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llmeval-env/lib/python3.10/site-packages/scipy/constants/__init__.py

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+r"""
+==================================
+Constants (:mod:`scipy.constants`)
+==================================
+
+.. currentmodule:: scipy.constants
+
+Physical and mathematical constants and units.
+
+
+Mathematical constants
+======================
+
+================  =================================================================
+``pi``            Pi
+``golden``        Golden ratio
+``golden_ratio``  Golden ratio
+================  =================================================================
+
+
+Physical constants
+==================
+
+===========================  =================================================================
+``c``                        speed of light in vacuum
+``speed_of_light``           speed of light in vacuum
+``mu_0``                     the magnetic constant :math:`\mu_0`
+``epsilon_0``                the electric constant (vacuum permittivity), :math:`\epsilon_0`
+``h``                        the Planck constant :math:`h`
+``Planck``                   the Planck constant :math:`h`
+``hbar``                     :math:`\hbar = h/(2\pi)`
+``G``                        Newtonian constant of gravitation
+``gravitational_constant``   Newtonian constant of gravitation
+``g``                        standard acceleration of gravity
+``e``                        elementary charge
+``elementary_charge``        elementary charge
+``R``                        molar gas constant
+``gas_constant``             molar gas constant
+``alpha``                    fine-structure constant
+``fine_structure``           fine-structure constant
+``N_A``                      Avogadro constant
+``Avogadro``                 Avogadro constant
+``k``                        Boltzmann constant
+``Boltzmann``                Boltzmann constant
+``sigma``                    Stefan-Boltzmann constant :math:`\sigma`
+``Stefan_Boltzmann``         Stefan-Boltzmann constant :math:`\sigma`
+``Wien``                     Wien displacement law constant
+``Rydberg``                  Rydberg constant
+``m_e``                      electron mass
+``electron_mass``            electron mass
+``m_p``                      proton mass
+``proton_mass``              proton mass
+``m_n``                      neutron mass
+``neutron_mass``             neutron mass
+===========================  =================================================================
+
+
+Constants database
+------------------
+
+In addition to the above variables, :mod:`scipy.constants` also contains the
+2018 CODATA recommended values [CODATA2018]_ database containing more physical
+constants.
+
+.. autosummary::
+   :toctree: generated/
+
+   value      -- Value in physical_constants indexed by key
+   unit       -- Unit in physical_constants indexed by key
+   precision  -- Relative precision in physical_constants indexed by key
+   find       -- Return list of physical_constant keys with a given string
+   ConstantWarning -- Constant sought not in newest CODATA data set
+
+.. data:: physical_constants
+
+   Dictionary of physical constants, of the format
+   ``physical_constants[name] = (value, unit, uncertainty)``.
+
+Available constants:
+
+======================================================================  ====
+%(constant_names)s
+======================================================================  ====
+
+
+Units
+=====
+
+SI prefixes
+-----------
+
+============  =================================================================
+``quetta``    :math:`10^{30}`
+``ronna``     :math:`10^{27}`
+``yotta``     :math:`10^{24}`
+``zetta``     :math:`10^{21}`
+``exa``       :math:`10^{18}`
+``peta``      :math:`10^{15}`
+``tera``      :math:`10^{12}`
+``giga``      :math:`10^{9}`
+``mega``      :math:`10^{6}`
+``kilo``      :math:`10^{3}`
+``hecto``     :math:`10^{2}`
+``deka``      :math:`10^{1}`
+``deci``      :math:`10^{-1}`
+``centi``     :math:`10^{-2}`
+``milli``     :math:`10^{-3}`
+``micro``     :math:`10^{-6}`
+``nano``      :math:`10^{-9}`
+``pico``      :math:`10^{-12}`
+``femto``     :math:`10^{-15}`
+``atto``      :math:`10^{-18}`
+``zepto``     :math:`10^{-21}`
+``yocto``     :math:`10^{-24}`
+``ronto``     :math:`10^{-27}`
+``quecto``    :math:`10^{-30}`
+============  =================================================================
+
+Binary prefixes
+---------------
+
+============  =================================================================
+``kibi``      :math:`2^{10}`
+``mebi``      :math:`2^{20}`
+``gibi``      :math:`2^{30}`
+``tebi``      :math:`2^{40}`
+``pebi``      :math:`2^{50}`
+``exbi``      :math:`2^{60}`
+``zebi``      :math:`2^{70}`
+``yobi``      :math:`2^{80}`
+============  =================================================================
+
+Mass
+----
+
+=================  ============================================================
+``gram``           :math:`10^{-3}` kg
+``metric_ton``     :math:`10^{3}` kg
+``grain``          one grain in kg
+``lb``             one pound (avoirdupous) in kg
+``pound``          one pound (avoirdupous) in kg
+``blob``           one inch version of a slug in kg (added in 1.0.0)
+``slinch``         one inch version of a slug in kg (added in 1.0.0)
+``slug``           one slug in kg (added in 1.0.0)
+``oz``             one ounce in kg
+``ounce``          one ounce in kg
+``stone``          one stone in kg
+``grain``          one grain in kg
+``long_ton``       one long ton in kg
+``short_ton``      one short ton in kg
+``troy_ounce``     one Troy ounce in kg
+``troy_pound``     one Troy pound in kg
+``carat``          one carat in kg
+``m_u``            atomic mass constant (in kg)
+``u``              atomic mass constant (in kg)
+``atomic_mass``    atomic mass constant (in kg)
+=================  ============================================================
+
+Angle
+-----
+
+=================  ============================================================
+``degree``         degree in radians
+``arcmin``         arc minute in radians
+``arcminute``      arc minute in radians
+``arcsec``         arc second in radians
+``arcsecond``      arc second in radians
+=================  ============================================================
+
+
+Time
+----
+
+=================  ============================================================
+``minute``         one minute in seconds
+``hour``           one hour in seconds
+``day``            one day in seconds
+``week``           one week in seconds
+``year``           one year (365 days) in seconds
+``Julian_year``    one Julian year (365.25 days) in seconds
+=================  ============================================================
+
+
+Length
+------
+
+=====================  ============================================================
+``inch``               one inch in meters
+``foot``               one foot in meters
+``yard``               one yard in meters
+``mile``               one mile in meters
+``mil``                one mil in meters
+``pt``                 one point in meters
+``point``              one point in meters
+``survey_foot``        one survey foot in meters
+``survey_mile``        one survey mile in meters
+``nautical_mile``      one nautical mile in meters
+``fermi``              one Fermi in meters
+``angstrom``           one Angstrom in meters
+``micron``             one micron in meters
+``au``                 one astronomical unit in meters
+``astronomical_unit``  one astronomical unit in meters
+``light_year``         one light year in meters
+``parsec``             one parsec in meters
+=====================  ============================================================
+
+Pressure
+--------
+
+=================  ============================================================
+``atm``            standard atmosphere in pascals
+``atmosphere``     standard atmosphere in pascals
+``bar``            one bar in pascals
+``torr``           one torr (mmHg) in pascals
+``mmHg``           one torr (mmHg) in pascals
+``psi``            one psi in pascals
+=================  ============================================================
+
+Area
+----
+
+=================  ============================================================
+``hectare``        one hectare in square meters
+``acre``           one acre in square meters
+=================  ============================================================
+
+
+Volume
+------
+
+===================    ========================================================
+``liter``              one liter in cubic meters
+``litre``              one liter in cubic meters
+``gallon``             one gallon (US) in cubic meters
+``gallon_US``          one gallon (US) in cubic meters
+``gallon_imp``         one gallon (UK) in cubic meters
+``fluid_ounce``        one fluid ounce (US) in cubic meters
+``fluid_ounce_US``     one fluid ounce (US) in cubic meters
+``fluid_ounce_imp``    one fluid ounce (UK) in cubic meters
+``bbl``                one barrel in cubic meters
+``barrel``             one barrel in cubic meters
+===================    ========================================================
+
+Speed
+-----
+
+==================    ==========================================================
+``kmh``               kilometers per hour in meters per second
+``mph``               miles per hour in meters per second
+``mach``              one Mach (approx., at 15 C, 1 atm) in meters per second
+``speed_of_sound``    one Mach (approx., at 15 C, 1 atm) in meters per second
+``knot``              one knot in meters per second
+==================    ==========================================================
+
+
+Temperature
+-----------
+
+=====================  =======================================================
+``zero_Celsius``       zero of Celsius scale in Kelvin
+``degree_Fahrenheit``  one Fahrenheit (only differences) in Kelvins
+=====================  =======================================================
+
+.. autosummary::
+   :toctree: generated/
+
+   convert_temperature
+
+Energy
+------
+
+====================  =======================================================
+``eV``                one electron volt in Joules
+``electron_volt``     one electron volt in Joules
+``calorie``           one calorie (thermochemical) in Joules
+``calorie_th``        one calorie (thermochemical) in Joules
+``calorie_IT``        one calorie (International Steam Table calorie, 1956) in Joules
+``erg``               one erg in Joules
+``Btu``               one British thermal unit (International Steam Table) in Joules
+``Btu_IT``            one British thermal unit (International Steam Table) in Joules
+``Btu_th``            one British thermal unit (thermochemical) in Joules
+``ton_TNT``           one ton of TNT in Joules
+====================  =======================================================
+
+Power
+-----
+
+====================  =======================================================
+``hp``                one horsepower in watts
+``horsepower``        one horsepower in watts
+====================  =======================================================
+
+Force
+-----
+
+====================  =======================================================
+``dyn``               one dyne in newtons
+``dyne``              one dyne in newtons
+``lbf``               one pound force in newtons
+``pound_force``       one pound force in newtons
+``kgf``               one kilogram force in newtons
+``kilogram_force``    one kilogram force in newtons
+====================  =======================================================
+
+Optics
+------
+
+.. autosummary::
+   :toctree: generated/
+
+   lambda2nu
+   nu2lambda
+
+References
+==========
+
+.. [CODATA2018] CODATA Recommended Values of the Fundamental
+   Physical Constants 2018.
+
+   https://physics.nist.gov/cuu/Constants/
+
+"""  # noqa: E501
+# Modules contributed by BasSw ([email protected])
+from ._codata import *
+from ._constants import *
+from ._codata import _obsolete_constants, physical_constants
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import codata, constants
+
+_constant_names_list = [(_k.lower(), _k, _v)
+                        for _k, _v in physical_constants.items()
+                        if _k not in _obsolete_constants]
+_constant_names = "\n".join(["``{}``{}  {} {}".format(_x[1], " "*(66-len(_x[1])),
+                                                  _x[2][0], _x[2][1])
+                             for _x in sorted(_constant_names_list)])
+if __doc__:
+    __doc__ = __doc__ % dict(constant_names=_constant_names)
+
+del _constant_names
+del _constant_names_list
+
+__all__ = [s for s in dir() if not s.startswith('_')]
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

llmeval-env/lib/python3.10/site-packages/scipy/constants/_constants.py

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+"""
+Collection of physical constants and conversion factors.
+
+Most constants are in SI units, so you can do
+print '10 mile per minute is', 10*mile/minute, 'm/s or', 10*mile/(minute*knot), 'knots'
+
+The list is not meant to be comprehensive, but just convenient for everyday use.
+"""
+
+from __future__ import annotations
+
+import math as _math
+from typing import TYPE_CHECKING, Any
+
+from ._codata import value as _cd
+import numpy as _np
+
+if TYPE_CHECKING:
+    import numpy.typing as npt
+
+"""
+BasSw 2006
+physical constants: imported from CODATA
+unit conversion: see e.g., NIST special publication 811
+Use at own risk: double-check values before calculating your Mars orbit-insertion burn.
+Some constants exist in a few variants, which are marked with suffixes.
+The ones without any suffix should be the most common ones.
+"""
+
+__all__ = [
+    'Avogadro', 'Boltzmann', 'Btu', 'Btu_IT', 'Btu_th', 'G',
+    'Julian_year', 'N_A', 'Planck', 'R', 'Rydberg',
+    'Stefan_Boltzmann', 'Wien', 'acre', 'alpha',
+    'angstrom', 'arcmin', 'arcminute', 'arcsec',
+    'arcsecond', 'astronomical_unit', 'atm',
+    'atmosphere', 'atomic_mass', 'atto', 'au', 'bar',
+    'barrel', 'bbl', 'blob', 'c', 'calorie',
+    'calorie_IT', 'calorie_th', 'carat', 'centi',
+    'convert_temperature', 'day', 'deci', 'degree',
+    'degree_Fahrenheit', 'deka', 'dyn', 'dyne', 'e',
+    'eV', 'electron_mass', 'electron_volt',
+    'elementary_charge', 'epsilon_0', 'erg',
+    'exa', 'exbi', 'femto', 'fermi', 'fine_structure',
+    'fluid_ounce', 'fluid_ounce_US', 'fluid_ounce_imp',
+    'foot', 'g', 'gallon', 'gallon_US', 'gallon_imp',
+    'gas_constant', 'gibi', 'giga', 'golden', 'golden_ratio',
+    'grain', 'gram', 'gravitational_constant', 'h', 'hbar',
+    'hectare', 'hecto', 'horsepower', 'hour', 'hp',
+    'inch', 'k', 'kgf', 'kibi', 'kilo', 'kilogram_force',
+    'kmh', 'knot', 'lambda2nu', 'lb', 'lbf',
+    'light_year', 'liter', 'litre', 'long_ton', 'm_e',
+    'm_n', 'm_p', 'm_u', 'mach', 'mebi', 'mega',
+    'metric_ton', 'micro', 'micron', 'mil', 'mile',
+    'milli', 'minute', 'mmHg', 'mph', 'mu_0', 'nano',
+    'nautical_mile', 'neutron_mass', 'nu2lambda',
+    'ounce', 'oz', 'parsec', 'pebi', 'peta',
+    'pi', 'pico', 'point', 'pound', 'pound_force',
+    'proton_mass', 'psi', 'pt', 'quecto', 'quetta', 'ronna', 'ronto',
+    'short_ton', 'sigma', 'slinch', 'slug', 'speed_of_light',
+    'speed_of_sound', 'stone', 'survey_foot',
+    'survey_mile', 'tebi', 'tera', 'ton_TNT',
+    'torr', 'troy_ounce', 'troy_pound', 'u',
+    'week', 'yard', 'year', 'yobi', 'yocto',
+    'yotta', 'zebi', 'zepto', 'zero_Celsius', 'zetta'
+]
+
+
+# mathematical constants
+pi = _math.pi
+golden = golden_ratio = (1 + _math.sqrt(5)) / 2
+
+# SI prefixes
+quetta = 1e30
+ronna = 1e27
+yotta = 1e24
+zetta = 1e21
+exa = 1e18
+peta = 1e15
+tera = 1e12
+giga = 1e9
+mega = 1e6
+kilo = 1e3
+hecto = 1e2
+deka = 1e1
+deci = 1e-1
+centi = 1e-2
+milli = 1e-3
+micro = 1e-6
+nano = 1e-9
+pico = 1e-12
+femto = 1e-15
+atto = 1e-18
+zepto = 1e-21
+yocto = 1e-24
+ronto = 1e-27
+quecto = 1e-30
+
+# binary prefixes
+kibi = 2**10
+mebi = 2**20
+gibi = 2**30
+tebi = 2**40
+pebi = 2**50
+exbi = 2**60
+zebi = 2**70
+yobi = 2**80
+
+# physical constants
+c = speed_of_light = _cd('speed of light in vacuum')
+mu_0 = _cd('vacuum mag. permeability')
+epsilon_0 = _cd('vacuum electric permittivity')
+h = Planck = _cd('Planck constant')
+hbar = h / (2 * pi)
+G = gravitational_constant = _cd('Newtonian constant of gravitation')
+g = _cd('standard acceleration of gravity')
+e = elementary_charge = _cd('elementary charge')
+R = gas_constant = _cd('molar gas constant')
+alpha = fine_structure = _cd('fine-structure constant')
+N_A = Avogadro = _cd('Avogadro constant')
+k = Boltzmann = _cd('Boltzmann constant')
+sigma = Stefan_Boltzmann = _cd('Stefan-Boltzmann constant')
+Wien = _cd('Wien wavelength displacement law constant')
+Rydberg = _cd('Rydberg constant')
+
+# mass in kg
+gram = 1e-3
+metric_ton = 1e3
+grain = 64.79891e-6
+lb = pound = 7000 * grain  # avoirdupois
+blob = slinch = pound * g / 0.0254  # lbf*s**2/in (added in 1.0.0)
+slug = blob / 12  # lbf*s**2/foot (added in 1.0.0)
+oz = ounce = pound / 16
+stone = 14 * pound
+long_ton = 2240 * pound
+short_ton = 2000 * pound
+
+troy_ounce = 480 * grain  # only for metals / gems
+troy_pound = 12 * troy_ounce
+carat = 200e-6
+
+m_e = electron_mass = _cd('electron mass')
+m_p = proton_mass = _cd('proton mass')
+m_n = neutron_mass = _cd('neutron mass')
+m_u = u = atomic_mass = _cd('atomic mass constant')
+
+# angle in rad
+degree = pi / 180
+arcmin = arcminute = degree / 60
+arcsec = arcsecond = arcmin / 60
+
+# time in second
+minute = 60.0
+hour = 60 * minute
+day = 24 * hour
+week = 7 * day
+year = 365 * day
+Julian_year = 365.25 * day
+
+# length in meter
+inch = 0.0254
+foot = 12 * inch
+yard = 3 * foot
+mile = 1760 * yard
+mil = inch / 1000
+pt = point = inch / 72  # typography
+survey_foot = 1200.0 / 3937
+survey_mile = 5280 * survey_foot
+nautical_mile = 1852.0
+fermi = 1e-15
+angstrom = 1e-10
+micron = 1e-6
+au = astronomical_unit = 149597870700.0
+light_year = Julian_year * c
+parsec = au / arcsec
+
+# pressure in pascal
+atm = atmosphere = _cd('standard atmosphere')
+bar = 1e5
+torr = mmHg = atm / 760
+psi = pound * g / (inch * inch)
+
+# area in meter**2
+hectare = 1e4
+acre = 43560 * foot**2
+
+# volume in meter**3
+litre = liter = 1e-3
+gallon = gallon_US = 231 * inch**3  # US
+# pint = gallon_US / 8
+fluid_ounce = fluid_ounce_US = gallon_US / 128
+bbl = barrel = 42 * gallon_US  # for oil
+
+gallon_imp = 4.54609e-3  # UK
+fluid_ounce_imp = gallon_imp / 160
+
+# speed in meter per second
+kmh = 1e3 / hour
+mph = mile / hour
+# approx value of mach at 15 degrees in 1 atm. Is this a common value?
+mach = speed_of_sound = 340.5
+knot = nautical_mile / hour
+
+# temperature in kelvin
+zero_Celsius = 273.15
+degree_Fahrenheit = 1/1.8  # only for differences
+
+# energy in joule
+eV = electron_volt = elementary_charge  # * 1 Volt
+calorie = calorie_th = 4.184
+calorie_IT = 4.1868
+erg = 1e-7
+Btu_th = pound * degree_Fahrenheit * calorie_th / gram
+Btu = Btu_IT = pound * degree_Fahrenheit * calorie_IT / gram
+ton_TNT = 1e9 * calorie_th
+# Wh = watt_hour
+
+# power in watt
+hp = horsepower = 550 * foot * pound * g
+
+# force in newton
+dyn = dyne = 1e-5
+lbf = pound_force = pound * g
+kgf = kilogram_force = g  # * 1 kg
+
+# functions for conversions that are not linear
+
+
+def convert_temperature(
+    val: npt.ArrayLike,
+    old_scale: str,
+    new_scale: str,
+) -> Any:
+    """
+    Convert from a temperature scale to another one among Celsius, Kelvin,
+    Fahrenheit, and Rankine scales.
+
+    Parameters
+    ----------
+    val : array_like
+        Value(s) of the temperature(s) to be converted expressed in the
+        original scale.
+    old_scale : str
+        Specifies as a string the original scale from which the temperature
+        value(s) will be converted. Supported scales are Celsius ('Celsius',
+        'celsius', 'C' or 'c'), Kelvin ('Kelvin', 'kelvin', 'K', 'k'),
+        Fahrenheit ('Fahrenheit', 'fahrenheit', 'F' or 'f'), and Rankine
+        ('Rankine', 'rankine', 'R', 'r').
+    new_scale : str
+        Specifies as a string the new scale to which the temperature
+        value(s) will be converted. Supported scales are Celsius ('Celsius',
+        'celsius', 'C' or 'c'), Kelvin ('Kelvin', 'kelvin', 'K', 'k'),
+        Fahrenheit ('Fahrenheit', 'fahrenheit', 'F' or 'f'), and Rankine
+        ('Rankine', 'rankine', 'R', 'r').
+
+    Returns
+    -------
+    res : float or array of floats
+        Value(s) of the converted temperature(s) expressed in the new scale.
+
+    Notes
+    -----
+    .. versionadded:: 0.18.0
+
+    Examples
+    --------
+    >>> from scipy.constants import convert_temperature
+    >>> import numpy as np
+    >>> convert_temperature(np.array([-40, 40]), 'Celsius', 'Kelvin')
+    array([ 233.15,  313.15])
+
+    """
+    # Convert from `old_scale` to Kelvin
+    if old_scale.lower() in ['celsius', 'c']:
+        tempo = _np.asanyarray(val) + zero_Celsius
+    elif old_scale.lower() in ['kelvin', 'k']:
+        tempo = _np.asanyarray(val)
+    elif old_scale.lower() in ['fahrenheit', 'f']:
+        tempo = (_np.asanyarray(val) - 32) * 5 / 9 + zero_Celsius
+    elif old_scale.lower() in ['rankine', 'r']:
+        tempo = _np.asanyarray(val) * 5 / 9
+    else:
+        raise NotImplementedError("%s scale is unsupported: supported scales "
+                                  "are Celsius, Kelvin, Fahrenheit, and "
+                                  "Rankine" % old_scale)
+    # and from Kelvin to `new_scale`.
+    if new_scale.lower() in ['celsius', 'c']:
+        res = tempo - zero_Celsius
+    elif new_scale.lower() in ['kelvin', 'k']:
+        res = tempo
+    elif new_scale.lower() in ['fahrenheit', 'f']:
+        res = (tempo - zero_Celsius) * 9 / 5 + 32
+    elif new_scale.lower() in ['rankine', 'r']:
+        res = tempo * 9 / 5
+    else:
+        raise NotImplementedError("'%s' scale is unsupported: supported "
+                                  "scales are 'Celsius', 'Kelvin', "
+                                  "'Fahrenheit', and 'Rankine'" % new_scale)
+
+    return res
+
+
+# optics
+
+
+def lambda2nu(lambda_: npt.ArrayLike) -> Any:
+    """
+    Convert wavelength to optical frequency
+
+    Parameters
+    ----------
+    lambda_ : array_like
+        Wavelength(s) to be converted.
+
+    Returns
+    -------
+    nu : float or array of floats
+        Equivalent optical frequency.
+
+    Notes
+    -----
+    Computes ``nu = c / lambda`` where c = 299792458.0, i.e., the
+    (vacuum) speed of light in meters/second.
+
+    Examples
+    --------
+    >>> from scipy.constants import lambda2nu, speed_of_light
+    >>> import numpy as np
+    >>> lambda2nu(np.array((1, speed_of_light)))
+    array([  2.99792458e+08,   1.00000000e+00])
+
+    """
+    return c / _np.asanyarray(lambda_)
+
+
+def nu2lambda(nu: npt.ArrayLike) -> Any:
+    """
+    Convert optical frequency to wavelength.
+
+    Parameters
+    ----------
+    nu : array_like
+        Optical frequency to be converted.
+
+    Returns
+    -------
+    lambda : float or array of floats
+        Equivalent wavelength(s).
+
+    Notes
+    -----
+    Computes ``lambda = c / nu`` where c = 299792458.0, i.e., the
+    (vacuum) speed of light in meters/second.
+
+    Examples
+    --------
+    >>> from scipy.constants import nu2lambda, speed_of_light
+    >>> import numpy as np
+    >>> nu2lambda(np.array((1, speed_of_light)))
+    array([  2.99792458e+08,   1.00000000e+00])
+
+    """
+    return c / _np.asanyarray(nu)

