pi))
+    >>> continuous_domain(sqrt(x - 2), x, Interval(-5, 5))
+    Interval(2, 5)
+    >>> continuous_domain(log(2*x - 1), x, S.Reals)
+    Interval.open(1/2, oo)
+
+    Returns
+    =======
+
+    :py:class:`~.Interval`
+        Union of all intervals where the function is continuous.
+
+    Raises
+    ======
+
+    NotImplementedError
+        If the method to determine continuity of such a function
+        has not yet been developed.
+
+    """
+    from sympy.solvers.inequalities import solve_univariate_inequality
+
+    if domain.is_subset(S.Reals):
+        constrained_interval = domain
+        for atom in f.atoms(Pow):
+            den = atom.exp.as_numer_denom()[1]
+            if den.is_even and den.is_nonzero:
+                constraint = solve_univariate_inequality(atom.base >= 0,
+                                                         symbol).as_set()
+                constrained_interval = Intersection(constraint,
+                                                    constrained_interval)
+
+        for atom in f.atoms(log):
+            constraint = solve_univariate_inequality(atom.args[0] > 0,
+                                                     symbol).as_set()
+            constrained_interval = Intersection(constraint,
+                                                constrained_interval)
+
+
+    return constrained_interval - singularities(f, symbol, domain)
+
+
+def function_range(f, symbol, domain):
+    """
+    Finds the range of a function in a given domain.
+    This method is limited by the ability to determine the singularities and
+    determine limits.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    symbol : :py:class:`~.Symbol`
+        The variable for which the range of function is to be determined.
+    domain : :py:class:`~.Interval`
+        The domain under which the range of the function has to be found.
+
+    Examples
+    ========
+
+    >>> from sympy import Interval, Symbol, S, exp, log, pi, sqrt, sin, tan
+    >>> from sympy.calculus.util import function_range
+    >>> x = Symbol('x')
+    >>> function_range(sin(x), x, Interval(0, 2*pi))
+    Interval(-1, 1)
+    >>> function_range(tan(x), x, Interval(-pi/2, pi/2))
+    Interval(-oo, oo)
+    >>> function_range(1/x, x, S.Reals)
+    Union(Interval.open(-oo, 0), Interval.open(0, oo))
+    >>> function_range(exp(x), x, S.Reals)
+    Interval.open(0, oo)
+    >>> function_range(log(x), x, S.Reals)
+    Interval(-oo, oo)
+    >>> function_range(sqrt(x), x, Interval(-5, 9))
+    Interval(0, 3)
+
+    Returns
+    =======
+
+    :py:class:`~.Interval`
+        Union of all ranges for all intervals under domain where function is
+        continuous.
+
+    Raises
+    ======
+
+    NotImplementedError
+        If any of the intervals, in the given domain, for which function
+        is continuous are not finite or real,
+        OR if the critical points of the function on the domain cannot be found.
+    """
+
+    if domain is S.EmptySet:
+        return S.EmptySet
+
+    period = periodicity(f, symbol)
+    if period == S.Zero:
+        # the expression is constant wrt symbol
+        return FiniteSet(f.expand())
+
+    from sympy.series.limits import limit
+    from sympy.solvers.solveset import solveset
+
+    if period is not None:
+        if isinstance(domain, Interval):
+            if (domain.inf - domain.sup).is_infinite:
+                domain = Interval(0, period)
+        elif isinstance(domain, Union):
+            for sub_dom in domain.args:
+                if isinstance(sub_dom, Interval) and \
+                ((sub_dom.inf - sub_dom.sup).is_infinite):
+                    domain = Interval(0, period)
+
+    intervals = continuous_domain(f, symbol, domain)
+    range_int = S.EmptySet
+    if isinstance(intervals,(Interval, FiniteSet)):
+        interval_iter = (intervals,)
+
+    elif isinstance(intervals, Union):
+        interval_iter = intervals.args
+
+    else:
+            raise NotImplementedError(filldedent('''
+                Unable to find range for the given domain.
+                '''))
+
+    for interval in interval_iter:
+        if isinstance(interval, FiniteSet):
+            for singleton in interval:
+                if singleton in domain:
+                    range_int += FiniteSet(f.subs(symbol, singleton))
+        elif isinstance(interval, Interval):
+            vals = S.EmptySet
+            critical_points = S.EmptySet
+            critical_values = S.EmptySet
+            bounds = ((interval.left_open, interval.inf, '+'),
+                   (interval.right_open, interval.sup, '-'))
+
+            for is_open, limit_point, direction in bounds:
+                if is_open:
+                    critical_values += FiniteSet(limit(f, symbol, limit_point, direction))
+                    vals += critical_values
+
+                else:
+                    vals += FiniteSet(f.subs(symbol, limit_point))
+
+            solution = solveset(f.diff(symbol), symbol, interval)
+
+            if not iterable(solution):
+                raise NotImplementedError(
+                        'Unable to find critical points for {}'.format(f))
+            if isinstance(solution, ImageSet):
+                raise NotImplementedError(
+                        'Infinite number of critical points for {}'.format(f))
+
+            critical_points += solution
+
+            for critical_point in critical_points:
+                vals += FiniteSet(f.subs(symbol, critical_point))
+
+            left_open, right_open = False, False
+
+            if critical_values is not S.EmptySet:
+                if critical_values.inf == vals.inf:
+                    left_open = True
+
+                if critical_values.sup == vals.sup:
+                    right_open = True
+
+            range_int += Interval(vals.inf, vals.sup, left_open, right_open)
+        else:
+            raise NotImplementedError(filldedent('''
+                Unable to find range for the given domain.
+                '''))
+
+    return range_int
+
+
+def not_empty_in(finset_intersection, *syms):
+    """
+    Finds the domain of the functions in ``finset_intersection`` in which the
+    ``finite_set`` is not-empty.
+
+    Parameters
+    ==========
+
+    finset_intersection : Intersection of FiniteSet
+        The unevaluated intersection of FiniteSet containing
+        real-valued functions with Union of Sets
+    syms : Tuple of symbols
+        Symbol for which domain is to be found
+
+    Raises
+    ======
+
+    NotImplementedError
+        The algorithms to find the non-emptiness of the given FiniteSet are
+        not yet implemented.
+    ValueError
+        The input is not valid.
+    RuntimeError
+        It is a bug, please report it to the github issue tracker
+        (https://github.com/sympy/sympy/issues).
+
+    Examples
+    ========
+
+    >>> from sympy import FiniteSet, Interval, not_empty_in, oo
+    >>> from sympy.abc import x
+    >>> not_empty_in(FiniteSet(x/2).intersect(Interval(0, 1)), x)
+    Interval(0, 2)
+    >>> not_empty_in(FiniteSet(x, x**2).intersect(Interval(1, 2)), x)
+    Union(Interval(1, 2), Interval(-sqrt(2), -1))
+    >>> not_empty_in(FiniteSet(x**2/(x + 2)).intersect(Interval(1, oo)), x)
+    Union(Interval.Lopen(-2, -1), Interval(2, oo))
+    """
+
+    # TODO: handle piecewise defined functions
+    # TODO: handle transcendental functions
+    # TODO: handle multivariate functions
+    if len(syms) == 0:
+        raise ValueError("One or more symbols must be given in syms.")
+
+    if finset_intersection is S.EmptySet:
+        return S.EmptySet
+
+    if isinstance(finset_intersection, Union):
+        elm_in_sets = finset_intersection.args[0]
+        return Union(not_empty_in(finset_intersection.args[1], *syms),
+                     elm_in_sets)
+
+    if isinstance(finset_intersection, FiniteSet):
+        finite_set = finset_intersection
+        _sets = S.Reals
+    else:
+        finite_set = finset_intersection.args[1]
+        _sets = finset_intersection.args[0]
+
+    if not isinstance(finite_set, FiniteSet):
+        raise ValueError('A FiniteSet must be given, not %s: %s' %
+                         (type(finite_set), finite_set))
+
+    if len(syms) == 1:
+        symb = syms[0]
+    else:
+        raise NotImplementedError('more than one variables %s not handled' %
+                                  (syms,))
+
+    def elm_domain(expr, intrvl):
+        """ Finds the domain of an expression in any given interval """
+        from sympy.solvers.solveset import solveset
+
+        _start = intrvl.start
+        _end = intrvl.end
+        _singularities = solveset(expr.as_numer_denom()[1], symb,
+                                  domain=S.Reals)
+
+        if intrvl.right_open:
+            if _end is S.Infinity:
+                _domain1 = S.Reals
+            else:
+                _domain1 = solveset(expr < _end, symb, domain=S.Reals)
+        else:
+            _domain1 = solveset(expr <= _end, symb, domain=S.Reals)
+
+        if intrvl.left_open:
+            if _start is S.NegativeInfinity:
+                _domain2 = S.Reals
+            else:
+                _domain2 = solveset(expr > _start, symb, domain=S.Reals)
+        else:
+            _domain2 = solveset(expr >= _start, symb, domain=S.Reals)
+
+        # domain in the interval
+        expr_with_sing = Intersection(_domain1, _domain2)
+        expr_domain = Complement(expr_with_sing, _singularities)
+        return expr_domain
+
+    if isinstance(_sets, Interval):
+        return Union(*[elm_domain(element, _sets) for element in finite_set])
+
+    if isinstance(_sets, Union):
+        _domain = S.EmptySet
+        for intrvl in _sets.args:
+            _domain_element = Union(*[elm_domain(element, intrvl)
+                                      for element in finite_set])
+            _domain = Union(_domain, _domain_element)
+        return _domain
+
+
+def periodicity(f, symbol, check=False):
+    """
+    Tests the given function for periodicity in the given symbol.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    symbol : :py:class:`~.Symbol`
+        The variable for which the period is to be determined.
+    check : bool, optional
+        The flag to verify whether the value being returned is a period or not.
+
+    Returns
+    =======
+
+    period
+        The period of the function is returned.
+        ``None`` is returned when the function is aperiodic or has a complex period.
+        The value of $0$ is returned as the period of a constant function.
+
+    Raises
+    ======
+
+    NotImplementedError
+        The value of the period computed cannot be verified.
+
+
+    Notes
+    =====
+
+    Currently, we do not support functions with a complex period.
+    The period of functions having complex periodic values such
+    as ``exp``, ``sinh`` is evaluated to ``None``.
+
+    The value returned might not be the "fundamental" period of the given
+    function i.e. it may not be the smallest periodic value of the function.
+
+    The verification of the period through the ``check`` flag is not reliable
+    due to internal simplification of the given expression. Hence, it is set
+    to ``False`` by default.
+
+    Examples
+    ========
+    >>> from sympy import periodicity, Symbol, sin, cos, tan, exp
+    >>> x = Symbol('x')
+    >>> f = sin(x) + sin(2*x) + sin(3*x)
+    >>> periodicity(f, x)
+    2*pi
+    >>> periodicity(sin(x)*cos(x), x)
+    pi
+    >>> periodicity(exp(tan(2*x) - 1), x)
+    pi/2
+    >>> periodicity(sin(4*x)**cos(2*x), x)
+    pi
+    >>> periodicity(exp(x), x)
+    """
+    if symbol.kind is not NumberKind:
+        raise NotImplementedError("Cannot use symbol of kind %s" % symbol.kind)
+    temp = Dummy('x', real=True)
+    f = f.subs(symbol, temp)
+    symbol = temp
+
+    def _check(orig_f, period):
+        '''Return the checked period or raise an error.'''
+        new_f = orig_f.subs(symbol, symbol + period)
+        if new_f.equals(orig_f):
+            return period
+        else:
+            raise NotImplementedError(filldedent('''
+                The period of the given function cannot be verified.
+                When `%s` was replaced with `%s + %s` in `%s`, the result
+                was `%s` which was not recognized as being the same as
+                the original function.
+                So either the period was wrong or the two forms were
+                not recognized as being equal.
+                Set check=False to obtain the value.''' %
+                (symbol, symbol, period, orig_f, new_f)))
+
+    orig_f = f
+    period = None
+
+    if isinstance(f, Relational):
+        f = f.lhs - f.rhs
+
+    f = f.simplify()
+
+    if symbol not in f.free_symbols:
+        return S.Zero
+
+    if isinstance(f, TrigonometricFunction):
+        try:
+            period = f.period(symbol)
+        except NotImplementedError:
+            pass
+
+    if isinstance(f, Abs):
+        arg = f.args[0]
+        if isinstance(arg, (sec, csc, cos)):
+            # all but tan and cot might have a
+            # a period that is half as large
+            # so recast as sin
+            arg = sin(arg.args[0])
+        period = periodicity(arg, symbol)
+        if period is not None and isinstance(arg, sin):
+            # the argument of Abs was a trigonometric other than
+            # cot or tan; test to see if the half-period
+            # is valid. Abs(arg) has behaviour equivalent to
+            # orig_f, so use that for test:
+            orig_f = Abs(arg)
+            try:
+                return _check(orig_f, period/2)
+            except NotImplementedError as err:
+                if check:
+                    raise NotImplementedError(err)
+            # else let new orig_f and period be
+            # checked below
+
+    if isinstance(f, exp) or (f.is_Pow and f.base == S.Exp1):
+        f = Pow(S.Exp1, expand_mul(f.exp))
+        if im(f) != 0:
+            period_real = periodicity(re(f), symbol)
+            period_imag = periodicity(im(f), symbol)
+            if period_real is not None and period_imag is not None:
+                period = lcim([period_real, period_imag])
+
+    if f.is_Pow and f.base != S.Exp1:
+        base, expo = f.args
+        base_has_sym = base.has(symbol)
+        expo_has_sym = expo.has(symbol)
+
+        if base_has_sym and not expo_has_sym:
+            period = periodicity(base, symbol)
+
+        elif expo_has_sym and not base_has_sym:
+            period = periodicity(expo, symbol)
+
+        else:
+            period = _periodicity(f.args, symbol)
+
+    elif f.is_Mul:
+        coeff, g = f.as_independent(symbol, as_Add=False)
+        if isinstance(g, TrigonometricFunction) or not equal_valued(coeff, 1):
+            period = periodicity(g, symbol)
+        else:
+            period = _periodicity(g.args, symbol)
+
+    elif f.is_Add:
+        k, g = f.as_independent(symbol)
+        if k is not S.Zero:
+            return periodicity(g, symbol)
+
+        period = _periodicity(g.args, symbol)
+
+    elif isinstance(f, Mod):
+        a, n = f.args
+
+        if a == symbol:
+            period = n
+        elif isinstance(a, TrigonometricFunction):
+            period = periodicity(a, symbol)
+        #check if 'f' is linear in 'symbol'
+        elif (a.is_polynomial(symbol) and degree(a, symbol) == 1 and
+            symbol not in n.free_symbols):
+                period = Abs(n / a.diff(symbol))
+
+    elif isinstance(f, Piecewise):
+        pass  # not handling Piecewise yet as the return type is not favorable
+
+    elif period is None:
+        from sympy.solvers.decompogen import compogen, decompogen
+        g_s = decompogen(f, symbol)
+        num_of_gs = len(g_s)
+        if num_of_gs > 1:
+            for index, g in enumerate(reversed(g_s)):
+                start_index = num_of_gs - 1 - index
+                g = compogen(g_s[start_index:], symbol)
+                if g not in (orig_f, f): # Fix for issue 12620
+                    period = periodicity(g, symbol)
+                    if period is not None:
+                        break
+
+    if period is not None:
+        if check:
+            return _check(orig_f, period)
+        return period
+
+    return None
+
+
+def _periodicity(args, symbol):
+    """
+    Helper for `periodicity` to find the period of a list of simpler
+    functions.
+    It uses the `lcim` method to find the least common period of
+    all the functions.
+
+    Parameters
+    ==========
+
+    args : Tuple of :py:class:`~.Symbol`
+        All the symbols present in a function.
+
+    symbol : :py:class:`~.Symbol`
+        The symbol over which the function is to be evaluated.
+
+    Returns
+    =======
+
+    period
+        The least common period of the function for all the symbols
+        of the function.
+        ``None`` if for at least one of the symbols the function is aperiodic.
+
+    """
+    periods = []
+    for f in args:
+        period = periodicity(f, symbol)
+        if period is None:
+            return None
+
+        if period is not S.Zero:
+            periods.append(period)
+
+    if len(periods) > 1:
+        return lcim(periods)
+
+    if periods:
+        return periods[0]
+
+
+def lcim(numbers):
+    """Returns the least common integral multiple of a list of numbers.
+
+    The numbers can be rational or irrational or a mixture of both.
+    `None` is returned for incommensurable numbers.
+
+    Parameters
+    ==========
+
+    numbers : list
+        Numbers (rational and/or irrational) for which lcim is to be found.
+
+    Returns
+    =======
+
+    number
+        lcim if it exists, otherwise ``None`` for incommensurable numbers.
+
+    Examples
+    ========
+
+    >>> from sympy.calculus.util import lcim
+    >>> from sympy import S, pi
+    >>> lcim([S(1)/2, S(3)/4, S(5)/6])
+    15/2
+    >>> lcim([2*pi, 3*pi, pi, pi/2])
+    6*pi
+    >>> lcim([S(1), 2*pi])
+    """
+    result = None
+    if all(num.is_irrational for num in numbers):
+        factorized_nums = [num.factor() for num in numbers]
+        factors_num = [num.as_coeff_Mul() for num in factorized_nums]
+        term = factors_num[0][1]
+        if all(factor == term for coeff, factor in factors_num):
+            common_term = term
+            coeffs = [coeff for coeff, factor in factors_num]
+            result = lcm_list(coeffs) * common_term
+
+    elif all(num.is_rational for num in numbers):
+        result = lcm_list(numbers)
+
+    else:
+        pass
+
+    return result
+
+def is_convex(f, *syms, domain=S.Reals):
+    r"""Determines the  convexity of the function passed in the argument.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    syms : Tuple of :py:class:`~.Symbol`
+        The variables with respect to which the convexity is to be determined.
+    domain : :py:class:`~.Interval`, optional
+        The domain over which the convexity of the function has to be checked.
+        If unspecified, S.Reals will be the default domain.
+
+    Returns
+    =======
+
+    bool
+        The method returns ``True`` if the function is convex otherwise it
+        returns ``False``.
+
+    Raises
+    ======
+
+    NotImplementedError
+        The check for the convexity of multivariate functions is not implemented yet.
+
+    Notes
+    =====
+
+    To determine concavity of a function pass `-f` as the concerned function.
+    To determine logarithmic convexity of a function pass `\log(f)` as
+    concerned function.
+    To determine logarithmic concavity of a function pass `-\log(f)` as
+    concerned function.
+
+    Currently, convexity check of multivariate functions is not handled.
+
+    Examples
+    ========
+
+    >>> from sympy import is_convex, symbols, exp, oo, Interval
+    >>> x = symbols('x')
+    >>> is_convex(exp(x), x)
+    True
+    >>> is_convex(x**3, x, domain = Interval(-1, oo))
+    False
+    >>> is_convex(1/x**2, x, domain=Interval.open(0, oo))
+    True
+
+    References
+    ==========
+
+    .. [1] https://en.wikipedia.org/wiki/Convex_function
+    .. [2] http://www.ifp.illinois.edu/~angelia/L3_convfunc.pdf
+    .. [3] https://en.wikipedia.org/wiki/Logarithmically_convex_function
+    .. [4] https://en.wikipedia.org/wiki/Logarithmically_concave_function
+    .. [5] https://en.wikipedia.org/wiki/Concave_function
+
+    """
+
+    if len(syms) > 1:
+        raise NotImplementedError(
+            "The check for the convexity of multivariate functions is not implemented yet.")
+
+    from sympy.solvers.inequalities import solve_univariate_inequality
+
+    f = _sympify(f)
+    var = syms[0]
+    if any(s in domain for s in singularities(f, var)):
+        return False
+
+    condition = f.diff(var, 2) < 0
+    if solve_univariate_inequality(condition, var, False, domain):
+        return False
+    return True
+
+
+def stationary_points(f, symbol, domain=S.Reals):
+    """
+    Returns the stationary points of a function (where derivative of the
+    function is 0) in the given domain.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    symbol : :py:class:`~.Symbol`
+        The variable for which the stationary points are to be determined.
+    domain : :py:class:`~.Interval`
+        The domain over which the stationary points have to be checked.
+        If unspecified, ``S.Reals`` will be the default domain.
+
+    Returns
+    =======
+
+    Set
+        A set of stationary points for the function. If there are no
+        stationary point, an :py:class:`~.EmptySet` is returned.
+
+    Examples
+    ========
+
+    >>> from sympy import Interval, Symbol, S, sin, pi, pprint, stationary_points
+    >>> x = Symbol('x')
+
+    >>> stationary_points(1/x, x, S.Reals)
+    EmptySet
+
+    >>> pprint(stationary_points(sin(x), x), use_unicode=False)
+              pi                              3*pi
+    {2*n*pi + -- | n in Integers} U {2*n*pi + ---- | n in Integers}
+              2                                2
+
+    >>> stationary_points(sin(x),x, Interval(0, 4*pi))
+    {pi/2, 3*pi/2, 5*pi/2, 7*pi/2}
+
+    """
+    from sympy.solvers.solveset import solveset
+
+    if domain is S.EmptySet:
+        return S.EmptySet
+
+    domain = continuous_domain(f, symbol, domain)
+    set = solveset(diff(f, symbol), symbol, domain)
+
+    return set
+
+
+def maximum(f, symbol, domain=S.Reals):
+    """
+    Returns the maximum value of a function in the given domain.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    symbol : :py:class:`~.Symbol`
+        The variable for maximum value needs to be determined.
+    domain : :py:class:`~.Interval`
+        The domain over which the maximum have to be checked.
+        If unspecified, then the global maximum is returned.
+
+    Returns
+    =======
+
+    number
+        Maximum value of the function in given domain.
+
+    Examples
+    ========
+
+    >>> from sympy import Interval, Symbol, S, sin, cos, pi, maximum
+    >>> x = Symbol('x')
+
+    >>> f = -x**2 + 2*x + 5
+    >>> maximum(f, x, S.Reals)
+    6
+
+    >>> maximum(sin(x), x, Interval(-pi, pi/4))
+    sqrt(2)/2
+
+    >>> maximum(sin(x)*cos(x), x)
+    1/2
+
+    """
+    if isinstance(symbol, Symbol):
+        if domain is S.EmptySet:
+            raise ValueError("Maximum value not defined for empty domain.")
+
+        return function_range(f, symbol, domain).sup
+    else:
+        raise ValueError("%s is not a valid symbol." % symbol)
+
+
+def minimum(f, symbol, domain=S.Reals):
+    """
+    Returns the minimum value of a function in the given domain.
+
+    Parameters
+    ==========
+
+    f : :py:class:`~.Expr`
+        The concerned function.
+    symbol : :py:class:`~.Symbol`
+        The variable for minimum value needs to be determined.
+    domain : :py:class:`~.Interval`
+        The domain over which the minimum have to be checked.
+        If unspecified, then the global minimum is returned.
+
+    Returns
+    =======
+
+    number
+        Minimum value of the function in the given domain.
+
+    Examples
+    ========
+
+    >>> from sympy import Interval, Symbol, S, sin, cos, minimum
+    >>> x = Symbol('x')
+
+    >>> f = x**2 + 2*x + 5
+    >>> minimum(f, x, S.Reals)
+    4
+
+    >>> minimum(sin(x), x, Interval(2, 3))
+    sin(3)
+
+    >>> minimum(sin(x)*cos(x), x)
+    -1/2
+
+    """
+    if isinstance(symbol, Symbol):
+        if domain is S.EmptySet:
+            raise ValueError("Minimum value not defined for empty domain.")