llmeval-env/lib/python3.10/site-packages/scipy/constants/codata.py

@@ -0,0 +1,24 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.constants` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'physical_constants', 'value', 'unit', 'precision', 'find',
+    'ConstantWarning', 'txt2002', 'txt2006', 'txt2010', 'txt2014',
+    'txt2018', 'parse_constants_2002to2014',
+    'parse_constants_2018toXXXX', 'k', 'c', 'mu0', 'epsilon0',
+    'exact_values', 'key', 'val', 'v'
+
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="constants", module="codata",
+                                   private_modules=["_codata"], all=__all__,
+                                   attribute=name)

llmeval-env/lib/python3.10/site-packages/scipy/constants/constants.py

@@ -0,0 +1,53 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.constants` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+
+__all__ = [  # noqa: F822
+    'Avogadro', 'Boltzmann', 'Btu', 'Btu_IT', 'Btu_th', 'G',
+    'Julian_year', 'N_A', 'Planck', 'R', 'Rydberg',
+    'Stefan_Boltzmann', 'Wien', 'acre', 'alpha',
+    'angstrom', 'arcmin', 'arcminute', 'arcsec',
+    'arcsecond', 'astronomical_unit', 'atm',
+    'atmosphere', 'atomic_mass', 'atto', 'au', 'bar',
+    'barrel', 'bbl', 'blob', 'c', 'calorie',
+    'calorie_IT', 'calorie_th', 'carat', 'centi',
+    'convert_temperature', 'day', 'deci', 'degree',
+    'degree_Fahrenheit', 'deka', 'dyn', 'dyne', 'e',
+    'eV', 'electron_mass', 'electron_volt',
+    'elementary_charge', 'epsilon_0', 'erg',
+    'exa', 'exbi', 'femto', 'fermi', 'fine_structure',
+    'fluid_ounce', 'fluid_ounce_US', 'fluid_ounce_imp',
+    'foot', 'g', 'gallon', 'gallon_US', 'gallon_imp',
+    'gas_constant', 'gibi', 'giga', 'golden', 'golden_ratio',
+    'grain', 'gram', 'gravitational_constant', 'h', 'hbar',
+    'hectare', 'hecto', 'horsepower', 'hour', 'hp',
+    'inch', 'k', 'kgf', 'kibi', 'kilo', 'kilogram_force',
+    'kmh', 'knot', 'lambda2nu', 'lb', 'lbf',
+    'light_year', 'liter', 'litre', 'long_ton', 'm_e',
+    'm_n', 'm_p', 'm_u', 'mach', 'mebi', 'mega',
+    'metric_ton', 'micro', 'micron', 'mil', 'mile',
+    'milli', 'minute', 'mmHg', 'mph', 'mu_0', 'nano',
+    'nautical_mile', 'neutron_mass', 'nu2lambda',
+    'ounce', 'oz', 'parsec', 'pebi', 'peta',
+    'pi', 'pico', 'point', 'pound', 'pound_force',
+    'proton_mass', 'psi', 'pt', 'short_ton',
+    'sigma', 'slinch', 'slug', 'speed_of_light',
+    'speed_of_sound', 'stone', 'survey_foot',
+    'survey_mile', 'tebi', 'tera', 'ton_TNT',
+    'torr', 'troy_ounce', 'troy_pound', 'u',
+    'week', 'yard', 'year', 'yobi', 'yocto',
+    'yotta', 'zebi', 'zepto', 'zero_Celsius', 'zetta'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="constants", module="constants",
+                                   private_modules=["_constants"], all=__all__,
+                                   attribute=name)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/__init__.py

@@ -0,0 +1,103 @@
+"""
+=========================================================
+Legacy discrete Fourier transforms (:mod:`scipy.fftpack`)
+=========================================================
+
+.. legacy::
+
+   New code should use :mod:`scipy.fft`.
+
+Fast Fourier Transforms (FFTs)
+==============================
+
+.. autosummary::
+   :toctree: generated/
+
+   fft - Fast (discrete) Fourier Transform (FFT)
+   ifft - Inverse FFT
+   fft2 - 2-D FFT
+   ifft2 - 2-D inverse FFT
+   fftn - N-D FFT
+   ifftn - N-D inverse FFT
+   rfft - FFT of strictly real-valued sequence
+   irfft - Inverse of rfft
+   dct - Discrete cosine transform
+   idct - Inverse discrete cosine transform
+   dctn - N-D Discrete cosine transform
+   idctn - N-D Inverse discrete cosine transform
+   dst - Discrete sine transform
+   idst - Inverse discrete sine transform
+   dstn - N-D Discrete sine transform
+   idstn - N-D Inverse discrete sine transform
+
+Differential and pseudo-differential operators
+==============================================
+
+.. autosummary::
+   :toctree: generated/
+
+   diff - Differentiation and integration of periodic sequences
+   tilbert - Tilbert transform:         cs_diff(x,h,h)
+   itilbert - Inverse Tilbert transform: sc_diff(x,h,h)
+   hilbert - Hilbert transform:         cs_diff(x,inf,inf)
+   ihilbert - Inverse Hilbert transform: sc_diff(x,inf,inf)
+   cs_diff - cosh/sinh pseudo-derivative of periodic sequences
+   sc_diff - sinh/cosh pseudo-derivative of periodic sequences
+   ss_diff - sinh/sinh pseudo-derivative of periodic sequences
+   cc_diff - cosh/cosh pseudo-derivative of periodic sequences
+   shift - Shift periodic sequences
+
+Helper functions
+================
+
+.. autosummary::
+   :toctree: generated/
+
+   fftshift - Shift the zero-frequency component to the center of the spectrum
+   ifftshift - The inverse of `fftshift`
+   fftfreq - Return the Discrete Fourier Transform sample frequencies
+   rfftfreq - DFT sample frequencies (for usage with rfft, irfft)
+   next_fast_len - Find the optimal length to zero-pad an FFT for speed
+
+Note that ``fftshift``, ``ifftshift`` and ``fftfreq`` are numpy functions
+exposed by ``fftpack``; importing them from ``numpy`` should be preferred.
+
+Convolutions (:mod:`scipy.fftpack.convolve`)
+============================================
+
+.. module:: scipy.fftpack.convolve
+
+.. autosummary::
+   :toctree: generated/
+
+   convolve
+   convolve_z
+   init_convolution_kernel
+   destroy_convolve_cache
+
+"""
+
+
+__all__ = ['fft','ifft','fftn','ifftn','rfft','irfft',
+           'fft2','ifft2',
+           'diff',
+           'tilbert','itilbert','hilbert','ihilbert',
+           'sc_diff','cs_diff','cc_diff','ss_diff',
+           'shift',
+           'fftfreq', 'rfftfreq',
+           'fftshift', 'ifftshift',
+           'next_fast_len',
+           'dct', 'idct', 'dst', 'idst', 'dctn', 'idctn', 'dstn', 'idstn'
+           ]
+
+from ._basic import *
+from ._pseudo_diffs import *
+from ._helper import *
+from ._realtransforms import *
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import basic, helper, pseudo_diffs, realtransforms
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/_basic.py

@@ -0,0 +1,428 @@
+"""
+Discrete Fourier Transforms - _basic.py
+"""
+# Created by Pearu Peterson, August,September 2002
+__all__ = ['fft','ifft','fftn','ifftn','rfft','irfft',
+           'fft2','ifft2']
+
+from scipy.fft import _pocketfft
+from ._helper import _good_shape
+
+
+def fft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Return discrete Fourier transform of real or complex sequence.
+
+    The returned complex array contains ``y(0), y(1),..., y(n-1)``, where
+
+    ``y(j) = (x * exp(-2*pi*sqrt(-1)*j*np.arange(n)/n)).sum()``.
+
+    Parameters
+    ----------
+    x : array_like
+        Array to Fourier transform.
+    n : int, optional
+        Length of the Fourier transform. If ``n < x.shape[axis]``, `x` is
+        truncated. If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the fft's are computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    z : complex ndarray
+        with the elements::
+
+            [y(0),y(1),..,y(n/2),y(1-n/2),...,y(-1)]        if n is even
+            [y(0),y(1),..,y((n-1)/2),y(-(n-1)/2),...,y(-1)]  if n is odd
+
+        where::
+
+            y(j) = sum[k=0..n-1] x[k] * exp(-sqrt(-1)*j*k* 2*pi/n), j = 0..n-1
+
+    See Also
+    --------
+    ifft : Inverse FFT
+    rfft : FFT of a real sequence
+
+    Notes
+    -----
+    The packing of the result is "standard": If ``A = fft(a, n)``, then
+    ``A[0]`` contains the zero-frequency term, ``A[1:n/2]`` contains the
+    positive-frequency terms, and ``A[n/2:]`` contains the negative-frequency
+    terms, in order of decreasingly negative frequency. So ,for an 8-point
+    transform, the frequencies of the result are [0, 1, 2, 3, -4, -3, -2, -1].
+    To rearrange the fft output so that the zero-frequency component is
+    centered, like [-4, -3, -2, -1,  0,  1,  2,  3], use `fftshift`.
+
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    This function is most efficient when `n` is a power of two, and least
+    efficient when `n` is prime.
+
+    Note that if ``x`` is real-valued, then ``A[j] == A[n-j].conjugate()``.
+    If ``x`` is real-valued and ``n`` is even, then ``A[n/2]`` is real.
+
+    If the data type of `x` is real, a "real FFT" algorithm is automatically
+    used, which roughly halves the computation time. To increase efficiency
+    a little further, use `rfft`, which does the same calculation, but only
+    outputs half of the symmetrical spectrum. If the data is both real and
+    symmetrical, the `dct` can again double the efficiency by generating
+    half of the spectrum from half of the signal.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fft, ifft
+    >>> x = np.arange(5)
+    >>> np.allclose(fft(ifft(x)), x, atol=1e-15)  # within numerical accuracy.
+    True
+
+    """
+    return _pocketfft.fft(x, n, axis, None, overwrite_x)
+
+
+def ifft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Return discrete inverse Fourier transform of real or complex sequence.
+
+    The returned complex array contains ``y(0), y(1),..., y(n-1)``, where
+
+    ``y(j) = (x * exp(2*pi*sqrt(-1)*j*np.arange(n)/n)).mean()``.
+
+    Parameters
+    ----------
+    x : array_like
+        Transformed data to invert.
+    n : int, optional
+        Length of the inverse Fourier transform.  If ``n < x.shape[axis]``,
+        `x` is truncated. If ``n > x.shape[axis]``, `x` is zero-padded.
+        The default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the ifft's are computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    ifft : ndarray of floats
+        The inverse discrete Fourier transform.
+
+    See Also
+    --------
+    fft : Forward FFT
+
+    Notes
+    -----
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    This function is most efficient when `n` is a power of two, and least
+    efficient when `n` is prime.
+
+    If the data type of `x` is real, a "real IFFT" algorithm is automatically
+    used, which roughly halves the computation time.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import fft, ifft
+    >>> import numpy as np
+    >>> x = np.arange(5)
+    >>> np.allclose(ifft(fft(x)), x, atol=1e-15)  # within numerical accuracy.
+    True
+
+    """
+    return _pocketfft.ifft(x, n, axis, None, overwrite_x)
+
+
+def rfft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Discrete Fourier transform of a real sequence.
+
+    Parameters
+    ----------
+    x : array_like, real-valued
+        The data to transform.
+    n : int, optional
+        Defines the length of the Fourier transform. If `n` is not specified
+        (the default) then ``n = x.shape[axis]``. If ``n < x.shape[axis]``,
+        `x` is truncated, if ``n > x.shape[axis]``, `x` is zero-padded.
+    axis : int, optional
+        The axis along which the transform is applied. The default is the
+        last axis.
+    overwrite_x : bool, optional
+        If set to true, the contents of `x` can be overwritten. Default is
+        False.
+
+    Returns
+    -------
+    z : real ndarray
+        The returned real array contains::
+
+          [y(0),Re(y(1)),Im(y(1)),...,Re(y(n/2))]              if n is even
+          [y(0),Re(y(1)),Im(y(1)),...,Re(y(n/2)),Im(y(n/2))]   if n is odd
+
+        where::
+
+          y(j) = sum[k=0..n-1] x[k] * exp(-sqrt(-1)*j*k*2*pi/n)
+          j = 0..n-1
+
+    See Also
+    --------
+    fft, irfft, scipy.fft.rfft
+
+    Notes
+    -----
+    Within numerical accuracy, ``y == rfft(irfft(y))``.
+
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    To get an output with a complex datatype, consider using the newer
+    function `scipy.fft.rfft`.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import fft, rfft
+    >>> a = [9, -9, 1, 3]
+    >>> fft(a)
+    array([  4. +0.j,   8.+12.j,  16. +0.j,   8.-12.j])
+    >>> rfft(a)
+    array([  4.,   8.,  12.,  16.])
+
+    """
+    return _pocketfft.rfft_fftpack(x, n, axis, None, overwrite_x)
+
+
+def irfft(x, n=None, axis=-1, overwrite_x=False):
+    """
+    Return inverse discrete Fourier transform of real sequence x.
+
+    The contents of `x` are interpreted as the output of the `rfft`
+    function.
+
+    Parameters
+    ----------
+    x : array_like
+        Transformed data to invert.
+    n : int, optional
+        Length of the inverse Fourier transform.
+        If n < x.shape[axis], x is truncated.
+        If n > x.shape[axis], x is zero-padded.
+        The default results in n = x.shape[axis].
+    axis : int, optional
+        Axis along which the ifft's are computed; the default is over
+        the last axis (i.e., axis=-1).
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    irfft : ndarray of floats
+        The inverse discrete Fourier transform.
+
+    See Also
+    --------
+    rfft, ifft, scipy.fft.irfft
+
+    Notes
+    -----
+    The returned real array contains::
+
+        [y(0),y(1),...,y(n-1)]
+
+    where for n is even::
+
+        y(j) = 1/n (sum[k=1..n/2-1] (x[2*k-1]+sqrt(-1)*x[2*k])
+                                     * exp(sqrt(-1)*j*k* 2*pi/n)
+                    + c.c. + x[0] + (-1)**(j) x[n-1])
+
+    and for n is odd::
+
+        y(j) = 1/n (sum[k=1..(n-1)/2] (x[2*k-1]+sqrt(-1)*x[2*k])
+                                     * exp(sqrt(-1)*j*k* 2*pi/n)
+                    + c.c. + x[0])
+
+    c.c. denotes complex conjugate of preceding expression.
+
+    For details on input parameters, see `rfft`.
+
+    To process (conjugate-symmetric) frequency-domain data with a complex
+    datatype, consider using the newer function `scipy.fft.irfft`.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import rfft, irfft
+    >>> a = [1.0, 2.0, 3.0, 4.0, 5.0]
+    >>> irfft(a)
+    array([ 2.6       , -3.16405192,  1.24398433, -1.14955713,  1.46962473])
+    >>> irfft(rfft(a))
+    array([1., 2., 3., 4., 5.])
+
+    """
+    return _pocketfft.irfft_fftpack(x, n, axis, None, overwrite_x)
+
+
+def fftn(x, shape=None, axes=None, overwrite_x=False):
+    """
+    Return multidimensional discrete Fourier transform.
+
+    The returned array contains::
+
+      y[j_1,..,j_d] = sum[k_1=0..n_1-1, ..., k_d=0..n_d-1]
+         x[k_1,..,k_d] * prod[i=1..d] exp(-sqrt(-1)*2*pi/n_i * j_i * k_i)
+
+    where d = len(x.shape) and n = x.shape.
+
+    Parameters
+    ----------
+    x : array_like
+        The (N-D) array to transform.
+    shape : int or array_like of ints or None, optional
+        The shape of the result. If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        The axes of `x` (`y` if `shape` is not None) along which the
+        transform is applied.
+        The default is over all axes.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed. Default is False.
+
+    Returns
+    -------
+    y : complex-valued N-D NumPy array
+        The (N-D) DFT of the input array.
+
+    See Also
+    --------
+    ifftn
+
+    Notes
+    -----
+    If ``x`` is real-valued, then
+    ``y[..., j_i, ...] == y[..., n_i-j_i, ...].conjugate()``.
+
+    Both single and double precision routines are implemented. Half precision
+    inputs will be converted to single precision. Non-floating-point inputs
+    will be converted to double precision. Long-double precision inputs are
+    not supported.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fftn, ifftn
+    >>> y = (-np.arange(16), 8 - np.arange(16), np.arange(16))
+    >>> np.allclose(y, fftn(ifftn(y)))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.fftn(x, shape, axes, None, overwrite_x)
+
+
+def ifftn(x, shape=None, axes=None, overwrite_x=False):
+    """
+    Return inverse multidimensional discrete Fourier transform.
+
+    The sequence can be of an arbitrary type.
+
+    The returned array contains::
+
+      y[j_1,..,j_d] = 1/p * sum[k_1=0..n_1-1, ..., k_d=0..n_d-1]
+         x[k_1,..,k_d] * prod[i=1..d] exp(sqrt(-1)*2*pi/n_i * j_i * k_i)
+
+    where ``d = len(x.shape)``, ``n = x.shape``, and ``p = prod[i=1..d] n_i``.
+
+    For description of parameters see `fftn`.
+
+    See Also
+    --------
+    fftn : for detailed information.
+
+    Examples
+    --------
+    >>> from scipy.fftpack import fftn, ifftn
+    >>> import numpy as np
+    >>> y = (-np.arange(16), 8 - np.arange(16), np.arange(16))
+    >>> np.allclose(y, ifftn(fftn(y)))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.ifftn(x, shape, axes, None, overwrite_x)
+
+
+def fft2(x, shape=None, axes=(-2,-1), overwrite_x=False):
+    """
+    2-D discrete Fourier transform.
+
+    Return the 2-D discrete Fourier transform of the 2-D argument
+    `x`.
+
+    See Also
+    --------
+    fftn : for detailed information.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fft2, ifft2
+    >>> y = np.mgrid[:5, :5][0]
+    >>> y
+    array([[0, 0, 0, 0, 0],
+           [1, 1, 1, 1, 1],
+           [2, 2, 2, 2, 2],
+           [3, 3, 3, 3, 3],
+           [4, 4, 4, 4, 4]])
+    >>> np.allclose(y, ifft2(fft2(y)))
+    True
+    """
+    return fftn(x,shape,axes,overwrite_x)
+
+
+def ifft2(x, shape=None, axes=(-2,-1), overwrite_x=False):
+    """
+    2-D discrete inverse Fourier transform of real or complex sequence.
+
+    Return inverse 2-D discrete Fourier transform of
+    arbitrary type sequence x.
+
+    See `ifft` for more information.
+
+    See Also
+    --------
+    fft2, ifft
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import fft2, ifft2
+    >>> y = np.mgrid[:5, :5][0]
+    >>> y
+    array([[0, 0, 0, 0, 0],
+           [1, 1, 1, 1, 1],
+           [2, 2, 2, 2, 2],
+           [3, 3, 3, 3, 3],
+           [4, 4, 4, 4, 4]])
+    >>> np.allclose(y, fft2(ifft2(y)))
+    True
+
+    """
+    return ifftn(x,shape,axes,overwrite_x)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/_helper.py

@@ -0,0 +1,115 @@
+import operator
+
+import numpy as np
+from numpy.fft import fftshift, ifftshift, fftfreq
+
+import scipy.fft._pocketfft.helper as _helper
+
+__all__ = ['fftshift', 'ifftshift', 'fftfreq', 'rfftfreq', 'next_fast_len']
+
+
+def rfftfreq(n, d=1.0):
+    """DFT sample frequencies (for usage with rfft, irfft).
+
+    The returned float array contains the frequency bins in
+    cycles/unit (with zero at the start) given a window length `n` and a
+    sample spacing `d`::
+
+      f = [0,1,1,2,2,...,n/2-1,n/2-1,n/2]/(d*n)   if n is even
+      f = [0,1,1,2,2,...,n/2-1,n/2-1,n/2,n/2]/(d*n)   if n is odd
+
+    Parameters
+    ----------
+    n : int
+        Window length.
+    d : scalar, optional
+        Sample spacing. Default is 1.
+
+    Returns
+    -------
+    out : ndarray
+        The array of length `n`, containing the sample frequencies.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy import fftpack
+    >>> sig = np.array([-2, 8, 6, 4, 1, 0, 3, 5], dtype=float)
+    >>> sig_fft = fftpack.rfft(sig)
+    >>> n = sig_fft.size
+    >>> timestep = 0.1
+    >>> freq = fftpack.rfftfreq(n, d=timestep)
+    >>> freq
+    array([ 0.  ,  1.25,  1.25,  2.5 ,  2.5 ,  3.75,  3.75,  5.  ])
+
+    """
+    n = operator.index(n)
+    if n < 0:
+        raise ValueError("n = %s is not valid. "
+                         "n must be a nonnegative integer." % n)
+
+    return (np.arange(1, n + 1, dtype=int) // 2) / float(n * d)
+
+
+def next_fast_len(target):
+    """
+    Find the next fast size of input data to `fft`, for zero-padding, etc.
+
+    SciPy's FFTPACK has efficient functions for radix {2, 3, 4, 5}, so this
+    returns the next composite of the prime factors 2, 3, and 5 which is
+    greater than or equal to `target`. (These are also known as 5-smooth
+    numbers, regular numbers, or Hamming numbers.)
+
+    Parameters
+    ----------
+    target : int
+        Length to start searching from. Must be a positive integer.
+
+    Returns
+    -------
+    out : int
+        The first 5-smooth number greater than or equal to `target`.
+
+    Notes
+    -----
+    .. versionadded:: 0.18.0
+
+    Examples
+    --------
+    On a particular machine, an FFT of prime length takes 133 ms:
+
+    >>> from scipy import fftpack
+    >>> import numpy as np
+    >>> rng = np.random.default_rng()
+    >>> min_len = 10007  # prime length is worst case for speed
+    >>> a = rng.standard_normal(min_len)
+    >>> b = fftpack.fft(a)
+
+    Zero-padding to the next 5-smooth length reduces computation time to
+    211 us, a speedup of 630 times:
+
+    >>> fftpack.next_fast_len(min_len)
+    10125
+    >>> b = fftpack.fft(a, 10125)
+
+    Rounding up to the next power of 2 is not optimal, taking 367 us to
+    compute, 1.7 times as long as the 5-smooth size:
+
+    >>> b = fftpack.fft(a, 16384)
+
+    """
+    # Real transforms use regular sizes so this is backwards compatible
+    return _helper.good_size(target, True)
+
+
+def _good_shape(x, shape, axes):
+    """Ensure that shape argument is valid for scipy.fftpack
+
+    scipy.fftpack does not support len(shape) < x.ndim when axes is not given.
+    """
+    if shape is not None and axes is None:
+        shape = _helper._iterable_of_int(shape, 'shape')
+        if len(shape) != np.ndim(x):
+            raise ValueError("when given, axes and shape arguments"
+                             " have to be of the same length")
+    return shape

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/_pseudo_diffs.py

@@ -0,0 +1,551 @@
+"""
+Differential and pseudo-differential operators.
+"""
+# Created by Pearu Peterson, September 2002
+
+__all__ = ['diff',
+           'tilbert','itilbert','hilbert','ihilbert',
+           'cs_diff','cc_diff','sc_diff','ss_diff',
+           'shift']
+
+from numpy import pi, asarray, sin, cos, sinh, cosh, tanh, iscomplexobj
+from . import convolve
+
+from scipy.fft._pocketfft.helper import _datacopied
+
+
+_cache = {}
+
+
+def diff(x,order=1,period=None, _cache=_cache):
+    """
+    Return kth derivative (or integral) of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = pow(sqrt(-1)*j*2*pi/period, order) * x_j
+      y_0 = 0 if order is not 0.
+
+    Parameters
+    ----------
+    x : array_like
+        Input array.
+    order : int, optional
+        The order of differentiation. Default order is 1. If order is
+        negative, then integration is carried out under the assumption
+        that ``x_0 == 0``.
+    period : float, optional
+        The assumed period of the sequence. Default is ``2*pi``.
+
+    Notes
+    -----
+    If ``sum(x, axis=0) = 0`` then ``diff(diff(x, k), -k) == x`` (within
+    numerical accuracy).
+
+    For odd order and even ``len(x)``, the Nyquist mode is taken zero.
+
+    """
+    tmp = asarray(x)
+    if order == 0:
+        return tmp
+    if iscomplexobj(tmp):
+        return diff(tmp.real,order,period)+1j*diff(tmp.imag,order,period)
+    if period is not None:
+        c = 2*pi/period
+    else:
+        c = 1.0
+    n = len(x)
+    omega = _cache.get((n,order,c))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,order=order,c=c):
+            if k:
+                return pow(c*k,order)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=order,
+                                                 zero_nyquist=1)
+        _cache[(n,order,c)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=order % 2,
+                             overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def tilbert(x, h, period=None, _cache=_cache):
+    """
+    Return h-Tilbert transform of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+        y_j = sqrt(-1)*coth(j*h*2*pi/period) * x_j
+        y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        The input array to transform.
+    h : float
+        Defines the parameter of the Tilbert transform.
+    period : float, optional
+        The assumed period of the sequence. Default period is ``2*pi``.
+
+    Returns
+    -------
+    tilbert : ndarray
+        The result of the transform.
+
+    Notes
+    -----
+    If ``sum(x, axis=0) == 0`` and ``n = len(x)`` is odd, then
+    ``tilbert(itilbert(x)) == x``.
+
+    If ``2 * pi * h / period`` is approximately 10 or larger, then
+    numerically ``tilbert == hilbert``
+    (theoretically oo-Tilbert == Hilbert).
+
+    For even ``len(x)``, the Nyquist mode of ``x`` is taken zero.
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return tilbert(tmp.real, h, period) + \
+               1j * tilbert(tmp.imag, h, period)
+
+    if period is not None:
+        h = h * 2 * pi / period
+
+    n = len(x)
+    omega = _cache.get((n, h))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k, h=h):
+            if k:
+                return 1.0/tanh(h*k)
+
+            return 0
+
+        omega = convolve.init_convolution_kernel(n, kernel, d=1)
+        _cache[(n,h)] = omega
+
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def itilbert(x,h,period=None, _cache=_cache):
+    """
+    Return inverse h-Tilbert transform of a periodic sequence x.
+
+    If ``x_j`` and ``y_j`` are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = -sqrt(-1)*tanh(j*h*2*pi/period) * x_j
+      y_0 = 0
+
+    For more details, see `tilbert`.
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return itilbert(tmp.real,h,period) + \
+               1j*itilbert(tmp.imag,h,period)
+    if period is not None:
+        h = h*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,h))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,h=h):
+            if k:
+                return -tanh(h*k)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[(n,h)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def hilbert(x, _cache=_cache):
+    """
+    Return Hilbert transform of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = sqrt(-1)*sign(j) * x_j
+      y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        The input array, should be periodic.
+    _cache : dict, optional
+        Dictionary that contains the kernel used to do a convolution with.
+
+    Returns
+    -------
+    y : ndarray
+        The transformed input.
+
+    See Also
+    --------
+    scipy.signal.hilbert : Compute the analytic signal, using the Hilbert
+                           transform.
+
+    Notes
+    -----
+    If ``sum(x, axis=0) == 0`` then ``hilbert(ihilbert(x)) == x``.
+
+    For even len(x), the Nyquist mode of x is taken zero.
+
+    The sign of the returned transform does not have a factor -1 that is more
+    often than not found in the definition of the Hilbert transform. Note also
+    that `scipy.signal.hilbert` does have an extra -1 factor compared to this
+    function.
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return hilbert(tmp.real)+1j*hilbert(tmp.imag)
+    n = len(x)
+    omega = _cache.get(n)
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k):
+            if k > 0:
+                return 1.0
+            elif k < 0:
+                return -1.0
+            return 0.0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[n] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+def ihilbert(x):
+    """
+    Return inverse Hilbert transform of a periodic sequence x.
+
+    If ``x_j`` and ``y_j`` are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = -sqrt(-1)*sign(j) * x_j
+      y_0 = 0
+
+    """
+    return -hilbert(x)
+
+
+_cache = {}
+
+
+def cs_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-cosh/sinh pseudo-derivative of a periodic sequence.
+
+    If ``x_j`` and ``y_j`` are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = -sqrt(-1)*cosh(j*a*2*pi/period)/sinh(j*b*2*pi/period) * x_j
+      y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a, b : float
+        Defines the parameters of the cosh/sinh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence. Default period is ``2*pi``.
+
+    Returns
+    -------
+    cs_diff : ndarray
+        Pseudo-derivative of periodic sequence `x`.
+
+    Notes
+    -----
+    For even len(`x`), the Nyquist mode of `x` is taken as zero.
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return cs_diff(tmp.real,a,b,period) + \
+               1j*cs_diff(tmp.imag,a,b,period)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            if k:
+                return -cosh(a*k)/sinh(b*k)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def sc_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-sinh/cosh pseudo-derivative of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = sqrt(-1)*sinh(j*a*2*pi/period)/cosh(j*b*2*pi/period) * x_j
+      y_0 = 0
+
+    Parameters
+    ----------
+    x : array_like
+        Input array.
+    a,b : float
+        Defines the parameters of the sinh/cosh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence x. Default is 2*pi.
+
+    Notes
+    -----
+    ``sc_diff(cs_diff(x,a,b),b,a) == x``
+    For even ``len(x)``, the Nyquist mode of x is taken as zero.
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return sc_diff(tmp.real,a,b,period) + \
+               1j*sc_diff(tmp.imag,a,b,period)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            if k:
+                return sinh(a*k)/cosh(b*k)
+            return 0
+        omega = convolve.init_convolution_kernel(n,kernel,d=1)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,swap_real_imag=1,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def ss_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-sinh/sinh pseudo-derivative of a periodic sequence x.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = sinh(j*a*2*pi/period)/sinh(j*b*2*pi/period) * x_j
+      y_0 = a/b * x_0
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a,b
+        Defines the parameters of the sinh/sinh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence x. Default is ``2*pi``.
+
+    Notes
+    -----
+    ``ss_diff(ss_diff(x,a,b),b,a) == x``
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return ss_diff(tmp.real,a,b,period) + \
+               1j*ss_diff(tmp.imag,a,b,period)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            if k:
+                return sinh(a*k)/sinh(b*k)
+            return float(a)/b
+        omega = convolve.init_convolution_kernel(n,kernel)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def cc_diff(x, a, b, period=None, _cache=_cache):
+    """
+    Return (a,b)-cosh/cosh pseudo-derivative of a periodic sequence.
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+      y_j = cosh(j*a*2*pi/period)/cosh(j*b*2*pi/period) * x_j
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a,b : float
+        Defines the parameters of the sinh/sinh pseudo-differential
+        operator.
+    period : float, optional
+        The period of the sequence x. Default is ``2*pi``.
+
+    Returns
+    -------
+    cc_diff : ndarray
+        Pseudo-derivative of periodic sequence `x`.
+
+    Notes
+    -----
+    ``cc_diff(cc_diff(x,a,b),b,a) == x``
+
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return cc_diff(tmp.real,a,b,period) + \
+               1j*cc_diff(tmp.imag,a,b,period)
+    if period is not None:
+        a = a*2*pi/period
+        b = b*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a,b))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel(k,a=a,b=b):
+            return cosh(a*k)/cosh(b*k)
+        omega = convolve.init_convolution_kernel(n,kernel)
+        _cache[(n,a,b)] = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve(tmp,omega,overwrite_x=overwrite_x)
+
+
+del _cache
+
+
+_cache = {}
+
+
+def shift(x, a, period=None, _cache=_cache):
+    """
+    Shift periodic sequence x by a: y(u) = x(u+a).
+
+    If x_j and y_j are Fourier coefficients of periodic functions x
+    and y, respectively, then::
+
+          y_j = exp(j*a*2*pi/period*sqrt(-1)) * x_f
+
+    Parameters
+    ----------
+    x : array_like
+        The array to take the pseudo-derivative from.
+    a : float
+        Defines the parameters of the sinh/sinh pseudo-differential
+    period : float, optional
+        The period of the sequences x and y. Default period is ``2*pi``.
+    """
+    tmp = asarray(x)
+    if iscomplexobj(tmp):
+        return shift(tmp.real,a,period)+1j*shift(tmp.imag,a,period)
+    if period is not None:
+        a = a*2*pi/period
+    n = len(x)
+    omega = _cache.get((n,a))
+    if omega is None:
+        if len(_cache) > 20:
+            while _cache:
+                _cache.popitem()
+
+        def kernel_real(k,a=a):
+            return cos(a*k)
+
+        def kernel_imag(k,a=a):
+            return sin(a*k)
+        omega_real = convolve.init_convolution_kernel(n,kernel_real,d=0,
+                                                      zero_nyquist=0)
+        omega_imag = convolve.init_convolution_kernel(n,kernel_imag,d=1,
+                                                      zero_nyquist=0)
+        _cache[(n,a)] = omega_real,omega_imag
+    else:
+        omega_real,omega_imag = omega
+    overwrite_x = _datacopied(tmp, x)
+    return convolve.convolve_z(tmp,omega_real,omega_imag,
+                               overwrite_x=overwrite_x)
+
+
+del _cache

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/_realtransforms.py

@@ -0,0 +1,598 @@
+"""
+Real spectrum transforms (DCT, DST, MDCT)
+"""
+
+__all__ = ['dct', 'idct', 'dst', 'idst', 'dctn', 'idctn', 'dstn', 'idstn']
+
+from scipy.fft import _pocketfft
+from ._helper import _good_shape
+
+_inverse_typemap = {1: 1, 2: 3, 3: 2, 4: 4}
+
+
+def dctn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Cosine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result. If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the DCT is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    idctn : Inverse multidimensional DCT
+
+    Notes
+    -----
+    For full details of the DCT types and normalization modes, as well as
+    references, see `dct`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dctn, idctn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idctn(dctn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dctn(x, type, shape, axes, norm, overwrite_x)
+
+
+def idctn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Cosine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result.  If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the IDCT is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dctn : multidimensional DCT
+
+    Notes
+    -----
+    For full details of the IDCT types and normalization modes, as well as
+    references, see `idct`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dctn, idctn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idctn(dctn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    type = _inverse_typemap[type]
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dctn(x, type, shape, axes, norm, overwrite_x)
+
+
+def dstn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Sine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result.  If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the DCT is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    idstn : Inverse multidimensional DST
+
+    Notes
+    -----
+    For full details of the DST types and normalization modes, as well as
+    references, see `dst`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dstn, idstn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idstn(dstn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dstn(x, type, shape, axes, norm, overwrite_x)
+
+
+def idstn(x, type=2, shape=None, axes=None, norm=None, overwrite_x=False):
+    """
+    Return multidimensional Discrete Sine Transform along the specified axes.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    shape : int or array_like of ints or None, optional
+        The shape of the result.  If both `shape` and `axes` (see below) are
+        None, `shape` is ``x.shape``; if `shape` is None but `axes` is
+        not None, then `shape` is ``numpy.take(x.shape, axes, axis=0)``.
+        If ``shape[i] > x.shape[i]``, the ith dimension is padded with zeros.
+        If ``shape[i] < x.shape[i]``, the ith dimension is truncated to
+        length ``shape[i]``.
+        If any element of `shape` is -1, the size of the corresponding
+        dimension of `x` is used.
+    axes : int or array_like of ints or None, optional
+        Axes along which the IDST is computed.
+        The default is over all axes.
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dstn : multidimensional DST
+
+    Notes
+    -----
+    For full details of the IDST types and normalization modes, as well as
+    references, see `idst`.
+
+    Examples
+    --------
+    >>> import numpy as np
+    >>> from scipy.fftpack import dstn, idstn
+    >>> rng = np.random.default_rng()
+    >>> y = rng.standard_normal((16, 16))
+    >>> np.allclose(y, idstn(dstn(y, norm='ortho'), norm='ortho'))
+    True
+
+    """
+    type = _inverse_typemap[type]
+    shape = _good_shape(x, shape, axes)
+    return _pocketfft.dstn(x, type, shape, axes, norm, overwrite_x)
+
+
+def dct(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    r"""
+    Return the Discrete Cosine Transform of arbitrary type sequence x.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated.  If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the dct is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    y : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    idct : Inverse DCT
+
+    Notes
+    -----
+    For a single dimension array ``x``, ``dct(x, norm='ortho')`` is equal to
+    MATLAB ``dct(x)``.
+
+    There are, theoretically, 8 types of the DCT, only the first 4 types are
+    implemented in scipy. 'The' DCT generally refers to DCT type 2, and 'the'
+    Inverse DCT generally refers to DCT type 3.
+
+    **Type I**
+
+    There are several definitions of the DCT-I; we use the following
+    (for ``norm=None``)
+
+    .. math::
+
+       y_k = x_0 + (-1)^k x_{N-1} + 2 \sum_{n=1}^{N-2} x_n \cos\left(
+       \frac{\pi k n}{N-1} \right)
+
+    If ``norm='ortho'``, ``x[0]`` and ``x[N-1]`` are multiplied by a scaling
+    factor of :math:`\sqrt{2}`, and ``y[k]`` is multiplied by a scaling factor
+    ``f``
+
+    .. math::
+
+        f = \begin{cases}
+         \frac{1}{2}\sqrt{\frac{1}{N-1}} & \text{if }k=0\text{ or }N-1, \\
+         \frac{1}{2}\sqrt{\frac{2}{N-1}} & \text{otherwise} \end{cases}
+
+    .. versionadded:: 1.2.0
+       Orthonormalization in DCT-I.
+
+    .. note::
+       The DCT-I is only supported for input size > 1.
+
+    **Type II**
+
+    There are several definitions of the DCT-II; we use the following
+    (for ``norm=None``)
+
+    .. math::
+
+       y_k = 2 \sum_{n=0}^{N-1} x_n \cos\left(\frac{\pi k(2n+1)}{2N} \right)
+
+    If ``norm='ortho'``, ``y[k]`` is multiplied by a scaling factor ``f``
+
+    .. math::
+       f = \begin{cases}
+       \sqrt{\frac{1}{4N}} & \text{if }k=0, \\
+       \sqrt{\frac{1}{2N}} & \text{otherwise} \end{cases}
+
+    which makes the corresponding matrix of coefficients orthonormal
+    (``O @ O.T = np.eye(N)``).
+
+    **Type III**
+
+    There are several definitions, we use the following (for ``norm=None``)
+
+    .. math::
+
+       y_k = x_0 + 2 \sum_{n=1}^{N-1} x_n \cos\left(\frac{\pi(2k+1)n}{2N}\right)
+
+    or, for ``norm='ortho'``
+
+    .. math::
+
+       y_k = \frac{x_0}{\sqrt{N}} + \sqrt{\frac{2}{N}} \sum_{n=1}^{N-1} x_n
+       \cos\left(\frac{\pi(2k+1)n}{2N}\right)
+
+    The (unnormalized) DCT-III is the inverse of the (unnormalized) DCT-II, up
+    to a factor `2N`. The orthonormalized DCT-III is exactly the inverse of
+    the orthonormalized DCT-II.
+
+    **Type IV**
+
+    There are several definitions of the DCT-IV; we use the following
+    (for ``norm=None``)
+
+    .. math::
+
+       y_k = 2 \sum_{n=0}^{N-1} x_n \cos\left(\frac{\pi(2k+1)(2n+1)}{4N} \right)
+
+    If ``norm='ortho'``, ``y[k]`` is multiplied by a scaling factor ``f``
+
+    .. math::
+
+        f = \frac{1}{\sqrt{2N}}
+
+    .. versionadded:: 1.2.0
+       Support for DCT-IV.
+
+    References
+    ----------
+    .. [1] 'A Fast Cosine Transform in One and Two Dimensions', by J.
+           Makhoul, `IEEE Transactions on acoustics, speech and signal
+           processing` vol. 28(1), pp. 27-34,
+           :doi:`10.1109/TASSP.1980.1163351` (1980).
+    .. [2] Wikipedia, "Discrete cosine transform",
+           https://en.wikipedia.org/wiki/Discrete_cosine_transform
+
+    Examples
+    --------
+    The Type 1 DCT is equivalent to the FFT (though faster) for real,
+    even-symmetrical inputs. The output is also real and even-symmetrical.
+    Half of the FFT input is used to generate half of the FFT output:
+
+    >>> from scipy.fftpack import fft, dct
+    >>> import numpy as np
+    >>> fft(np.array([4., 3., 5., 10., 5., 3.])).real
+    array([ 30.,  -8.,   6.,  -2.,   6.,  -8.])
+    >>> dct(np.array([4., 3., 5., 10.]), 1)
+    array([ 30.,  -8.,   6.,  -2.])
+
+    """
+    return _pocketfft.dct(x, type, n, axis, norm, overwrite_x)
+
+
+def idct(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    """
+    Return the Inverse Discrete Cosine Transform of an arbitrary type sequence.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DCT (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated.  If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the idct is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    idct : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dct : Forward DCT
+
+    Notes
+    -----
+    For a single dimension array `x`, ``idct(x, norm='ortho')`` is equal to
+    MATLAB ``idct(x)``.
+
+    'The' IDCT is the IDCT of type 2, which is the same as DCT of type 3.
+
+    IDCT of type 1 is the DCT of type 1, IDCT of type 2 is the DCT of type
+    3, and IDCT of type 3 is the DCT of type 2. IDCT of type 4 is the DCT
+    of type 4. For the definition of these types, see `dct`.
+
+    Examples
+    --------
+    The Type 1 DCT is equivalent to the DFT for real, even-symmetrical
+    inputs. The output is also real and even-symmetrical. Half of the IFFT
+    input is used to generate half of the IFFT output:
+
+    >>> from scipy.fftpack import ifft, idct
+    >>> import numpy as np
+    >>> ifft(np.array([ 30.,  -8.,   6.,  -2.,   6.,  -8.])).real
+    array([  4.,   3.,   5.,  10.,   5.,   3.])
+    >>> idct(np.array([ 30.,  -8.,   6.,  -2.]), 1) / 6
+    array([  4.,   3.,   5.,  10.])
+
+    """
+    type = _inverse_typemap[type]
+    return _pocketfft.dct(x, type, n, axis, norm, overwrite_x)
+
+
+def dst(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    r"""
+    Return the Discrete Sine Transform of arbitrary type sequence x.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated.  If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the dst is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    dst : ndarray of reals
+        The transformed input array.
+
+    See Also
+    --------
+    idst : Inverse DST
+
+    Notes
+    -----
+    For a single dimension array ``x``.
+
+    There are, theoretically, 8 types of the DST for different combinations of
+    even/odd boundary conditions and boundary off sets [1]_, only the first
+    4 types are implemented in scipy.
+
+    **Type I**
+
+    There are several definitions of the DST-I; we use the following
+    for ``norm=None``. DST-I assumes the input is odd around `n=-1` and `n=N`.
+
+    .. math::
+
+        y_k = 2 \sum_{n=0}^{N-1} x_n \sin\left(\frac{\pi(k+1)(n+1)}{N+1}\right)
+
+    Note that the DST-I is only supported for input size > 1.
+    The (unnormalized) DST-I is its own inverse, up to a factor `2(N+1)`.
+    The orthonormalized DST-I is exactly its own inverse.
+
+    **Type II**
+
+    There are several definitions of the DST-II; we use the following for
+    ``norm=None``. DST-II assumes the input is odd around `n=-1/2` and
+    `n=N-1/2`; the output is odd around :math:`k=-1` and even around `k=N-1`
+
+    .. math::
+
+        y_k = 2 \sum_{n=0}^{N-1} x_n \sin\left(\frac{\pi(k+1)(2n+1)}{2N}\right)
+
+    if ``norm='ortho'``, ``y[k]`` is multiplied by a scaling factor ``f``
+
+    .. math::
+
+        f = \begin{cases}
+        \sqrt{\frac{1}{4N}} & \text{if }k = 0, \\
+        \sqrt{\frac{1}{2N}} & \text{otherwise} \end{cases}
+
+    **Type III**
+
+    There are several definitions of the DST-III, we use the following (for
+    ``norm=None``). DST-III assumes the input is odd around `n=-1` and even
+    around `n=N-1`
+
+    .. math::
+
+        y_k = (-1)^k x_{N-1} + 2 \sum_{n=0}^{N-2} x_n \sin\left(
+        \frac{\pi(2k+1)(n+1)}{2N}\right)
+
+    The (unnormalized) DST-III is the inverse of the (unnormalized) DST-II, up
+    to a factor `2N`. The orthonormalized DST-III is exactly the inverse of the
+    orthonormalized DST-II.
+
+    .. versionadded:: 0.11.0
+
+    **Type IV**
+
+    There are several definitions of the DST-IV, we use the following (for
+    ``norm=None``). DST-IV assumes the input is odd around `n=-0.5` and even
+    around `n=N-0.5`
+
+    .. math::
+
+        y_k = 2 \sum_{n=0}^{N-1} x_n \sin\left(\frac{\pi(2k+1)(2n+1)}{4N}\right)
+
+    The (unnormalized) DST-IV is its own inverse, up to a factor `2N`. The
+    orthonormalized DST-IV is exactly its own inverse.
+
+    .. versionadded:: 1.2.0
+       Support for DST-IV.
+
+    References
+    ----------
+    .. [1] Wikipedia, "Discrete sine transform",
+           https://en.wikipedia.org/wiki/Discrete_sine_transform
+
+    """
+    return _pocketfft.dst(x, type, n, axis, norm, overwrite_x)
+
+
+def idst(x, type=2, n=None, axis=-1, norm=None, overwrite_x=False):
+    """
+    Return the Inverse Discrete Sine Transform of an arbitrary type sequence.
+
+    Parameters
+    ----------
+    x : array_like
+        The input array.
+    type : {1, 2, 3, 4}, optional
+        Type of the DST (see Notes). Default type is 2.
+    n : int, optional
+        Length of the transform.  If ``n < x.shape[axis]``, `x` is
+        truncated. If ``n > x.shape[axis]``, `x` is zero-padded. The
+        default results in ``n = x.shape[axis]``.
+    axis : int, optional
+        Axis along which the idst is computed; the default is over the
+        last axis (i.e., ``axis=-1``).
+    norm : {None, 'ortho'}, optional
+        Normalization mode (see Notes). Default is None.
+    overwrite_x : bool, optional
+        If True, the contents of `x` can be destroyed; the default is False.
+
+    Returns
+    -------
+    idst : ndarray of real
+        The transformed input array.
+
+    See Also
+    --------
+    dst : Forward DST
+
+    Notes
+    -----
+    'The' IDST is the IDST of type 2, which is the same as DST of type 3.
+
+    IDST of type 1 is the DST of type 1, IDST of type 2 is the DST of type
+    3, and IDST of type 3 is the DST of type 2. For the definition of these
+    types, see `dst`.
+
+    .. versionadded:: 0.11.0
+
+    """
+    type = _inverse_typemap[type]
+    return _pocketfft.dst(x, type, n, axis, norm, overwrite_x)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/basic.py