+
+        return function_range(f, symbol, domain).inf
+    else:
+        raise ValueError("%s is not a valid symbol." % symbol)

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

@@ -0,0 +1,18 @@
+r"""
+The :py:mod:`~sympy.holonomic` module is intended to deal with holonomic functions along
+with various operations on them like addition, multiplication, composition,
+integration and differentiation. The module also implements various kinds of
+conversions such as converting holonomic functions to a different form and the
+other way around.
+"""
+
+from .holonomic import (DifferentialOperator, HolonomicFunction, DifferentialOperators,
+    from_hyper, from_meijerg, expr_to_holonomic)
+from .recurrence import RecurrenceOperators, RecurrenceOperator, HolonomicSequence
+
+__all__ = [
+    'DifferentialOperator', 'HolonomicFunction', 'DifferentialOperators',
+    'from_hyper', 'from_meijerg', 'expr_to_holonomic',
+
+    'RecurrenceOperators', 'RecurrenceOperator', 'HolonomicSequence',
+]

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

@@ -0,0 +1,2899 @@
+"""
+This module implements Holonomic Functions and
+various operations on them.
+"""
+
+from sympy.core import Add, Mul, Pow
+from sympy.core.numbers import (NaN, Infinity, NegativeInfinity, Float, I, pi,
+        equal_valued)
+from sympy.core.singleton import S
+from sympy.core.sorting import ordered
+from sympy.core.symbol import Dummy, Symbol
+from sympy.core.sympify import sympify
+from sympy.functions.combinatorial.factorials import binomial, factorial, rf
+from sympy.functions.elementary.exponential import exp_polar, exp, log
+from sympy.functions.elementary.hyperbolic import (cosh, sinh)
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.elementary.trigonometric import (cos, sin, sinc)
+from sympy.functions.special.error_functions import (Ci, Shi, Si, erf, erfc, erfi)
+from sympy.functions.special.gamma_functions import gamma
+from sympy.functions.special.hyper import hyper, meijerg
+from sympy.integrals import meijerint
+from sympy.matrices import Matrix
+from sympy.polys.rings import PolyElement
+from sympy.polys.fields import FracElement
+from sympy.polys.domains import QQ, RR
+from sympy.polys.polyclasses import DMF
+from sympy.polys.polyroots import roots
+from sympy.polys.polytools import Poly
+from sympy.polys.matrices import DomainMatrix
+from sympy.printing import sstr
+from sympy.series.limits import limit
+from sympy.series.order import Order
+from sympy.simplify.hyperexpand import hyperexpand
+from sympy.simplify.simplify import nsimplify
+from sympy.solvers.solvers import solve
+
+from .recurrence import HolonomicSequence, RecurrenceOperator, RecurrenceOperators
+from .holonomicerrors import (NotPowerSeriesError, NotHyperSeriesError,
+    SingularityError, NotHolonomicError)
+
+
+def _find_nonzero_solution(r, homosys):
+    ones = lambda shape: DomainMatrix.ones(shape, r.domain)
+    particular, nullspace = r._solve(homosys)
+    nullity = nullspace.shape[0]
+    nullpart = ones((1, nullity)) * nullspace
+    sol = (particular + nullpart).transpose()
+    return sol
+
+
+
+def DifferentialOperators(base, generator):
+    r"""
+    This function is used to create annihilators using ``Dx``.
+
+    Explanation
+    ===========
+
+    Returns an Algebra of Differential Operators also called Weyl Algebra
+    and the operator for differentiation i.e. the ``Dx`` operator.
+
+    Parameters
+    ==========
+
+    base:
+        Base polynomial ring for the algebra.
+        The base polynomial ring is the ring of polynomials in :math:`x` that
+        will appear as coefficients in the operators.
+    generator:
+        Generator of the algebra which can
+        be either a noncommutative ``Symbol`` or a string. e.g. "Dx" or "D".
+
+    Examples
+    ========
+
+    >>> from sympy import ZZ
+    >>> from sympy.abc import x
+    >>> from sympy.holonomic.holonomic import DifferentialOperators
+    >>> R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    >>> R
+    Univariate Differential Operator Algebra in intermediate Dx over the base ring ZZ[x]
+    >>> Dx*x
+    (1) + (x)*Dx
+    """
+
+    ring = DifferentialOperatorAlgebra(base, generator)
+    return (ring, ring.derivative_operator)
+
+
+class DifferentialOperatorAlgebra:
+    r"""
+    An Ore Algebra is a set of noncommutative polynomials in the
+    intermediate ``Dx`` and coefficients in a base polynomial ring :math:`A`.
+    It follows the commutation rule:
+
+    .. math ::
+       Dxa = \sigma(a)Dx + \delta(a)
+
+    for :math:`a \subset A`.
+
+    Where :math:`\sigma: A \Rightarrow A` is an endomorphism and :math:`\delta: A \rightarrow A`
+    is a skew-derivation i.e. :math:`\delta(ab) = \delta(a) b + \sigma(a) \delta(b)`.
+
+    If one takes the sigma as identity map and delta as the standard derivation
+    then it becomes the algebra of Differential Operators also called
+    a Weyl Algebra i.e. an algebra whose elements are Differential Operators.
+
+    This class represents a Weyl Algebra and serves as the parent ring for
+    Differential Operators.
+
+    Examples
+    ========
+
+    >>> from sympy import ZZ
+    >>> from sympy import symbols
+    >>> from sympy.holonomic.holonomic import DifferentialOperators
+    >>> x = symbols('x')
+    >>> R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    >>> R
+    Univariate Differential Operator Algebra in intermediate Dx over the base ring
+    ZZ[x]
+
+    See Also
+    ========
+
+    DifferentialOperator
+    """
+
+    def __init__(self, base, generator):
+        # the base polynomial ring for the algebra
+        self.base = base
+        # the operator representing differentiation i.e. `Dx`
+        self.derivative_operator = DifferentialOperator(
+            [base.zero, base.one], self)
+
+        if generator is None:
+            self.gen_symbol = Symbol('Dx', commutative=False)
+        else:
+            if isinstance(generator, str):
+                self.gen_symbol = Symbol(generator, commutative=False)
+            elif isinstance(generator, Symbol):
+                self.gen_symbol = generator
+
+    def __str__(self):
+        string = 'Univariate Differential Operator Algebra in intermediate '\
+            + sstr(self.gen_symbol) + ' over the base ring ' + \
+            (self.base).__str__()
+
+        return string
+
+    __repr__ = __str__
+
+    def __eq__(self, other):
+        if self.base == other.base and self.gen_symbol == other.gen_symbol:
+            return True
+        else:
+            return False
+
+
+class DifferentialOperator:
+    """
+    Differential Operators are elements of Weyl Algebra. The Operators
+    are defined by a list of polynomials in the base ring and the
+    parent ring of the Operator i.e. the algebra it belongs to.
+
+    Explanation
+    ===========
+
+    Takes a list of polynomials for each power of ``Dx`` and the
+    parent ring which must be an instance of DifferentialOperatorAlgebra.
+
+    A Differential Operator can be created easily using
+    the operator ``Dx``. See examples below.
+
+    Examples
+    ========
+
+    >>> from sympy.holonomic.holonomic import DifferentialOperator, DifferentialOperators
+    >>> from sympy import ZZ
+    >>> from sympy import symbols
+    >>> x = symbols('x')
+    >>> R, Dx = DifferentialOperators(ZZ.old_poly_ring(x),'Dx')
+
+    >>> DifferentialOperator([0, 1, x**2], R)
+    (1)*Dx + (x**2)*Dx**2
+
+    >>> (x*Dx*x + 1 - Dx**2)**2
+    (2*x**2 + 2*x + 1) + (4*x**3 + 2*x**2 - 4)*Dx + (x**4 - 6*x - 2)*Dx**2 + (-2*x**2)*Dx**3 + (1)*Dx**4
+
+    See Also
+    ========
+
+    DifferentialOperatorAlgebra
+    """
+
+    _op_priority = 20
+
+    def __init__(self, list_of_poly, parent):
+        """
+        Parameters
+        ==========
+
+        list_of_poly:
+            List of polynomials belonging to the base ring of the algebra.
+        parent:
+            Parent algebra of the operator.
+        """
+
+        # the parent ring for this operator
+        # must be an DifferentialOperatorAlgebra object
+        self.parent = parent
+        base = self.parent.base
+        self.x = base.gens[0] if isinstance(base.gens[0], Symbol) else base.gens[0][0]
+        # sequence of polynomials in x for each power of Dx
+        # the list should not have trailing zeroes
+        # represents the operator
+        # convert the expressions into ring elements using from_sympy
+        for i, j in enumerate(list_of_poly):
+            if not isinstance(j, base.dtype):
+                list_of_poly[i] = base.from_sympy(sympify(j))
+            else:
+                list_of_poly[i] = base.from_sympy(base.to_sympy(j))
+
+        self.listofpoly = list_of_poly
+        # highest power of `Dx`
+        self.order = len(self.listofpoly) - 1
+
+    def __mul__(self, other):
+        """
+        Multiplies two DifferentialOperator and returns another
+        DifferentialOperator instance using the commutation rule
+        Dx*a = a*Dx + a'
+        """
+
+        listofself = self.listofpoly
+
+        if not isinstance(other, DifferentialOperator):
+            if not isinstance(other, self.parent.base.dtype):
+                listofother = [self.parent.base.from_sympy(sympify(other))]
+
+            else:
+                listofother = [other]
+        else:
+            listofother = other.listofpoly
+
+        # multiplies a polynomial `b` with a list of polynomials
+        def _mul_dmp_diffop(b, listofother):
+            if isinstance(listofother, list):
+                sol = []
+                for i in listofother:
+                    sol.append(i * b)
+                return sol
+            else:
+                return [b * listofother]
+
+        sol = _mul_dmp_diffop(listofself[0], listofother)
+
+        # compute Dx^i * b
+        def _mul_Dxi_b(b):
+            sol1 = [self.parent.base.zero]
+            sol2 = []
+
+            if isinstance(b, list):
+                for i in b:
+                    sol1.append(i)
+                    sol2.append(i.diff())
+            else:
+                sol1.append(self.parent.base.from_sympy(b))
+                sol2.append(self.parent.base.from_sympy(b).diff())
+
+            return _add_lists(sol1, sol2)
+
+        for i in range(1, len(listofself)):
+            # find Dx^i * b in ith iteration
+            listofother = _mul_Dxi_b(listofother)
+            # solution = solution + listofself[i] * (Dx^i * b)
+            sol = _add_lists(sol, _mul_dmp_diffop(listofself[i], listofother))
+
+        return DifferentialOperator(sol, self.parent)
+
+    def __rmul__(self, other):
+        if not isinstance(other, DifferentialOperator):
+
+            if not isinstance(other, self.parent.base.dtype):
+                other = (self.parent.base).from_sympy(sympify(other))
+
+            sol = []
+            for j in self.listofpoly:
+                sol.append(other * j)
+
+            return DifferentialOperator(sol, self.parent)
+
+    def __add__(self, other):
+        if isinstance(other, DifferentialOperator):
+
+            sol = _add_lists(self.listofpoly, other.listofpoly)
+            return DifferentialOperator(sol, self.parent)
+
+        else:
+            list_self = self.listofpoly
+            if not isinstance(other, self.parent.base.dtype):
+                list_other = [((self.parent).base).from_sympy(sympify(other))]
+            else:
+                list_other = [other]
+            sol = []
+            sol.append(list_self[0] + list_other[0])
+            sol += list_self[1:]
+
+            return DifferentialOperator(sol, self.parent)
+
+    __radd__ = __add__
+
+    def __sub__(self, other):
+        return self + (-1) * other
+
+    def __rsub__(self, other):
+        return (-1) * self + other
+
+    def __neg__(self):
+        return -1 * self
+
+    def __truediv__(self, other):
+        return self * (S.One / other)
+
+    def __pow__(self, n):
+        if n == 1:
+            return self
+        if n == 0:
+            return DifferentialOperator([self.parent.base.one], self.parent)
+
+        # if self is `Dx`
+        if self.listofpoly == self.parent.derivative_operator.listofpoly:
+            sol = [self.parent.base.zero]*n
+            sol.append(self.parent.base.one)
+            return DifferentialOperator(sol, self.parent)
+
+        # the general case
+        else:
+            if n % 2 == 1:
+                powreduce = self**(n - 1)
+                return powreduce * self
+            elif n % 2 == 0:
+                powreduce = self**(n / 2)
+                return powreduce * powreduce
+
+    def __str__(self):
+        listofpoly = self.listofpoly
+        print_str = ''
+
+        for i, j in enumerate(listofpoly):
+            if j == self.parent.base.zero:
+                continue
+
+            if i == 0:
+                print_str += '(' + sstr(j) + ')'
+                continue
+
+            if print_str:
+                print_str += ' + '
+
+            if i == 1:
+                print_str += '(' + sstr(j) + ')*%s' %(self.parent.gen_symbol)
+                continue
+
+            print_str += '(' + sstr(j) + ')' + '*%s**' %(self.parent.gen_symbol) + sstr(i)
+
+        return print_str
+
+    __repr__ = __str__
+
+    def __eq__(self, other):
+        if isinstance(other, DifferentialOperator):
+            if self.listofpoly == other.listofpoly and self.parent == other.parent:
+                return True
+            else:
+                return False
+        else:
+            if self.listofpoly[0] == other:
+                for i in self.listofpoly[1:]:
+                    if i is not self.parent.base.zero:
+                        return False
+                return True
+            else:
+                return False
+
+    def is_singular(self, x0):
+        """
+        Checks if the differential equation is singular at x0.
+        """
+
+        base = self.parent.base
+        return x0 in roots(base.to_sympy(self.listofpoly[-1]), self.x)
+
+
+class HolonomicFunction:
+    r"""
+    A Holonomic Function is a solution to a linear homogeneous ordinary
+    differential equation with polynomial coefficients. This differential
+    equation can also be represented by an annihilator i.e. a Differential
+    Operator ``L`` such that :math:`L.f = 0`. For uniqueness of these functions,
+    initial conditions can also be provided along with the annihilator.
+
+    Explanation
+    ===========
+
+    Holonomic functions have closure properties and thus forms a ring.
+    Given two Holonomic Functions f and g, their sum, product,
+    integral and derivative is also a Holonomic Function.
+
+    For ordinary points initial condition should be a vector of values of
+    the derivatives i.e. :math:`[y(x_0), y'(x_0), y''(x_0) ... ]`.
+
+    For regular singular points initial conditions can also be provided in this
+    format:
+    :math:`{s0: [C_0, C_1, ...], s1: [C^1_0, C^1_1, ...], ...}`
+    where s0, s1, ... are the roots of indicial equation and vectors
+    :math:`[C_0, C_1, ...], [C^0_0, C^0_1, ...], ...` are the corresponding initial
+    terms of the associated power series. See Examples below.
+
+    Examples
+    ========
+
+    >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+    >>> from sympy import QQ
+    >>> from sympy import symbols, S
+    >>> x = symbols('x')
+    >>> R, Dx = DifferentialOperators(QQ.old_poly_ring(x),'Dx')
+
+    >>> p = HolonomicFunction(Dx - 1, x, 0, [1])  # e^x
+    >>> q = HolonomicFunction(Dx**2 + 1, x, 0, [0, 1])  # sin(x)
+
+    >>> p + q  # annihilator of e^x + sin(x)
+    HolonomicFunction((-1) + (1)*Dx + (-1)*Dx**2 + (1)*Dx**3, x, 0, [1, 2, 1])
+
+    >>> p * q  # annihilator of e^x * sin(x)
+    HolonomicFunction((2) + (-2)*Dx + (1)*Dx**2, x, 0, [0, 1])
+
+    An example of initial conditions for regular singular points,
+    the indicial equation has only one root `1/2`.
+
+    >>> HolonomicFunction(-S(1)/2 + x*Dx, x, 0, {S(1)/2: [1]})
+    HolonomicFunction((-1/2) + (x)*Dx, x, 0, {1/2: [1]})
+
+    >>> HolonomicFunction(-S(1)/2 + x*Dx, x, 0, {S(1)/2: [1]}).to_expr()
+    sqrt(x)
+
+    To plot a Holonomic Function, one can use `.evalf()` for numerical
+    computation. Here's an example on `sin(x)**2/x` using numpy and matplotlib.
+
+    >>> import sympy.holonomic # doctest: +SKIP
+    >>> from sympy import var, sin # doctest: +SKIP
+    >>> import matplotlib.pyplot as plt # doctest: +SKIP
+    >>> import numpy as np # doctest: +SKIP
+    >>> var("x") # doctest: +SKIP
+    >>> r = np.linspace(1, 5, 100) # doctest: +SKIP
+    >>> y = sympy.holonomic.expr_to_holonomic(sin(x)**2/x, x0=1).evalf(r) # doctest: +SKIP
+    >>> plt.plot(r, y, label="holonomic function") # doctest: +SKIP
+    >>> plt.show() # doctest: +SKIP
+
+    """
+
+    _op_priority = 20
+
+    def __init__(self, annihilator, x, x0=0, y0=None):
+        """
+
+        Parameters
+        ==========
+
+        annihilator:
+            Annihilator of the Holonomic Function, represented by a
+            `DifferentialOperator` object.
+        x:
+            Variable of the function.
+        x0:
+            The point at which initial conditions are stored.
+            Generally an integer.
+        y0:
+            The initial condition. The proper format for the initial condition
+            is described in class docstring. To make the function unique,
+            length of the vector `y0` should be equal to or greater than the
+            order of differential equation.
+        """
+
+        # initial condition
+        self.y0 = y0
+        # the point for initial conditions, default is zero.
+        self.x0 = x0
+        # differential operator L such that L.f = 0
+        self.annihilator = annihilator
+        self.x = x
+
+    def __str__(self):
+        if self._have_init_cond():
+            str_sol = 'HolonomicFunction(%s, %s, %s, %s)' % (str(self.annihilator),\
+                sstr(self.x), sstr(self.x0), sstr(self.y0))
+        else:
+            str_sol = 'HolonomicFunction(%s, %s)' % (str(self.annihilator),\
+                sstr(self.x))
+
+        return str_sol
+
+    __repr__ = __str__
+
+    def unify(self, other):
+        """
+        Unifies the base polynomial ring of a given two Holonomic
+        Functions.
+        """
+
+        R1 = self.annihilator.parent.base
+        R2 = other.annihilator.parent.base
+
+        dom1 = R1.dom
+        dom2 = R2.dom
+
+        if R1 == R2:
+            return (self, other)
+
+        R = (dom1.unify(dom2)).old_poly_ring(self.x)
+
+        newparent, _ = DifferentialOperators(R, str(self.annihilator.parent.gen_symbol))
+
+        sol1 = [R1.to_sympy(i) for i in self.annihilator.listofpoly]
+        sol2 = [R2.to_sympy(i) for i in other.annihilator.listofpoly]
+
+        sol1 = DifferentialOperator(sol1, newparent)
+        sol2 = DifferentialOperator(sol2, newparent)
+
+        sol1 = HolonomicFunction(sol1, self.x, self.x0, self.y0)
+        sol2 = HolonomicFunction(sol2, other.x, other.x0, other.y0)
+
+        return (sol1, sol2)
+
+    def is_singularics(self):
+        """
+        Returns True if the function have singular initial condition
+        in the dictionary format.
+
+        Returns False if the function have ordinary initial condition
+        in the list format.
+
+        Returns None for all other cases.
+        """
+
+        if isinstance(self.y0, dict):
+            return True
+        elif isinstance(self.y0, list):
+            return False
+
+    def _have_init_cond(self):
+        """
+        Checks if the function have initial condition.
+        """
+        return bool(self.y0)
+
+    def _singularics_to_ord(self):
+        """
+        Converts a singular initial condition to ordinary if possible.
+        """
+        a = list(self.y0)[0]
+        b = self.y0[a]
+
+        if len(self.y0) == 1 and a == int(a) and a > 0:
+            y0 = []
+            a = int(a)
+            for i in range(a):
+                y0.append(S.Zero)
+            y0 += [j * factorial(a + i) for i, j in enumerate(b)]
+
+            return HolonomicFunction(self.annihilator, self.x, self.x0, y0)
+
+    def __add__(self, other):
+        # if the ground domains are different
+        if self.annihilator.parent.base != other.annihilator.parent.base:
+            a, b = self.unify(other)
+            return a + b
+
+        deg1 = self.annihilator.order
+        deg2 = other.annihilator.order
+        dim = max(deg1, deg2)
+        R = self.annihilator.parent.base
+        K = R.get_field()
+
+        rowsself = [self.annihilator]
+        rowsother = [other.annihilator]
+        gen = self.annihilator.parent.derivative_operator
+
+        # constructing annihilators up to order dim
+        for i in range(dim - deg1):
+            diff1 = (gen * rowsself[-1])
+            rowsself.append(diff1)
+
+        for i in range(dim - deg2):
+            diff2 = (gen * rowsother[-1])
+            rowsother.append(diff2)
+
+        row = rowsself + rowsother
+
+        # constructing the matrix of the ansatz
+        r = []
+
+        for expr in row:
+            p = []
+            for i in range(dim + 1):
+                if i >= len(expr.listofpoly):
+                    p.append(K.zero)
+                else:
+                    p.append(K.new(expr.listofpoly[i].rep))
+            r.append(p)
+
+        # solving the linear system using gauss jordan solver
+        r = DomainMatrix(r, (len(row), dim+1), K).transpose()
+        homosys = DomainMatrix.zeros((dim+1, 1), K)
+        sol = _find_nonzero_solution(r, homosys)
+
+        # if a solution is not obtained then increasing the order by 1 in each
+        # iteration
+        while sol.is_zero_matrix:
+            dim += 1
+
+            diff1 = (gen * rowsself[-1])
+            rowsself.append(diff1)
+
+            diff2 = (gen * rowsother[-1])
+            rowsother.append(diff2)
+
+            row = rowsself + rowsother
+            r = []
+
+            for expr in row:
+                p = []
+                for i in range(dim + 1):
+                    if i >= len(expr.listofpoly):
+                        p.append(K.zero)
+                    else:
+                        p.append(K.new(expr.listofpoly[i].rep))
+                r.append(p)
+
+            # solving the linear system using gauss jordan solver
+            r = DomainMatrix(r, (len(row), dim+1), K).transpose()
+            homosys = DomainMatrix.zeros((dim+1, 1), K)
+            sol = _find_nonzero_solution(r, homosys)
+
+        # taking only the coefficients needed to multiply with `self`
+        # can be also be done the other way by taking R.H.S and multiplying with
+        # `other`
+        sol = sol.flat()[:dim + 1 - deg1]
+        sol1 = _normalize(sol, self.annihilator.parent)
+        # annihilator of the solution
+        sol = sol1 * (self.annihilator)
+        sol = _normalize(sol.listofpoly, self.annihilator.parent, negative=False)
+
+        if not (self._have_init_cond() and other._have_init_cond()):
+            return HolonomicFunction(sol, self.x)
+
+        # both the functions have ordinary initial conditions
+        if self.is_singularics() == False and other.is_singularics() == False:
+
+            # directly add the corresponding value
+            if self.x0 == other.x0:
+                # try to extended the initial conditions
+                # using the annihilator
+                y1 = _extend_y0(self, sol.order)
+                y2 = _extend_y0(other, sol.order)
+                y0 = [a + b for a, b in zip(y1, y2)]
+                return HolonomicFunction(sol, self.x, self.x0, y0)
+
+            else:
+                # change the initial conditions to a same point
+                selfat0 = self.annihilator.is_singular(0)
+                otherat0 = other.annihilator.is_singular(0)
+
+                if self.x0 == 0 and not selfat0 and not otherat0:
+                    return self + other.change_ics(0)
+
+                elif other.x0 == 0 and not selfat0 and not otherat0:
+                    return self.change_ics(0) + other
+
+                else:
+                    selfatx0 = self.annihilator.is_singular(self.x0)
+                    otheratx0 = other.annihilator.is_singular(self.x0)
+
+                    if not selfatx0 and not otheratx0:
+                        return self + other.change_ics(self.x0)
+
+                    else:
+                        return self.change_ics(other.x0) + other
+
+        if self.x0 != other.x0:
+            return HolonomicFunction(sol, self.x)
+
+        # if the functions have singular_ics
+        y1 = None
+        y2 = None
+
+        if self.is_singularics() == False and other.is_singularics() == True:
+            # convert the ordinary initial condition to singular.