@@ -0,0 +1,20 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'fft','ifft','fftn','ifftn','rfft','irfft',
+    'fft2','ifft2'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="basic",
+                                   private_modules=["_basic"], all=__all__,
+                                   attribute=name)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/helper.py

@@ -0,0 +1,19 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'fftshift', 'ifftshift', 'fftfreq', 'rfftfreq', 'next_fast_len'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="helper",
+                                   private_modules=["_helper"], all=__all__,
+                                   attribute=name)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/pseudo_diffs.py

@@ -0,0 +1,22 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'diff',
+    'tilbert', 'itilbert', 'hilbert', 'ihilbert',
+    'cs_diff', 'cc_diff', 'sc_diff', 'ss_diff',
+    'shift', 'iscomplexobj', 'convolve'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="pseudo_diffs",
+                                   private_modules=["_pseudo_diffs"], all=__all__,
+                                   attribute=name)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/realtransforms.py

@@ -0,0 +1,19 @@
+# This file is not meant for public use and will be removed in SciPy v2.0.0.
+# Use the `scipy.fftpack` namespace for importing the functions
+# included below.
+
+from scipy._lib.deprecation import _sub_module_deprecation
+
+__all__ = [  # noqa: F822
+    'dct', 'idct', 'dst', 'idst', 'dctn', 'idctn', 'dstn', 'idstn'
+]
+
+
+def __dir__():
+    return __all__
+
+
+def __getattr__(name):
+    return _sub_module_deprecation(sub_package="fftpack", module="realtransforms",
+                                   private_modules=["_realtransforms"], all=__all__,
+                                   attribute=name)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/tests/test_basic.py

@@ -0,0 +1,873 @@
+# Created by Pearu Peterson, September 2002
+
+from numpy.testing import (assert_, assert_equal, assert_array_almost_equal,
+                           assert_array_almost_equal_nulp, assert_array_less)
+import pytest
+from pytest import raises as assert_raises
+from scipy.fftpack import ifft, fft, fftn, ifftn, rfft, irfft, fft2
+
+from numpy import (arange, array, asarray, zeros, dot, exp, pi,
+                   swapaxes, double, cdouble)
+import numpy as np
+import numpy.fft
+from numpy.random import rand
+
+# "large" composite numbers supported by FFTPACK
+LARGE_COMPOSITE_SIZES = [
+    2**13,
+    2**5 * 3**5,
+    2**3 * 3**3 * 5**2,
+]
+SMALL_COMPOSITE_SIZES = [
+    2,
+    2*3*5,
+    2*2*3*3,
+]
+# prime
+LARGE_PRIME_SIZES = [
+    2011
+]
+SMALL_PRIME_SIZES = [
+    29
+]
+
+
+def _assert_close_in_norm(x, y, rtol, size, rdt):
+    # helper function for testing
+    err_msg = f"size: {size}  rdt: {rdt}"
+    assert_array_less(np.linalg.norm(x - y), rtol*np.linalg.norm(x), err_msg)
+
+
+def random(size):
+    return rand(*size)
+
+
+def direct_dft(x):
+    x = asarray(x)
+    n = len(x)
+    y = zeros(n, dtype=cdouble)
+    w = -arange(n)*(2j*pi/n)
+    for i in range(n):
+        y[i] = dot(exp(i*w), x)
+    return y
+
+
+def direct_idft(x):
+    x = asarray(x)
+    n = len(x)
+    y = zeros(n, dtype=cdouble)
+    w = arange(n)*(2j*pi/n)
+    for i in range(n):
+        y[i] = dot(exp(i*w), x)/n
+    return y
+
+
+def direct_dftn(x):
+    x = asarray(x)
+    for axis in range(len(x.shape)):
+        x = fft(x, axis=axis)
+    return x
+
+
+def direct_idftn(x):
+    x = asarray(x)
+    for axis in range(len(x.shape)):
+        x = ifft(x, axis=axis)
+    return x
+
+
+def direct_rdft(x):
+    x = asarray(x)
+    n = len(x)
+    w = -arange(n)*(2j*pi/n)
+    r = zeros(n, dtype=double)
+    for i in range(n//2+1):
+        y = dot(exp(i*w), x)
+        if i:
+            r[2*i-1] = y.real
+            if 2*i < n:
+                r[2*i] = y.imag
+        else:
+            r[0] = y.real
+    return r
+
+
+def direct_irdft(x):
+    x = asarray(x)
+    n = len(x)
+    x1 = zeros(n, dtype=cdouble)
+    for i in range(n//2+1):
+        if i:
+            if 2*i < n:
+                x1[i] = x[2*i-1] + 1j*x[2*i]
+                x1[n-i] = x[2*i-1] - 1j*x[2*i]
+            else:
+                x1[i] = x[2*i-1]
+        else:
+            x1[0] = x[0]
+    return direct_idft(x1).real
+
+
+class _TestFFTBase:
+    def setup_method(self):
+        self.cdt = None
+        self.rdt = None
+        np.random.seed(1234)
+
+    def test_definition(self):
+        x = np.array([1,2,3,4+1j,1,2,3,4+2j], dtype=self.cdt)
+        y = fft(x)
+        assert_equal(y.dtype, self.cdt)
+        y1 = direct_dft(x)
+        assert_array_almost_equal(y,y1)
+        x = np.array([1,2,3,4+0j,5], dtype=self.cdt)
+        assert_array_almost_equal(fft(x),direct_dft(x))
+
+    def test_n_argument_real(self):
+        x1 = np.array([1,2,3,4], dtype=self.rdt)
+        x2 = np.array([1,2,3,4], dtype=self.rdt)
+        y = fft([x1,x2],n=4)
+        assert_equal(y.dtype, self.cdt)
+        assert_equal(y.shape,(2,4))
+        assert_array_almost_equal(y[0],direct_dft(x1))
+        assert_array_almost_equal(y[1],direct_dft(x2))
+
+    def _test_n_argument_complex(self):
+        x1 = np.array([1,2,3,4+1j], dtype=self.cdt)
+        x2 = np.array([1,2,3,4+1j], dtype=self.cdt)
+        y = fft([x1,x2],n=4)
+        assert_equal(y.dtype, self.cdt)
+        assert_equal(y.shape,(2,4))
+        assert_array_almost_equal(y[0],direct_dft(x1))
+        assert_array_almost_equal(y[1],direct_dft(x2))
+
+    def test_invalid_sizes(self):
+        assert_raises(ValueError, fft, [])
+        assert_raises(ValueError, fft, [[1,1],[2,2]], -5)
+
+
+class TestDoubleFFT(_TestFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex128
+        self.rdt = np.float64
+
+
+class TestSingleFFT(_TestFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex64
+        self.rdt = np.float32
+
+    reason = ("single-precision FFT implementation is partially disabled, "
+              "until accuracy issues with large prime powers are resolved")
+
+    @pytest.mark.xfail(run=False, reason=reason)
+    def test_notice(self):
+        pass
+
+
+class TestFloat16FFT:
+
+    def test_1_argument_real(self):
+        x1 = np.array([1, 2, 3, 4], dtype=np.float16)
+        y = fft(x1, n=4)
+        assert_equal(y.dtype, np.complex64)
+        assert_equal(y.shape, (4, ))
+        assert_array_almost_equal(y, direct_dft(x1.astype(np.float32)))
+
+    def test_n_argument_real(self):
+        x1 = np.array([1, 2, 3, 4], dtype=np.float16)
+        x2 = np.array([1, 2, 3, 4], dtype=np.float16)
+        y = fft([x1, x2], n=4)
+        assert_equal(y.dtype, np.complex64)
+        assert_equal(y.shape, (2, 4))
+        assert_array_almost_equal(y[0], direct_dft(x1.astype(np.float32)))
+        assert_array_almost_equal(y[1], direct_dft(x2.astype(np.float32)))
+
+
+class _TestIFFTBase:
+    def setup_method(self):
+        np.random.seed(1234)
+
+    def test_definition(self):
+        x = np.array([1,2,3,4+1j,1,2,3,4+2j], self.cdt)
+        y = ifft(x)
+        y1 = direct_idft(x)
+        assert_equal(y.dtype, self.cdt)
+        assert_array_almost_equal(y,y1)
+
+        x = np.array([1,2,3,4+0j,5], self.cdt)
+        assert_array_almost_equal(ifft(x),direct_idft(x))
+
+    def test_definition_real(self):
+        x = np.array([1,2,3,4,1,2,3,4], self.rdt)
+        y = ifft(x)
+        assert_equal(y.dtype, self.cdt)
+        y1 = direct_idft(x)
+        assert_array_almost_equal(y,y1)
+
+        x = np.array([1,2,3,4,5], dtype=self.rdt)
+        assert_equal(y.dtype, self.cdt)
+        assert_array_almost_equal(ifft(x),direct_idft(x))
+
+    def test_random_complex(self):
+        for size in [1,51,111,100,200,64,128,256,1024]:
+            x = random([size]).astype(self.cdt)
+            x = random([size]).astype(self.cdt) + 1j*x
+            y1 = ifft(fft(x))
+            y2 = fft(ifft(x))
+            assert_equal(y1.dtype, self.cdt)
+            assert_equal(y2.dtype, self.cdt)
+            assert_array_almost_equal(y1, x)
+            assert_array_almost_equal(y2, x)
+
+    def test_random_real(self):
+        for size in [1,51,111,100,200,64,128,256,1024]:
+            x = random([size]).astype(self.rdt)
+            y1 = ifft(fft(x))
+            y2 = fft(ifft(x))
+            assert_equal(y1.dtype, self.cdt)
+            assert_equal(y2.dtype, self.cdt)
+            assert_array_almost_equal(y1, x)
+            assert_array_almost_equal(y2, x)
+
+    def test_size_accuracy(self):
+        # Sanity check for the accuracy for prime and non-prime sized inputs
+        if self.rdt == np.float32:
+            rtol = 1e-5
+        elif self.rdt == np.float64:
+            rtol = 1e-10
+
+        for size in LARGE_COMPOSITE_SIZES + LARGE_PRIME_SIZES:
+            np.random.seed(1234)
+            x = np.random.rand(size).astype(self.rdt)
+            y = ifft(fft(x))
+            _assert_close_in_norm(x, y, rtol, size, self.rdt)
+            y = fft(ifft(x))
+            _assert_close_in_norm(x, y, rtol, size, self.rdt)
+
+            x = (x + 1j*np.random.rand(size)).astype(self.cdt)
+            y = ifft(fft(x))
+            _assert_close_in_norm(x, y, rtol, size, self.rdt)
+            y = fft(ifft(x))
+            _assert_close_in_norm(x, y, rtol, size, self.rdt)
+
+    def test_invalid_sizes(self):
+        assert_raises(ValueError, ifft, [])
+        assert_raises(ValueError, ifft, [[1,1],[2,2]], -5)
+
+
+class TestDoubleIFFT(_TestIFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex128
+        self.rdt = np.float64
+
+
+class TestSingleIFFT(_TestIFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex64
+        self.rdt = np.float32
+
+
+class _TestRFFTBase:
+    def setup_method(self):
+        np.random.seed(1234)
+
+    def test_definition(self):
+        for t in [[1, 2, 3, 4, 1, 2, 3, 4], [1, 2, 3, 4, 1, 2, 3, 4, 5]]:
+            x = np.array(t, dtype=self.rdt)
+            y = rfft(x)
+            y1 = direct_rdft(x)
+            assert_array_almost_equal(y,y1)
+            assert_equal(y.dtype, self.rdt)
+
+    def test_invalid_sizes(self):
+        assert_raises(ValueError, rfft, [])
+        assert_raises(ValueError, rfft, [[1,1],[2,2]], -5)
+
+    # See gh-5790
+    class MockSeries:
+        def __init__(self, data):
+            self.data = np.asarray(data)
+
+        def __getattr__(self, item):
+            try:
+                return getattr(self.data, item)
+            except AttributeError as e:
+                raise AttributeError("'MockSeries' object "
+                                      f"has no attribute '{item}'") from e
+
+    def test_non_ndarray_with_dtype(self):
+        x = np.array([1., 2., 3., 4., 5.])
+        xs = _TestRFFTBase.MockSeries(x)
+
+        expected = [1, 2, 3, 4, 5]
+        rfft(xs)
+
+        # Data should not have been overwritten
+        assert_equal(x, expected)
+        assert_equal(xs.data, expected)
+
+    def test_complex_input(self):
+        assert_raises(TypeError, rfft, np.arange(4, dtype=np.complex64))
+
+
+class TestRFFTDouble(_TestRFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex128
+        self.rdt = np.float64
+
+
+class TestRFFTSingle(_TestRFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex64
+        self.rdt = np.float32
+
+
+class _TestIRFFTBase:
+    def setup_method(self):
+        np.random.seed(1234)
+
+    def test_definition(self):
+        x1 = [1,2,3,4,1,2,3,4]
+        x1_1 = [1,2+3j,4+1j,2+3j,4,2-3j,4-1j,2-3j]
+        x2 = [1,2,3,4,1,2,3,4,5]
+        x2_1 = [1,2+3j,4+1j,2+3j,4+5j,4-5j,2-3j,4-1j,2-3j]
+
+        def _test(x, xr):
+            y = irfft(np.array(x, dtype=self.rdt))
+            y1 = direct_irdft(x)
+            assert_equal(y.dtype, self.rdt)
+            assert_array_almost_equal(y,y1, decimal=self.ndec)
+            assert_array_almost_equal(y,ifft(xr), decimal=self.ndec)
+
+        _test(x1, x1_1)
+        _test(x2, x2_1)
+
+    def test_random_real(self):
+        for size in [1,51,111,100,200,64,128,256,1024]:
+            x = random([size]).astype(self.rdt)
+            y1 = irfft(rfft(x))
+            y2 = rfft(irfft(x))
+            assert_equal(y1.dtype, self.rdt)
+            assert_equal(y2.dtype, self.rdt)
+            assert_array_almost_equal(y1, x, decimal=self.ndec,
+                                       err_msg="size=%d" % size)
+            assert_array_almost_equal(y2, x, decimal=self.ndec,
+                                       err_msg="size=%d" % size)
+
+    def test_size_accuracy(self):
+        # Sanity check for the accuracy for prime and non-prime sized inputs
+        if self.rdt == np.float32:
+            rtol = 1e-5
+        elif self.rdt == np.float64:
+            rtol = 1e-10
+
+        for size in LARGE_COMPOSITE_SIZES + LARGE_PRIME_SIZES:
+            np.random.seed(1234)
+            x = np.random.rand(size).astype(self.rdt)
+            y = irfft(rfft(x))
+            _assert_close_in_norm(x, y, rtol, size, self.rdt)
+            y = rfft(irfft(x))
+            _assert_close_in_norm(x, y, rtol, size, self.rdt)
+
+    def test_invalid_sizes(self):
+        assert_raises(ValueError, irfft, [])
+        assert_raises(ValueError, irfft, [[1,1],[2,2]], -5)
+
+    def test_complex_input(self):
+        assert_raises(TypeError, irfft, np.arange(4, dtype=np.complex64))
+
+
+# self.ndec is bogus; we should have a assert_array_approx_equal for number of
+# significant digits
+
+class TestIRFFTDouble(_TestIRFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex128
+        self.rdt = np.float64
+        self.ndec = 14
+
+
+class TestIRFFTSingle(_TestIRFFTBase):
+    def setup_method(self):
+        self.cdt = np.complex64
+        self.rdt = np.float32
+        self.ndec = 5
+
+
+class Testfft2:
+    def setup_method(self):
+        np.random.seed(1234)
+
+    def test_regression_244(self):
+        """FFT returns wrong result with axes parameter."""
+        # fftn (and hence fft2) used to break when both axes and shape were
+        # used
+        x = numpy.ones((4, 4, 2))
+        y = fft2(x, shape=(8, 8), axes=(-3, -2))
+        y_r = numpy.fft.fftn(x, s=(8, 8), axes=(-3, -2))
+        assert_array_almost_equal(y, y_r)
+
+    def test_invalid_sizes(self):
+        assert_raises(ValueError, fft2, [[]])
+        assert_raises(ValueError, fft2, [[1, 1], [2, 2]], (4, -3))
+
+
+class TestFftnSingle:
+    def setup_method(self):
+        np.random.seed(1234)
+
+    def test_definition(self):
+        x = [[1, 2, 3],
+             [4, 5, 6],
+             [7, 8, 9]]
+        y = fftn(np.array(x, np.float32))
+        assert_(y.dtype == np.complex64,
+                msg="double precision output with single precision")
+
+        y_r = np.array(fftn(x), np.complex64)
+        assert_array_almost_equal_nulp(y, y_r)
+
+    @pytest.mark.parametrize('size', SMALL_COMPOSITE_SIZES + SMALL_PRIME_SIZES)
+    def test_size_accuracy_small(self, size):
+        x = np.random.rand(size, size) + 1j*np.random.rand(size, size)
+        y1 = fftn(x.real.astype(np.float32))
+        y2 = fftn(x.real.astype(np.float64)).astype(np.complex64)
+
+        assert_equal(y1.dtype, np.complex64)
+        assert_array_almost_equal_nulp(y1, y2, 2000)
+
+    @pytest.mark.parametrize('size', LARGE_COMPOSITE_SIZES + LARGE_PRIME_SIZES)
+    def test_size_accuracy_large(self, size):
+        x = np.random.rand(size, 3) + 1j*np.random.rand(size, 3)
+        y1 = fftn(x.real.astype(np.float32))
+        y2 = fftn(x.real.astype(np.float64)).astype(np.complex64)
+
+        assert_equal(y1.dtype, np.complex64)
+        assert_array_almost_equal_nulp(y1, y2, 2000)
+
+    def test_definition_float16(self):
+        x = [[1, 2, 3],
+             [4, 5, 6],
+             [7, 8, 9]]
+        y = fftn(np.array(x, np.float16))
+        assert_equal(y.dtype, np.complex64)
+        y_r = np.array(fftn(x), np.complex64)
+        assert_array_almost_equal_nulp(y, y_r)
+
+    @pytest.mark.parametrize('size', SMALL_COMPOSITE_SIZES + SMALL_PRIME_SIZES)
+    def test_float16_input_small(self, size):
+        x = np.random.rand(size, size) + 1j*np.random.rand(size, size)
+        y1 = fftn(x.real.astype(np.float16))
+        y2 = fftn(x.real.astype(np.float64)).astype(np.complex64)
+
+        assert_equal(y1.dtype, np.complex64)
+        assert_array_almost_equal_nulp(y1, y2, 5e5)
+
+    @pytest.mark.parametrize('size', LARGE_COMPOSITE_SIZES + LARGE_PRIME_SIZES)
+    def test_float16_input_large(self, size):
+        x = np.random.rand(size, 3) + 1j*np.random.rand(size, 3)
+        y1 = fftn(x.real.astype(np.float16))
+        y2 = fftn(x.real.astype(np.float64)).astype(np.complex64)
+
+        assert_equal(y1.dtype, np.complex64)
+        assert_array_almost_equal_nulp(y1, y2, 2e6)
+
+
+class TestFftn:
+    def setup_method(self):
+        np.random.seed(1234)
+
+    def test_definition(self):
+        x = [[1, 2, 3],
+             [4, 5, 6],
+             [7, 8, 9]]
+        y = fftn(x)
+        assert_array_almost_equal(y, direct_dftn(x))
+
+        x = random((20, 26))
+        assert_array_almost_equal(fftn(x), direct_dftn(x))
+
+        x = random((5, 4, 3, 20))
+        assert_array_almost_equal(fftn(x), direct_dftn(x))
+
+    def test_axes_argument(self):
+        # plane == ji_plane, x== kji_space
+        plane1 = [[1, 2, 3],
+                  [4, 5, 6],
+                  [7, 8, 9]]
+        plane2 = [[10, 11, 12],
+                  [13, 14, 15],
+                  [16, 17, 18]]
+        plane3 = [[19, 20, 21],
+                  [22, 23, 24],
+                  [25, 26, 27]]
+        ki_plane1 = [[1, 2, 3],
+                     [10, 11, 12],
+                     [19, 20, 21]]
+        ki_plane2 = [[4, 5, 6],
+                     [13, 14, 15],
+                     [22, 23, 24]]
+        ki_plane3 = [[7, 8, 9],
+                     [16, 17, 18],
+                     [25, 26, 27]]
+        jk_plane1 = [[1, 10, 19],
+                     [4, 13, 22],
+                     [7, 16, 25]]
+        jk_plane2 = [[2, 11, 20],
+                     [5, 14, 23],
+                     [8, 17, 26]]
+        jk_plane3 = [[3, 12, 21],
+                     [6, 15, 24],
+                     [9, 18, 27]]
+        kj_plane1 = [[1, 4, 7],
+                     [10, 13, 16], [19, 22, 25]]
+        kj_plane2 = [[2, 5, 8],
+                     [11, 14, 17], [20, 23, 26]]
+        kj_plane3 = [[3, 6, 9],
+                     [12, 15, 18], [21, 24, 27]]
+        ij_plane1 = [[1, 4, 7],
+                     [2, 5, 8],
+                     [3, 6, 9]]
+        ij_plane2 = [[10, 13, 16],
+                     [11, 14, 17],
+                     [12, 15, 18]]
+        ij_plane3 = [[19, 22, 25],
+                     [20, 23, 26],
+                     [21, 24, 27]]
+        ik_plane1 = [[1, 10, 19],
+                     [2, 11, 20],
+                     [3, 12, 21]]
+        ik_plane2 = [[4, 13, 22],
+                     [5, 14, 23],
+                     [6, 15, 24]]
+        ik_plane3 = [[7, 16, 25],
+                     [8, 17, 26],
+                     [9, 18, 27]]
+        ijk_space = [jk_plane1, jk_plane2, jk_plane3]
+        ikj_space = [kj_plane1, kj_plane2, kj_plane3]
+        jik_space = [ik_plane1, ik_plane2, ik_plane3]
+        jki_space = [ki_plane1, ki_plane2, ki_plane3]
+        kij_space = [ij_plane1, ij_plane2, ij_plane3]
+        x = array([plane1, plane2, plane3])
+
+        assert_array_almost_equal(fftn(x),
+                                  fftn(x, axes=(-3, -2, -1)))  # kji_space
+        assert_array_almost_equal(fftn(x), fftn(x, axes=(0, 1, 2)))
+        assert_array_almost_equal(fftn(x, axes=(0, 2)), fftn(x, axes=(0, -1)))
+        y = fftn(x, axes=(2, 1, 0))  # ijk_space
+        assert_array_almost_equal(swapaxes(y, -1, -3), fftn(ijk_space))
+        y = fftn(x, axes=(2, 0, 1))  # ikj_space
+        assert_array_almost_equal(swapaxes(swapaxes(y, -1, -3), -1, -2),
+                                  fftn(ikj_space))
+        y = fftn(x, axes=(1, 2, 0))  # jik_space
+        assert_array_almost_equal(swapaxes(swapaxes(y, -1, -3), -3, -2),
+                                  fftn(jik_space))
+        y = fftn(x, axes=(1, 0, 2))  # jki_space
+        assert_array_almost_equal(swapaxes(y, -2, -3), fftn(jki_space))
+        y = fftn(x, axes=(0, 2, 1))  # kij_space
+        assert_array_almost_equal(swapaxes(y, -2, -1), fftn(kij_space))
+
+        y = fftn(x, axes=(-2, -1))  # ji_plane
+        assert_array_almost_equal(fftn(plane1), y[0])
+        assert_array_almost_equal(fftn(plane2), y[1])
+        assert_array_almost_equal(fftn(plane3), y[2])
+
+        y = fftn(x, axes=(1, 2))  # ji_plane
+        assert_array_almost_equal(fftn(plane1), y[0])
+        assert_array_almost_equal(fftn(plane2), y[1])
+        assert_array_almost_equal(fftn(plane3), y[2])
+
+        y = fftn(x, axes=(-3, -2))  # kj_plane
+        assert_array_almost_equal(fftn(x[:, :, 0]), y[:, :, 0])
+        assert_array_almost_equal(fftn(x[:, :, 1]), y[:, :, 1])
+        assert_array_almost_equal(fftn(x[:, :, 2]), y[:, :, 2])
+
+        y = fftn(x, axes=(-3, -1))  # ki_plane
+        assert_array_almost_equal(fftn(x[:, 0, :]), y[:, 0, :])
+        assert_array_almost_equal(fftn(x[:, 1, :]), y[:, 1, :])
+        assert_array_almost_equal(fftn(x[:, 2, :]), y[:, 2, :])
+
+        y = fftn(x, axes=(-1, -2))  # ij_plane
+        assert_array_almost_equal(fftn(ij_plane1), swapaxes(y[0], -2, -1))
+        assert_array_almost_equal(fftn(ij_plane2), swapaxes(y[1], -2, -1))
+        assert_array_almost_equal(fftn(ij_plane3), swapaxes(y[2], -2, -1))
+
+        y = fftn(x, axes=(-1, -3))  # ik_plane
+        assert_array_almost_equal(fftn(ik_plane1),
+                                  swapaxes(y[:, 0, :], -1, -2))
+        assert_array_almost_equal(fftn(ik_plane2),
+                                  swapaxes(y[:, 1, :], -1, -2))
+        assert_array_almost_equal(fftn(ik_plane3),
+                                  swapaxes(y[:, 2, :], -1, -2))
+
+        y = fftn(x, axes=(-2, -3))  # jk_plane
+        assert_array_almost_equal(fftn(jk_plane1),
+                                  swapaxes(y[:, :, 0], -1, -2))
+        assert_array_almost_equal(fftn(jk_plane2),
+                                  swapaxes(y[:, :, 1], -1, -2))
+        assert_array_almost_equal(fftn(jk_plane3),
+                                  swapaxes(y[:, :, 2], -1, -2))
+
+        y = fftn(x, axes=(-1,))  # i_line
+        for i in range(3):
+            for j in range(3):
+                assert_array_almost_equal(fft(x[i, j, :]), y[i, j, :])
+        y = fftn(x, axes=(-2,))  # j_line
+        for i in range(3):
+            for j in range(3):
+                assert_array_almost_equal(fft(x[i, :, j]), y[i, :, j])
+        y = fftn(x, axes=(0,))  # k_line
+        for i in range(3):
+            for j in range(3):
+                assert_array_almost_equal(fft(x[:, i, j]), y[:, i, j])
+
+        y = fftn(x, axes=())  # point
+        assert_array_almost_equal(y, x)
+
+    def test_shape_argument(self):
+        small_x = [[1, 2, 3],
+                   [4, 5, 6]]
+        large_x1 = [[1, 2, 3, 0],
+                    [4, 5, 6, 0],
+                    [0, 0, 0, 0],
+                    [0, 0, 0, 0]]
+
+        y = fftn(small_x, shape=(4, 4))
+        assert_array_almost_equal(y, fftn(large_x1))
+
+        y = fftn(small_x, shape=(3, 4))
+        assert_array_almost_equal(y, fftn(large_x1[:-1]))
+
+    def test_shape_axes_argument(self):
+        small_x = [[1, 2, 3],
+                   [4, 5, 6],
+                   [7, 8, 9]]
+        large_x1 = array([[1, 2, 3, 0],
+                          [4, 5, 6, 0],
+                          [7, 8, 9, 0],
+                          [0, 0, 0, 0]])
+        y = fftn(small_x, shape=(4, 4), axes=(-2, -1))
+        assert_array_almost_equal(y, fftn(large_x1))
+        y = fftn(small_x, shape=(4, 4), axes=(-1, -2))
+
+        assert_array_almost_equal(y, swapaxes(
+            fftn(swapaxes(large_x1, -1, -2)), -1, -2))
+
+    def test_shape_axes_argument2(self):
+        # Change shape of the last axis
+        x = numpy.random.random((10, 5, 3, 7))
+        y = fftn(x, axes=(-1,), shape=(8,))
+        assert_array_almost_equal(y, fft(x, axis=-1, n=8))
+
+        # Change shape of an arbitrary axis which is not the last one
+        x = numpy.random.random((10, 5, 3, 7))
+        y = fftn(x, axes=(-2,), shape=(8,))
+        assert_array_almost_equal(y, fft(x, axis=-2, n=8))
+
+        # Change shape of axes: cf #244, where shape and axes were mixed up
+        x = numpy.random.random((4, 4, 2))
+        y = fftn(x, axes=(-3, -2), shape=(8, 8))
+        assert_array_almost_equal(y,
+                                  numpy.fft.fftn(x, axes=(-3, -2), s=(8, 8)))
+
+    def test_shape_argument_more(self):
+        x = zeros((4, 4, 2))
+        with assert_raises(ValueError,
+                           match="when given, axes and shape arguments"
+                           " have to be of the same length"):
+            fftn(x, shape=(8, 8, 2, 1))
+
+    def test_invalid_sizes(self):
+        with assert_raises(ValueError,
+                           match="invalid number of data points"
+                           r" \(\[1, 0\]\) specified"):
+            fftn([[]])
+
+        with assert_raises(ValueError,
+                           match="invalid number of data points"
+                           r" \(\[4, -3\]\) specified"):
+            fftn([[1, 1], [2, 2]], (4, -3))
+
+
+class TestIfftn:
+    dtype = None
+    cdtype = None
+
+    def setup_method(self):
+        np.random.seed(1234)
+
+    @pytest.mark.parametrize('dtype,cdtype,maxnlp',
+                             [(np.float64, np.complex128, 2000),
+                              (np.float32, np.complex64, 3500)])
+    def test_definition(self, dtype, cdtype, maxnlp):
+        x = np.array([[1, 2, 3],
+                      [4, 5, 6],
+                      [7, 8, 9]], dtype=dtype)
+        y = ifftn(x)
+        assert_equal(y.dtype, cdtype)
+        assert_array_almost_equal_nulp(y, direct_idftn(x), maxnlp)
+
+        x = random((20, 26))
+        assert_array_almost_equal_nulp(ifftn(x), direct_idftn(x), maxnlp)
+
+        x = random((5, 4, 3, 20))
+        assert_array_almost_equal_nulp(ifftn(x), direct_idftn(x), maxnlp)
+
+    @pytest.mark.parametrize('maxnlp', [2000, 3500])
+    @pytest.mark.parametrize('size', [1, 2, 51, 32, 64, 92])
+    def test_random_complex(self, maxnlp, size):
+        x = random([size, size]) + 1j*random([size, size])
+        assert_array_almost_equal_nulp(ifftn(fftn(x)), x, maxnlp)
+        assert_array_almost_equal_nulp(fftn(ifftn(x)), x, maxnlp)
+
+    def test_invalid_sizes(self):
+        with assert_raises(ValueError,
+                           match="invalid number of data points"
+                           r" \(\[1, 0\]\) specified"):
+            ifftn([[]])
+
+        with assert_raises(ValueError,
+                           match="invalid number of data points"
+                           r" \(\[4, -3\]\) specified"):
+            ifftn([[1, 1], [2, 2]], (4, -3))
+
+
+class FakeArray:
+    def __init__(self, data):
+        self._data = data
+        self.__array_interface__ = data.__array_interface__
+
+
+class FakeArray2:
+    def __init__(self, data):
+        self._data = data
+
+    def __array__(self, dtype=None, copy=None):
+        return self._data
+
+
+class TestOverwrite:
+    """Check input overwrite behavior of the FFT functions."""
+
+    real_dtypes = (np.float32, np.float64)
+    dtypes = real_dtypes + (np.complex64, np.complex128)
+    fftsizes = [8, 16, 32]
+
+    def _check(self, x, routine, fftsize, axis, overwrite_x):
+        x2 = x.copy()
+        for fake in [lambda x: x, FakeArray, FakeArray2]:
+            routine(fake(x2), fftsize, axis, overwrite_x=overwrite_x)
+
+            sig = "{}({}{!r}, {!r}, axis={!r}, overwrite_x={!r})".format(
+                routine.__name__, x.dtype, x.shape, fftsize, axis, overwrite_x)
+            if not overwrite_x:
+                assert_equal(x2, x, err_msg="spurious overwrite in %s" % sig)
+
+    def _check_1d(self, routine, dtype, shape, axis, overwritable_dtypes,
+                  fftsize, overwrite_x):
+        np.random.seed(1234)
+        if np.issubdtype(dtype, np.complexfloating):
+            data = np.random.randn(*shape) + 1j*np.random.randn(*shape)
+        else:
+            data = np.random.randn(*shape)
+        data = data.astype(dtype)
+
+        self._check(data, routine, fftsize, axis,
+                    overwrite_x=overwrite_x)
+
+    @pytest.mark.parametrize('dtype', dtypes)
+    @pytest.mark.parametrize('fftsize', fftsizes)
+    @pytest.mark.parametrize('overwrite_x', [True, False])
+    @pytest.mark.parametrize('shape,axes', [((16,), -1),
+                                            ((16, 2), 0),
+                                            ((2, 16), 1)])
+    def test_fft_ifft(self, dtype, fftsize, overwrite_x, shape, axes):
+        overwritable = (np.complex128, np.complex64)
+        self._check_1d(fft, dtype, shape, axes, overwritable,
+                       fftsize, overwrite_x)
+        self._check_1d(ifft, dtype, shape, axes, overwritable,
+                       fftsize, overwrite_x)
+
+    @pytest.mark.parametrize('dtype', real_dtypes)
+    @pytest.mark.parametrize('fftsize', fftsizes)
+    @pytest.mark.parametrize('overwrite_x', [True, False])
+    @pytest.mark.parametrize('shape,axes', [((16,), -1),
+                                            ((16, 2), 0),
+                                            ((2, 16), 1)])
+    def test_rfft_irfft(self, dtype, fftsize, overwrite_x, shape, axes):
+        overwritable = self.real_dtypes
+        self._check_1d(irfft, dtype, shape, axes, overwritable,
+                       fftsize, overwrite_x)
+        self._check_1d(rfft, dtype, shape, axes, overwritable,
+                       fftsize, overwrite_x)
+
+    def _check_nd_one(self, routine, dtype, shape, axes, overwritable_dtypes,
+                      overwrite_x):
+        np.random.seed(1234)
+        if np.issubdtype(dtype, np.complexfloating):
+            data = np.random.randn(*shape) + 1j*np.random.randn(*shape)
+        else:
+            data = np.random.randn(*shape)
+        data = data.astype(dtype)
+
+        def fftshape_iter(shp):
+            if len(shp) <= 0:
+                yield ()
+            else:
+                for j in (shp[0]//2, shp[0], shp[0]*2):
+                    for rest in fftshape_iter(shp[1:]):
+                        yield (j,) + rest
+
+        if axes is None:
+            part_shape = shape
+        else:
+            part_shape = tuple(np.take(shape, axes))
+
+        for fftshape in fftshape_iter(part_shape):
+            self._check(data, routine, fftshape, axes,
+                        overwrite_x=overwrite_x)
+            if data.ndim > 1:
+                self._check(data.T, routine, fftshape, axes,
+                            overwrite_x=overwrite_x)
+
+    @pytest.mark.parametrize('dtype', dtypes)
+    @pytest.mark.parametrize('overwrite_x', [True, False])
+    @pytest.mark.parametrize('shape,axes', [((16,), None),
+                                            ((16,), (0,)),
+                                            ((16, 2), (0,)),
+                                            ((2, 16), (1,)),
+                                            ((8, 16), None),
+                                            ((8, 16), (0, 1)),
+                                            ((8, 16, 2), (0, 1)),
+                                            ((8, 16, 2), (1, 2)),
+                                            ((8, 16, 2), (0,)),
+                                            ((8, 16, 2), (1,)),
+                                            ((8, 16, 2), (2,)),
+                                            ((8, 16, 2), None),
+                                            ((8, 16, 2), (0, 1, 2))])
+    def test_fftn_ifftn(self, dtype, overwrite_x, shape, axes):
+        overwritable = (np.complex128, np.complex64)
+        self._check_nd_one(fftn, dtype, shape, axes, overwritable,
+                           overwrite_x)
+        self._check_nd_one(ifftn, dtype, shape, axes, overwritable,
+                           overwrite_x)
+
+
+@pytest.mark.parametrize('func', [fftn, ifftn, fft2])
+def test_shape_axes_ndarray(func):
+    # Test fftn and ifftn work with NumPy arrays for shape and axes arguments
+    # Regression test for gh-13342
+    a = np.random.rand(10, 10)
+
+    expect = func(a, shape=(5, 5))
+    actual = func(a, shape=np.array([5, 5]))
+    assert_equal(expect, actual)
+
+    expect = func(a, axes=(-1,))
+    actual = func(a, axes=np.array([-1,]))
+    assert_equal(expect, actual)
+
+    expect = func(a, shape=(4, 7), axes=(1, 0))
+    actual = func(a, shape=np.array([4, 7]), axes=np.array([1, 0]))
+    assert_equal(expect, actual)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/tests/test_helper.py