+            _y0 = [j / factorial(i) for i, j in enumerate(self.y0)]
+            y1 = {S.Zero: _y0}
+            y2 = other.y0
+        elif self.is_singularics() == True and other.is_singularics() == False:
+            _y0 = [j / factorial(i) for i, j in enumerate(other.y0)]
+            y1 = self.y0
+            y2 = {S.Zero: _y0}
+        elif self.is_singularics() == True and other.is_singularics() == True:
+            y1 = self.y0
+            y2 = other.y0
+
+        # computing singular initial condition for the result
+        # taking union of the series terms of both functions
+        y0 = {}
+        for i in y1:
+            # add corresponding initial terms if the power
+            # on `x` is same
+            if i in y2:
+                y0[i] = [a + b for a, b in zip(y1[i], y2[i])]
+            else:
+                y0[i] = y1[i]
+        for i in y2:
+            if i not in y1:
+                y0[i] = y2[i]
+        return HolonomicFunction(sol, self.x, self.x0, y0)
+
+    def integrate(self, limits, initcond=False):
+        """
+        Integrates the given holonomic function.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import QQ
+        >>> from sympy import symbols
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(QQ.old_poly_ring(x),'Dx')
+        >>> HolonomicFunction(Dx - 1, x, 0, [1]).integrate((x, 0, x))  # e^x - 1
+        HolonomicFunction((-1)*Dx + (1)*Dx**2, x, 0, [0, 1])
+        >>> HolonomicFunction(Dx**2 + 1, x, 0, [1, 0]).integrate((x, 0, x))
+        HolonomicFunction((1)*Dx + (1)*Dx**3, x, 0, [0, 1, 0])
+        """
+
+        # to get the annihilator, just multiply by Dx from right
+        D = self.annihilator.parent.derivative_operator
+
+        # if the function have initial conditions of the series format
+        if self.is_singularics() == True:
+
+            r = self._singularics_to_ord()
+            if r:
+                return r.integrate(limits, initcond=initcond)
+
+            # computing singular initial condition for the function
+            # produced after integration.
+            y0 = {}
+            for i in self.y0:
+                c = self.y0[i]
+                c2 = []
+                for j, cj in enumerate(c):
+                    if cj == 0:
+                        c2.append(S.Zero)
+
+                    # if power on `x` is -1, the integration becomes log(x)
+                    # TODO: Implement this case
+                    elif i + j + 1 == 0:
+                        raise NotImplementedError("logarithmic terms in the series are not supported")
+                    else:
+                        c2.append(cj / S(i + j + 1))
+                y0[i + 1] = c2
+
+            if hasattr(limits, "__iter__"):
+                raise NotImplementedError("Definite integration for singular initial conditions")
+
+            return HolonomicFunction(self.annihilator * D, self.x, self.x0, y0)
+
+        # if no initial conditions are available for the function
+        if not self._have_init_cond():
+            if initcond:
+                return HolonomicFunction(self.annihilator * D, self.x, self.x0, [S.Zero])
+            return HolonomicFunction(self.annihilator * D, self.x)
+
+        # definite integral
+        # initial conditions for the answer will be stored at point `a`,
+        # where `a` is the lower limit of the integrand
+        if hasattr(limits, "__iter__"):
+
+            if len(limits) == 3 and limits[0] == self.x:
+                x0 = self.x0
+                a = limits[1]
+                b = limits[2]
+                definite = True
+
+        else:
+            definite = False
+
+        y0 = [S.Zero]
+        y0 += self.y0
+
+        indefinite_integral = HolonomicFunction(self.annihilator * D, self.x, self.x0, y0)
+
+        if not definite:
+            return indefinite_integral
+
+        # use evalf to get the values at `a`
+        if x0 != a:
+            try:
+                indefinite_expr = indefinite_integral.to_expr()
+            except (NotHyperSeriesError, NotPowerSeriesError):
+                indefinite_expr = None
+
+            if indefinite_expr:
+                lower = indefinite_expr.subs(self.x, a)
+                if isinstance(lower, NaN):
+                    lower = indefinite_expr.limit(self.x, a)
+            else:
+                lower = indefinite_integral.evalf(a)
+
+            if b == self.x:
+                y0[0] = y0[0] - lower
+                return HolonomicFunction(self.annihilator * D, self.x, x0, y0)
+
+            elif S(b).is_Number:
+                if indefinite_expr:
+                    upper = indefinite_expr.subs(self.x, b)
+                    if isinstance(upper, NaN):
+                        upper = indefinite_expr.limit(self.x, b)
+                else:
+                    upper = indefinite_integral.evalf(b)
+
+                return upper - lower
+
+
+        # if the upper limit is `x`, the answer will be a function
+        if b == self.x:
+            return HolonomicFunction(self.annihilator * D, self.x, a, y0)
+
+        # if the upper limits is a Number, a numerical value will be returned
+        elif S(b).is_Number:
+            try:
+                s = HolonomicFunction(self.annihilator * D, self.x, a,\
+                    y0).to_expr()
+                indefinite = s.subs(self.x, b)
+                if not isinstance(indefinite, NaN):
+                    return indefinite
+                else:
+                    return s.limit(self.x, b)
+            except (NotHyperSeriesError, NotPowerSeriesError):
+                return HolonomicFunction(self.annihilator * D, self.x, a, y0).evalf(b)
+
+        return HolonomicFunction(self.annihilator * D, self.x)
+
+    def diff(self, *args, **kwargs):
+        r"""
+        Differentiation of the given Holonomic function.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import ZZ
+        >>> from sympy import symbols
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(ZZ.old_poly_ring(x),'Dx')
+        >>> HolonomicFunction(Dx**2 + 1, x, 0, [0, 1]).diff().to_expr()
+        cos(x)
+        >>> HolonomicFunction(Dx - 2, x, 0, [1]).diff().to_expr()
+        2*exp(2*x)
+
+        See Also
+        ========
+
+        integrate
+        """
+        kwargs.setdefault('evaluate', True)
+        if args:
+            if args[0] != self.x:
+                return S.Zero
+            elif len(args) == 2:
+                sol = self
+                for i in range(args[1]):
+                    sol = sol.diff(args[0])
+                return sol
+
+        ann = self.annihilator
+
+        # if the function is constant.
+        if ann.listofpoly[0] == ann.parent.base.zero and ann.order == 1:
+            return S.Zero
+
+        # if the coefficient of y in the differential equation is zero.
+        # a shifting is done to compute the answer in this case.
+        elif ann.listofpoly[0] == ann.parent.base.zero:
+
+            sol = DifferentialOperator(ann.listofpoly[1:], ann.parent)
+
+            if self._have_init_cond():
+                # if ordinary initial condition
+                if self.is_singularics() == False:
+                    return HolonomicFunction(sol, self.x, self.x0, self.y0[1:])
+                # TODO: support for singular initial condition
+                return HolonomicFunction(sol, self.x)
+            else:
+                return HolonomicFunction(sol, self.x)
+
+        # the general algorithm
+        R = ann.parent.base
+        K = R.get_field()
+
+        seq_dmf = [K.new(i.rep) for i in ann.listofpoly]
+
+        # -y = a1*y'/a0 + a2*y''/a0 ... + an*y^n/a0
+        rhs = [i / seq_dmf[0] for i in seq_dmf[1:]]
+        rhs.insert(0, K.zero)
+
+        # differentiate both lhs and rhs
+        sol = _derivate_diff_eq(rhs)
+
+        # add the term y' in lhs to rhs
+        sol = _add_lists(sol, [K.zero, K.one])
+
+        sol = _normalize(sol[1:], self.annihilator.parent, negative=False)
+
+        if not self._have_init_cond() or self.is_singularics() == True:
+            return HolonomicFunction(sol, self.x)
+
+        y0 = _extend_y0(self, sol.order + 1)[1:]
+        return HolonomicFunction(sol, self.x, self.x0, y0)
+
+    def __eq__(self, other):
+        if self.annihilator == other.annihilator:
+            if self.x == other.x:
+                if self._have_init_cond() and other._have_init_cond():
+                    if self.x0 == other.x0 and self.y0 == other.y0:
+                        return True
+                    else:
+                        return False
+                else:
+                    return True
+            else:
+                return False
+        else:
+            return False
+
+    def __mul__(self, other):
+        ann_self = self.annihilator
+
+        if not isinstance(other, HolonomicFunction):
+            other = sympify(other)
+
+            if other.has(self.x):
+                raise NotImplementedError(" Can't multiply a HolonomicFunction and expressions/functions.")
+
+            if not self._have_init_cond():
+                return self
+            else:
+                y0 = _extend_y0(self, ann_self.order)
+                y1 = []
+
+                for j in y0:
+                    y1.append((Poly.new(j, self.x) * other).rep)
+
+                return HolonomicFunction(ann_self, self.x, self.x0, y1)
+
+        if self.annihilator.parent.base != other.annihilator.parent.base:
+            a, b = self.unify(other)
+            return a * b
+
+        ann_other = other.annihilator
+
+        list_self = []
+        list_other = []
+
+        a = ann_self.order
+        b = ann_other.order
+
+        R = ann_self.parent.base
+        K = R.get_field()
+
+        for j in ann_self.listofpoly:
+            list_self.append(K.new(j.rep))
+
+        for j in ann_other.listofpoly:
+            list_other.append(K.new(j.rep))
+
+        # will be used to reduce the degree
+        self_red = [-list_self[i] / list_self[a] for i in range(a)]
+
+        other_red = [-list_other[i] / list_other[b] for i in range(b)]
+
+        # coeff_mull[i][j] is the coefficient of Dx^i(f).Dx^j(g)
+        coeff_mul = [[K.zero for i in range(b + 1)] for j in range(a + 1)]
+        coeff_mul[0][0] = K.one
+
+        # making the ansatz
+        lin_sys_elements = [[coeff_mul[i][j] for i in range(a) for j in range(b)]]
+        lin_sys = DomainMatrix(lin_sys_elements, (1, a*b), K).transpose()
+
+        homo_sys = DomainMatrix.zeros((a*b, 1), K)
+
+        sol = _find_nonzero_solution(lin_sys, homo_sys)
+
+        # until a non trivial solution is found
+        while sol.is_zero_matrix:
+
+            # updating the coefficients Dx^i(f).Dx^j(g) for next degree
+            for i in range(a - 1, -1, -1):
+                for j in range(b - 1, -1, -1):
+                    coeff_mul[i][j + 1] += coeff_mul[i][j]
+                    coeff_mul[i + 1][j] += coeff_mul[i][j]
+                    if isinstance(coeff_mul[i][j], K.dtype):
+                        coeff_mul[i][j] = DMFdiff(coeff_mul[i][j])
+                    else:
+                        coeff_mul[i][j] = coeff_mul[i][j].diff(self.x)
+
+            # reduce the terms to lower power using annihilators of f, g
+            for i in range(a + 1):
+                if not coeff_mul[i][b].is_zero:
+                    for j in range(b):
+                        coeff_mul[i][j] += other_red[j] * \
+                            coeff_mul[i][b]
+                    coeff_mul[i][b] = K.zero
+
+            # not d2 + 1, as that is already covered in previous loop
+            for j in range(b):
+                if not coeff_mul[a][j] == 0:
+                    for i in range(a):
+                        coeff_mul[i][j] += self_red[i] * \
+                            coeff_mul[a][j]
+                    coeff_mul[a][j] = K.zero
+
+            lin_sys_elements.append([coeff_mul[i][j] for i in range(a) for j in range(b)])
+            lin_sys = DomainMatrix(lin_sys_elements, (len(lin_sys_elements), a*b), K).transpose()
+
+            sol = _find_nonzero_solution(lin_sys, homo_sys)
+
+        sol_ann = _normalize(sol.flat(), self.annihilator.parent, negative=False)
+
+        if not (self._have_init_cond() and other._have_init_cond()):
+            return HolonomicFunction(sol_ann, self.x)
+
+        if self.is_singularics() == False and other.is_singularics() == False:
+
+            # if both the conditions are at same point
+            if self.x0 == other.x0:
+
+                # try to find more initial conditions
+                y0_self = _extend_y0(self, sol_ann.order)
+                y0_other = _extend_y0(other, sol_ann.order)
+                # h(x0) = f(x0) * g(x0)
+                y0 = [y0_self[0] * y0_other[0]]
+
+                # coefficient of Dx^j(f)*Dx^i(g) in Dx^i(fg)
+                for i in range(1, min(len(y0_self), len(y0_other))):
+                    coeff = [[0 for i in range(i + 1)] for j in range(i + 1)]
+                    for j in range(i + 1):
+                        for k in range(i + 1):
+                            if j + k == i:
+                                coeff[j][k] = binomial(i, j)
+
+                    sol = 0
+                    for j in range(i + 1):
+                        for k in range(i + 1):
+                            sol += coeff[j][k]* y0_self[j] * y0_other[k]
+
+                    y0.append(sol)
+
+                return HolonomicFunction(sol_ann, self.x, self.x0, y0)
+
+            # if the points are different, consider one
+            else:
+
+                selfat0 = self.annihilator.is_singular(0)
+                otherat0 = other.annihilator.is_singular(0)
+
+                if self.x0 == 0 and not selfat0 and not otherat0:
+                    return self * other.change_ics(0)
+
+                elif other.x0 == 0 and not selfat0 and not otherat0:
+                    return self.change_ics(0) * other
+
+                else:
+                    selfatx0 = self.annihilator.is_singular(self.x0)
+                    otheratx0 = other.annihilator.is_singular(self.x0)
+
+                    if not selfatx0 and not otheratx0:
+                        return self * other.change_ics(self.x0)
+
+                    else:
+                        return self.change_ics(other.x0) * other
+
+        if self.x0 != other.x0:
+            return HolonomicFunction(sol_ann, self.x)
+
+        # if the functions have singular_ics
+        y1 = None
+        y2 = None
+
+        if self.is_singularics() == False and other.is_singularics() == True:
+            _y0 = [j / factorial(i) for i, j in enumerate(self.y0)]
+            y1 = {S.Zero: _y0}
+            y2 = other.y0
+        elif self.is_singularics() == True and other.is_singularics() == False:
+            _y0 = [j / factorial(i) for i, j in enumerate(other.y0)]
+            y1 = self.y0
+            y2 = {S.Zero: _y0}
+        elif self.is_singularics() == True and other.is_singularics() == True:
+            y1 = self.y0
+            y2 = other.y0
+
+        y0 = {}
+        # multiply every possible pair of the series terms
+        for i in y1:
+            for j in y2:
+                k = min(len(y1[i]), len(y2[j]))
+                c = []
+                for a in range(k):
+                    s = S.Zero
+                    for b in range(a + 1):
+                        s += y1[i][b] * y2[j][a - b]
+                    c.append(s)
+                if not i + j in y0:
+                    y0[i + j] = c
+                else:
+                    y0[i + j] = [a + b for a, b in zip(c, y0[i + j])]
+        return HolonomicFunction(sol_ann, self.x, self.x0, y0)
+
+    __rmul__ = __mul__
+
+    def __sub__(self, other):
+        return self + other * -1
+
+    def __rsub__(self, other):
+        return self * -1 + other
+
+    def __neg__(self):
+        return -1 * self
+
+    def __truediv__(self, other):
+        return self * (S.One / other)
+
+    def __pow__(self, n):
+        if self.annihilator.order <= 1:
+            ann = self.annihilator
+            parent = ann.parent
+
+            if self.y0 is None:
+                y0 = None
+            else:
+                y0 = [list(self.y0)[0] ** n]
+
+            p0 = ann.listofpoly[0]
+            p1 = ann.listofpoly[1]
+
+            p0 = (Poly.new(p0, self.x) * n).rep
+
+            sol = [parent.base.to_sympy(i) for i in [p0, p1]]
+            dd = DifferentialOperator(sol, parent)
+            return HolonomicFunction(dd, self.x, self.x0, y0)
+        if n < 0:
+            raise NotHolonomicError("Negative Power on a Holonomic Function")
+        if n == 0:
+            Dx = self.annihilator.parent.derivative_operator
+            return HolonomicFunction(Dx, self.x, S.Zero, [S.One])
+        if n == 1:
+            return self
+        else:
+            if n % 2 == 1:
+                powreduce = self**(n - 1)
+                return powreduce * self
+            elif n % 2 == 0:
+                powreduce = self**(n / 2)
+                return powreduce * powreduce
+
+    def degree(self):
+        """
+        Returns the highest power of `x` in the annihilator.
+        """
+        sol = [i.degree() for i in self.annihilator.listofpoly]
+        return max(sol)
+
+    def composition(self, expr, *args, **kwargs):
+        """
+        Returns function after composition of a holonomic
+        function with an algebraic function. The method cannot compute
+        initial conditions for the result by itself, so they can be also be
+        provided.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import QQ
+        >>> from sympy import symbols
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(QQ.old_poly_ring(x),'Dx')
+        >>> HolonomicFunction(Dx - 1, x).composition(x**2, 0, [1])  # e^(x**2)
+        HolonomicFunction((-2*x) + (1)*Dx, x, 0, [1])
+        >>> HolonomicFunction(Dx**2 + 1, x).composition(x**2 - 1, 1, [1, 0])
+        HolonomicFunction((4*x**3) + (-1)*Dx + (x)*Dx**2, x, 1, [1, 0])
+
+        See Also
+        ========
+
+        from_hyper
+        """
+
+        R = self.annihilator.parent
+        a = self.annihilator.order
+        diff = expr.diff(self.x)
+        listofpoly = self.annihilator.listofpoly
+
+        for i, j in enumerate(listofpoly):
+            if isinstance(j, self.annihilator.parent.base.dtype):
+                listofpoly[i] = self.annihilator.parent.base.to_sympy(j)
+
+        r = listofpoly[a].subs({self.x:expr})
+        subs = [-listofpoly[i].subs({self.x:expr}) / r for i in range (a)]
+        coeffs = [S.Zero for i in range(a)]  # coeffs[i] == coeff of (D^i f)(a) in D^k (f(a))
+        coeffs[0] = S.One
+        system = [coeffs]
+        homogeneous = Matrix([[S.Zero for i in range(a)]]).transpose()
+        while True:
+            coeffs_next = [p.diff(self.x) for p in coeffs]
+            for i in range(a - 1):
+                coeffs_next[i + 1] += (coeffs[i] * diff)
+            for i in range(a):
+                coeffs_next[i] += (coeffs[-1] * subs[i] * diff)
+            coeffs = coeffs_next
+            # check for linear relations
+            system.append(coeffs)
+            sol, taus = (Matrix(system).transpose()
+                ).gauss_jordan_solve(homogeneous)
+            if sol.is_zero_matrix is not True:
+                break
+
+        tau = list(taus)[0]
+        sol = sol.subs(tau, 1)
+        sol = _normalize(sol[0:], R, negative=False)
+
+        # if initial conditions are given for the resulting function
+        if args:
+            return HolonomicFunction(sol, self.x, args[0], args[1])
+        return HolonomicFunction(sol, self.x)
+
+    def to_sequence(self, lb=True):
+        r"""
+        Finds recurrence relation for the coefficients in the series expansion
+        of the function about :math:`x_0`, where :math:`x_0` is the point at
+        which the initial condition is stored.
+
+        Explanation
+        ===========
+
+        If the point :math:`x_0` is ordinary, solution of the form :math:`[(R, n_0)]`
+        is returned. Where :math:`R` is the recurrence relation and :math:`n_0` is the
+        smallest ``n`` for which the recurrence holds true.
+
+        If the point :math:`x_0` is regular singular, a list of solutions in
+        the format :math:`(R, p, n_0)` is returned, i.e. `[(R, p, n_0), ... ]`.
+        Each tuple in this vector represents a recurrence relation :math:`R`
+        associated with a root of the indicial equation ``p``. Conditions of
+        a different format can also be provided in this case, see the
+        docstring of HolonomicFunction class.
+
+        If it's not possible to numerically compute a initial condition,
+        it is returned as a symbol :math:`C_j`, denoting the coefficient of
+        :math:`(x - x_0)^j` in the power series about :math:`x_0`.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import QQ
+        >>> from sympy import symbols, S
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(QQ.old_poly_ring(x),'Dx')
+        >>> HolonomicFunction(Dx - 1, x, 0, [1]).to_sequence()
+        [(HolonomicSequence((-1) + (n + 1)Sn, n), u(0) = 1, 0)]
+        >>> HolonomicFunction((1 + x)*Dx**2 + Dx, x, 0, [0, 1]).to_sequence()
+        [(HolonomicSequence((n**2) + (n**2 + n)Sn, n), u(0) = 0, u(1) = 1, u(2) = -1/2, 2)]
+        >>> HolonomicFunction(-S(1)/2 + x*Dx, x, 0, {S(1)/2: [1]}).to_sequence()
+        [(HolonomicSequence((n), n), u(0) = 1, 1/2, 1)]
+
+        See Also
+        ========
+
+        HolonomicFunction.series
+
+        References
+        ==========
+
+        .. [1] https://hal.inria.fr/inria-00070025/document
+        .. [2] https://www3.risc.jku.at/publications/download/risc_2244/DIPLFORM.pdf
+
+        """
+
+        if self.x0 != 0:
+            return self.shift_x(self.x0).to_sequence()
+
+        # check whether a power series exists if the point is singular
+        if self.annihilator.is_singular(self.x0):
+            return self._frobenius(lb=lb)
+
+        dict1 = {}
+        n = Symbol('n', integer=True)
+        dom = self.annihilator.parent.base.dom
+        R, _ = RecurrenceOperators(dom.old_poly_ring(n), 'Sn')
+
+        # substituting each term of the form `x^k Dx^j` in the
+        # annihilator, according to the formula below:
+        # x^k Dx^j = Sum(rf(n + 1 - k, j) * a(n + j - k) * x^n, (n, k, oo))
+        # for explanation see [2].
+        for i, j in enumerate(self.annihilator.listofpoly):
+
+            listofdmp = j.all_coeffs()
+            degree = len(listofdmp) - 1
+
+            for k in range(degree + 1):
+                coeff = listofdmp[degree - k]
+
+                if coeff == 0:
+                    continue
+
+                if (i - k, k) in dict1:
+                    dict1[(i - k, k)] += (dom.to_sympy(coeff) * rf(n - k + 1, i))
+                else:
+                    dict1[(i - k, k)] = (dom.to_sympy(coeff) * rf(n - k + 1, i))
+
+
+        sol = []
+        keylist = [i[0] for i in dict1]
+        lower = min(keylist)
+        upper = max(keylist)
+        degree = self.degree()
+
+        # the recurrence relation holds for all values of
+        # n greater than smallest_n, i.e. n >= smallest_n
+        smallest_n = lower + degree
+        dummys = {}
+        eqs = []
+        unknowns = []
+
+        # an appropriate shift of the recurrence
+        for j in range(lower, upper + 1):
+            if j in keylist:
+                temp = S.Zero
+                for k in dict1.keys():
+                    if k[0] == j:
+                        temp += dict1[k].subs(n, n - lower)
+                sol.append(temp)
+            else:
+                sol.append(S.Zero)
+
+        # the recurrence relation
+        sol = RecurrenceOperator(sol, R)
+
+        # computing the initial conditions for recurrence
+        order = sol.order
+        all_roots = roots(R.base.to_sympy(sol.listofpoly[-1]), n, filter='Z')
+        all_roots = all_roots.keys()
+
+        if all_roots:
+            max_root = max(all_roots) + 1
+            smallest_n = max(max_root, smallest_n)
+        order += smallest_n
+
+        y0 = _extend_y0(self, order)
+        u0 = []
+
+        # u(n) = y^n(0)/factorial(n)
+        for i, j in enumerate(y0):
+            u0.append(j / factorial(i))
+
+        # if sufficient conditions can't be computed then
+        # try to use the series method i.e.