@@ -0,0 +1,54 @@
+# Created by Pearu Peterson, September 2002
+
+__usage__ = """
+Build fftpack:
+  python setup_fftpack.py build
+Run tests if scipy is installed:
+  python -c 'import scipy;scipy.fftpack.test(<level>)'
+Run tests if fftpack is not installed:
+  python tests/test_helper.py [<level>]
+"""
+
+from numpy.testing import assert_array_almost_equal
+from scipy.fftpack import fftshift, ifftshift, fftfreq, rfftfreq
+
+from numpy import pi, random
+
+class TestFFTShift:
+
+    def test_definition(self):
+        x = [0,1,2,3,4,-4,-3,-2,-1]
+        y = [-4,-3,-2,-1,0,1,2,3,4]
+        assert_array_almost_equal(fftshift(x),y)
+        assert_array_almost_equal(ifftshift(y),x)
+        x = [0,1,2,3,4,-5,-4,-3,-2,-1]
+        y = [-5,-4,-3,-2,-1,0,1,2,3,4]
+        assert_array_almost_equal(fftshift(x),y)
+        assert_array_almost_equal(ifftshift(y),x)
+
+    def test_inverse(self):
+        for n in [1,4,9,100,211]:
+            x = random.random((n,))
+            assert_array_almost_equal(ifftshift(fftshift(x)),x)
+
+
+class TestFFTFreq:
+
+    def test_definition(self):
+        x = [0,1,2,3,4,-4,-3,-2,-1]
+        assert_array_almost_equal(9*fftfreq(9),x)
+        assert_array_almost_equal(9*pi*fftfreq(9,pi),x)
+        x = [0,1,2,3,4,-5,-4,-3,-2,-1]
+        assert_array_almost_equal(10*fftfreq(10),x)
+        assert_array_almost_equal(10*pi*fftfreq(10,pi),x)
+
+
+class TestRFFTFreq:
+
+    def test_definition(self):
+        x = [0,1,1,2,2,3,3,4,4]
+        assert_array_almost_equal(9*rfftfreq(9),x)
+        assert_array_almost_equal(9*pi*rfftfreq(9,pi),x)
+        x = [0,1,1,2,2,3,3,4,4,5]
+        assert_array_almost_equal(10*rfftfreq(10),x)
+        assert_array_almost_equal(10*pi*rfftfreq(10,pi),x)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/tests/test_import.py

@@ -0,0 +1,31 @@
+"""Test possibility of patching fftpack with pyfftw.
+
+No module source outside of scipy.fftpack should contain an import of
+the form `from scipy.fftpack import ...`, so that a simple replacement
+of scipy.fftpack by the corresponding fftw interface completely swaps
+the two FFT implementations.
+
+Because this simply inspects source files, we only need to run the test
+on one version of Python.
+"""
+
+
+from pathlib import Path
+import re
+import tokenize
+from numpy.testing import assert_
+import scipy
+
+class TestFFTPackImport:
+    def test_fftpack_import(self):
+        base = Path(scipy.__file__).parent
+        regexp = r"\s*from.+\.fftpack import .*\n"
+        for path in base.rglob("*.py"):
+            if base / "fftpack" in path.parents:
+                continue
+            # use tokenize to auto-detect encoding on systems where no
+            # default encoding is defined (e.g., LANG='C')
+            with tokenize.open(str(path)) as file:
+                assert_(all(not re.fullmatch(regexp, line)
+                            for line in file),
+                        f"{path} contains an import from fftpack")

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/tests/test_pseudo_diffs.py

@@ -0,0 +1,380 @@
+# Created by Pearu Peterson, September 2002
+
+__usage__ = """
+Build fftpack:
+  python setup_fftpack.py build
+Run tests if scipy is installed:
+  python -c 'import scipy;scipy.fftpack.test(<level>)'
+Run tests if fftpack is not installed:
+  python tests/test_pseudo_diffs.py [<level>]
+"""
+
+from numpy.testing import (assert_equal, assert_almost_equal,
+                           assert_array_almost_equal)
+from scipy.fftpack import (diff, fft, ifft, tilbert, itilbert, hilbert,
+                           ihilbert, shift, fftfreq, cs_diff, sc_diff,
+                           ss_diff, cc_diff)
+
+import numpy as np
+from numpy import arange, sin, cos, pi, exp, tanh, sum, sign
+from numpy.random import random
+
+
+def direct_diff(x,k=1,period=None):
+    fx = fft(x)
+    n = len(fx)
+    if period is None:
+        period = 2*pi
+    w = fftfreq(n)*2j*pi/period*n
+    if k < 0:
+        w = 1 / w**k
+        w[0] = 0.0
+    else:
+        w = w**k
+    if n > 2000:
+        w[250:n-250] = 0.0
+    return ifft(w*fx).real
+
+
+def direct_tilbert(x,h=1,period=None):
+    fx = fft(x)
+    n = len(fx)
+    if period is None:
+        period = 2*pi
+    w = fftfreq(n)*h*2*pi/period*n
+    w[0] = 1
+    w = 1j/tanh(w)
+    w[0] = 0j
+    return ifft(w*fx)
+
+
+def direct_itilbert(x,h=1,period=None):
+    fx = fft(x)
+    n = len(fx)
+    if period is None:
+        period = 2*pi
+    w = fftfreq(n)*h*2*pi/period*n
+    w = -1j*tanh(w)
+    return ifft(w*fx)
+
+
+def direct_hilbert(x):
+    fx = fft(x)
+    n = len(fx)
+    w = fftfreq(n)*n
+    w = 1j*sign(w)
+    return ifft(w*fx)
+
+
+def direct_ihilbert(x):
+    return -direct_hilbert(x)
+
+
+def direct_shift(x,a,period=None):
+    n = len(x)
+    if period is None:
+        k = fftfreq(n)*1j*n
+    else:
+        k = fftfreq(n)*2j*pi/period*n
+    return ifft(fft(x)*exp(k*a)).real
+
+
+class TestDiff:
+
+    def test_definition(self):
+        for n in [16,17,64,127,32]:
+            x = arange(n)*2*pi/n
+            assert_array_almost_equal(diff(sin(x)),direct_diff(sin(x)))
+            assert_array_almost_equal(diff(sin(x),2),direct_diff(sin(x),2))
+            assert_array_almost_equal(diff(sin(x),3),direct_diff(sin(x),3))
+            assert_array_almost_equal(diff(sin(x),4),direct_diff(sin(x),4))
+            assert_array_almost_equal(diff(sin(x),5),direct_diff(sin(x),5))
+            assert_array_almost_equal(diff(sin(2*x),3),direct_diff(sin(2*x),3))
+            assert_array_almost_equal(diff(sin(2*x),4),direct_diff(sin(2*x),4))
+            assert_array_almost_equal(diff(cos(x)),direct_diff(cos(x)))
+            assert_array_almost_equal(diff(cos(x),2),direct_diff(cos(x),2))
+            assert_array_almost_equal(diff(cos(x),3),direct_diff(cos(x),3))
+            assert_array_almost_equal(diff(cos(x),4),direct_diff(cos(x),4))
+            assert_array_almost_equal(diff(cos(2*x)),direct_diff(cos(2*x)))
+            assert_array_almost_equal(diff(sin(x*n/8)),direct_diff(sin(x*n/8)))
+            assert_array_almost_equal(diff(cos(x*n/8)),direct_diff(cos(x*n/8)))
+            for k in range(5):
+                assert_array_almost_equal(diff(sin(4*x),k),direct_diff(sin(4*x),k))
+                assert_array_almost_equal(diff(cos(4*x),k),direct_diff(cos(4*x),k))
+
+    def test_period(self):
+        for n in [17,64]:
+            x = arange(n)/float(n)
+            assert_array_almost_equal(diff(sin(2*pi*x),period=1),
+                                      2*pi*cos(2*pi*x))
+            assert_array_almost_equal(diff(sin(2*pi*x),3,period=1),
+                                      -(2*pi)**3*cos(2*pi*x))
+
+    def test_sin(self):
+        for n in [32,64,77]:
+            x = arange(n)*2*pi/n
+            assert_array_almost_equal(diff(sin(x)),cos(x))
+            assert_array_almost_equal(diff(cos(x)),-sin(x))
+            assert_array_almost_equal(diff(sin(x),2),-sin(x))
+            assert_array_almost_equal(diff(sin(x),4),sin(x))
+            assert_array_almost_equal(diff(sin(4*x)),4*cos(4*x))
+            assert_array_almost_equal(diff(sin(sin(x))),cos(x)*cos(sin(x)))
+
+    def test_expr(self):
+        for n in [64,77,100,128,256,512,1024,2048,4096,8192][:5]:
+            x = arange(n)*2*pi/n
+            f = sin(x)*cos(4*x)+exp(sin(3*x))
+            df = cos(x)*cos(4*x)-4*sin(x)*sin(4*x)+3*cos(3*x)*exp(sin(3*x))
+            ddf = -17*sin(x)*cos(4*x)-8*cos(x)*sin(4*x)\
+                 - 9*sin(3*x)*exp(sin(3*x))+9*cos(3*x)**2*exp(sin(3*x))
+            d1 = diff(f)
+            assert_array_almost_equal(d1,df)
+            assert_array_almost_equal(diff(df),ddf)
+            assert_array_almost_equal(diff(f,2),ddf)
+            assert_array_almost_equal(diff(ddf,-1),df)
+
+    def test_expr_large(self):
+        for n in [2048,4096]:
+            x = arange(n)*2*pi/n
+            f = sin(x)*cos(4*x)+exp(sin(3*x))
+            df = cos(x)*cos(4*x)-4*sin(x)*sin(4*x)+3*cos(3*x)*exp(sin(3*x))
+            ddf = -17*sin(x)*cos(4*x)-8*cos(x)*sin(4*x)\
+                 - 9*sin(3*x)*exp(sin(3*x))+9*cos(3*x)**2*exp(sin(3*x))
+            assert_array_almost_equal(diff(f),df)
+            assert_array_almost_equal(diff(df),ddf)
+            assert_array_almost_equal(diff(ddf,-1),df)
+            assert_array_almost_equal(diff(f,2),ddf)
+
+    def test_int(self):
+        n = 64
+        x = arange(n)*2*pi/n
+        assert_array_almost_equal(diff(sin(x),-1),-cos(x))
+        assert_array_almost_equal(diff(sin(x),-2),-sin(x))
+        assert_array_almost_equal(diff(sin(x),-4),sin(x))
+        assert_array_almost_equal(diff(2*cos(2*x),-1),sin(2*x))
+
+    def test_random_even(self):
+        for k in [0,2,4,6]:
+            for n in [60,32,64,56,55]:
+                f = random((n,))
+                af = sum(f,axis=0)/n
+                f = f-af
+                # zeroing Nyquist mode:
+                f = diff(diff(f,1),-1)
+                assert_almost_equal(sum(f,axis=0),0.0)
+                assert_array_almost_equal(diff(diff(f,k),-k),f)
+                assert_array_almost_equal(diff(diff(f,-k),k),f)
+
+    def test_random_odd(self):
+        for k in [0,1,2,3,4,5,6]:
+            for n in [33,65,55]:
+                f = random((n,))
+                af = sum(f,axis=0)/n
+                f = f-af
+                assert_almost_equal(sum(f,axis=0),0.0)
+                assert_array_almost_equal(diff(diff(f,k),-k),f)
+                assert_array_almost_equal(diff(diff(f,-k),k),f)
+
+    def test_zero_nyquist(self):
+        for k in [0,1,2,3,4,5,6]:
+            for n in [32,33,64,56,55]:
+                f = random((n,))
+                af = sum(f,axis=0)/n
+                f = f-af
+                # zeroing Nyquist mode:
+                f = diff(diff(f,1),-1)
+                assert_almost_equal(sum(f,axis=0),0.0)
+                assert_array_almost_equal(diff(diff(f,k),-k),f)
+                assert_array_almost_equal(diff(diff(f,-k),k),f)
+
+
+class TestTilbert:
+
+    def test_definition(self):
+        for h in [0.1,0.5,1,5.5,10]:
+            for n in [16,17,64,127]:
+                x = arange(n)*2*pi/n
+                y = tilbert(sin(x),h)
+                y1 = direct_tilbert(sin(x),h)
+                assert_array_almost_equal(y,y1)
+                assert_array_almost_equal(tilbert(sin(x),h),
+                                          direct_tilbert(sin(x),h))
+                assert_array_almost_equal(tilbert(sin(2*x),h),
+                                          direct_tilbert(sin(2*x),h))
+
+    def test_random_even(self):
+        for h in [0.1,0.5,1,5.5,10]:
+            for n in [32,64,56]:
+                f = random((n,))
+                af = sum(f,axis=0)/n
+                f = f-af
+                assert_almost_equal(sum(f,axis=0),0.0)
+                assert_array_almost_equal(direct_tilbert(direct_itilbert(f,h),h),f)
+
+    def test_random_odd(self):
+        for h in [0.1,0.5,1,5.5,10]:
+            for n in [33,65,55]:
+                f = random((n,))
+                af = sum(f,axis=0)/n
+                f = f-af
+                assert_almost_equal(sum(f,axis=0),0.0)
+                assert_array_almost_equal(itilbert(tilbert(f,h),h),f)
+                assert_array_almost_equal(tilbert(itilbert(f,h),h),f)
+
+
+class TestITilbert:
+
+    def test_definition(self):
+        for h in [0.1,0.5,1,5.5,10]:
+            for n in [16,17,64,127]:
+                x = arange(n)*2*pi/n
+                y = itilbert(sin(x),h)
+                y1 = direct_itilbert(sin(x),h)
+                assert_array_almost_equal(y,y1)
+                assert_array_almost_equal(itilbert(sin(x),h),
+                                          direct_itilbert(sin(x),h))
+                assert_array_almost_equal(itilbert(sin(2*x),h),
+                                          direct_itilbert(sin(2*x),h))
+
+
+class TestHilbert:
+
+    def test_definition(self):
+        for n in [16,17,64,127]:
+            x = arange(n)*2*pi/n
+            y = hilbert(sin(x))
+            y1 = direct_hilbert(sin(x))
+            assert_array_almost_equal(y,y1)
+            assert_array_almost_equal(hilbert(sin(2*x)),
+                                      direct_hilbert(sin(2*x)))
+
+    def test_tilbert_relation(self):
+        for n in [16,17,64,127]:
+            x = arange(n)*2*pi/n
+            f = sin(x)+cos(2*x)*sin(x)
+            y = hilbert(f)
+            y1 = direct_hilbert(f)
+            assert_array_almost_equal(y,y1)
+            y2 = tilbert(f,h=10)
+            assert_array_almost_equal(y,y2)
+
+    def test_random_odd(self):
+        for n in [33,65,55]:
+            f = random((n,))
+            af = sum(f,axis=0)/n
+            f = f-af
+            assert_almost_equal(sum(f,axis=0),0.0)
+            assert_array_almost_equal(ihilbert(hilbert(f)),f)
+            assert_array_almost_equal(hilbert(ihilbert(f)),f)
+
+    def test_random_even(self):
+        for n in [32,64,56]:
+            f = random((n,))
+            af = sum(f,axis=0)/n
+            f = f-af
+            # zeroing Nyquist mode:
+            f = diff(diff(f,1),-1)
+            assert_almost_equal(sum(f,axis=0),0.0)
+            assert_array_almost_equal(direct_hilbert(direct_ihilbert(f)),f)
+            assert_array_almost_equal(hilbert(ihilbert(f)),f)
+
+
+class TestIHilbert:
+
+    def test_definition(self):
+        for n in [16,17,64,127]:
+            x = arange(n)*2*pi/n
+            y = ihilbert(sin(x))
+            y1 = direct_ihilbert(sin(x))
+            assert_array_almost_equal(y,y1)
+            assert_array_almost_equal(ihilbert(sin(2*x)),
+                                      direct_ihilbert(sin(2*x)))
+
+    def test_itilbert_relation(self):
+        for n in [16,17,64,127]:
+            x = arange(n)*2*pi/n
+            f = sin(x)+cos(2*x)*sin(x)
+            y = ihilbert(f)
+            y1 = direct_ihilbert(f)
+            assert_array_almost_equal(y,y1)
+            y2 = itilbert(f,h=10)
+            assert_array_almost_equal(y,y2)
+
+
+class TestShift:
+
+    def test_definition(self):
+        for n in [18,17,64,127,32,2048,256]:
+            x = arange(n)*2*pi/n
+            for a in [0.1,3]:
+                assert_array_almost_equal(shift(sin(x),a),direct_shift(sin(x),a))
+                assert_array_almost_equal(shift(sin(x),a),sin(x+a))
+                assert_array_almost_equal(shift(cos(x),a),cos(x+a))
+                assert_array_almost_equal(shift(cos(2*x)+sin(x),a),
+                                          cos(2*(x+a))+sin(x+a))
+                assert_array_almost_equal(shift(exp(sin(x)),a),exp(sin(x+a)))
+            assert_array_almost_equal(shift(sin(x),2*pi),sin(x))
+            assert_array_almost_equal(shift(sin(x),pi),-sin(x))
+            assert_array_almost_equal(shift(sin(x),pi/2),cos(x))
+
+
+class TestOverwrite:
+    """Check input overwrite behavior """
+
+    real_dtypes = (np.float32, np.float64)
+    dtypes = real_dtypes + (np.complex64, np.complex128)
+
+    def _check(self, x, routine, *args, **kwargs):
+        x2 = x.copy()
+        routine(x2, *args, **kwargs)
+        sig = routine.__name__
+        if args:
+            sig += repr(args)
+        if kwargs:
+            sig += repr(kwargs)
+        assert_equal(x2, x, err_msg="spurious overwrite in %s" % sig)
+
+    def _check_1d(self, routine, dtype, shape, *args, **kwargs):
+        np.random.seed(1234)
+        if np.issubdtype(dtype, np.complexfloating):
+            data = np.random.randn(*shape) + 1j*np.random.randn(*shape)
+        else:
+            data = np.random.randn(*shape)
+        data = data.astype(dtype)
+        self._check(data, routine, *args, **kwargs)
+
+    def test_diff(self):
+        for dtype in self.dtypes:
+            self._check_1d(diff, dtype, (16,))
+
+    def test_tilbert(self):
+        for dtype in self.dtypes:
+            self._check_1d(tilbert, dtype, (16,), 1.6)
+
+    def test_itilbert(self):
+        for dtype in self.dtypes:
+            self._check_1d(itilbert, dtype, (16,), 1.6)
+
+    def test_hilbert(self):
+        for dtype in self.dtypes:
+            self._check_1d(hilbert, dtype, (16,))
+
+    def test_cs_diff(self):
+        for dtype in self.dtypes:
+            self._check_1d(cs_diff, dtype, (16,), 1.0, 4.0)
+
+    def test_sc_diff(self):
+        for dtype in self.dtypes:
+            self._check_1d(sc_diff, dtype, (16,), 1.0, 4.0)
+
+    def test_ss_diff(self):
+        for dtype in self.dtypes:
+            self._check_1d(ss_diff, dtype, (16,), 1.0, 4.0)
+
+    def test_cc_diff(self):
+        for dtype in self.dtypes:
+            self._check_1d(cc_diff, dtype, (16,), 1.0, 4.0)
+
+    def test_shift(self):
+        for dtype in self.dtypes:
+            self._check_1d(shift, dtype, (16,), 1.0)

llmeval-env/lib/python3.10/site-packages/scipy/fftpack/tests/test_real_transforms.py