+        # equate the coefficients of x^k in the equation formed by
+        # substituting the series in differential equation, to zero.
+        if len(u0) < order:
+
+            for i in range(degree):
+                eq = S.Zero
+
+                for j in dict1:
+
+                    if i + j[0] < 0:
+                        dummys[i + j[0]] = S.Zero
+
+                    elif i + j[0] < len(u0):
+                        dummys[i + j[0]] = u0[i + j[0]]
+
+                    elif not i + j[0] in dummys:
+                        dummys[i + j[0]] = Symbol('C_%s' %(i + j[0]))
+                        unknowns.append(dummys[i + j[0]])
+
+                    if j[1] <= i:
+                        eq += dict1[j].subs(n, i) * dummys[i + j[0]]
+
+                eqs.append(eq)
+
+            # solve the system of equations formed
+            soleqs = solve(eqs, *unknowns)
+
+            if isinstance(soleqs, dict):
+
+                for i in range(len(u0), order):
+
+                    if i not in dummys:
+                        dummys[i] = Symbol('C_%s' %i)
+
+                    if dummys[i] in soleqs:
+                        u0.append(soleqs[dummys[i]])
+
+                    else:
+                        u0.append(dummys[i])
+
+                if lb:
+                    return [(HolonomicSequence(sol, u0), smallest_n)]
+                return [HolonomicSequence(sol, u0)]
+
+            for i in range(len(u0), order):
+
+                if i not in dummys:
+                    dummys[i] = Symbol('C_%s' %i)
+
+                s = False
+                for j in soleqs:
+                    if dummys[i] in j:
+                        u0.append(j[dummys[i]])
+                        s = True
+                if not s:
+                    u0.append(dummys[i])
+
+        if lb:
+            return [(HolonomicSequence(sol, u0), smallest_n)]
+
+        return [HolonomicSequence(sol, u0)]
+
+    def _frobenius(self, lb=True):
+        # compute the roots of indicial equation
+        indicialroots = self._indicial()
+
+        reals = []
+        compl = []
+        for i in ordered(indicialroots.keys()):
+            if i.is_real:
+                reals.extend([i] * indicialroots[i])
+            else:
+                a, b = i.as_real_imag()
+                compl.extend([(i, a, b)] * indicialroots[i])
+
+        # sort the roots for a fixed ordering of solution
+        compl.sort(key=lambda x : x[1])
+        compl.sort(key=lambda x : x[2])
+        reals.sort()
+
+        # grouping the roots, roots differ by an integer are put in the same group.
+        grp = []
+
+        for i in reals:
+            intdiff = False
+            if len(grp) == 0:
+                grp.append([i])
+                continue
+            for j in grp:
+                if int(j[0] - i) == j[0] - i:
+                    j.append(i)
+                    intdiff = True
+                    break
+            if not intdiff:
+                grp.append([i])
+
+        # True if none of the roots differ by an integer i.e.
+        # each element in group have only one member
+        independent = True if all(len(i) == 1 for i in grp) else False
+
+        allpos = all(i >= 0 for i in reals)
+        allint = all(int(i) == i for i in reals)
+
+        # if initial conditions are provided
+        # then use them.
+        if self.is_singularics() == True:
+            rootstoconsider = []
+            for i in ordered(self.y0.keys()):
+                for j in ordered(indicialroots.keys()):
+                    if equal_valued(j, i):
+                        rootstoconsider.append(i)
+
+        elif allpos and allint:
+            rootstoconsider = [min(reals)]
+
+        elif independent:
+            rootstoconsider = [i[0] for i in grp] + [j[0] for j in compl]
+
+        elif not allint:
+            rootstoconsider = []
+            for i in reals:
+                if not int(i) == i:
+                    rootstoconsider.append(i)
+
+        elif not allpos:
+
+            if not self._have_init_cond() or S(self.y0[0]).is_finite ==  False:
+                rootstoconsider = [min(reals)]
+
+            else:
+                posroots = []
+                for i in reals:
+                    if i >= 0:
+                        posroots.append(i)
+                rootstoconsider = [min(posroots)]
+
+        n = Symbol('n', integer=True)
+        dom = self.annihilator.parent.base.dom
+        R, _ = RecurrenceOperators(dom.old_poly_ring(n), 'Sn')
+
+        finalsol = []
+        char = ord('C')
+
+        for p in rootstoconsider:
+            dict1 = {}
+
+            for i, j in enumerate(self.annihilator.listofpoly):
+
+                listofdmp = j.all_coeffs()
+                degree = len(listofdmp) - 1
+
+                for k in range(degree + 1):
+                    coeff = listofdmp[degree - k]
+
+                    if coeff == 0:
+                        continue
+
+                    if (i - k, k - i) in dict1:
+                        dict1[(i - k, k - i)] += (dom.to_sympy(coeff) * rf(n - k + 1 + p, i))
+                    else:
+                        dict1[(i - k, k - i)] = (dom.to_sympy(coeff) * rf(n - k + 1 + p, i))
+
+            sol = []
+            keylist = [i[0] for i in dict1]
+            lower = min(keylist)
+            upper = max(keylist)
+            degree = max([i[1] for i in dict1])
+            degree2 = min([i[1] for i in dict1])
+
+            smallest_n = lower + degree
+            dummys = {}
+            eqs = []
+            unknowns = []
+
+            for j in range(lower, upper + 1):
+                if j in keylist:
+                    temp = S.Zero
+                    for k in dict1.keys():
+                        if k[0] == j:
+                            temp += dict1[k].subs(n, n - lower)
+                    sol.append(temp)
+                else:
+                    sol.append(S.Zero)
+
+            # the recurrence relation
+            sol = RecurrenceOperator(sol, R)
+
+            # computing the initial conditions for recurrence
+            order = sol.order
+            all_roots = roots(R.base.to_sympy(sol.listofpoly[-1]), n, filter='Z')
+            all_roots = all_roots.keys()
+
+            if all_roots:
+                max_root = max(all_roots) + 1
+                smallest_n = max(max_root, smallest_n)
+            order += smallest_n
+
+            u0 = []
+
+            if self.is_singularics() == True:
+                u0 = self.y0[p]
+
+            elif self.is_singularics() == False and p >= 0 and int(p) == p and len(rootstoconsider) == 1:
+                y0 = _extend_y0(self, order + int(p))
+                # u(n) = y^n(0)/factorial(n)
+                if len(y0) > int(p):
+                    for i in range(int(p), len(y0)):
+                        u0.append(y0[i] / factorial(i))
+
+            if len(u0) < order:
+
+                for i in range(degree2, degree):
+                    eq = S.Zero
+
+                    for j in dict1:
+                        if i + j[0] < 0:
+                            dummys[i + j[0]] = S.Zero
+
+                        elif i + j[0] < len(u0):
+                            dummys[i + j[0]] = u0[i + j[0]]
+
+                        elif not i + j[0] in dummys:
+                            letter = chr(char) + '_%s' %(i + j[0])
+                            dummys[i + j[0]] = Symbol(letter)
+                            unknowns.append(dummys[i + j[0]])
+
+                        if j[1] <= i:
+                            eq += dict1[j].subs(n, i) * dummys[i + j[0]]
+
+                    eqs.append(eq)
+
+                # solve the system of equations formed
+                soleqs = solve(eqs, *unknowns)
+
+                if isinstance(soleqs, dict):
+
+                    for i in range(len(u0), order):
+
+                        if i not in dummys:
+                            letter = chr(char) + '_%s' %i
+                            dummys[i] = Symbol(letter)
+
+                        if dummys[i] in soleqs:
+                            u0.append(soleqs[dummys[i]])
+
+                        else:
+                            u0.append(dummys[i])
+
+                    if lb:
+                        finalsol.append((HolonomicSequence(sol, u0), p, smallest_n))
+                        continue
+                    else:
+                        finalsol.append((HolonomicSequence(sol, u0), p))
+                        continue
+
+                for i in range(len(u0), order):
+
+                    if i not in dummys:
+                        letter = chr(char) + '_%s' %i
+                        dummys[i] = Symbol(letter)
+
+                    s = False
+                    for j in soleqs:
+                        if dummys[i] in j:
+                            u0.append(j[dummys[i]])
+                            s = True
+                    if not s:
+                        u0.append(dummys[i])
+            if lb:
+                finalsol.append((HolonomicSequence(sol, u0), p, smallest_n))
+
+            else:
+                finalsol.append((HolonomicSequence(sol, u0), p))
+            char += 1
+        return finalsol
+
+    def series(self, n=6, coefficient=False, order=True, _recur=None):
+        r"""
+        Finds the power series expansion of given holonomic function about :math:`x_0`.
+
+        Explanation
+        ===========
+
+        A list of series might be returned if :math:`x_0` is a regular point with
+        multiple roots of the indicial equation.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import QQ
+        >>> from sympy import symbols
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(QQ.old_poly_ring(x),'Dx')
+        >>> HolonomicFunction(Dx - 1, x, 0, [1]).series()  # e^x
+        1 + x + x**2/2 + x**3/6 + x**4/24 + x**5/120 + O(x**6)
+        >>> HolonomicFunction(Dx**2 + 1, x, 0, [0, 1]).series(n=8)  # sin(x)
+        x - x**3/6 + x**5/120 - x**7/5040 + O(x**8)
+
+        See Also
+        ========
+
+        HolonomicFunction.to_sequence
+        """
+
+        if _recur is None:
+            recurrence = self.to_sequence()
+        else:
+            recurrence = _recur
+
+        if isinstance(recurrence, tuple) and len(recurrence) == 2:
+            recurrence = recurrence[0]
+            constantpower = 0
+        elif isinstance(recurrence, tuple) and len(recurrence) == 3:
+            constantpower = recurrence[1]
+            recurrence = recurrence[0]
+
+        elif len(recurrence) == 1 and len(recurrence[0]) == 2:
+            recurrence = recurrence[0][0]
+            constantpower = 0
+        elif len(recurrence) == 1 and len(recurrence[0]) == 3:
+            constantpower = recurrence[0][1]
+            recurrence = recurrence[0][0]
+        else:
+            sol = []
+            for i in recurrence:
+                sol.append(self.series(_recur=i))
+            return sol
+
+        n = n - int(constantpower)
+        l = len(recurrence.u0) - 1
+        k = recurrence.recurrence.order
+        x = self.x
+        x0 = self.x0
+        seq_dmp = recurrence.recurrence.listofpoly
+        R = recurrence.recurrence.parent.base
+        K = R.get_field()
+        seq = []
+
+        for i, j in enumerate(seq_dmp):
+            seq.append(K.new(j.rep))
+
+        sub = [-seq[i] / seq[k] for i in range(k)]
+        sol = list(recurrence.u0)
+
+        if l + 1 >= n:
+            pass
+        else:
+            # use the initial conditions to find the next term
+            for i in range(l + 1 - k, n - k):
+                coeff = S.Zero
+                for j in range(k):
+                    if i + j >= 0:
+                        coeff += DMFsubs(sub[j], i) * sol[i + j]
+                sol.append(coeff)
+
+        if coefficient:
+            return sol
+
+        ser = S.Zero
+        for i, j in enumerate(sol):
+            ser += x**(i + constantpower) * j
+        if order:
+            ser += Order(x**(n + int(constantpower)), x)
+        if x0 != 0:
+            return ser.subs(x, x - x0)
+        return ser
+
+    def _indicial(self):
+        """
+        Computes roots of the Indicial equation.
+        """
+
+        if self.x0 != 0:
+            return self.shift_x(self.x0)._indicial()
+
+        list_coeff = self.annihilator.listofpoly
+        R = self.annihilator.parent.base
+        x = self.x
+        s = R.zero
+        y = R.one
+
+        def _pole_degree(poly):
+            root_all = roots(R.to_sympy(poly), x, filter='Z')
+            if 0 in root_all.keys():
+                return root_all[0]
+            else:
+                return 0
+
+        degree = [j.degree() for j in list_coeff]
+        degree = max(degree)
+        inf = 10 * (max(1, degree) + max(1, self.annihilator.order))
+
+        deg = lambda q: inf if q.is_zero else _pole_degree(q)
+        b = deg(list_coeff[0])
+
+        for j in range(1, len(list_coeff)):
+            b = min(b, deg(list_coeff[j]) - j)
+
+        for i, j in enumerate(list_coeff):
+            listofdmp = j.all_coeffs()
+            degree = len(listofdmp) - 1
+            if - i - b <= 0 and degree - i - b >= 0:
+                s = s + listofdmp[degree - i - b] * y
+            y *= x - i
+
+        return roots(R.to_sympy(s), x)
+
+    def evalf(self, points, method='RK4', h=0.05, derivatives=False):
+        r"""
+        Finds numerical value of a holonomic function using numerical methods.
+        (RK4 by default). A set of points (real or complex) must be provided
+        which will be the path for the numerical integration.
+
+        Explanation
+        ===========
+
+        The path should be given as a list :math:`[x_1, x_2, \dots x_n]`. The numerical
+        values will be computed at each point in this order
+        :math:`x_1 \rightarrow x_2 \rightarrow x_3 \dots \rightarrow x_n`.
+
+        Returns values of the function at :math:`x_1, x_2, \dots x_n` in a list.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import QQ
+        >>> from sympy import symbols
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(QQ.old_poly_ring(x),'Dx')
+
+        A straight line on the real axis from (0 to 1)
+
+        >>> r = [0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1]
+
+        Runge-Kutta 4th order on e^x from 0.1 to 1.
+        Exact solution at 1 is 2.71828182845905
+
+        >>> HolonomicFunction(Dx - 1, x, 0, [1]).evalf(r)
+        [1.10517083333333, 1.22140257085069, 1.34985849706254, 1.49182424008069,
+        1.64872063859684, 1.82211796209193, 2.01375162659678, 2.22553956329232,
+        2.45960141378007, 2.71827974413517]
+
+        Euler's method for the same
+
+        >>> HolonomicFunction(Dx - 1, x, 0, [1]).evalf(r, method='Euler')
+        [1.1, 1.21, 1.331, 1.4641, 1.61051, 1.771561, 1.9487171, 2.14358881,
+        2.357947691, 2.5937424601]
+
+        One can also observe that the value obtained using Runge-Kutta 4th order
+        is much more accurate than Euler's method.
+        """
+
+        from sympy.holonomic.numerical import _evalf
+        lp = False
+
+        # if a point `b` is given instead of a mesh
+        if not hasattr(points, "__iter__"):
+            lp = True
+            b = S(points)
+            if self.x0 == b:
+                return _evalf(self, [b], method=method, derivatives=derivatives)[-1]
+
+            if not b.is_Number:
+                raise NotImplementedError
+
+            a = self.x0
+            if a > b:
+                h = -h
+            n = int((b - a) / h)
+            points = [a + h]
+            for i in range(n - 1):
+                points.append(points[-1] + h)
+
+        for i in roots(self.annihilator.parent.base.to_sympy(self.annihilator.listofpoly[-1]), self.x):
+            if i == self.x0 or i in points:
+                raise SingularityError(self, i)
+
+        if lp:
+            return _evalf(self, points, method=method, derivatives=derivatives)[-1]
+        return _evalf(self, points, method=method, derivatives=derivatives)
+
+    def change_x(self, z):
+        """
+        Changes only the variable of Holonomic Function, for internal
+        purposes. For composition use HolonomicFunction.composition()
+        """
+
+        dom = self.annihilator.parent.base.dom
+        R = dom.old_poly_ring(z)
+        parent, _ = DifferentialOperators(R, 'Dx')
+        sol = []
+        for j in self.annihilator.listofpoly:
+            sol.append(R(j.rep))
+        sol =  DifferentialOperator(sol, parent)
+        return HolonomicFunction(sol, z, self.x0, self.y0)
+
+    def shift_x(self, a):
+        """
+        Substitute `x + a` for `x`.
+        """
+
+        x = self.x
+        listaftershift = self.annihilator.listofpoly
+        base = self.annihilator.parent.base
+
+        sol = [base.from_sympy(base.to_sympy(i).subs(x, x + a)) for i in listaftershift]
+        sol = DifferentialOperator(sol, self.annihilator.parent)
+        x0 = self.x0 - a
+        if not self._have_init_cond():
+            return HolonomicFunction(sol, x)
+        return HolonomicFunction(sol, x, x0, self.y0)
+
+    def to_hyper(self, as_list=False, _recur=None):
+        r"""
+        Returns a hypergeometric function (or linear combination of them)
+        representing the given holonomic function.
+
+        Explanation
+        ===========
+
+        Returns an answer of the form:
+        `a_1 \cdot x^{b_1} \cdot{hyper()} + a_2 \cdot x^{b_2} \cdot{hyper()} \dots`
+
+        This is very useful as one can now use ``hyperexpand`` to find the
+        symbolic expressions/functions.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import ZZ
+        >>> from sympy import symbols
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(ZZ.old_poly_ring(x),'Dx')
+        >>> # sin(x)
+        >>> HolonomicFunction(Dx**2 + 1, x, 0, [0, 1]).to_hyper()
+        x*hyper((), (3/2,), -x**2/4)
+        >>> # exp(x)
+        >>> HolonomicFunction(Dx - 1, x, 0, [1]).to_hyper()
+        hyper((), (), x)
+
+        See Also
+        ========
+
+        from_hyper, from_meijerg
+        """
+
+        if _recur is None:
+            recurrence = self.to_sequence()
+        else:
+            recurrence = _recur
+
+        if isinstance(recurrence, tuple) and len(recurrence) == 2:
+            smallest_n = recurrence[1]
+            recurrence = recurrence[0]
+            constantpower = 0
+        elif isinstance(recurrence, tuple) and len(recurrence) == 3:
+            smallest_n = recurrence[2]
+            constantpower = recurrence[1]
+            recurrence = recurrence[0]
+        elif len(recurrence) == 1 and len(recurrence[0]) == 2:
+            smallest_n = recurrence[0][1]
+            recurrence = recurrence[0][0]
+            constantpower = 0
+        elif len(recurrence) == 1 and len(recurrence[0]) == 3:
+            smallest_n = recurrence[0][2]
+            constantpower = recurrence[0][1]
+            recurrence = recurrence[0][0]
+        else:
+            sol = self.to_hyper(as_list=as_list, _recur=recurrence[0])
+            for i in recurrence[1:]:
+                sol += self.to_hyper(as_list=as_list, _recur=i)
+            return sol
+
+        u0 = recurrence.u0
+        r = recurrence.recurrence
+        x = self.x
+        x0 = self.x0
+
+        # order of the recurrence relation
+        m = r.order
+
+        # when no recurrence exists, and the power series have finite terms
+        if m == 0:
+            nonzeroterms = roots(r.parent.base.to_sympy(r.listofpoly[0]), recurrence.n, filter='R')
+
+            sol = S.Zero
+            for j, i in enumerate(nonzeroterms):
+
+                if i < 0 or int(i) != i:
+                    continue
+
+                i = int(i)
+                if i < len(u0):
+                    if isinstance(u0[i], (PolyElement, FracElement)):
+                        u0[i] = u0[i].as_expr()
+                    sol += u0[i] * x**i
+
+                else:
+                    sol += Symbol('C_%s' %j) * x**i
+
+            if isinstance(sol, (PolyElement, FracElement)):
+                sol = sol.as_expr() * x**constantpower
+            else:
+                sol = sol * x**constantpower
+            if as_list:
+                if x0 != 0:
+                    return [(sol.subs(x, x - x0), )]
+                return [(sol, )]
+            if x0 != 0:
+                return sol.subs(x, x - x0)
+            return sol
+
+        if smallest_n + m > len(u0):
+            raise NotImplementedError("Can't compute sufficient Initial Conditions")
+
+        # check if the recurrence represents a hypergeometric series
+        is_hyper = True
+
+        for i in range(1, len(r.listofpoly)-1):
+            if r.listofpoly[i] != r.parent.base.zero:
+                is_hyper = False
+                break
+
+        if not is_hyper:
+            raise NotHyperSeriesError(self, self.x0)
+
+        a = r.listofpoly[0]
+        b = r.listofpoly[-1]
+
+        # the constant multiple of argument of hypergeometric function
+        if isinstance(a.rep[0], (PolyElement, FracElement)):
+            c = - (S(a.rep[0].as_expr()) * m**(a.degree())) / (S(b.rep[0].as_expr()) * m**(b.degree()))
+        else:
+            c = - (S(a.rep[0]) * m**(a.degree())) / (S(b.rep[0]) * m**(b.degree()))
+
+        sol = 0
+
+        arg1 = roots(r.parent.base.to_sympy(a), recurrence.n)
+        arg2 = roots(r.parent.base.to_sympy(b), recurrence.n)
+
+        # iterate through the initial conditions to find
+        # the hypergeometric representation of the given
+        # function.
+        # The answer will be a linear combination
+        # of different hypergeometric series which satisfies
+        # the recurrence.
+        if as_list:
+            listofsol = []
+        for i in range(smallest_n + m):
+
+            # if the recurrence relation doesn't hold for `n = i`,
+            # then a Hypergeometric representation doesn't exist.
+            # add the algebraic term a * x**i to the solution,
+            # where a is u0[i]
+            if i < smallest_n:
+                if as_list:
+                    listofsol.append(((S(u0[i]) * x**(i+constantpower)).subs(x, x-x0), ))
+                else:
+                    sol += S(u0[i]) * x**i
+                continue
+
+            # if the coefficient u0[i] is zero, then the
+            # independent hypergeomtric series starting with
+            # x**i is not a part of the answer.
+            if S(u0[i]) == 0:
+                continue
+
+            ap = []
+            bq = []
+
+            # substitute m * n + i for n
+            for k in ordered(arg1.keys()):
+                ap.extend([nsimplify((i - k) / m)] * arg1[k])
+
+            for k in ordered(arg2.keys()):
+                bq.extend([nsimplify((i - k) / m)] * arg2[k])
+
+            # convention of (k + 1) in the denominator
+            if 1 in bq:
+                bq.remove(1)
+            else:
+                ap.append(1)
+            if as_list:
+                listofsol.append(((S(u0[i])*x**(i+constantpower)).subs(x, x-x0), (hyper(ap, bq, c*x**m)).subs(x, x-x0)))
+            else:
+                sol += S(u0[i]) * hyper(ap, bq, c * x**m) * x**i
+        if as_list:
+            return listofsol
+        sol = sol * x**constantpower
+        if x0 != 0:
+            return sol.subs(x, x - x0)
+
+        return sol
+
+    def to_expr(self):
+        """
+        Converts a Holonomic Function back to elementary functions.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic.holonomic import HolonomicFunction, DifferentialOperators
+        >>> from sympy import ZZ
+        >>> from sympy import symbols, S
+        >>> x = symbols('x')
+        >>> R, Dx = DifferentialOperators(ZZ.old_poly_ring(x),'Dx')
+        >>> HolonomicFunction(x**2*Dx**2 + x*Dx + (x**2 - 1), x, 0, [0, S(1)/2]).to_expr()
+        besselj(1, x)
+        >>> HolonomicFunction((1 + x)*Dx**3 + Dx**2, x, 0, [1, 1, 1]).to_expr()
+        x*log(x + 1) + log(x + 1) + 1
+
+        """
+
+        return hyperexpand(self.to_hyper()).simplify()
+
+    def change_ics(self, b, lenics=None):
+        """
+        Changes the point `x0` to ``b`` for initial conditions.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic import expr_to_holonomic
+        >>> from sympy import symbols, sin, exp
+        >>> x = symbols('x')
+
+        >>> expr_to_holonomic(sin(x)).change_ics(1)
+        HolonomicFunction((1) + (1)*Dx**2, x, 1, [sin(1), cos(1)])
+
+        >>> expr_to_holonomic(exp(x)).change_ics(2)
+        HolonomicFunction((-1) + (1)*Dx, x, 2, [exp(2)])
+        """
+
+        symbolic = True
+
+        if lenics is None and len(self.y0) > self.annihilator.order:
+            lenics = len(self.y0)
+        dom = self.annihilator.parent.base.domain
+
+        try:
+            sol = expr_to_holonomic(self.to_expr(), x=self.x, x0=b, lenics=lenics, domain=dom)
+        except (NotPowerSeriesError, NotHyperSeriesError):
+            symbolic = False
+
+        if symbolic and sol.x0 == b:
+            return sol
+
+        y0 = self.evalf(b, derivatives=True)
+        return HolonomicFunction(self.annihilator, self.x, b, y0)
+
+    def to_meijerg(self):
+        """
+        Returns a linear combination of Meijer G-functions.