@@ -0,0 +1,815 @@
+from os.path import join, dirname
+
+import numpy as np
+from numpy.testing import assert_array_almost_equal, assert_equal
+import pytest
+from pytest import raises as assert_raises
+
+from scipy.fftpack._realtransforms import (
+    dct, idct, dst, idst, dctn, idctn, dstn, idstn)
+
+# Matlab reference data
+MDATA = np.load(join(dirname(__file__), 'test.npz'))
+X = [MDATA['x%d' % i] for i in range(8)]
+Y = [MDATA['y%d' % i] for i in range(8)]
+
+# FFTW reference data: the data are organized as follows:
+#    * SIZES is an array containing all available sizes
+#    * for every type (1, 2, 3, 4) and every size, the array dct_type_size
+#    contains the output of the DCT applied to the input np.linspace(0, size-1,
+#    size)
+FFTWDATA_DOUBLE = np.load(join(dirname(__file__), 'fftw_double_ref.npz'))
+FFTWDATA_SINGLE = np.load(join(dirname(__file__), 'fftw_single_ref.npz'))
+FFTWDATA_SIZES = FFTWDATA_DOUBLE['sizes']
+
+
+def fftw_dct_ref(type, size, dt):
+    x = np.linspace(0, size-1, size).astype(dt)
+    dt = np.result_type(np.float32, dt)
+    if dt == np.float64:
+        data = FFTWDATA_DOUBLE
+    elif dt == np.float32:
+        data = FFTWDATA_SINGLE
+    else:
+        raise ValueError()
+    y = (data['dct_%d_%d' % (type, size)]).astype(dt)
+    return x, y, dt
+
+
+def fftw_dst_ref(type, size, dt):
+    x = np.linspace(0, size-1, size).astype(dt)
+    dt = np.result_type(np.float32, dt)
+    if dt == np.float64:
+        data = FFTWDATA_DOUBLE
+    elif dt == np.float32:
+        data = FFTWDATA_SINGLE
+    else:
+        raise ValueError()
+    y = (data['dst_%d_%d' % (type, size)]).astype(dt)
+    return x, y, dt
+
+
+def dct_2d_ref(x, **kwargs):
+    """Calculate reference values for testing dct2."""
+    x = np.array(x, copy=True)
+    for row in range(x.shape[0]):
+        x[row, :] = dct(x[row, :], **kwargs)
+    for col in range(x.shape[1]):
+        x[:, col] = dct(x[:, col], **kwargs)
+    return x
+
+
+def idct_2d_ref(x, **kwargs):
+    """Calculate reference values for testing idct2."""
+    x = np.array(x, copy=True)
+    for row in range(x.shape[0]):
+        x[row, :] = idct(x[row, :], **kwargs)
+    for col in range(x.shape[1]):
+        x[:, col] = idct(x[:, col], **kwargs)
+    return x
+
+
+def dst_2d_ref(x, **kwargs):
+    """Calculate reference values for testing dst2."""
+    x = np.array(x, copy=True)
+    for row in range(x.shape[0]):
+        x[row, :] = dst(x[row, :], **kwargs)
+    for col in range(x.shape[1]):
+        x[:, col] = dst(x[:, col], **kwargs)
+    return x
+
+
+def idst_2d_ref(x, **kwargs):
+    """Calculate reference values for testing idst2."""
+    x = np.array(x, copy=True)
+    for row in range(x.shape[0]):
+        x[row, :] = idst(x[row, :], **kwargs)
+    for col in range(x.shape[1]):
+        x[:, col] = idst(x[:, col], **kwargs)
+    return x
+
+
+def naive_dct1(x, norm=None):
+    """Calculate textbook definition version of DCT-I."""
+    x = np.array(x, copy=True)
+    N = len(x)
+    M = N-1
+    y = np.zeros(N)
+    m0, m = 1, 2
+    if norm == 'ortho':
+        m0 = np.sqrt(1.0/M)
+        m = np.sqrt(2.0/M)
+    for k in range(N):
+        for n in range(1, N-1):
+            y[k] += m*x[n]*np.cos(np.pi*n*k/M)
+        y[k] += m0 * x[0]
+        y[k] += m0 * x[N-1] * (1 if k % 2 == 0 else -1)
+    if norm == 'ortho':
+        y[0] *= 1/np.sqrt(2)
+        y[N-1] *= 1/np.sqrt(2)
+    return y
+
+
+def naive_dst1(x, norm=None):
+    """Calculate textbook definition version  of DST-I."""
+    x = np.array(x, copy=True)
+    N = len(x)
+    M = N+1
+    y = np.zeros(N)
+    for k in range(N):
+        for n in range(N):
+            y[k] += 2*x[n]*np.sin(np.pi*(n+1.0)*(k+1.0)/M)
+    if norm == 'ortho':
+        y *= np.sqrt(0.5/M)
+    return y
+
+
+def naive_dct4(x, norm=None):
+    """Calculate textbook definition version of DCT-IV."""
+    x = np.array(x, copy=True)
+    N = len(x)
+    y = np.zeros(N)
+    for k in range(N):
+        for n in range(N):
+            y[k] += x[n]*np.cos(np.pi*(n+0.5)*(k+0.5)/(N))
+    if norm == 'ortho':
+        y *= np.sqrt(2.0/N)
+    else:
+        y *= 2
+    return y
+
+
+def naive_dst4(x, norm=None):
+    """Calculate textbook definition version of DST-IV."""
+    x = np.array(x, copy=True)
+    N = len(x)
+    y = np.zeros(N)
+    for k in range(N):
+        for n in range(N):
+            y[k] += x[n]*np.sin(np.pi*(n+0.5)*(k+0.5)/(N))
+    if norm == 'ortho':
+        y *= np.sqrt(2.0/N)
+    else:
+        y *= 2
+    return y
+
+
+class TestComplex:
+    def test_dct_complex64(self):
+        y = dct(1j*np.arange(5, dtype=np.complex64))
+        x = 1j*dct(np.arange(5))
+        assert_array_almost_equal(x, y)
+
+    def test_dct_complex(self):
+        y = dct(np.arange(5)*1j)
+        x = 1j*dct(np.arange(5))
+        assert_array_almost_equal(x, y)
+
+    def test_idct_complex(self):
+        y = idct(np.arange(5)*1j)
+        x = 1j*idct(np.arange(5))
+        assert_array_almost_equal(x, y)
+
+    def test_dst_complex64(self):
+        y = dst(np.arange(5, dtype=np.complex64)*1j)
+        x = 1j*dst(np.arange(5))
+        assert_array_almost_equal(x, y)
+
+    def test_dst_complex(self):
+        y = dst(np.arange(5)*1j)
+        x = 1j*dst(np.arange(5))
+        assert_array_almost_equal(x, y)
+
+    def test_idst_complex(self):
+        y = idst(np.arange(5)*1j)
+        x = 1j*idst(np.arange(5))
+        assert_array_almost_equal(x, y)
+
+
+class _TestDCTBase:
+    def setup_method(self):
+        self.rdt = None
+        self.dec = 14
+        self.type = None
+
+    def test_definition(self):
+        for i in FFTWDATA_SIZES:
+            x, yr, dt = fftw_dct_ref(self.type, i, self.rdt)
+            y = dct(x, type=self.type)
+            assert_equal(y.dtype, dt)
+            # XXX: we divide by np.max(y) because the tests fail otherwise. We
+            # should really use something like assert_array_approx_equal. The
+            # difference is due to fftw using a better algorithm w.r.t error
+            # propagation compared to the ones from fftpack.
+            assert_array_almost_equal(y / np.max(y), yr / np.max(y), decimal=self.dec,
+                    err_msg="Size %d failed" % i)
+
+    def test_axis(self):
+        nt = 2
+        for i in [7, 8, 9, 16, 32, 64]:
+            x = np.random.randn(nt, i)
+            y = dct(x, type=self.type)
+            for j in range(nt):
+                assert_array_almost_equal(y[j], dct(x[j], type=self.type),
+                        decimal=self.dec)
+
+            x = x.T
+            y = dct(x, axis=0, type=self.type)
+            for j in range(nt):
+                assert_array_almost_equal(y[:,j], dct(x[:,j], type=self.type),
+                        decimal=self.dec)
+
+
+class _TestDCTIBase(_TestDCTBase):
+    def test_definition_ortho(self):
+        # Test orthornomal mode.
+        dt = np.result_type(np.float32, self.rdt)
+        for xr in X:
+            x = np.array(xr, dtype=self.rdt)
+            y = dct(x, norm='ortho', type=1)
+            y2 = naive_dct1(x, norm='ortho')
+            assert_equal(y.dtype, dt)
+            assert_array_almost_equal(y / np.max(y), y2 / np.max(y), decimal=self.dec)
+
+class _TestDCTIIBase(_TestDCTBase):
+    def test_definition_matlab(self):
+        # Test correspondence with MATLAB (orthornomal mode).
+        dt = np.result_type(np.float32, self.rdt)
+        for xr, yr in zip(X, Y):
+            x = np.array(xr, dtype=dt)
+            y = dct(x, norm="ortho", type=2)
+            assert_equal(y.dtype, dt)
+            assert_array_almost_equal(y, yr, decimal=self.dec)
+
+
+class _TestDCTIIIBase(_TestDCTBase):
+    def test_definition_ortho(self):
+        # Test orthornomal mode.
+        dt = np.result_type(np.float32, self.rdt)
+        for xr in X:
+            x = np.array(xr, dtype=self.rdt)
+            y = dct(x, norm='ortho', type=2)
+            xi = dct(y, norm="ortho", type=3)
+            assert_equal(xi.dtype, dt)
+            assert_array_almost_equal(xi, x, decimal=self.dec)
+
+class _TestDCTIVBase(_TestDCTBase):
+    def test_definition_ortho(self):
+        # Test orthornomal mode.
+        dt = np.result_type(np.float32, self.rdt)
+        for xr in X:
+            x = np.array(xr, dtype=self.rdt)
+            y = dct(x, norm='ortho', type=4)
+            y2 = naive_dct4(x, norm='ortho')
+            assert_equal(y.dtype, dt)
+            assert_array_almost_equal(y / np.max(y), y2 / np.max(y), decimal=self.dec)
+
+
+class TestDCTIDouble(_TestDCTIBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 10
+        self.type = 1
+
+
+class TestDCTIFloat(_TestDCTIBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 4
+        self.type = 1
+
+
+class TestDCTIInt(_TestDCTIBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 1
+
+
+class TestDCTIIDouble(_TestDCTIIBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 10
+        self.type = 2
+
+
+class TestDCTIIFloat(_TestDCTIIBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 5
+        self.type = 2
+
+
+class TestDCTIIInt(_TestDCTIIBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 2
+
+
+class TestDCTIIIDouble(_TestDCTIIIBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 14
+        self.type = 3
+
+
+class TestDCTIIIFloat(_TestDCTIIIBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 5
+        self.type = 3
+
+
+class TestDCTIIIInt(_TestDCTIIIBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 3
+
+
+class TestDCTIVDouble(_TestDCTIVBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 12
+        self.type = 3
+
+
+class TestDCTIVFloat(_TestDCTIVBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 5
+        self.type = 3
+
+
+class TestDCTIVInt(_TestDCTIVBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 3
+
+
+class _TestIDCTBase:
+    def setup_method(self):
+        self.rdt = None
+        self.dec = 14
+        self.type = None
+
+    def test_definition(self):
+        for i in FFTWDATA_SIZES:
+            xr, yr, dt = fftw_dct_ref(self.type, i, self.rdt)
+            x = idct(yr, type=self.type)
+            if self.type == 1:
+                x /= 2 * (i-1)
+            else:
+                x /= 2 * i
+            assert_equal(x.dtype, dt)
+            # XXX: we divide by np.max(y) because the tests fail otherwise. We
+            # should really use something like assert_array_approx_equal. The
+            # difference is due to fftw using a better algorithm w.r.t error
+            # propagation compared to the ones from fftpack.
+            assert_array_almost_equal(x / np.max(x), xr / np.max(x), decimal=self.dec,
+                    err_msg="Size %d failed" % i)
+
+
+class TestIDCTIDouble(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 10
+        self.type = 1
+
+
+class TestIDCTIFloat(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 4
+        self.type = 1
+
+
+class TestIDCTIInt(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 4
+        self.type = 1
+
+
+class TestIDCTIIDouble(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 10
+        self.type = 2
+
+
+class TestIDCTIIFloat(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 5
+        self.type = 2
+
+
+class TestIDCTIIInt(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 2
+
+
+class TestIDCTIIIDouble(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 14
+        self.type = 3
+
+
+class TestIDCTIIIFloat(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 5
+        self.type = 3
+
+
+class TestIDCTIIIInt(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 3
+
+class TestIDCTIVDouble(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 12
+        self.type = 4
+
+
+class TestIDCTIVFloat(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 5
+        self.type = 4
+
+
+class TestIDCTIVInt(_TestIDCTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 4
+
+class _TestDSTBase:
+    def setup_method(self):
+        self.rdt = None  # dtype
+        self.dec = None  # number of decimals to match
+        self.type = None  # dst type
+
+    def test_definition(self):
+        for i in FFTWDATA_SIZES:
+            xr, yr, dt = fftw_dst_ref(self.type, i, self.rdt)
+            y = dst(xr, type=self.type)
+            assert_equal(y.dtype, dt)
+            # XXX: we divide by np.max(y) because the tests fail otherwise. We
+            # should really use something like assert_array_approx_equal. The
+            # difference is due to fftw using a better algorithm w.r.t error
+            # propagation compared to the ones from fftpack.
+            assert_array_almost_equal(y / np.max(y), yr / np.max(y), decimal=self.dec,
+                    err_msg="Size %d failed" % i)
+
+
+class _TestDSTIBase(_TestDSTBase):
+    def test_definition_ortho(self):
+        # Test orthornomal mode.
+        dt = np.result_type(np.float32, self.rdt)
+        for xr in X:
+            x = np.array(xr, dtype=self.rdt)
+            y = dst(x, norm='ortho', type=1)
+            y2 = naive_dst1(x, norm='ortho')
+            assert_equal(y.dtype, dt)
+            assert_array_almost_equal(y / np.max(y), y2 / np.max(y), decimal=self.dec)
+
+class _TestDSTIVBase(_TestDSTBase):
+    def test_definition_ortho(self):
+        # Test orthornomal mode.
+        dt = np.result_type(np.float32, self.rdt)
+        for xr in X:
+            x = np.array(xr, dtype=self.rdt)
+            y = dst(x, norm='ortho', type=4)
+            y2 = naive_dst4(x, norm='ortho')
+            assert_equal(y.dtype, dt)
+            assert_array_almost_equal(y, y2, decimal=self.dec)
+
+class TestDSTIDouble(_TestDSTIBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 12
+        self.type = 1
+
+
+class TestDSTIFloat(_TestDSTIBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 4
+        self.type = 1
+
+
+class TestDSTIInt(_TestDSTIBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 1
+
+
+class TestDSTIIDouble(_TestDSTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 14
+        self.type = 2
+
+
+class TestDSTIIFloat(_TestDSTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 6
+        self.type = 2
+
+
+class TestDSTIIInt(_TestDSTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 6
+        self.type = 2
+
+
+class TestDSTIIIDouble(_TestDSTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 14
+        self.type = 3
+
+
+class TestDSTIIIFloat(_TestDSTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 7
+        self.type = 3
+
+
+class TestDSTIIIInt(_TestDSTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 7
+        self.type = 3
+
+
+class TestDSTIVDouble(_TestDSTIVBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 12
+        self.type = 4
+
+
+class TestDSTIVFloat(_TestDSTIVBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 4
+        self.type = 4
+
+
+class TestDSTIVInt(_TestDSTIVBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 5
+        self.type = 4
+
+
+class _TestIDSTBase:
+    def setup_method(self):
+        self.rdt = None
+        self.dec = None
+        self.type = None
+
+    def test_definition(self):
+        for i in FFTWDATA_SIZES:
+            xr, yr, dt = fftw_dst_ref(self.type, i, self.rdt)
+            x = idst(yr, type=self.type)
+            if self.type == 1:
+                x /= 2 * (i+1)
+            else:
+                x /= 2 * i
+            assert_equal(x.dtype, dt)
+            # XXX: we divide by np.max(x) because the tests fail otherwise. We
+            # should really use something like assert_array_approx_equal. The
+            # difference is due to fftw using a better algorithm w.r.t error
+            # propagation compared to the ones from fftpack.
+            assert_array_almost_equal(x / np.max(x), xr / np.max(x), decimal=self.dec,
+                    err_msg="Size %d failed" % i)
+
+
+class TestIDSTIDouble(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 12
+        self.type = 1
+
+
+class TestIDSTIFloat(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 4
+        self.type = 1
+
+
+class TestIDSTIInt(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 4
+        self.type = 1
+
+
+class TestIDSTIIDouble(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 14
+        self.type = 2
+
+
+class TestIDSTIIFloat(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 6
+        self.type = 2
+
+
+class TestIDSTIIInt(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 6
+        self.type = 2
+
+
+class TestIDSTIIIDouble(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 14
+        self.type = 3
+
+
+class TestIDSTIIIFloat(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 6
+        self.type = 3
+
+
+class TestIDSTIIIInt(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 6
+        self.type = 3
+
+
+class TestIDSTIVDouble(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float64
+        self.dec = 12
+        self.type = 4
+
+
+class TestIDSTIVFloat(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = np.float32
+        self.dec = 6
+        self.type = 4
+
+
+class TestIDSTIVnt(_TestIDSTBase):
+    def setup_method(self):
+        self.rdt = int
+        self.dec = 6
+        self.type = 4
+
+
+class TestOverwrite:
+    """Check input overwrite behavior."""
+
+    real_dtypes = [np.float32, np.float64]
+
+    def _check(self, x, routine, type, fftsize, axis, norm, overwrite_x, **kw):
+        x2 = x.copy()
+        routine(x2, type, fftsize, axis, norm, overwrite_x=overwrite_x)
+
+        sig = "{}({}{!r}, {!r}, axis={!r}, overwrite_x={!r})".format(
+            routine.__name__, x.dtype, x.shape, fftsize, axis, overwrite_x)
+        if not overwrite_x:
+            assert_equal(x2, x, err_msg="spurious overwrite in %s" % sig)
+
+    def _check_1d(self, routine, dtype, shape, axis):
+        np.random.seed(1234)
+        if np.issubdtype(dtype, np.complexfloating):
+            data = np.random.randn(*shape) + 1j*np.random.randn(*shape)
+        else:
+            data = np.random.randn(*shape)
+        data = data.astype(dtype)
+
+        for type in [1, 2, 3, 4]:
+            for overwrite_x in [True, False]:
+                for norm in [None, 'ortho']:
+                    self._check(data, routine, type, None, axis, norm,
+                                overwrite_x)
+
+    def test_dct(self):
+        for dtype in self.real_dtypes:
+            self._check_1d(dct, dtype, (16,), -1)
+            self._check_1d(dct, dtype, (16, 2), 0)
+            self._check_1d(dct, dtype, (2, 16), 1)
+
+    def test_idct(self):
+        for dtype in self.real_dtypes:
+            self._check_1d(idct, dtype, (16,), -1)
+            self._check_1d(idct, dtype, (16, 2), 0)
+            self._check_1d(idct, dtype, (2, 16), 1)
+
+    def test_dst(self):
+        for dtype in self.real_dtypes:
+            self._check_1d(dst, dtype, (16,), -1)
+            self._check_1d(dst, dtype, (16, 2), 0)
+            self._check_1d(dst, dtype, (2, 16), 1)
+
+    def test_idst(self):
+        for dtype in self.real_dtypes:
+            self._check_1d(idst, dtype, (16,), -1)
+            self._check_1d(idst, dtype, (16, 2), 0)
+            self._check_1d(idst, dtype, (2, 16), 1)
+
+
+class Test_DCTN_IDCTN:
+    dec = 14
+    dct_type = [1, 2, 3, 4]
+    norms = [None, 'ortho']
+    rstate = np.random.RandomState(1234)
+    shape = (32, 16)
+    data = rstate.randn(*shape)
+
+    @pytest.mark.parametrize('fforward,finverse', [(dctn, idctn),
+                                                   (dstn, idstn)])
+    @pytest.mark.parametrize('axes', [None,
+                                      1, (1,), [1],
+                                      0, (0,), [0],
+                                      (0, 1), [0, 1],
+                                      (-2, -1), [-2, -1]])
+    @pytest.mark.parametrize('dct_type', dct_type)
+    @pytest.mark.parametrize('norm', ['ortho'])
+    def test_axes_round_trip(self, fforward, finverse, axes, dct_type, norm):
+        tmp = fforward(self.data, type=dct_type, axes=axes, norm=norm)
+        tmp = finverse(tmp, type=dct_type, axes=axes, norm=norm)
+        assert_array_almost_equal(self.data, tmp, decimal=12)
+
+    @pytest.mark.parametrize('fforward,fforward_ref', [(dctn, dct_2d_ref),
+                                                       (dstn, dst_2d_ref)])
+    @pytest.mark.parametrize('dct_type', dct_type)
+    @pytest.mark.parametrize('norm', norms)
+    def test_dctn_vs_2d_reference(self, fforward, fforward_ref,
+                                  dct_type, norm):
+        y1 = fforward(self.data, type=dct_type, axes=None, norm=norm)
+        y2 = fforward_ref(self.data, type=dct_type, norm=norm)
+        assert_array_almost_equal(y1, y2, decimal=11)
+
+    @pytest.mark.parametrize('finverse,finverse_ref', [(idctn, idct_2d_ref),
+                                                       (idstn, idst_2d_ref)])
+    @pytest.mark.parametrize('dct_type', dct_type)
+    @pytest.mark.parametrize('norm', [None, 'ortho'])
+    def test_idctn_vs_2d_reference(self, finverse, finverse_ref,
+                                   dct_type, norm):
+        fdata = dctn(self.data, type=dct_type, norm=norm)
+        y1 = finverse(fdata, type=dct_type, norm=norm)
+        y2 = finverse_ref(fdata, type=dct_type, norm=norm)
+        assert_array_almost_equal(y1, y2, decimal=11)
+
+    @pytest.mark.parametrize('fforward,finverse', [(dctn, idctn),
+                                                   (dstn, idstn)])
+    def test_axes_and_shape(self, fforward, finverse):
+        with assert_raises(ValueError,
+                           match="when given, axes and shape arguments"
+                           " have to be of the same length"):
+            fforward(self.data, shape=self.data.shape[0], axes=(0, 1))
+
+        with assert_raises(ValueError,
+                           match="when given, axes and shape arguments"
+                           " have to be of the same length"):
+            fforward(self.data, shape=self.data.shape[0], axes=None)
+
+        with assert_raises(ValueError,
+                           match="when given, axes and shape arguments"
+                           " have to be of the same length"):
+            fforward(self.data, shape=self.data.shape, axes=0)
+
+    @pytest.mark.parametrize('fforward', [dctn, dstn])
+    def test_shape(self, fforward):
+        tmp = fforward(self.data, shape=(128, 128), axes=None)
+        assert_equal(tmp.shape, (128, 128))
+
+    @pytest.mark.parametrize('fforward,finverse', [(dctn, idctn),
+                                                   (dstn, idstn)])
+    @pytest.mark.parametrize('axes', [1, (1,), [1],
+                                      0, (0,), [0]])
+    def test_shape_is_none_with_axes(self, fforward, finverse, axes):
+        tmp = fforward(self.data, shape=None, axes=axes, norm='ortho')
+        tmp = finverse(tmp, shape=None, axes=axes, norm='ortho')
+        assert_array_almost_equal(self.data, tmp, decimal=self.dec)

llmeval-env/lib/python3.10/site-packages/scipy/optimize/README

@@ -0,0 +1,76 @@
+From the website for the L-BFGS-B code (from at
+http://www.ece.northwestern.edu/~nocedal/lbfgsb.html):
+
+"""
+L-BFGS-B is a limited-memory quasi-Newton code for bound-constrained
+optimization, i.e. for problems where the only constraints are of the
+form l<= x <= u.
+"""
+
+This is a Python wrapper (using F2PY) written by David M. Cooke
+<[email protected]> and released as version 0.9 on April 9, 2004.
+The wrapper was slightly modified by Joonas Paalasmaa for the 3.0 version
+in March 2012.
+
+License of L-BFGS-B (Fortran code)
+==================================
+
+The version included here (in lbfgsb.f) is 3.0 (released April 25, 2011). It was
+written by Ciyou Zhu, Richard Byrd, and Jorge Nocedal <[email protected]>. It
+carries the following condition for use:
+
+  """
+  This software is freely available, but we expect that all publications
+  describing work using this software, or all commercial products using it,
+  quote at least one of the references given below. This software is released
+  under the BSD License.
+  
+  References
+    * R. H. Byrd, P. Lu and J. Nocedal. A Limited Memory Algorithm for Bound
+      Constrained Optimization, (1995), SIAM Journal on Scientific and
+      Statistical Computing, 16, 5, pp. 1190-1208.
+    * C. Zhu, R. H. Byrd and J. Nocedal. L-BFGS-B: Algorithm 778: L-BFGS-B,
+      FORTRAN routines for large scale bound constrained optimization (1997),
+      ACM Transactions on Mathematical Software, 23, 4, pp. 550 - 560.
+    * J.L. Morales and J. Nocedal. L-BFGS-B: Remark on Algorithm 778: L-BFGS-B,
+      FORTRAN routines for large scale bound constrained optimization (2011),
+      ACM Transactions on Mathematical Software, 38, 1.
+  """
+
+The Python wrapper
+==================
+
+This code uses F2PY (http://cens.ioc.ee/projects/f2py2e/) to generate
+the wrapper around the Fortran code.
+
+The Python code and wrapper are copyrighted 2004 by David M. Cooke
+<[email protected]>.
+
+Example usage
+=============
+
+An example of the usage is given at the bottom of the lbfgsb.py file.
+Run it with 'python lbfgsb.py'.
+
+License for the Python wrapper
+==============================
+
+Copyright (c) 2004 David M. Cooke <[email protected]>
+
+Permission is hereby granted, free of charge, to any person obtaining a copy of
+this software and associated documentation files (the "Software"), to deal in
+the Software without restriction, including without limitation the rights to
+use, copy, modify, merge, publish, distribute, sublicense, and/or sell copies
+of the Software, and to permit persons to whom the Software is furnished to do
+so, subject to the following conditions:
+
+The above copyright notice and this permission notice shall be included in all
+copies or substantial portions of the Software.
+
+THE SOFTWARE IS PROVIDED "AS IS", WITHOUT WARRANTY OF ANY KIND, EXPRESS OR
+IMPLIED, INCLUDING BUT NOT LIMITED TO THE WARRANTIES OF MERCHANTABILITY,
+FITNESS FOR A PARTICULAR PURPOSE AND NONINFRINGEMENT. IN NO EVENT SHALL THE
+AUTHORS OR COPYRIGHT HOLDERS BE LIABLE FOR ANY CLAIM, DAMAGES OR OTHER
+LIABILITY, WHETHER IN AN ACTION OF CONTRACT, TORT OR OTHERWISE, ARISING FROM,
+OUT OF OR IN CONNECTION WITH THE SOFTWARE OR THE USE OR OTHER DEALINGS IN THE
+SOFTWARE.