+
+        Examples
+        ========
+
+        >>> from sympy.holonomic import expr_to_holonomic
+        >>> from sympy import sin, cos, hyperexpand, log, symbols
+        >>> x = symbols('x')
+        >>> hyperexpand(expr_to_holonomic(cos(x) + sin(x)).to_meijerg())
+        sin(x) + cos(x)
+        >>> hyperexpand(expr_to_holonomic(log(x)).to_meijerg()).simplify()
+        log(x)
+
+        See Also
+        ========
+
+        to_hyper
+        """
+
+        # convert to hypergeometric first
+        rep = self.to_hyper(as_list=True)
+        sol = S.Zero
+
+        for i in rep:
+            if len(i) == 1:
+                sol += i[0]
+
+            elif len(i) == 2:
+                sol += i[0] * _hyper_to_meijerg(i[1])
+
+        return sol
+
+
+def from_hyper(func, x0=0, evalf=False):
+    r"""
+    Converts a hypergeometric function to holonomic.
+    ``func`` is the Hypergeometric Function and ``x0`` is the point at
+    which initial conditions are required.
+
+    Examples
+    ========
+
+    >>> from sympy.holonomic.holonomic import from_hyper
+    >>> from sympy import symbols, hyper, S
+    >>> x = symbols('x')
+    >>> from_hyper(hyper([], [S(3)/2], x**2/4))
+    HolonomicFunction((-x) + (2)*Dx + (x)*Dx**2, x, 1, [sinh(1), -sinh(1) + cosh(1)])
+    """
+
+    a = func.ap
+    b = func.bq
+    z = func.args[2]
+    x = z.atoms(Symbol).pop()
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+
+    # generalized hypergeometric differential equation
+    xDx = x*Dx
+    r1 = 1
+    for ai in a:  # XXX gives sympify error if Mul is used with list of all factors
+        r1 *= xDx + ai
+    xDx_1 = xDx - 1
+    # r2 = Mul(*([Dx] + [xDx_1 + bi for bi in b]))  # XXX gives sympify error
+    r2 = Dx
+    for bi in b:
+        r2 *= xDx_1 + bi
+    sol = r1 - r2
+
+    simp = hyperexpand(func)
+
+    if simp in (Infinity, NegativeInfinity):
+        return HolonomicFunction(sol, x).composition(z)
+
+    def _find_conditions(simp, x, x0, order, evalf=False):
+        y0 = []
+        for i in range(order):
+            if evalf:
+                val = simp.subs(x, x0).evalf()
+            else:
+                val = simp.subs(x, x0)
+            # return None if it is Infinite or NaN
+            if val.is_finite is False or isinstance(val, NaN):
+                return None
+            y0.append(val)
+            simp = simp.diff(x)
+        return y0
+
+    # if the function is known symbolically
+    if not isinstance(simp, hyper):
+        y0 = _find_conditions(simp, x, x0, sol.order)
+        while not y0:
+            # if values don't exist at 0, then try to find initial
+            # conditions at 1. If it doesn't exist at 1 too then
+            # try 2 and so on.
+            x0 += 1
+            y0 = _find_conditions(simp, x, x0, sol.order)
+
+        return HolonomicFunction(sol, x).composition(z, x0, y0)
+
+    if isinstance(simp, hyper):
+        x0 = 1
+        # use evalf if the function can't be simplified
+        y0 = _find_conditions(simp, x, x0, sol.order, evalf)
+        while not y0:
+            x0 += 1
+            y0 = _find_conditions(simp, x, x0, sol.order, evalf)
+        return HolonomicFunction(sol, x).composition(z, x0, y0)
+
+    return HolonomicFunction(sol, x).composition(z)
+
+
+def from_meijerg(func, x0=0, evalf=False, initcond=True, domain=QQ):
+    """
+    Converts a Meijer G-function to Holonomic.
+    ``func`` is the G-Function and ``x0`` is the point at
+    which initial conditions are required.
+
+    Examples
+    ========
+
+    >>> from sympy.holonomic.holonomic import from_meijerg
+    >>> from sympy import symbols, meijerg, S
+    >>> x = symbols('x')
+    >>> from_meijerg(meijerg(([], []), ([S(1)/2], [0]), x**2/4))
+    HolonomicFunction((1) + (1)*Dx**2, x, 0, [0, 1/sqrt(pi)])
+    """
+
+    a = func.ap
+    b = func.bq
+    n = len(func.an)
+    m = len(func.bm)
+    p = len(a)
+    z = func.args[2]
+    x = z.atoms(Symbol).pop()
+    R, Dx = DifferentialOperators(domain.old_poly_ring(x), 'Dx')
+
+    # compute the differential equation satisfied by the
+    # Meijer G-function.
+    xDx = x*Dx
+    xDx1 = xDx + 1
+    r1 = x*(-1)**(m + n - p)
+    for ai in a:  # XXX gives sympify error if args given in list
+        r1 *= xDx1 - ai
+    # r2 = Mul(*[xDx - bi for bi in b])  # gives sympify error
+    r2 = 1
+    for bi in b:
+        r2 *= xDx - bi
+    sol = r1 - r2
+
+    if not initcond:
+        return HolonomicFunction(sol, x).composition(z)
+
+    simp = hyperexpand(func)
+
+    if simp in (Infinity, NegativeInfinity):
+        return HolonomicFunction(sol, x).composition(z)
+
+    def _find_conditions(simp, x, x0, order, evalf=False):
+        y0 = []
+        for i in range(order):
+            if evalf:
+                val = simp.subs(x, x0).evalf()
+            else:
+                val = simp.subs(x, x0)
+            if val.is_finite is False or isinstance(val, NaN):
+                return None
+            y0.append(val)
+            simp = simp.diff(x)
+        return y0
+
+    # computing initial conditions
+    if not isinstance(simp, meijerg):
+        y0 = _find_conditions(simp, x, x0, sol.order)
+        while not y0:
+            x0 += 1
+            y0 = _find_conditions(simp, x, x0, sol.order)
+
+        return HolonomicFunction(sol, x).composition(z, x0, y0)
+
+    if isinstance(simp, meijerg):
+        x0 = 1
+        y0 = _find_conditions(simp, x, x0, sol.order, evalf)
+        while not y0:
+            x0 += 1
+            y0 = _find_conditions(simp, x, x0, sol.order, evalf)
+
+        return HolonomicFunction(sol, x).composition(z, x0, y0)
+
+    return HolonomicFunction(sol, x).composition(z)
+
+
+x_1 = Dummy('x_1')
+_lookup_table = None
+domain_for_table = None
+from sympy.integrals.meijerint import _mytype
+
+
+def expr_to_holonomic(func, x=None, x0=0, y0=None, lenics=None, domain=None, initcond=True):
+    """
+    Converts a function or an expression to a holonomic function.
+
+    Parameters
+    ==========
+
+    func:
+        The expression to be converted.
+    x:
+        variable for the function.
+    x0:
+        point at which initial condition must be computed.
+    y0:
+        One can optionally provide initial condition if the method
+        is not able to do it automatically.
+    lenics:
+        Number of terms in the initial condition. By default it is
+        equal to the order of the annihilator.
+    domain:
+        Ground domain for the polynomials in ``x`` appearing as coefficients
+        in the annihilator.
+    initcond:
+        Set it false if you do not want the initial conditions to be computed.
+
+    Examples
+    ========
+
+    >>> from sympy.holonomic.holonomic import expr_to_holonomic
+    >>> from sympy import sin, exp, symbols
+    >>> x = symbols('x')
+    >>> expr_to_holonomic(sin(x))
+    HolonomicFunction((1) + (1)*Dx**2, x, 0, [0, 1])
+    >>> expr_to_holonomic(exp(x))
+    HolonomicFunction((-1) + (1)*Dx, x, 0, [1])
+
+    See Also
+    ========
+
+    sympy.integrals.meijerint._rewrite1, _convert_poly_rat_alg, _create_table
+    """
+    func = sympify(func)
+    syms = func.free_symbols
+
+    if not x:
+        if len(syms) == 1:
+            x= syms.pop()
+        else:
+            raise ValueError("Specify the variable for the function")
+    elif x in syms:
+        syms.remove(x)
+
+    extra_syms = list(syms)
+
+    if domain is None:
+        if func.has(Float):
+            domain = RR
+        else:
+            domain = QQ
+        if len(extra_syms) != 0:
+            domain = domain[extra_syms].get_field()
+
+    # try to convert if the function is polynomial or rational
+    solpoly = _convert_poly_rat_alg(func, x, x0=x0, y0=y0, lenics=lenics, domain=domain, initcond=initcond)
+    if solpoly:
+        return solpoly
+
+    # create the lookup table
+    global _lookup_table, domain_for_table
+    if not _lookup_table:
+        domain_for_table = domain
+        _lookup_table = {}
+        _create_table(_lookup_table, domain=domain)
+    elif domain != domain_for_table:
+        domain_for_table = domain
+        _lookup_table = {}
+        _create_table(_lookup_table, domain=domain)
+
+    # use the table directly to convert to Holonomic
+    if func.is_Function:
+        f = func.subs(x, x_1)
+        t = _mytype(f, x_1)
+        if t in _lookup_table:
+            l = _lookup_table[t]
+            sol = l[0][1].change_x(x)
+        else:
+            sol = _convert_meijerint(func, x, initcond=False, domain=domain)
+            if not sol:
+                raise NotImplementedError
+            if y0:
+                sol.y0 = y0
+            if y0 or not initcond:
+                sol.x0 = x0
+                return sol
+            if not lenics:
+                lenics = sol.annihilator.order
+            _y0 = _find_conditions(func, x, x0, lenics)
+            while not _y0:
+                x0 += 1
+                _y0 = _find_conditions(func, x, x0, lenics)
+            return HolonomicFunction(sol.annihilator, x, x0, _y0)
+
+        if y0 or not initcond:
+            sol = sol.composition(func.args[0])
+            if y0:
+                sol.y0 = y0
+            sol.x0 = x0
+            return sol
+        if not lenics:
+            lenics = sol.annihilator.order
+
+        _y0 = _find_conditions(func, x, x0, lenics)
+        while not _y0:
+            x0 += 1
+            _y0 = _find_conditions(func, x, x0, lenics)
+        return sol.composition(func.args[0], x0, _y0)
+
+    # iterate through the expression recursively
+    args = func.args
+    f = func.func
+    sol = expr_to_holonomic(args[0], x=x, initcond=False, domain=domain)
+
+    if f is Add:
+        for i in range(1, len(args)):
+            sol += expr_to_holonomic(args[i], x=x, initcond=False, domain=domain)
+
+    elif f is Mul:
+        for i in range(1, len(args)):
+            sol *= expr_to_holonomic(args[i], x=x, initcond=False, domain=domain)
+
+    elif f is Pow:
+        sol = sol**args[1]
+    sol.x0 = x0
+    if not sol:
+        raise NotImplementedError
+    if y0:
+        sol.y0 = y0
+    if y0 or not initcond:
+        return sol
+    if sol.y0:
+        return sol
+    if not lenics:
+        lenics = sol.annihilator.order
+    if sol.annihilator.is_singular(x0):
+        r = sol._indicial()
+        l = list(r)
+        if len(r) == 1 and r[l[0]] == S.One:
+            r = l[0]
+            g = func / (x - x0)**r
+            singular_ics = _find_conditions(g, x, x0, lenics)
+            singular_ics = [j / factorial(i) for i, j in enumerate(singular_ics)]
+            y0 = {r:singular_ics}
+            return HolonomicFunction(sol.annihilator, x, x0, y0)
+
+    _y0 = _find_conditions(func, x, x0, lenics)
+    while not _y0:
+        x0 += 1
+        _y0 = _find_conditions(func, x, x0, lenics)
+
+    return HolonomicFunction(sol.annihilator, x, x0, _y0)
+
+
+## Some helper functions ##
+
+def _normalize(list_of, parent, negative=True):
+    """
+    Normalize a given annihilator
+    """
+
+    num = []
+    denom = []
+    base = parent.base
+    K = base.get_field()
+    lcm_denom = base.from_sympy(S.One)
+    list_of_coeff = []
+
+    # convert polynomials to the elements of associated
+    # fraction field
+    for i, j in enumerate(list_of):
+        if isinstance(j, base.dtype):
+            list_of_coeff.append(K.new(j.rep))
+        elif not isinstance(j, K.dtype):
+            list_of_coeff.append(K.from_sympy(sympify(j)))
+        else:
+            list_of_coeff.append(j)
+
+        # corresponding numerators of the sequence of polynomials
+        num.append(list_of_coeff[i].numer())
+
+        # corresponding denominators
+        denom.append(list_of_coeff[i].denom())
+
+    # lcm of denominators in the coefficients
+    for i in denom:
+        lcm_denom = i.lcm(lcm_denom)
+
+    if negative:
+        lcm_denom = -lcm_denom
+
+    lcm_denom = K.new(lcm_denom.rep)
+
+    # multiply the coefficients with lcm
+    for i, j in enumerate(list_of_coeff):
+        list_of_coeff[i] = j * lcm_denom
+
+    gcd_numer = base((list_of_coeff[-1].numer() / list_of_coeff[-1].denom()).rep)
+
+    # gcd of numerators in the coefficients
+    for i in num:
+        gcd_numer = i.gcd(gcd_numer)
+
+    gcd_numer = K.new(gcd_numer.rep)
+
+    # divide all the coefficients by the gcd
+    for i, j in enumerate(list_of_coeff):
+        frac_ans = j / gcd_numer
+        list_of_coeff[i] = base((frac_ans.numer() / frac_ans.denom()).rep)
+
+    return DifferentialOperator(list_of_coeff, parent)
+
+
+def _derivate_diff_eq(listofpoly):
+    """
+    Let a differential equation a0(x)y(x) + a1(x)y'(x) + ... = 0
+    where a0, a1,... are polynomials or rational functions. The function
+    returns b0, b1, b2... such that the differential equation
+    b0(x)y(x) + b1(x)y'(x) +... = 0 is formed after differentiating the
+    former equation.
+    """
+
+    sol = []
+    a = len(listofpoly) - 1
+    sol.append(DMFdiff(listofpoly[0]))
+
+    for i, j in enumerate(listofpoly[1:]):
+        sol.append(DMFdiff(j) + listofpoly[i])
+
+    sol.append(listofpoly[a])
+    return sol
+
+
+def _hyper_to_meijerg(func):
+    """
+    Converts a `hyper` to meijerg.
+    """
+    ap = func.ap
+    bq = func.bq
+
+    ispoly = any(i <= 0 and int(i) == i for i in ap)
+    if ispoly:
+        return hyperexpand(func)
+
+    z = func.args[2]
+
+    # parameters of the `meijerg` function.
+    an = (1 - i for i in ap)
+    anp = ()
+    bm = (S.Zero, )
+    bmq = (1 - i for i in bq)
+
+    k = S.One
+
+    for i in bq:
+        k = k * gamma(i)
+
+    for i in ap:
+        k = k / gamma(i)
+
+    return k * meijerg(an, anp, bm, bmq, -z)
+
+
+def _add_lists(list1, list2):
+    """Takes polynomial sequences of two annihilators a and b and returns
+    the list of polynomials of sum of a and b.
+    """
+    if len(list1) <= len(list2):
+        sol = [a + b for a, b in zip(list1, list2)] + list2[len(list1):]
+    else:
+        sol = [a + b for a, b in zip(list1, list2)] + list1[len(list2):]
+    return sol
+
+
+def _extend_y0(Holonomic, n):
+    """
+    Tries to find more initial conditions by substituting the initial
+    value point in the differential equation.
+    """
+
+    if Holonomic.annihilator.is_singular(Holonomic.x0) or Holonomic.is_singularics() == True:
+        return Holonomic.y0
+
+    annihilator = Holonomic.annihilator
+    a = annihilator.order
+
+    listofpoly = []
+
+    y0 = Holonomic.y0
+    R = annihilator.parent.base
+    K = R.get_field()
+
+    for i, j in enumerate(annihilator.listofpoly):
+            if isinstance(j, annihilator.parent.base.dtype):
+                listofpoly.append(K.new(j.rep))
+
+    if len(y0) < a or n <= len(y0):
+        return y0
+    else:
+        list_red = [-listofpoly[i] / listofpoly[a]
+                    for i in range(a)]
+        if len(y0) > a:
+            y1 = [y0[i] for i in range(a)]
+        else:
+            y1 = list(y0)
+        for i in range(n - a):
+            sol = 0
+            for a, b in zip(y1, list_red):
+                r = DMFsubs(b, Holonomic.x0)
+                if not getattr(r, 'is_finite', True):
+                    return y0
+                if isinstance(r, (PolyElement, FracElement)):
+                    r = r.as_expr()
+                sol += a * r
+            y1.append(sol)
+            list_red = _derivate_diff_eq(list_red)
+
+        return y0 + y1[len(y0):]
+
+
+def DMFdiff(frac):
+    # differentiate a DMF object represented as p/q
+    if not isinstance(frac, DMF):
+        return frac.diff()
+
+    K = frac.ring
+    p = K.numer(frac)
+    q = K.denom(frac)
+    sol_num = - p * q.diff() + q * p.diff()
+    sol_denom = q**2
+    return K((sol_num.rep, sol_denom.rep))
+
+
+def DMFsubs(frac, x0, mpm=False):
+    # substitute the point x0 in DMF object of the form p/q
+    if not isinstance(frac, DMF):
+        return frac
+
+    p = frac.num
+    q = frac.den
+    sol_p = S.Zero
+    sol_q = S.Zero
+
+    if mpm:
+        from mpmath import mp
+
+    for i, j in enumerate(reversed(p)):
+        if mpm:
+            j = sympify(j)._to_mpmath(mp.prec)
+        sol_p += j * x0**i
+
+    for i, j in enumerate(reversed(q)):
+        if mpm:
+            j = sympify(j)._to_mpmath(mp.prec)
+        sol_q += j * x0**i
+
+    if isinstance(sol_p, (PolyElement, FracElement)):
+        sol_p = sol_p.as_expr()
+    if isinstance(sol_q, (PolyElement, FracElement)):
+        sol_q = sol_q.as_expr()
+
+    return sol_p / sol_q
+
+
+def _convert_poly_rat_alg(func, x, x0=0, y0=None, lenics=None, domain=QQ, initcond=True):
+    """
+    Converts polynomials, rationals and algebraic functions to holonomic.
+    """
+
+    ispoly = func.is_polynomial()
+    if not ispoly:
+        israt = func.is_rational_function()
+    else:
+        israt = True
+
+    if not (ispoly or israt):
+        basepoly, ratexp = func.as_base_exp()
+        if basepoly.is_polynomial() and ratexp.is_Number:
+            if isinstance(ratexp, Float):
+                ratexp = nsimplify(ratexp)
+            m, n = ratexp.p, ratexp.q
+            is_alg = True
+        else:
+            is_alg = False
+    else:
+        is_alg = True
+
+    if not (ispoly or israt or is_alg):
+        return None
+
+    R = domain.old_poly_ring(x)
+    _, Dx = DifferentialOperators(R, 'Dx')
+
+    # if the function is constant
+    if not func.has(x):
+        return HolonomicFunction(Dx, x, 0, [func])
+
+    if ispoly:
+        # differential equation satisfied by polynomial
+        sol = func * Dx - func.diff(x)
+        sol = _normalize(sol.listofpoly, sol.parent, negative=False)
+        is_singular = sol.is_singular(x0)
+
+        # try to compute the conditions for singular points
+        if y0 is None and x0 == 0 and is_singular:
+            rep = R.from_sympy(func).rep
+            for i, j in enumerate(reversed(rep)):
+                if j == 0:
+                    continue
+                else:
+                    coeff = list(reversed(rep))[i:]
+                    indicial = i
+                    break
+            for i, j in enumerate(coeff):
+                if isinstance(j, (PolyElement, FracElement)):
+                    coeff[i] = j.as_expr()
+            y0 = {indicial: S(coeff)}
+
+    elif israt:
+        p, q = func.as_numer_denom()
+        # differential equation satisfied by rational
+        sol = p * q * Dx + p * q.diff(x) - q * p.diff(x)
+        sol = _normalize(sol.listofpoly, sol.parent, negative=False)
+
+    elif is_alg:
+        sol = n * (x / m) * Dx - 1
+        sol = HolonomicFunction(sol, x).composition(basepoly).annihilator
+        is_singular = sol.is_singular(x0)
+
+        # try to compute the conditions for singular points
+        if y0 is None and x0 == 0 and is_singular and \
+            (lenics is None or lenics <= 1):
+            rep = R.from_sympy(basepoly).rep
+            for i, j in enumerate(reversed(rep)):
+                if j == 0:
+                    continue
+                if isinstance(j, (PolyElement, FracElement)):
+                    j = j.as_expr()
+
+                coeff = S(j)**ratexp
+                indicial = S(i) * ratexp
+                break
+            if isinstance(coeff, (PolyElement, FracElement)):
+                coeff = coeff.as_expr()
+            y0 = {indicial: S([coeff])}
+
+    if y0 or not initcond:
+        return HolonomicFunction(sol, x, x0, y0)
+
+    if not lenics:
+        lenics = sol.order
+
+    if sol.is_singular(x0):
+        r = HolonomicFunction(sol, x, x0)._indicial()
+        l = list(r)
+        if len(r) == 1 and r[l[0]] == S.One:
+            r = l[0]
+            g = func / (x - x0)**r
+            singular_ics = _find_conditions(g, x, x0, lenics)
+            singular_ics = [j / factorial(i) for i, j in enumerate(singular_ics)]
+            y0 = {r:singular_ics}
+            return HolonomicFunction(sol, x, x0, y0)
+
+    y0 = _find_conditions(func, x, x0, lenics)
+    while not y0:
+        x0 += 1
+        y0 = _find_conditions(func, x, x0, lenics)
+
+    return HolonomicFunction(sol, x, x0, y0)
+
+
+def _convert_meijerint(func, x, initcond=True, domain=QQ):
+    args = meijerint._rewrite1(func, x)
+
+    if args:
+        fac, po, g, _ = args
+    else:
+        return None
+
+    # lists for sum of meijerg functions
+    fac_list = [fac * i[0] for i in g]
+    t = po.as_base_exp()
+    s = t[1] if t[0] == x else S.Zero
+    po_list = [s + i[1] for i in g]
+    G_list = [i[2] for i in g]
+
+    # finds meijerg representation of x**s * meijerg(a1 ... ap, b1 ... bq, z)
+    def _shift(func, s):
+        z = func.args[-1]
+        if z.has(I):
+            z = z.subs(exp_polar, exp)
+
+        d = z.collect(x, evaluate=False)
+        b = list(d)[0]
+        a = d[b]
+
+        t = b.as_base_exp()
+        b = t[1] if t[0] == x else S.Zero
+        r = s / b
+        an = (i + r for i in func.args[0][0])
+        ap = (i + r for i in func.args[0][1])
+        bm = (i + r for i in func.args[1][0])
+        bq = (i + r for i in func.args[1][1])
+
+        return a**-r, meijerg((an, ap), (bm, bq), z)
+
+    coeff, m = _shift(G_list[0], po_list[0])
+    sol = fac_list[0] * coeff * from_meijerg(m, initcond=initcond, domain=domain)
+
+    # add all the meijerg functions after converting to holonomic
+    for i in range(1, len(G_list)):
+        coeff, m = _shift(G_list[i], po_list[i])
+        sol += fac_list[i] * coeff * from_meijerg(m, initcond=initcond, domain=domain)
+
+    return sol
+
+
+def _create_table(table, domain=QQ):
+    """
+    Creates the look-up table. For a similar implementation
+    see meijerint._create_lookup_table.
+    """
+
+    def add(formula, annihilator, arg, x0=0, y0=()):
+        """
+        Adds a formula in the dictionary
+        """
+        table.setdefault(_mytype(formula, x_1), []).append((formula,
+            HolonomicFunction(annihilator, arg, x0, y0)))
+
+    R = domain.old_poly_ring(x_1)
+    _, Dx = DifferentialOperators(R, 'Dx')
+
+    # add some basic functions
+    add(sin(x_1), Dx**2 + 1, x_1, 0, [0, 1])
+    add(cos(x_1), Dx**2 + 1, x_1, 0, [1, 0])
+    add(exp(x_1), Dx - 1, x_1, 0, 1)
+    add(log(x_1), Dx + x_1*Dx**2, x_1, 1, [0, 1])
+
+    add(erf(x_1), 2*x_1*Dx + Dx**2, x_1, 0, [0, 2/sqrt(pi)])
+    add(erfc(x_1), 2*x_1*Dx + Dx**2, x_1, 0, [1, -2/sqrt(pi)])
+    add(erfi(x_1), -2*x_1*Dx + Dx**2, x_1, 0, [0, 2/sqrt(pi)])
+
+    add(sinh(x_1), Dx**2 - 1, x_1, 0, [0, 1])
+    add(cosh(x_1), Dx**2 - 1, x_1, 0, [1, 0])
+
+    add(sinc(x_1), x_1 + 2*Dx + x_1*Dx**2, x_1)
+
+    add(Si(x_1), x_1*Dx + 2*Dx**2 + x_1*Dx**3, x_1)
+    add(Ci(x_1), x_1*Dx + 2*Dx**2 + x_1*Dx**3, x_1)
+
+    add(Shi(x_1), -x_1*Dx + 2*Dx**2 + x_1*Dx**3, x_1)
+
+
+def _find_conditions(func, x, x0, order):
+    y0 = []
+    for i in range(order):
+        val = func.subs(x, x0)
+        if isinstance(val, NaN):
+            val = limit(func, x, x0)
+        if val.is_finite is False or isinstance(val, NaN):
+            return None
+        y0.append(val)
+        func = func.diff(x)
+    return y0

llmeval-env/lib/python3.10/site-packages/sympy/holonomic/holonomicerrors.py

@@ -0,0 +1,49 @@
+""" Common Exceptions for `holonomic` module. """
+
+class BaseHolonomicError(Exception):
+
+    def new(self, *args):
+        raise NotImplementedError("abstract base class")
+
+class NotPowerSeriesError(BaseHolonomicError):
+
+    def __init__(self, holonomic, x0):
+        self.holonomic = holonomic
+        self.x0 = x0
+
+    def __str__(self):
+        s = 'A Power Series does not exists for '
+        s += str(self.holonomic)
+        s += ' about %s.' %self.x0
+        return s
+
+class NotHolonomicError(BaseHolonomicError):
+
+    def __init__(self, m):
+        self.m = m
+
+    def __str__(self):
+        return self.m
+
+class SingularityError(BaseHolonomicError):
+
+    def __init__(self, holonomic, x0):
+        self.holonomic = holonomic
+        self.x0 = x0
+
+    def __str__(self):
+        s = str(self.holonomic)
+        s += ' has a singularity at %s.' %self.x0
+        return s
+
+class NotHyperSeriesError(BaseHolonomicError):
+
+    def __init__(self, holonomic, x0):
+        self.holonomic = holonomic
+        self.x0 = x0
+
+    def __str__(self):
+        s = 'Power series expansion of '
+        s += str(self.holonomic)
+        s += ' about %s is not hypergeometric' %self.x0
+        return s

llmeval-env/lib/python3.10/site-packages/sympy/holonomic/numerical.py

@@ -0,0 +1,109 @@
+"""Numerical Methods for Holonomic Functions"""
+
+from sympy.core.sympify import sympify
+from sympy.holonomic.holonomic import DMFsubs
+
+from mpmath import mp
+
+
+def _evalf(func, points, derivatives=False, method='RK4'):
+    """
+    Numerical methods for numerical integration along a given set of
+    points in the complex plane.
+    """
+
+    ann = func.annihilator
+    a = ann.order
+    R = ann.parent.base
+    K = R.get_field()
+
+    if method == 'Euler':
+        meth = _euler
+    else:
+        meth = _rk4
+
+    dmf = []
+    for j in ann.listofpoly:
+        dmf.append(K.new(j.rep))
+
+    red = [-dmf[i] / dmf[a] for i in range(a)]
+
+    y0 = func.y0
+    if len(y0) < a:
+        raise TypeError("Not Enough Initial Conditions")
+    x0 = func.x0
+    sol = [meth(red, x0, points[0], y0, a)]
+
+    for i, j in enumerate(points[1:]):
+        sol.append(meth(red, points[i], j, sol[-1], a))
+
+    if not derivatives:
+        return [sympify(i[0]) for i in sol]
+    else:
+        return sympify(sol)
+
+
+def _euler(red, x0, x1, y0, a):
+    """
+    Euler's method for numerical integration.
+    From x0 to x1 with initial values given at x0 as vector y0.
+    """
+
+    A = sympify(x0)._to_mpmath(mp.prec)
+    B = sympify(x1)._to_mpmath(mp.prec)
+    y_0 = [sympify(i)._to_mpmath(mp.prec) for i in y0]
+    h = B - A
+    f_0 = y_0[1:]
+    f_0_n = 0
+
+    for i in range(a):
+        f_0_n += sympify(DMFsubs(red[i], A, mpm=True))._to_mpmath(mp.prec) * y_0[i]
+    f_0.append(f_0_n)
+
+    sol = []
+    for i in range(a):
+        sol.append(y_0[i] + h * f_0[i])
+
+    return sol
+
+
+def _rk4(red, x0, x1, y0, a):
+    """
+    Runge-Kutta 4th order numerical method.
+    """
+
+    A = sympify(x0)._to_mpmath(mp.prec)
+    B = sympify(x1)._to_mpmath(mp.prec)
+    y_0 = [sympify(i)._to_mpmath(mp.prec) for i in y0]
+    h = B - A
+
+    f_0_n = 0
+    f_1_n = 0
+    f_2_n = 0
+    f_3_n = 0
+
+    f_0 = y_0[1:]
+    for i in range(a):
+        f_0_n += sympify(DMFsubs(red[i], A, mpm=True))._to_mpmath(mp.prec) * y_0[i]
+    f_0.append(f_0_n)
+
+    f_1 = [y_0[i] + f_0[i]*h/2 for i in range(1, a)]
+    for i in range(a):
+        f_1_n += sympify(DMFsubs(red[i], A + h/2, mpm=True))._to_mpmath(mp.prec) * (y_0[i] + f_0[i]*h/2)
+    f_1.append(f_1_n)
+
+    f_2 = [y_0[i] + f_1[i]*h/2 for i in range(1, a)]
+    for i in range(a):
+        f_2_n += sympify(DMFsubs(red[i], A + h/2, mpm=True))._to_mpmath(mp.prec) * (y_0[i] + f_1[i]*h/2)
+    f_2.append(f_2_n)
+
+    f_3 = [y_0[i] + f_2[i]*h for i in range(1, a)]
+    for i in range(a):
+        f_3_n += sympify(DMFsubs(red[i], A + h, mpm=True))._to_mpmath(mp.prec) * (y_0[i] + f_2[i]*h)
+    f_3.append(f_3_n)
+
+    sol = []
+    for i in range(a):
+        sol.append(y_0[i] + h * (f_0[i]+2*f_1[i]+2*f_2[i]+f_3[i])/6)
+
+    return sol

llmeval-env/lib/python3.10/site-packages/sympy/holonomic/recurrence.py

@@ -0,0 +1,365 @@
+"""Recurrence Operators"""
+
+from sympy.core.singleton import S
+from sympy.core.symbol import (Symbol, symbols)
+from sympy.printing import sstr
+from sympy.core.sympify import sympify
+
+
+def RecurrenceOperators(base, generator):
+    """
+    Returns an Algebra of Recurrence Operators and the operator for
+    shifting i.e. the `Sn` operator.
+    The first argument needs to be the base polynomial ring for the algebra
+    and the second argument must be a generator which can be either a
+    noncommutative Symbol or a string.
+
+    Examples
+    ========
+
+    >>> from sympy import ZZ
+    >>> from sympy import symbols
+    >>> from sympy.holonomic.recurrence import RecurrenceOperators
+    >>> n = symbols('n', integer=True)
+    >>> R, Sn = RecurrenceOperators(ZZ.old_poly_ring(n), 'Sn')
+    """
+
+    ring = RecurrenceOperatorAlgebra(base, generator)
+    return (ring, ring.shift_operator)
+
+
+class RecurrenceOperatorAlgebra:
+    """
+    A Recurrence Operator Algebra is a set of noncommutative polynomials
+    in intermediate `Sn` and coefficients in a base ring A. It follows the
+    commutation rule:
+    Sn * a(n) = a(n + 1) * Sn
+
+    This class represents a Recurrence Operator Algebra and serves as the parent ring
+    for Recurrence Operators.
+
+    Examples
+    ========
+
+    >>> from sympy import ZZ
+    >>> from sympy import symbols
+    >>> from sympy.holonomic.recurrence import RecurrenceOperators
+    >>> n = symbols('n', integer=True)
+    >>> R, Sn = RecurrenceOperators(ZZ.old_poly_ring(n), 'Sn')
+    >>> R
+    Univariate Recurrence Operator Algebra in intermediate Sn over the base ring
+    ZZ[n]
+
+    See Also
+    ========
+
+    RecurrenceOperator
+    """
+
+    def __init__(self, base, generator):
+        # the base ring for the algebra
+        self.base = base
+        # the operator representing shift i.e. `Sn`
+        self.shift_operator = RecurrenceOperator(
+            [base.zero, base.one], self)
+
+        if generator is None:
+            self.gen_symbol = symbols('Sn', commutative=False)
+        else:
+            if isinstance(generator, str):
+                self.gen_symbol = symbols(generator, commutative=False)
+            elif isinstance(generator, Symbol):
+                self.gen_symbol = generator
+
+    def __str__(self):
+        string = 'Univariate Recurrence Operator Algebra in intermediate '\
+            + sstr(self.gen_symbol) + ' over the base ring ' + \
+            (self.base).__str__()
+
+        return string
+
+    __repr__ = __str__
+
+    def __eq__(self, other):
+        if self.base == other.base and self.gen_symbol == other.gen_symbol:
+            return True
+        else:
+            return False
+
+
+def _add_lists(list1, list2):
+    if len(list1) <= len(list2):
+        sol = [a + b for a, b in zip(list1, list2)] + list2[len(list1):]
+    else:
+        sol = [a + b for a, b in zip(list1, list2)] + list1[len(list2):]
+    return sol
+
+
+class RecurrenceOperator:
+    """
+    The Recurrence Operators are defined by a list of polynomials
+    in the base ring and the parent ring of the Operator.
+
+    Explanation
+    ===========
+
+    Takes a list of polynomials for each power of Sn and the
+    parent ring which must be an instance of RecurrenceOperatorAlgebra.
+
+    A Recurrence Operator can be created easily using
+    the operator `Sn`. See examples below.
+
+    Examples
+    ========
+
+    >>> from sympy.holonomic.recurrence import RecurrenceOperator, RecurrenceOperators
+    >>> from sympy import ZZ
+    >>> from sympy import symbols
+    >>> n = symbols('n', integer=True)
+    >>> R, Sn = RecurrenceOperators(ZZ.old_poly_ring(n),'Sn')
+
+    >>> RecurrenceOperator([0, 1, n**2], R)
+    (1)Sn + (n**2)Sn**2
+
+    >>> Sn*n
+    (n + 1)Sn
+
+    >>> n*Sn*n + 1 - Sn**2*n
+    (1) + (n**2 + n)Sn + (-n - 2)Sn**2
+
+    See Also
+    ========
+
+    DifferentialOperatorAlgebra
+    """
+
+    _op_priority = 20
+
+    def __init__(self, list_of_poly, parent):
+        # the parent ring for this operator
+        # must be an RecurrenceOperatorAlgebra object
+        self.parent = parent
+        # sequence of polynomials in n for each power of Sn
+        # represents the operator
+        # convert the expressions into ring elements using from_sympy
+        if isinstance(list_of_poly, list):
+            for i, j in enumerate(list_of_poly):
+                if isinstance(j, int):
+                    list_of_poly[i] = self.parent.base.from_sympy(S(j))
+                elif not isinstance(j, self.parent.base.dtype):
+                    list_of_poly[i] = self.parent.base.from_sympy(j)
+
+            self.listofpoly = list_of_poly
+        self.order = len(self.listofpoly) - 1
+
+    def __mul__(self, other):
+        """
+        Multiplies two Operators and returns another
+        RecurrenceOperator instance using the commutation rule
+        Sn * a(n) = a(n + 1) * Sn
+        """
+
+        listofself = self.listofpoly
+        base = self.parent.base
+
+        if not isinstance(other, RecurrenceOperator):
+            if not isinstance(other, self.parent.base.dtype):
+                listofother = [self.parent.base.from_sympy(sympify(other))]
+
+            else:
+                listofother = [other]
+        else:
+            listofother = other.listofpoly
+        # multiply a polynomial `b` with a list of polynomials
+
+        def _mul_dmp_diffop(b, listofother):
+            if isinstance(listofother, list):
+                sol = []
+                for i in listofother:
+                    sol.append(i * b)
+                return sol
+            else:
+                return [b * listofother]
+
+        sol = _mul_dmp_diffop(listofself[0], listofother)
+
+        # compute Sn^i * b
+        def _mul_Sni_b(b):
+            sol = [base.zero]
+
+            if isinstance(b, list):
+                for i in b:
+                    j = base.to_sympy(i).subs(base.gens[0], base.gens[0] + S.One)
+                    sol.append(base.from_sympy(j))
+
+            else:
+                j = b.subs(base.gens[0], base.gens[0] + S.One)
+                sol.append(base.from_sympy(j))
+
+            return sol
+
+        for i in range(1, len(listofself)):
+            # find Sn^i * b in ith iteration
+            listofother = _mul_Sni_b(listofother)
+            # solution = solution + listofself[i] * (Sn^i * b)
+            sol = _add_lists(sol, _mul_dmp_diffop(listofself[i], listofother))
+
+        return RecurrenceOperator(sol, self.parent)
+
+    def __rmul__(self, other):
+        if not isinstance(other, RecurrenceOperator):
+
+            if isinstance(other, int):
+                other = S(other)
+
+            if not isinstance(other, self.parent.base.dtype):
+                other = (self.parent.base).from_sympy(other)
+
+            sol = []
+            for j in self.listofpoly:
+                sol.append(other * j)
+
+            return RecurrenceOperator(sol, self.parent)
+
+    def __add__(self, other):
+        if isinstance(other, RecurrenceOperator):
+
+            sol = _add_lists(self.listofpoly, other.listofpoly)
+            return RecurrenceOperator(sol, self.parent)
+
+        else:
+
+            if isinstance(other, int):
+                other = S(other)
+            list_self = self.listofpoly
+            if not isinstance(other, self.parent.base.dtype):
+                list_other = [((self.parent).base).from_sympy(other)]
+            else:
+                list_other = [other]
+            sol = []
+            sol.append(list_self[0] + list_other[0])
+            sol += list_self[1:]
+
+            return RecurrenceOperator(sol, self.parent)
+
+    __radd__ = __add__
+
+    def __sub__(self, other):
+        return self + (-1) * other
+
+    def __rsub__(self, other):
+        return (-1) * self + other
+
+    def __pow__(self, n):
+        if n == 1:
+            return self
+        if n == 0:
+            return RecurrenceOperator([self.parent.base.one], self.parent)
+        # if self is `Sn`
+        if self.listofpoly == self.parent.shift_operator.listofpoly:
+            sol = []
+            for i in range(0, n):
+                sol.append(self.parent.base.zero)
+            sol.append(self.parent.base.one)
+
+            return RecurrenceOperator(sol, self.parent)
+
+        else:
+            if n % 2 == 1:
+                powreduce = self**(n - 1)
+                return powreduce * self
+            elif n % 2 == 0:
+                powreduce = self**(n / 2)
+                return powreduce * powreduce
+
+    def __str__(self):
+        listofpoly = self.listofpoly
+        print_str = ''
+
+        for i, j in enumerate(listofpoly):
+            if j == self.parent.base.zero:
+                continue
+
+            if i == 0:
+                print_str += '(' + sstr(j) + ')'
+                continue
+
+            if print_str:
+                print_str += ' + '
+
+            if i == 1:
+                print_str += '(' + sstr(j) + ')Sn'
+                continue
+
+            print_str += '(' + sstr(j) + ')' + 'Sn**' + sstr(i)
+
+        return print_str
+
+    __repr__ = __str__
+
+    def __eq__(self, other):
+        if isinstance(other, RecurrenceOperator):
+            if self.listofpoly == other.listofpoly and self.parent == other.parent:
+                return True
+            else:
+                return False
+        else:
+            if self.listofpoly[0] == other:
+                for i in self.listofpoly[1:]:
+                    if i is not self.parent.base.zero:
+                        return False
+                return True
+            else:
+                return False
+
+
+class HolonomicSequence:
+    """
+    A Holonomic Sequence is a type of sequence satisfying a linear homogeneous
+    recurrence relation with Polynomial coefficients. Alternatively, A sequence
+    is Holonomic if and only if its generating function is a Holonomic Function.
+    """
+
+    def __init__(self, recurrence, u0=[]):
+        self.recurrence = recurrence
+        if not isinstance(u0, list):
+            self.u0 = [u0]
+        else:
+            self.u0 = u0
+
+        if len(self.u0) == 0:
+            self._have_init_cond = False
+        else:
+            self._have_init_cond = True
+        self.n = recurrence.parent.base.gens[0]
+
+    def __repr__(self):
+        str_sol = 'HolonomicSequence(%s, %s)' % ((self.recurrence).__repr__(), sstr(self.n))
+        if not self._have_init_cond:
+            return str_sol
+        else:
+            cond_str = ''
+            seq_str = 0
+            for i in self.u0:
+                cond_str += ', u(%s) = %s' % (sstr(seq_str), sstr(i))
+                seq_str += 1
+
+            sol = str_sol + cond_str
+            return sol
+
+    __str__ = __repr__
+
+    def __eq__(self, other):
+        if self.recurrence == other.recurrence:
+            if self.n == other.n:
+                if self._have_init_cond and other._have_init_cond:
+                    if self.u0 == other.u0:
+                        return True
+                    else:
+                        return False
+                else:
+                    return True
+            else:
+                return False
+        else:
+            return False

llmeval-env/lib/python3.10/site-packages/sympy/holonomic/tests/test_holonomic.py

@@ -0,0 +1,830 @@
+from sympy.holonomic import (DifferentialOperator, HolonomicFunction,
+                             DifferentialOperators, from_hyper,
+                             from_meijerg, expr_to_holonomic)
+from sympy.holonomic.recurrence import RecurrenceOperators, HolonomicSequence
+from sympy.core import EulerGamma
+from sympy.core.numbers import (I, Rational, pi)
+from sympy.core.singleton import S
+from sympy.core.symbol import (Symbol, symbols)
+from sympy.functions.elementary.exponential import (exp, log)
+from sympy.functions.elementary.hyperbolic import (asinh, cosh)
+from sympy.functions.elementary.miscellaneous import sqrt
+from sympy.functions.elementary.trigonometric import (cos, sin)
+from sympy.functions.special.bessel import besselj
+from sympy.functions.special.beta_functions import beta
+from sympy.functions.special.error_functions import (Ci, Si, erf, erfc)
+from sympy.functions.special.gamma_functions import gamma
+from sympy.functions.special.hyper import (hyper, meijerg)
+from sympy.printing.str import sstr
+from sympy.series.order import O
+from sympy.simplify.hyperexpand import hyperexpand
+from sympy.polys.domains.integerring import ZZ
+from sympy.polys.domains.rationalfield import QQ
+from sympy.polys.domains.realfield import RR
+
+
+def test_DifferentialOperator():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    assert Dx == R.derivative_operator
+    assert Dx == DifferentialOperator([R.base.zero, R.base.one], R)
+    assert x * Dx + x**2 * Dx**2 == DifferentialOperator([0, x, x**2], R)
+    assert (x**2 + 1) + Dx + x * \
+        Dx**5 == DifferentialOperator([x**2 + 1, 1, 0, 0, 0, x], R)
+    assert (x * Dx + x**2 + 1 - Dx * (x**3 + x))**3 == (-48 * x**6) + \
+        (-57 * x**7) * Dx + (-15 * x**8) * Dx**2 + (-x**9) * Dx**3
+    p = (x * Dx**2 + (x**2 + 3) * Dx**5) * (Dx + x**2)
+    q = (2 * x) + (4 * x**2) * Dx + (x**3) * Dx**2 + \
+        (20 * x**2 + x + 60) * Dx**3 + (10 * x**3 + 30 * x) * Dx**4 + \
+        (x**4 + 3 * x**2) * Dx**5 + (x**2 + 3) * Dx**6
+    assert p == q
+
+
+def test_HolonomicFunction_addition():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx**2 * x, x)
+    q = HolonomicFunction((2) * Dx + (x) * Dx**2, x)
+    assert p == q
+    p = HolonomicFunction(x * Dx + 1, x)
+    q = HolonomicFunction(Dx + 1, x)
+    r = HolonomicFunction((x - 2) + (x**2 - 2) * Dx + (x**2 - x) * Dx**2, x)
+    assert p + q == r
+    p = HolonomicFunction(x * Dx + Dx**2 * (x**2 + 2), x)
+    q = HolonomicFunction(Dx - 3, x)
+    r = HolonomicFunction((-54 * x**2 - 126 * x - 150) + (-135 * x**3 - 252 * x**2 - 270 * x + 140) * Dx +\
+                 (-27 * x**4 - 24 * x**2 + 14 * x - 150) * Dx**2 + \
+                 (9 * x**4 + 15 * x**3 + 38 * x**2 + 30 * x +40) * Dx**3, x)
+    assert p + q == r
+    p = HolonomicFunction(Dx**5 - 1, x)
+    q = HolonomicFunction(x**3 + Dx, x)
+    r = HolonomicFunction((-x**18 + 45*x**14 - 525*x**10 + 1575*x**6 - x**3 - 630*x**2) + \
+        (-x**15 + 30*x**11 - 195*x**7 + 210*x**3 - 1)*Dx + (x**18 - 45*x**14 + 525*x**10 - \
+        1575*x**6 + x**3 + 630*x**2)*Dx**5 + (x**15 - 30*x**11 + 195*x**7 - 210*x**3 + \
+        1)*Dx**6, x)
+    assert p+q == r
+
+    p = x**2 + 3*x + 8
+    q = x**3 - 7*x + 5
+    p = p*Dx - p.diff()
+    q = q*Dx - q.diff()
+    r = HolonomicFunction(p, x) + HolonomicFunction(q, x)
+    s = HolonomicFunction((6*x**2 + 18*x + 14) + (-4*x**3 - 18*x**2 - 62*x + 10)*Dx +\
+        (x**4 + 6*x**3 + 31*x**2 - 10*x - 71)*Dx**2, x)
+    assert r == s
+
+
+def test_HolonomicFunction_multiplication():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx+x+x*Dx**2, x)
+    q = HolonomicFunction(x*Dx+Dx*x+Dx**2, x)
+    r = HolonomicFunction((8*x**6 + 4*x**4 + 6*x**2 + 3) + (24*x**5 - 4*x**3 + 24*x)*Dx + \
+        (8*x**6 + 20*x**4 + 12*x**2 + 2)*Dx**2 + (8*x**5 + 4*x**3 + 4*x)*Dx**3 + \
+        (2*x**4 + x**2)*Dx**4, x)
+    assert p*q == r
+    p = HolonomicFunction(Dx**2+1, x)
+    q = HolonomicFunction(Dx-1, x)
+    r = HolonomicFunction((2) + (-2)*Dx + (1)*Dx**2, x)
+    assert p*q == r
+    p = HolonomicFunction(Dx**2+1+x+Dx, x)
+    q = HolonomicFunction((Dx*x-1)**2, x)
+    r = HolonomicFunction((4*x**7 + 11*x**6 + 16*x**5 + 4*x**4 - 6*x**3 - 7*x**2 - 8*x - 2) + \
+        (8*x**6 + 26*x**5 + 24*x**4 - 3*x**3 - 11*x**2 - 6*x - 2)*Dx + \
+        (8*x**6 + 18*x**5 + 15*x**4 - 3*x**3 - 6*x**2 - 6*x - 2)*Dx**2 + (8*x**5 + \
+            10*x**4 + 6*x**3 - 2*x**2 - 4*x)*Dx**3 + (4*x**5 + 3*x**4 - x**2)*Dx**4, x)
+    assert p*q == r
+    p = HolonomicFunction(x*Dx**2-1, x)
+    q = HolonomicFunction(Dx*x-x, x)
+    r = HolonomicFunction((x - 3) + (-2*x + 2)*Dx + (x)*Dx**2, x)
+    assert p*q == r
+
+
+def test_addition_initial_condition():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx-1, x, 0, [3])
+    q = HolonomicFunction(Dx**2+1, x, 0, [1, 0])
+    r = HolonomicFunction(-1 + Dx - Dx**2 + Dx**3, x, 0, [4, 3, 2])
+    assert p + q == r
+    p = HolonomicFunction(Dx - x + Dx**2, x, 0, [1, 2])
+    q = HolonomicFunction(Dx**2 + x, x, 0, [1, 0])
+    r = HolonomicFunction((-x**4 - x**3/4 - x**2 + Rational(1, 4)) + (x**3 + x**2/4 + x*Rational(3, 4) + 1)*Dx + \
+        (x*Rational(-3, 2) + Rational(7, 4))*Dx**2 + (x**2 - x*Rational(7, 4) + Rational(1, 4))*Dx**3 + (x**2 + x/4 + S.Half)*Dx**4, x, 0, [2, 2, -2, 2])
+    assert p + q == r
+    p = HolonomicFunction(Dx**2 + 4*x*Dx + x**2, x, 0, [3, 4])
+    q = HolonomicFunction(Dx**2 + 1, x, 0, [1, 1])
+    r = HolonomicFunction((x**6 + 2*x**4 - 5*x**2 - 6) + (4*x**5 + 36*x**3 - 32*x)*Dx + \
+         (x**6 + 3*x**4 + 5*x**2 - 9)*Dx**2 + (4*x**5 + 36*x**3 - 32*x)*Dx**3 + (x**4 + \
+            10*x**2 - 3)*Dx**4, x, 0, [4, 5, -1, -17])
+    assert p + q == r
+    q = HolonomicFunction(Dx**3 + x, x, 2, [3, 0, 1])
+    p = HolonomicFunction(Dx - 1, x, 2, [1])
+    r = HolonomicFunction((-x**2 - x + 1) + (x**2 + x)*Dx + (-x - 2)*Dx**3 + \
+        (x + 1)*Dx**4, x, 2, [4, 1, 2, -5 ])
+    assert p + q == r
+    p = expr_to_holonomic(sin(x))
+    q = expr_to_holonomic(1/x, x0=1)
+    r = HolonomicFunction((x**2 + 6) + (x**3 + 2*x)*Dx + (x**2 + 6)*Dx**2 + (x**3 + 2*x)*Dx**3, \
+        x, 1, [sin(1) + 1, -1 + cos(1), -sin(1) + 2])
+    assert p + q == r
+    C_1 = symbols('C_1')
+    p = expr_to_holonomic(sqrt(x))
+    q = expr_to_holonomic(sqrt(x**2-x))
+    r = (p + q).to_expr().subs(C_1, -I/2).expand()
+    assert r == I*sqrt(x)*sqrt(-x + 1) + sqrt(x)
+
+
+def test_multiplication_initial_condition():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx**2 + x*Dx - 1, x, 0, [3, 1])
+    q = HolonomicFunction(Dx**2 + 1, x, 0, [1, 1])
+    r = HolonomicFunction((x**4 + 14*x**2 + 60) + 4*x*Dx + (x**4 + 9*x**2 + 20)*Dx**2 + \
+        (2*x**3 + 18*x)*Dx**3 + (x**2 + 10)*Dx**4, x, 0, [3, 4, 2, 3])
+    assert p * q == r
+    p = HolonomicFunction(Dx**2 + x, x, 0, [1, 0])
+    q = HolonomicFunction(Dx**3 - x**2, x, 0, [3, 3, 3])
+    r = HolonomicFunction((x**8 - 37*x**7/27 - 10*x**6/27 - 164*x**5/9 - 184*x**4/9 + \
+        160*x**3/27 + 404*x**2/9 + 8*x + Rational(40, 3)) + (6*x**7 - 128*x**6/9 - 98*x**5/9 - 28*x**4/9 + \
+        8*x**3/9 + 28*x**2 + x*Rational(40, 9) - 40)*Dx + (3*x**6 - 82*x**5/9 + 76*x**4/9 + 4*x**3/3 + \
+        220*x**2/9 - x*Rational(80, 3))*Dx**2 + (-2*x**6 + 128*x**5/27 - 2*x**4/3 -80*x**2/9 + Rational(200, 9))*Dx**3 + \
+        (3*x**5 - 64*x**4/9 - 28*x**3/9 + 6*x**2 - x*Rational(20, 9) - Rational(20, 3))*Dx**4 + (-4*x**3 + 64*x**2/9 + \
+            x*Rational(8, 3))*Dx**5 + (x**4 - 64*x**3/27 - 4*x**2/3 + Rational(20, 9))*Dx**6, x, 0, [3, 3, 3, -3, -12, -24])
+    assert p * q == r
+    p = HolonomicFunction(Dx - 1, x, 0, [2])
+    q = HolonomicFunction(Dx**2 + 1, x, 0, [0, 1])
+    r = HolonomicFunction(2 -2*Dx + Dx**2, x, 0, [0, 2])
+    assert p * q == r
+    q = HolonomicFunction(x*Dx**2 + 1 + 2*Dx, x, 0,[0, 1])
+    r = HolonomicFunction((x - 1) + (-2*x + 2)*Dx + x*Dx**2, x, 0, [0, 2])
+    assert p * q == r
+    p = HolonomicFunction(Dx**2 - 1, x, 0, [1, 3])
+    q = HolonomicFunction(Dx**3 + 1, x, 0, [1, 2, 1])
+    r = HolonomicFunction(6*Dx + 3*Dx**2 + 2*Dx**3 - 3*Dx**4 + Dx**6, x, 0, [1, 5, 14, 17, 17, 2])
+    assert p * q == r
+    p = expr_to_holonomic(sin(x))
+    q = expr_to_holonomic(1/x, x0=1)
+    r = HolonomicFunction(x + 2*Dx + x*Dx**2, x, 1, [sin(1), -sin(1) + cos(1)])
+    assert p * q == r
+    p = expr_to_holonomic(sqrt(x))
+    q = expr_to_holonomic(sqrt(x**2-x))
+    r = (p * q).to_expr()
+    assert r == I*x*sqrt(-x + 1)
+
+
+def test_HolonomicFunction_composition():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx-1, x).composition(x**2+x)
+    r = HolonomicFunction((-2*x - 1) + Dx, x)
+    assert p == r
+    p = HolonomicFunction(Dx**2+1, x).composition(x**5+x**2+1)
+    r = HolonomicFunction((125*x**12 + 150*x**9 + 60*x**6 + 8*x**3) + (-20*x**3 - 2)*Dx + \
+        (5*x**4 + 2*x)*Dx**2, x)
+    assert p == r
+    p = HolonomicFunction(Dx**2*x+x, x).composition(2*x**3+x**2+1)
+    r = HolonomicFunction((216*x**9 + 324*x**8 + 180*x**7 + 152*x**6 + 112*x**5 + \
+        36*x**4 + 4*x**3) + (24*x**4 + 16*x**3 + 3*x**2 - 6*x - 1)*Dx + (6*x**5 + 5*x**4 + \
+        x**3 + 3*x**2 + x)*Dx**2, x)
+    assert p == r
+    p = HolonomicFunction(Dx**2+1, x).composition(1-x**2)
+    r = HolonomicFunction((4*x**3) - Dx + x*Dx**2, x)
+    assert p == r
+    p = HolonomicFunction(Dx**2+1, x).composition(x - 2/(x**2 + 1))
+    r = HolonomicFunction((x**12 + 6*x**10 + 12*x**9 + 15*x**8 + 48*x**7 + 68*x**6 + \
+        72*x**5 + 111*x**4 + 112*x**3 + 54*x**2 + 12*x + 1) + (12*x**8 + 32*x**6 + \
+        24*x**4 - 4)*Dx + (x**12 + 6*x**10 + 4*x**9 + 15*x**8 + 16*x**7 + 20*x**6 + 24*x**5+ \
+        15*x**4 + 16*x**3 + 6*x**2 + 4*x + 1)*Dx**2, x)
+    assert p == r
+
+
+def test_from_hyper():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    p = hyper([1, 1], [Rational(3, 2)], x**2/4)
+    q = HolonomicFunction((4*x) + (5*x**2 - 8)*Dx + (x**3 - 4*x)*Dx**2, x, 1, [2*sqrt(3)*pi/9, -4*sqrt(3)*pi/27 + Rational(4, 3)])
+    r = from_hyper(p)
+    assert r == q
+    p = from_hyper(hyper([1], [Rational(3, 2)], x**2/4))
+    q = HolonomicFunction(-x + (-x**2/2 + 2)*Dx + x*Dx**2, x)
+    # x0 = 1
+    y0 = '[sqrt(pi)*exp(1/4)*erf(1/2), -sqrt(pi)*exp(1/4)*erf(1/2)/2 + 1]'
+    assert sstr(p.y0) == y0
+    assert q.annihilator == p.annihilator
+
+
+def test_from_meijerg():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    p = from_meijerg(meijerg(([], [Rational(3, 2)]), ([S.Half], [S.Half, 1]), x))
+    q = HolonomicFunction(x/2 - Rational(1, 4) + (-x**2 + x/4)*Dx + x**2*Dx**2 + x**3*Dx**3, x, 1, \
+        [1/sqrt(pi), 1/(2*sqrt(pi)), -1/(4*sqrt(pi))])
+    assert p == q
+    p = from_meijerg(meijerg(([], []), ([0], []), x))
+    q = HolonomicFunction(1 + Dx, x, 0, [1])
+    assert p == q
+    p = from_meijerg(meijerg(([1], []), ([S.Half], [0]), x))
+    q = HolonomicFunction((x + S.Half)*Dx + x*Dx**2, x, 1, [sqrt(pi)*erf(1), exp(-1)])
+    assert p == q
+    p = from_meijerg(meijerg(([0], [1]), ([0], []), 2*x**2))
+    q = HolonomicFunction((3*x**2 - 1)*Dx + x**3*Dx**2, x, 1, [-exp(Rational(-1, 2)) + 1, -exp(Rational(-1, 2))])
+    assert p == q
+
+
+def test_to_Sequence():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    n = symbols('n', integer=True)
+    _, Sn = RecurrenceOperators(ZZ.old_poly_ring(n), 'Sn')
+    p = HolonomicFunction(x**2*Dx**4 + x + Dx, x).to_sequence()
+    q = [(HolonomicSequence(1 + (n + 2)*Sn**2 + (n**4 + 6*n**3 + 11*n**2 + 6*n)*Sn**3), 0, 1)]
+    assert p == q
+    p = HolonomicFunction(x**2*Dx**4 + x**3 + Dx**2, x).to_sequence()
+    q = [(HolonomicSequence(1 + (n**4 + 14*n**3 + 72*n**2 + 163*n + 140)*Sn**5), 0, 0)]
+    assert p == q
+    p = HolonomicFunction(x**3*Dx**4 + 1 + Dx**2, x).to_sequence()
+    q = [(HolonomicSequence(1 + (n**4 - 2*n**3 - n**2 + 2*n)*Sn + (n**2 + 3*n + 2)*Sn**2), 0, 0)]
+    assert p == q
+    p = HolonomicFunction(3*x**3*Dx**4 + 2*x*Dx + x*Dx**3, x).to_sequence()
+    q = [(HolonomicSequence(2*n + (3*n**4 - 6*n**3 - 3*n**2 + 6*n)*Sn + (n**3 + 3*n**2 + 2*n)*Sn**2), 0, 1)]
+    assert p == q
+
+
+def test_to_Sequence_Initial_Coniditons():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    n = symbols('n', integer=True)
+    _, Sn = RecurrenceOperators(QQ.old_poly_ring(n), 'Sn')
+    p = HolonomicFunction(Dx - 1, x, 0, [1]).to_sequence()
+    q = [(HolonomicSequence(-1 + (n + 1)*Sn, 1), 0)]
+    assert p == q
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [0, 1]).to_sequence()
+    q = [(HolonomicSequence(1 + (n**2 + 3*n + 2)*Sn**2, [0, 1]), 0)]
+    assert p == q
+    p = HolonomicFunction(Dx**2 + 1 + x**3*Dx, x, 0, [2, 3]).to_sequence()
+    q = [(HolonomicSequence(n + Sn**2 + (n**2 + 7*n + 12)*Sn**4, [2, 3, -1, Rational(-1, 2), Rational(1, 12)]), 1)]
+    assert p == q
+    p = HolonomicFunction(x**3*Dx**5 + 1 + Dx, x).to_sequence()
+    q = [(HolonomicSequence(1 + (n + 1)*Sn + (n**5 - 5*n**3 + 4*n)*Sn**2), 0, 3)]
+    assert p == q
+    C_0, C_1, C_2, C_3 = symbols('C_0, C_1, C_2, C_3')
+    p = expr_to_holonomic(log(1+x**2))
+    q = [(HolonomicSequence(n**2 + (n**2 + 2*n)*Sn**2, [0, 0, C_2]), 0, 1)]
+    assert p.to_sequence() == q
+    p = p.diff()
+    q = [(HolonomicSequence((n + 2) + (n + 2)*Sn**2, [C_0, 0]), 1, 0)]
+    assert p.to_sequence() == q
+    p = expr_to_holonomic(erf(x) + x).to_sequence()
+    q = [(HolonomicSequence((2*n**2 - 2*n) + (n**3 + 2*n**2 - n - 2)*Sn**2, [0, 1 + 2/sqrt(pi), 0, C_3]), 0, 2)]
+    assert p == q
+
+def test_series():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx**2 + 2*x*Dx, x, 0, [0, 1]).series(n=10)
+    q = x - x**3/3 + x**5/10 - x**7/42 + x**9/216 + O(x**10)
+    assert p == q
+    p = HolonomicFunction(Dx - 1, x).composition(x**2, 0, [1])  # e^(x**2)
+    q = HolonomicFunction(Dx**2 + 1, x, 0, [1, 0])  # cos(x)
+    r = (p * q).series(n=10)  # expansion of cos(x) * exp(x**2)
+    s = 1 + x**2/2 + x**4/24 - 31*x**6/720 - 179*x**8/8064 + O(x**10)
+    assert r == s
+    t = HolonomicFunction((1 + x)*Dx**2 + Dx, x, 0, [0, 1])  # log(1 + x)
+    r = (p * t + q).series(n=10)
+    s = 1 + x - x**2 + 4*x**3/3 - 17*x**4/24 + 31*x**5/30 - 481*x**6/720 +\
+     71*x**7/105 - 20159*x**8/40320 + 379*x**9/840 + O(x**10)
+    assert r == s
+    p = HolonomicFunction((6+6*x-3*x**2) - (10*x-3*x**2-3*x**3)*Dx + \
+        (4-6*x**3+2*x**4)*Dx**2, x, 0, [0, 1]).series(n=7)
+    q = x + x**3/6 - 3*x**4/16 + x**5/20 - 23*x**6/960 + O(x**7)
+    assert p == q
+    p = HolonomicFunction((6+6*x-3*x**2) - (10*x-3*x**2-3*x**3)*Dx + \
+        (4-6*x**3+2*x**4)*Dx**2, x, 0, [1, 0]).series(n=7)
+    q = 1 - 3*x**2/4 - x**3/4 - 5*x**4/32 - 3*x**5/40 - 17*x**6/384 + O(x**7)
+    assert p == q
+    p = expr_to_holonomic(erf(x) + x).series(n=10)
+    C_3 = symbols('C_3')
+    q = (erf(x) + x).series(n=10)
+    assert p.subs(C_3, -2/(3*sqrt(pi))) == q
+    assert expr_to_holonomic(sqrt(x**3 + x)).series(n=10) == sqrt(x**3 + x).series(n=10)
+    assert expr_to_holonomic((2*x - 3*x**2)**Rational(1, 3)).series() == ((2*x - 3*x**2)**Rational(1, 3)).series()
+    assert  expr_to_holonomic(sqrt(x**2-x)).series() == (sqrt(x**2-x)).series()
+    assert expr_to_holonomic(cos(x)**2/x**2, y0={-2: [1, 0, -1]}).series(n=10) == (cos(x)**2/x**2).series(n=10)
+    assert expr_to_holonomic(cos(x)**2/x**2, x0=1).series(n=10).together() == (cos(x)**2/x**2).series(n=10, x0=1).together()
+    assert expr_to_holonomic(cos(x-1)**2/(x-1)**2, x0=1, y0={-2: [1, 0, -1]}).series(n=10) \
+        == (cos(x-1)**2/(x-1)**2).series(x0=1, n=10)
+
+def test_evalf_euler():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+
+    # log(1+x)
+    p = HolonomicFunction((1 + x)*Dx**2 + Dx, x, 0, [0, 1])
+
+    # path taken is a straight line from 0 to 1, on the real axis
+    r = [0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1]
+    s = '0.699525841805253'  # approx. equal to log(2) i.e. 0.693147180559945
+    assert sstr(p.evalf(r, method='Euler')[-1]) == s
+
+    # path taken is a triangle 0-->1+i-->2
+    r = [0.1 + 0.1*I]
+    for i in range(9):
+        r.append(r[-1]+0.1+0.1*I)
+    for i in range(10):
+        r.append(r[-1]+0.1-0.1*I)
+
+    # close to the exact solution 1.09861228866811
+    # imaginary part also close to zero
+    s = '1.07530466271334 - 0.0251200594793912*I'
+    assert sstr(p.evalf(r, method='Euler')[-1]) == s
+
+    # sin(x)
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [0, 1])
+    s = '0.905546532085401 - 6.93889390390723e-18*I'
+    assert sstr(p.evalf(r, method='Euler')[-1]) == s
+
+    # computing sin(pi/2) using this method
+    # using a linear path from 0 to pi/2
+    r = [0.1]
+    for i in range(14):
+        r.append(r[-1] + 0.1)
+    r.append(pi/2)
+    s = '1.08016557252834' # close to 1.0 (exact solution)
+    assert sstr(p.evalf(r, method='Euler')[-1]) == s
+
+    # trying different path, a rectangle (0-->i-->pi/2 + i-->pi/2)
+    # computing the same value sin(pi/2) using different path
+    r = [0.1*I]
+    for i in range(9):
+        r.append(r[-1]+0.1*I)
+    for i in range(15):
+        r.append(r[-1]+0.1)
+    r.append(pi/2+I)
+    for i in range(10):
+        r.append(r[-1]-0.1*I)
+
+    # close to 1.0
+    s = '0.976882381836257 - 1.65557671738537e-16*I'
+    assert sstr(p.evalf(r, method='Euler')[-1]) == s
+
+    # cos(x)
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [1, 0])
+    # compute cos(pi) along 0-->pi
+    r = [0.05]
+    for i in range(61):
+        r.append(r[-1]+0.05)
+    r.append(pi)
+    # close to -1 (exact answer)
+    s = '-1.08140824719196'
+    assert sstr(p.evalf(r, method='Euler')[-1]) == s
+
+    # a rectangular path (0 -> i -> 2+i -> 2)
+    r = [0.1*I]
+    for i in range(9):
+        r.append(r[-1]+0.1*I)
+    for i in range(20):
+        r.append(r[-1]+0.1)
+    for i in range(10):
+        r.append(r[-1]-0.1*I)
+
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [1,1]).evalf(r, method='Euler')
+    s = '0.501421652861245 - 3.88578058618805e-16*I'
+    assert sstr(p[-1]) == s
+
+def test_evalf_rk4():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+
+    # log(1+x)
+    p = HolonomicFunction((1 + x)*Dx**2 + Dx, x, 0, [0, 1])
+
+    # path taken is a straight line from 0 to 1, on the real axis
+    r = [0.1, 0.2, 0.3, 0.4, 0.5, 0.6, 0.7, 0.8, 0.9, 1]
+    s = '0.693146363174626'  # approx. equal to log(2) i.e. 0.693147180559945
+    assert sstr(p.evalf(r)[-1]) == s
+
+    # path taken is a triangle 0-->1+i-->2
+    r = [0.1 + 0.1*I]
+    for i in range(9):
+        r.append(r[-1]+0.1+0.1*I)
+    for i in range(10):
+        r.append(r[-1]+0.1-0.1*I)
+
+    # close to the exact solution 1.09861228866811
+    # imaginary part also close to zero
+    s = '1.098616 + 1.36083e-7*I'
+    assert sstr(p.evalf(r)[-1].n(7)) == s
+
+    # sin(x)
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [0, 1])
+    s = '0.90929463522785 + 1.52655665885959e-16*I'
+    assert sstr(p.evalf(r)[-1]) == s
+
+    # computing sin(pi/2) using this method
+    # using a linear path from 0 to pi/2
+    r = [0.1]
+    for i in range(14):
+        r.append(r[-1] + 0.1)
+    r.append(pi/2)
+    s = '0.999999895088917' # close to 1.0 (exact solution)
+    assert sstr(p.evalf(r)[-1]) == s
+
+    # trying different path, a rectangle (0-->i-->pi/2 + i-->pi/2)
+    # computing the same value sin(pi/2) using different path
+    r = [0.1*I]
+    for i in range(9):
+        r.append(r[-1]+0.1*I)
+    for i in range(15):
+        r.append(r[-1]+0.1)
+    r.append(pi/2+I)
+    for i in range(10):
+        r.append(r[-1]-0.1*I)
+
+    # close to 1.0
+    s = '1.00000003415141 + 6.11940487991086e-16*I'
+    assert sstr(p.evalf(r)[-1]) == s
+
+    # cos(x)
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [1, 0])
+    # compute cos(pi) along 0-->pi
+    r = [0.05]
+    for i in range(61):
+        r.append(r[-1]+0.05)
+    r.append(pi)
+    # close to -1 (exact answer)
+    s = '-0.999999993238714'
+    assert sstr(p.evalf(r)[-1]) == s
+
+    # a rectangular path (0 -> i -> 2+i -> 2)
+    r = [0.1*I]
+    for i in range(9):
+        r.append(r[-1]+0.1*I)
+    for i in range(20):
+        r.append(r[-1]+0.1)
+    for i in range(10):
+        r.append(r[-1]-0.1*I)
+
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [1,1]).evalf(r)
+    s = '0.493152791638442 - 1.41553435639707e-15*I'
+    assert sstr(p[-1]) == s
+
+
+def test_expr_to_holonomic():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    p = expr_to_holonomic((sin(x)/x)**2)
+    q = HolonomicFunction(8*x + (4*x**2 + 6)*Dx + 6*x*Dx**2 + x**2*Dx**3, x, 0, \
+        [1, 0, Rational(-2, 3)])
+    assert p == q
+    p = expr_to_holonomic(1/(1+x**2)**2)
+    q = HolonomicFunction(4*x + (x**2 + 1)*Dx, x, 0, [1])
+    assert p == q
+    p = expr_to_holonomic(exp(x)*sin(x)+x*log(1+x))
+    q = HolonomicFunction((2*x**3 + 10*x**2 + 20*x + 18) + (-2*x**4 - 10*x**3 - 20*x**2 \
+        - 18*x)*Dx + (2*x**5 + 6*x**4 + 7*x**3 + 8*x**2 + 10*x - 4)*Dx**2 + \
+        (-2*x**5 - 5*x**4 - 2*x**3 + 2*x**2 - x + 4)*Dx**3 + (x**5 + 2*x**4 - x**3 - \
+        7*x**2/2 + x + Rational(5, 2))*Dx**4, x, 0, [0, 1, 4, -1])
+    assert p == q
+    p = expr_to_holonomic(x*exp(x)+cos(x)+1)
+    q = HolonomicFunction((-x - 3)*Dx + (x + 2)*Dx**2 + (-x - 3)*Dx**3 + (x + 2)*Dx**4, x, \
+        0, [2, 1, 1, 3])
+    assert p == q
+    assert (x*exp(x)+cos(x)+1).series(n=10) == p.series(n=10)
+    p = expr_to_holonomic(log(1 + x)**2 + 1)
+    q = HolonomicFunction(Dx + (3*x + 3)*Dx**2 + (x**2 + 2*x + 1)*Dx**3, x, 0, [1, 0, 2])
+    assert p == q
+    p = expr_to_holonomic(erf(x)**2 + x)
+    q = HolonomicFunction((8*x**4 - 2*x**2 + 2)*Dx**2 + (6*x**3 - x/2)*Dx**3 + \
+        (x**2+ Rational(1, 4))*Dx**4, x, 0, [0, 1, 8/pi, 0])
+    assert p == q
+    p = expr_to_holonomic(cosh(x)*x)
+    q = HolonomicFunction((-x**2 + 2) -2*x*Dx + x**2*Dx**2, x, 0, [0, 1])
+    assert p == q
+    p = expr_to_holonomic(besselj(2, x))
+    q = HolonomicFunction((x**2 - 4) + x*Dx + x**2*Dx**2, x, 0, [0, 0])
+    assert p == q
+    p = expr_to_holonomic(besselj(0, x) + exp(x))
+    q = HolonomicFunction((-x**2 - x/2 + S.Half) + (x**2 - x/2 - Rational(3, 2))*Dx + (-x**2 + x/2 + 1)*Dx**2 +\
+        (x**2 + x/2)*Dx**3, x, 0, [2, 1, S.Half])
+    assert p == q
+    p = expr_to_holonomic(sin(x)**2/x)
+    q = HolonomicFunction(4 + 4*x*Dx + 3*Dx**2 + x*Dx**3, x, 0, [0, 1, 0])
+    assert p == q
+    p = expr_to_holonomic(sin(x)**2/x, x0=2)
+    q = HolonomicFunction((4) + (4*x)*Dx + (3)*Dx**2 + (x)*Dx**3, x, 2, [sin(2)**2/2,
+        sin(2)*cos(2) - sin(2)**2/4, -3*sin(2)**2/4 + cos(2)**2 - sin(2)*cos(2)])
+    assert p == q
+    p = expr_to_holonomic(log(x)/2 - Ci(2*x)/2 + Ci(2)/2)
+    q = HolonomicFunction(4*Dx + 4*x*Dx**2 + 3*Dx**3 + x*Dx**4, x, 0, \
+        [-log(2)/2 - EulerGamma/2 + Ci(2)/2, 0, 1, 0])
+    assert p == q
+    p = p.to_expr()
+    q = log(x)/2 - Ci(2*x)/2 + Ci(2)/2
+    assert p == q
+    p = expr_to_holonomic(x**S.Half, x0=1)
+    q = HolonomicFunction(x*Dx - S.Half, x, 1, [1])
+    assert p == q
+    p = expr_to_holonomic(sqrt(1 + x**2))
+    q = HolonomicFunction((-x) + (x**2 + 1)*Dx, x, 0, [1])
+    assert p == q
+    assert (expr_to_holonomic(sqrt(x) + sqrt(2*x)).to_expr()-\
+        (sqrt(x) + sqrt(2*x))).simplify() == 0
+    assert expr_to_holonomic(3*x+2*sqrt(x)).to_expr() == 3*x+2*sqrt(x)
+    p = expr_to_holonomic((x**4+x**3+5*x**2+3*x+2)/x**2, lenics=3)
+    q = HolonomicFunction((-2*x**4 - x**3 + 3*x + 4) + (x**5 + x**4 + 5*x**3 + 3*x**2 + \
+        2*x)*Dx, x, 0, {-2: [2, 3, 5]})
+    assert p == q
+    p = expr_to_holonomic(1/(x-1)**2, lenics=3, x0=1)
+    q = HolonomicFunction((2) + (x - 1)*Dx, x, 1, {-2: [1, 0, 0]})
+    assert p == q
+    a = symbols("a")
+    p = expr_to_holonomic(sqrt(a*x), x=x)
+    assert p.to_expr() == sqrt(a)*sqrt(x)
+
+def test_to_hyper():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx - 2, x, 0, [3]).to_hyper()
+    q = 3 * hyper([], [], 2*x)
+    assert p == q
+    p = hyperexpand(HolonomicFunction((1 + x) * Dx - 3, x, 0, [2]).to_hyper()).expand()
+    q = 2*x**3 + 6*x**2 + 6*x + 2
+    assert p == q
+    p = HolonomicFunction((1 + x)*Dx**2 + Dx, x, 0, [0, 1]).to_hyper()
+    q = -x**2*hyper((2, 2, 1), (3, 2), -x)/2 + x
+    assert p == q
+    p = HolonomicFunction(2*x*Dx + Dx**2, x, 0, [0, 2/sqrt(pi)]).to_hyper()
+    q = 2*x*hyper((S.Half,), (Rational(3, 2),), -x**2)/sqrt(pi)
+    assert p == q
+    p = hyperexpand(HolonomicFunction(2*x*Dx + Dx**2, x, 0, [1, -2/sqrt(pi)]).to_hyper())
+    q = erfc(x)
+    assert p.rewrite(erfc) == q
+    p =  hyperexpand(HolonomicFunction((x**2 - 1) + x*Dx + x**2*Dx**2,
+        x, 0, [0, S.Half]).to_hyper())
+    q = besselj(1, x)
+    assert p == q
+    p = hyperexpand(HolonomicFunction(x*Dx**2 + Dx + x, x, 0, [1, 0]).to_hyper())
+    q = besselj(0, x)
+    assert p == q
+
+def test_to_expr():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(Dx - 1, x, 0, [1]).to_expr()
+    q = exp(x)
+    assert p == q
+    p = HolonomicFunction(Dx**2 + 1, x, 0, [1, 0]).to_expr()
+    q = cos(x)
+    assert p == q
+    p = HolonomicFunction(Dx**2 - 1, x, 0, [1, 0]).to_expr()
+    q = cosh(x)
+    assert p == q
+    p = HolonomicFunction(2 + (4*x - 1)*Dx + \
+        (x**2 - x)*Dx**2, x, 0, [1, 2]).to_expr().expand()
+    q = 1/(x**2 - 2*x + 1)
+    assert p == q
+    p = expr_to_holonomic(sin(x)**2/x).integrate((x, 0, x)).to_expr()
+    q = (sin(x)**2/x).integrate((x, 0, x))
+    assert p == q
+    C_0, C_1, C_2, C_3 = symbols('C_0, C_1, C_2, C_3')
+    p = expr_to_holonomic(log(1+x**2)).to_expr()
+    q = C_2*log(x**2 + 1)
+    assert p == q
+    p = expr_to_holonomic(log(1+x**2)).diff().to_expr()
+    q = C_0*x/(x**2 + 1)
+    assert p == q
+    p = expr_to_holonomic(erf(x) + x).to_expr()
+    q = 3*C_3*x - 3*sqrt(pi)*C_3*erf(x)/2 + x + 2*x/sqrt(pi)
+    assert p == q
+    p = expr_to_holonomic(sqrt(x), x0=1).to_expr()
+    assert p == sqrt(x)
+    assert expr_to_holonomic(sqrt(x)).to_expr() == sqrt(x)
+    p = expr_to_holonomic(sqrt(1 + x**2)).to_expr()
+    assert p == sqrt(1+x**2)
+    p = expr_to_holonomic((2*x**2 + 1)**Rational(2, 3)).to_expr()
+    assert p == (2*x**2 + 1)**Rational(2, 3)
+    p = expr_to_holonomic(sqrt(-x**2+2*x)).to_expr()
+    assert p == sqrt(x)*sqrt(-x + 2)
+    p = expr_to_holonomic((-2*x**3+7*x)**Rational(2, 3)).to_expr()
+    q = x**Rational(2, 3)*(-2*x**2 + 7)**Rational(2, 3)
+    assert p == q
+    p = from_hyper(hyper((-2, -3), (S.Half, ), x))
+    s = hyperexpand(hyper((-2, -3), (S.Half, ), x))
+    D_0 = Symbol('D_0')
+    C_0 = Symbol('C_0')
+    assert (p.to_expr().subs({C_0:1, D_0:0}) - s).simplify() == 0
+    p.y0 = {0: [1], S.Half: [0]}
+    assert p.to_expr() == s
+    assert expr_to_holonomic(x**5).to_expr() == x**5
+    assert expr_to_holonomic(2*x**3-3*x**2).to_expr().expand() == \
+        2*x**3-3*x**2
+    a = symbols("a")
+    p = (expr_to_holonomic(1.4*x)*expr_to_holonomic(a*x, x)).to_expr()
+    q = 1.4*a*x**2
+    assert p == q
+    p = (expr_to_holonomic(1.4*x)+expr_to_holonomic(a*x, x)).to_expr()
+    q = x*(a + 1.4)
+    assert p == q
+    p = (expr_to_holonomic(1.4*x)+expr_to_holonomic(x)).to_expr()
+    assert p == 2.4*x
+
+
+def test_integrate():
+    x = symbols('x')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = expr_to_holonomic(sin(x)**2/x, x0=1).integrate((x, 2, 3))
+    q = '0.166270406994788'
+    assert sstr(p) == q
+    p = expr_to_holonomic(sin(x)).integrate((x, 0, x)).to_expr()
+    q = 1 - cos(x)
+    assert p == q
+    p = expr_to_holonomic(sin(x)).integrate((x, 0, 3))
+    q = 1 - cos(3)
+    assert p == q
+    p = expr_to_holonomic(sin(x)/x, x0=1).integrate((x, 1, 2))
+    q = '0.659329913368450'
+    assert sstr(p) == q
+    p = expr_to_holonomic(sin(x)**2/x, x0=1).integrate((x, 1, 0))
+    q = '-0.423690480850035'
+    assert sstr(p) == q
+    p = expr_to_holonomic(sin(x)/x)
+    assert p.integrate(x).to_expr() == Si(x)
+    assert p.integrate((x, 0, 2)) == Si(2)
+    p = expr_to_holonomic(sin(x)**2/x)
+    q = p.to_expr()
+    assert p.integrate(x).to_expr() == q.integrate((x, 0, x))
+    assert p.integrate((x, 0, 1)) == q.integrate((x, 0, 1))
+    assert expr_to_holonomic(1/x, x0=1).integrate(x).to_expr() == log(x)
+    p = expr_to_holonomic((x + 1)**3*exp(-x), x0=-1).integrate(x).to_expr()
+    q = (-x**3 - 6*x**2 - 15*x + 6*exp(x + 1) - 16)*exp(-x)
+    assert p == q
+    p = expr_to_holonomic(cos(x)**2/x**2, y0={-2: [1, 0, -1]}).integrate(x).to_expr()
+    q = -Si(2*x) - cos(x)**2/x
+    assert p == q
+    p = expr_to_holonomic(sqrt(x**2+x)).integrate(x).to_expr()
+    q = (x**Rational(3, 2)*(2*x**2 + 3*x + 1) - x*sqrt(x + 1)*asinh(sqrt(x)))/(4*x*sqrt(x + 1))
+    assert p == q
+    p = expr_to_holonomic(sqrt(x**2+1)).integrate(x).to_expr()
+    q = (sqrt(x**2+1)).integrate(x)
+    assert (p-q).simplify() == 0
+    p = expr_to_holonomic(1/x**2, y0={-2:[1, 0, 0]})
+    r = expr_to_holonomic(1/x**2, lenics=3)
+    assert p == r
+    q = expr_to_holonomic(cos(x)**2)
+    assert (r*q).integrate(x).to_expr() == -Si(2*x) - cos(x)**2/x
+
+
+def test_diff():
+    x, y = symbols('x, y')
+    R, Dx = DifferentialOperators(ZZ.old_poly_ring(x), 'Dx')
+    p = HolonomicFunction(x*Dx**2 + 1, x, 0, [0, 1])
+    assert p.diff().to_expr() == p.to_expr().diff().simplify()
+    p = HolonomicFunction(Dx**2 - 1, x, 0, [1, 0])
+    assert p.diff(x, 2).to_expr() == p.to_expr()
+    p = expr_to_holonomic(Si(x))
+    assert p.diff().to_expr() == sin(x)/x
+    assert p.diff(y) == 0
+    C_0, C_1, C_2, C_3 = symbols('C_0, C_1, C_2, C_3')
+    q = Si(x)
+    assert p.diff(x).to_expr() == q.diff()
+    assert p.diff(x, 2).to_expr().subs(C_0, Rational(-1, 3)).cancel() == q.diff(x, 2).cancel()
+    assert p.diff(x, 3).series().subs({C_3: Rational(-1, 3), C_0: 0}) == q.diff(x, 3).series()
+
+
+def test_extended_domain_in_expr_to_holonomic():
+    x = symbols('x')
+    p = expr_to_holonomic(1.2*cos(3.1*x))
+    assert p.to_expr() == 1.2*cos(3.1*x)
+    assert sstr(p.integrate(x).to_expr()) == '0.387096774193548*sin(3.1*x)'
+    _, Dx = DifferentialOperators(RR.old_poly_ring(x), 'Dx')
+    p = expr_to_holonomic(1.1329138213*x)
+    q = HolonomicFunction((-1.1329138213) + (1.1329138213*x)*Dx, x, 0, {1: [1.1329138213]})
+    assert p == q
+    assert p.to_expr() == 1.1329138213*x
+    assert sstr(p.integrate((x, 1, 2))) == sstr((1.1329138213*x).integrate((x, 1, 2)))
+    y, z = symbols('y, z')
+    p = expr_to_holonomic(sin(x*y*z), x=x)
+    assert p.to_expr() == sin(x*y*z)
+    assert p.integrate(x).to_expr() == (-cos(x*y*z) + 1)/(y*z)
+    p = expr_to_holonomic(sin(x*y + z), x=x).integrate(x).to_expr()
+    q = (cos(z) - cos(x*y + z))/y
+    assert p == q
+    a = symbols('a')
+    p = expr_to_holonomic(a*x, x)
+    assert p.to_expr() == a*x
+    assert p.integrate(x).to_expr() == a*x**2/2
+    D_2, C_1 = symbols("D_2, C_1")
+    p = expr_to_holonomic(x) + expr_to_holonomic(1.2*cos(x))
+    p = p.to_expr().subs(D_2, 0)
+    assert p - x - 1.2*cos(1.0*x) == 0
+    p = expr_to_holonomic(x) * expr_to_holonomic(1.2*cos(x))
+    p = p.to_expr().subs(C_1, 0)
+    assert p - 1.2*x*cos(1.0*x) == 0
+
+
+def test_to_meijerg():
+    x = symbols('x')
+    assert hyperexpand(expr_to_holonomic(sin(x)).to_meijerg()) == sin(x)
+    assert hyperexpand(expr_to_holonomic(cos(x)).to_meijerg()) == cos(x)
+    assert hyperexpand(expr_to_holonomic(exp(x)).to_meijerg()) == exp(x)
+    assert hyperexpand(expr_to_holonomic(log(x)).to_meijerg()).simplify() == log(x)
+    assert expr_to_holonomic(4*x**2/3 + 7).to_meijerg() == 4*x**2/3 + 7
+    assert hyperexpand(expr_to_holonomic(besselj(2, x), lenics=3).to_meijerg()) == besselj(2, x)
+    p = hyper((Rational(-1, 2), -3), (), x)
+    assert from_hyper(p).to_meijerg() == hyperexpand(p)
+    p = hyper((S.One, S(3)), (S(2), ), x)
+    assert (hyperexpand(from_hyper(p).to_meijerg()) - hyperexpand(p)).expand() == 0
+    p = from_hyper(hyper((-2, -3), (S.Half, ), x))
+    s = hyperexpand(hyper((-2, -3), (S.Half, ), x))
+    C_0 = Symbol('C_0')
+    C_1 = Symbol('C_1')
+    D_0 = Symbol('D_0')
+    assert (hyperexpand(p.to_meijerg()).subs({C_0:1, D_0:0}) - s).simplify() == 0
+    p.y0 = {0: [1], S.Half: [0]}
+    assert (hyperexpand(p.to_meijerg()) - s).simplify() == 0
+    p = expr_to_holonomic(besselj(S.Half, x), initcond=False)
+    assert (p.to_expr() - (D_0*sin(x) + C_0*cos(x) + C_1*sin(x))/sqrt(x)).simplify() == 0
+    p = expr_to_holonomic(besselj(S.Half, x), y0={Rational(-1, 2): [sqrt(2)/sqrt(pi), sqrt(2)/sqrt(pi)]})
+    assert (p.to_expr() - besselj(S.Half, x) - besselj(Rational(-1, 2), x)).simplify() == 0
+
+
+def test_gaussian():
+    mu, x = symbols("mu x")
+    sd = symbols("sd", positive=True)
+    Q = QQ[mu, sd].get_field()
+    e = sqrt(2)*exp(-(-mu + x)**2/(2*sd**2))/(2*sqrt(pi)*sd)
+    h1 = expr_to_holonomic(e, x, domain=Q)
+
+    _, Dx = DifferentialOperators(Q.old_poly_ring(x), 'Dx')
+    h2 = HolonomicFunction((-mu/sd**2 + x/sd**2) + (1)*Dx, x)
+
+    assert h1 == h2
+
+
+def test_beta():
+    a, b, x = symbols("a b x", positive=True)
+    e = x**(a - 1)*(-x + 1)**(b - 1)/beta(a, b)
+    Q = QQ[a, b].get_field()
+    h1 = expr_to_holonomic(e, x, domain=Q)
+
+    _, Dx = DifferentialOperators(Q.old_poly_ring(x), 'Dx')
+    h2 = HolonomicFunction((a + x*(-a - b + 2) - 1) + (x**2 - x)*Dx, x)
+
+    assert h1 == h2
+
+
+def test_gamma():
+    a, b, x = symbols("a b x", positive=True)
+    e = b**(-a)*x**(a - 1)*exp(-x/b)/gamma(a)
+    Q = QQ[a, b].get_field()
+    h1 = expr_to_holonomic(e, x, domain=Q)
+
+    _, Dx = DifferentialOperators(Q.old_poly_ring(x), 'Dx')
+    h2 = HolonomicFunction((-a + 1 + x/b) + (x)*Dx, x)
+
+    assert h1 == h2
+
+
+def test_symbolic_power():
+    x, n = symbols("x n")
+    Q = QQ[n].get_field()
+    _, Dx = DifferentialOperators(Q.old_poly_ring(x), 'Dx')
+    h1 = HolonomicFunction((-1) + (x)*Dx, x) ** -n
+    h2 = HolonomicFunction((n) + (x)*Dx, x)
+
+    assert h1 == h2
+
+
+def test_negative_power():
+    x = symbols("x")
+    _, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    h1 = HolonomicFunction((-1) + (x)*Dx, x) ** -2
+    h2 = HolonomicFunction((2) + (x)*Dx, x)
+
+    assert h1 == h2
+
+
+def test_expr_in_power():
+    x, n = symbols("x n")
+    Q = QQ[n].get_field()
+    _, Dx = DifferentialOperators(Q.old_poly_ring(x), 'Dx')
+    h1 = HolonomicFunction((-1) + (x)*Dx, x) ** (n - 3)
+    h2 = HolonomicFunction((-n + 3) + (x)*Dx, x)
+
+    assert h1 == h2
+
+def test_DifferentialOperatorEqPoly():
+    x = symbols('x', integer=True)
+    R, Dx = DifferentialOperators(QQ.old_poly_ring(x), 'Dx')
+    do = DifferentialOperator([x**2, R.base.zero, R.base.zero], R)
+    do2 = DifferentialOperator([x**2, 1, x], R)
+    assert not do == do2
+
+    # polynomial comparison issue, see https://github.com/sympy/sympy/pull/15799
+    # should work once that is solved
+    # p = do.listofpoly[0]
+    # assert do == p
+
+    p2 = do2.listofpoly[0]
+    assert not do2 == p2

llmeval-env/lib/python3.10/site-packages/sympy/holonomic/tests/test_recurrence.py

@@ -0,0 +1,29 @@
+from sympy.holonomic.recurrence import RecurrenceOperators, RecurrenceOperator
+from sympy.core.symbol import symbols
+from sympy.polys.domains.rationalfield import QQ
+
+def test_RecurrenceOperator():
+    n = symbols('n', integer=True)
+    R, Sn = RecurrenceOperators(QQ.old_poly_ring(n), 'Sn')
+    assert Sn*n == (n + 1)*Sn
+    assert Sn*n**2 == (n**2+1+2*n)*Sn
+    assert Sn**2*n**2 == (n**2 + 4*n + 4)*Sn**2
+    p = (Sn**3*n**2 + Sn*n)**2
+    q = (n**2 + 3*n + 2)*Sn**2 + (2*n**3 + 19*n**2 + 57*n + 52)*Sn**4 + (n**4 + 18*n**3 + \
+        117*n**2 + 324*n + 324)*Sn**6
+    assert p == q
+
+def test_RecurrenceOperatorEqPoly():
+    n = symbols('n', integer=True)
+    R, Sn = RecurrenceOperators(QQ.old_poly_ring(n), 'Sn')
+    rr = RecurrenceOperator([n**2, 0, 0], R)
+    rr2 = RecurrenceOperator([n**2, 1, n], R)
+    assert not rr == rr2
+
+    # polynomial comparison issue, see https://github.com/sympy/sympy/pull/15799
+    # should work once that is solved
+    # d = rr.listofpoly[0]
+    # assert rr == d
+
+    d2 = rr2.listofpoly[0]
+    assert not rr2 == d2