llmeval-env/lib/python3.10/site-packages/scipy/optimize/__init__.py

@@ -0,0 +1,451 @@
+"""
+=====================================================
+Optimization and root finding (:mod:`scipy.optimize`)
+=====================================================
+
+.. currentmodule:: scipy.optimize
+
+.. toctree::
+   :hidden:
+
+   optimize.cython_optimize
+
+SciPy ``optimize`` provides functions for minimizing (or maximizing)
+objective functions, possibly subject to constraints. It includes
+solvers for nonlinear problems (with support for both local and global
+optimization algorithms), linear programming, constrained
+and nonlinear least-squares, root finding, and curve fitting.
+
+Common functions and objects, shared across different solvers, are:
+
+.. autosummary::
+   :toctree: generated/
+
+   show_options - Show specific options optimization solvers.
+   OptimizeResult - The optimization result returned by some optimizers.
+   OptimizeWarning - The optimization encountered problems.
+
+
+Optimization
+============
+
+Scalar functions optimization
+-----------------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   minimize_scalar - Interface for minimizers of univariate functions
+
+The `minimize_scalar` function supports the following methods:
+
+.. toctree::
+
+   optimize.minimize_scalar-brent
+   optimize.minimize_scalar-bounded
+   optimize.minimize_scalar-golden
+
+Local (multivariate) optimization
+---------------------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   minimize - Interface for minimizers of multivariate functions.
+
+The `minimize` function supports the following methods:
+
+.. toctree::
+
+   optimize.minimize-neldermead
+   optimize.minimize-powell
+   optimize.minimize-cg
+   optimize.minimize-bfgs
+   optimize.minimize-newtoncg
+   optimize.minimize-lbfgsb
+   optimize.minimize-tnc
+   optimize.minimize-cobyla
+   optimize.minimize-slsqp
+   optimize.minimize-trustconstr
+   optimize.minimize-dogleg
+   optimize.minimize-trustncg
+   optimize.minimize-trustkrylov
+   optimize.minimize-trustexact
+
+Constraints are passed to `minimize` function as a single object or
+as a list of objects from the following classes:
+
+.. autosummary::
+   :toctree: generated/
+
+   NonlinearConstraint - Class defining general nonlinear constraints.
+   LinearConstraint - Class defining general linear constraints.
+
+Simple bound constraints are handled separately and there is a special class
+for them:
+
+.. autosummary::
+   :toctree: generated/
+
+   Bounds - Bound constraints.
+
+Quasi-Newton strategies implementing `HessianUpdateStrategy`
+interface can be used to approximate the Hessian in `minimize`
+function (available only for the 'trust-constr' method). Available
+quasi-Newton methods implementing this interface are:
+
+.. autosummary::
+   :toctree: generated/
+
+   BFGS - Broyden-Fletcher-Goldfarb-Shanno (BFGS) Hessian update strategy.
+   SR1 - Symmetric-rank-1 Hessian update strategy.
+
+.. _global_optimization:
+
+Global optimization
+-------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   basinhopping - Basinhopping stochastic optimizer.
+   brute - Brute force searching optimizer.
+   differential_evolution - Stochastic optimizer using differential evolution.
+
+   shgo - Simplicial homology global optimizer.
+   dual_annealing - Dual annealing stochastic optimizer.
+   direct - DIRECT (Dividing Rectangles) optimizer.
+
+Least-squares and curve fitting
+===============================
+
+Nonlinear least-squares
+-----------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   least_squares - Solve a nonlinear least-squares problem with bounds on the variables.
+
+Linear least-squares
+--------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   nnls - Linear least-squares problem with non-negativity constraint.
+   lsq_linear - Linear least-squares problem with bound constraints.
+   isotonic_regression - Least squares problem of isotonic regression via PAVA.
+
+Curve fitting
+-------------
+
+.. autosummary::
+   :toctree: generated/
+
+   curve_fit -- Fit curve to a set of points.
+
+Root finding
+============
+
+Scalar functions
+----------------
+.. autosummary::
+   :toctree: generated/
+
+   root_scalar - Unified interface for nonlinear solvers of scalar functions.
+   brentq - quadratic interpolation Brent method.
+   brenth - Brent method, modified by Harris with hyperbolic extrapolation.
+   ridder - Ridder's method.
+   bisect - Bisection method.
+   newton - Newton's method (also Secant and Halley's methods).
+   toms748 - Alefeld, Potra & Shi Algorithm 748.
+   RootResults - The root finding result returned by some root finders.
+
+The `root_scalar` function supports the following methods:
+
+.. toctree::
+
+   optimize.root_scalar-brentq
+   optimize.root_scalar-brenth
+   optimize.root_scalar-bisect
+   optimize.root_scalar-ridder
+   optimize.root_scalar-newton
+   optimize.root_scalar-toms748
+   optimize.root_scalar-secant
+   optimize.root_scalar-halley
+
+
+
+The table below lists situations and appropriate methods, along with
+*asymptotic* convergence rates per iteration (and per function evaluation)
+for successful convergence to a simple root(*).
+Bisection is the slowest of them all, adding one bit of accuracy for each
+function evaluation, but is guaranteed to converge.
+The other bracketing methods all (eventually) increase the number of accurate
+bits by about 50% for every function evaluation.
+The derivative-based methods, all built on `newton`, can converge quite quickly
+if the initial value is close to the root.  They can also be applied to
+functions defined on (a subset of) the complex plane.
+
++-------------+----------+----------+-----------+-------------+-------------+----------------+
+| Domain of f | Bracket? |    Derivatives?      | Solvers     |        Convergence           |
++             +          +----------+-----------+             +-------------+----------------+
+|             |          | `fprime` | `fprime2` |             | Guaranteed? |  Rate(s)(*)    |
++=============+==========+==========+===========+=============+=============+================+
+| `R`         | Yes      | N/A      | N/A       | - bisection | - Yes       | - 1 "Linear"   |
+|             |          |          |           | - brentq    | - Yes       | - >=1, <= 1.62 |
+|             |          |          |           | - brenth    | - Yes       | - >=1, <= 1.62 |
+|             |          |          |           | - ridder    | - Yes       | - 2.0 (1.41)   |
+|             |          |          |           | - toms748   | - Yes       | - 2.7 (1.65)   |
++-------------+----------+----------+-----------+-------------+-------------+----------------+
+| `R` or `C`  | No       | No       | No        | secant      | No          | 1.62 (1.62)    |
++-------------+----------+----------+-----------+-------------+-------------+----------------+
+| `R` or `C`  | No       | Yes      | No        | newton      | No          | 2.00 (1.41)    |
++-------------+----------+----------+-----------+-------------+-------------+----------------+
+| `R` or `C`  | No       | Yes      | Yes       | halley      | No          | 3.00 (1.44)    |
++-------------+----------+----------+-----------+-------------+-------------+----------------+
+
+.. seealso::
+
+   `scipy.optimize.cython_optimize` -- Typed Cython versions of root finding functions
+
+Fixed point finding:
+
+.. autosummary::
+   :toctree: generated/
+
+   fixed_point - Single-variable fixed-point solver.
+
+Multidimensional
+----------------
+
+.. autosummary::
+   :toctree: generated/
+
+   root - Unified interface for nonlinear solvers of multivariate functions.
+
+The `root` function supports the following methods:
+
+.. toctree::
+
+   optimize.root-hybr
+   optimize.root-lm
+   optimize.root-broyden1
+   optimize.root-broyden2
+   optimize.root-anderson
+   optimize.root-linearmixing
+   optimize.root-diagbroyden
+   optimize.root-excitingmixing
+   optimize.root-krylov
+   optimize.root-dfsane
+
+Linear programming / MILP
+=========================
+
+.. autosummary::
+   :toctree: generated/
+
+   milp -- Mixed integer linear programming.
+   linprog -- Unified interface for minimizers of linear programming problems.
+
+The `linprog` function supports the following methods:
+
+.. toctree::
+
+   optimize.linprog-simplex
+   optimize.linprog-interior-point
+   optimize.linprog-revised_simplex
+   optimize.linprog-highs-ipm
+   optimize.linprog-highs-ds
+   optimize.linprog-highs
+
+The simplex, interior-point, and revised simplex methods support callback
+functions, such as:
+
+.. autosummary::
+   :toctree: generated/
+
+   linprog_verbose_callback -- Sample callback function for linprog (simplex).
+
+Assignment problems
+===================
+
+.. autosummary::
+   :toctree: generated/
+
+   linear_sum_assignment -- Solves the linear-sum assignment problem.
+   quadratic_assignment -- Solves the quadratic assignment problem.
+
+The `quadratic_assignment` function supports the following methods:
+
+.. toctree::
+
+   optimize.qap-faq
+   optimize.qap-2opt
+
+Utilities
+=========
+
+Finite-difference approximation
+-------------------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   approx_fprime - Approximate the gradient of a scalar function.
+   check_grad - Check the supplied derivative using finite differences.
+
+
+Line search
+-----------
+
+.. autosummary::
+   :toctree: generated/
+
+   bracket - Bracket a minimum, given two starting points.
+   line_search - Return a step that satisfies the strong Wolfe conditions.
+
+Hessian approximation
+---------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   LbfgsInvHessProduct - Linear operator for L-BFGS approximate inverse Hessian.
+   HessianUpdateStrategy - Interface for implementing Hessian update strategies
+
+Benchmark problems
+------------------
+
+.. autosummary::
+   :toctree: generated/
+
+   rosen - The Rosenbrock function.
+   rosen_der - The derivative of the Rosenbrock function.
+   rosen_hess - The Hessian matrix of the Rosenbrock function.
+   rosen_hess_prod - Product of the Rosenbrock Hessian with a vector.
+
+Legacy functions
+================
+
+The functions below are not recommended for use in new scripts;
+all of these methods are accessible via a newer, more consistent
+interfaces, provided by the interfaces above.
+
+Optimization
+------------
+
+General-purpose multivariate methods:
+
+.. autosummary::
+   :toctree: generated/
+
+   fmin - Nelder-Mead Simplex algorithm.
+   fmin_powell - Powell's (modified) conjugate direction method.
+   fmin_cg - Non-linear (Polak-Ribiere) conjugate gradient algorithm.
+   fmin_bfgs - Quasi-Newton method (Broydon-Fletcher-Goldfarb-Shanno).
+   fmin_ncg - Line-search Newton Conjugate Gradient.
+
+Constrained multivariate methods:
+
+.. autosummary::
+   :toctree: generated/
+
+   fmin_l_bfgs_b - Zhu, Byrd, and Nocedal's constrained optimizer.
+   fmin_tnc - Truncated Newton code.
+   fmin_cobyla - Constrained optimization by linear approximation.
+   fmin_slsqp - Minimization using sequential least-squares programming.
+
+Univariate (scalar) minimization methods:
+
+.. autosummary::
+   :toctree: generated/
+
+   fminbound - Bounded minimization of a scalar function.
+   brent - 1-D function minimization using Brent method.
+   golden - 1-D function minimization using Golden Section method.
+
+Least-squares
+-------------
+
+.. autosummary::
+   :toctree: generated/
+
+   leastsq - Minimize the sum of squares of M equations in N unknowns.
+
+Root finding
+------------
+
+General nonlinear solvers:
+
+.. autosummary::
+   :toctree: generated/
+
+   fsolve - Non-linear multivariable equation solver.
+   broyden1 - Broyden's first method.
+   broyden2 - Broyden's second method.
+   NoConvergence -  Exception raised when nonlinear solver does not converge.
+
+Large-scale nonlinear solvers:
+
+.. autosummary::
+   :toctree: generated/
+
+   newton_krylov
+   anderson
+
+   BroydenFirst
+   InverseJacobian
+   KrylovJacobian
+
+Simple iteration solvers:
+
+.. autosummary::
+   :toctree: generated/
+
+   excitingmixing
+   linearmixing
+   diagbroyden
+
+"""  # noqa: E501
+
+from ._optimize import *
+from ._minimize import *
+from ._root import *
+from ._root_scalar import *
+from ._minpack_py import *
+from ._zeros_py import *
+from ._lbfgsb_py import fmin_l_bfgs_b, LbfgsInvHessProduct
+from ._tnc import fmin_tnc
+from ._cobyla_py import fmin_cobyla
+from ._nonlin import *
+from ._slsqp_py import fmin_slsqp
+from ._nnls import nnls
+from ._basinhopping import basinhopping
+from ._linprog import linprog, linprog_verbose_callback
+from ._lsap import linear_sum_assignment
+from ._differentialevolution import differential_evolution
+from ._lsq import least_squares, lsq_linear
+from ._isotonic import isotonic_regression
+from ._constraints import (NonlinearConstraint,
+                           LinearConstraint,
+                           Bounds)
+from ._hessian_update_strategy import HessianUpdateStrategy, BFGS, SR1
+from ._shgo import shgo
+from ._dual_annealing import dual_annealing
+from ._qap import quadratic_assignment
+from ._direct_py import direct
+from ._milp import milp
+
+# Deprecated namespaces, to be removed in v2.0.0
+from . import (
+    cobyla, lbfgsb, linesearch, minpack, minpack2, moduleTNC, nonlin, optimize,
+    slsqp, tnc, zeros
+)
+
+__all__ = [s for s in dir() if not s.startswith('_')]
+
+from scipy._lib._testutils import PytestTester
+test = PytestTester(__name__)
+del PytestTester

llmeval-env/lib/python3.10/site-packages/scipy/optimize/_basinhopping.py

@@ -0,0 +1,753 @@
+"""
+basinhopping: The basinhopping global optimization algorithm
+"""
+import numpy as np
+import math
+import inspect
+import scipy.optimize
+from scipy._lib._util import check_random_state
+
+__all__ = ['basinhopping']
+
+
+_params = (inspect.Parameter('res_new', kind=inspect.Parameter.KEYWORD_ONLY),
+           inspect.Parameter('res_old', kind=inspect.Parameter.KEYWORD_ONLY))
+_new_accept_test_signature = inspect.Signature(parameters=_params)
+
+
+class Storage:
+    """
+    Class used to store the lowest energy structure
+    """
+    def __init__(self, minres):
+        self._add(minres)
+
+    def _add(self, minres):
+        self.minres = minres
+        self.minres.x = np.copy(minres.x)
+
+    def update(self, minres):
+        if minres.success and (minres.fun < self.minres.fun
+                               or not self.minres.success):
+            self._add(minres)
+            return True
+        else:
+            return False
+
+    def get_lowest(self):
+        return self.minres
+
+
+class BasinHoppingRunner:
+    """This class implements the core of the basinhopping algorithm.
+
+    x0 : ndarray
+        The starting coordinates.
+    minimizer : callable
+        The local minimizer, with signature ``result = minimizer(x)``.
+        The return value is an `optimize.OptimizeResult` object.
+    step_taking : callable
+        This function displaces the coordinates randomly. Signature should
+        be ``x_new = step_taking(x)``. Note that `x` may be modified in-place.
+    accept_tests : list of callables
+        Each test is passed the kwargs `f_new`, `x_new`, `f_old` and
+        `x_old`. These tests will be used to judge whether or not to accept
+        the step. The acceptable return values are True, False, or ``"force
+        accept"``. If any of the tests return False then the step is rejected.
+        If ``"force accept"``, then this will override any other tests in
+        order to accept the step. This can be used, for example, to forcefully
+        escape from a local minimum that ``basinhopping`` is trapped in.
+    disp : bool, optional
+        Display status messages.
+
+    """
+    def __init__(self, x0, minimizer, step_taking, accept_tests, disp=False):
+        self.x = np.copy(x0)
+        self.minimizer = minimizer
+        self.step_taking = step_taking
+        self.accept_tests = accept_tests
+        self.disp = disp
+
+        self.nstep = 0
+
+        # initialize return object
+        self.res = scipy.optimize.OptimizeResult()
+        self.res.minimization_failures = 0
+
+        # do initial minimization
+        minres = minimizer(self.x)
+        if not minres.success:
+            self.res.minimization_failures += 1
+            if self.disp:
+                print("warning: basinhopping: local minimization failure")
+        self.x = np.copy(minres.x)
+        self.energy = minres.fun
+        self.incumbent_minres = minres  # best minimize result found so far
+        if self.disp:
+            print("basinhopping step %d: f %g" % (self.nstep, self.energy))
+
+        # initialize storage class
+        self.storage = Storage(minres)
+
+        if hasattr(minres, "nfev"):
+            self.res.nfev = minres.nfev
+        if hasattr(minres, "njev"):
+            self.res.njev = minres.njev
+        if hasattr(minres, "nhev"):
+            self.res.nhev = minres.nhev
+
+    def _monte_carlo_step(self):
+        """Do one Monte Carlo iteration
+
+        Randomly displace the coordinates, minimize, and decide whether
+        or not to accept the new coordinates.
+        """
+        # Take a random step.  Make a copy of x because the step_taking
+        # algorithm might change x in place
+        x_after_step = np.copy(self.x)
+        x_after_step = self.step_taking(x_after_step)
+
+        # do a local minimization
+        minres = self.minimizer(x_after_step)
+        x_after_quench = minres.x
+        energy_after_quench = minres.fun
+        if not minres.success:
+            self.res.minimization_failures += 1
+            if self.disp:
+                print("warning: basinhopping: local minimization failure")
+        if hasattr(minres, "nfev"):
+            self.res.nfev += minres.nfev
+        if hasattr(minres, "njev"):
+            self.res.njev += minres.njev
+        if hasattr(minres, "nhev"):
+            self.res.nhev += minres.nhev
+
+        # accept the move based on self.accept_tests. If any test is False,
+        # then reject the step.  If any test returns the special string
+        # 'force accept', then accept the step regardless. This can be used
+        # to forcefully escape from a local minimum if normal basin hopping
+        # steps are not sufficient.
+        accept = True
+        for test in self.accept_tests:
+            if inspect.signature(test) == _new_accept_test_signature:
+                testres = test(res_new=minres, res_old=self.incumbent_minres)
+            else:
+                testres = test(f_new=energy_after_quench, x_new=x_after_quench,
+                               f_old=self.energy, x_old=self.x)
+
+            if testres == 'force accept':
+                accept = True
+                break
+            elif testres is None:
+                raise ValueError("accept_tests must return True, False, or "
+                                 "'force accept'")
+            elif not testres:
+                accept = False
+
+        # Report the result of the acceptance test to the take step class.
+        # This is for adaptive step taking
+        if hasattr(self.step_taking, "report"):
+            self.step_taking.report(accept, f_new=energy_after_quench,
+                                    x_new=x_after_quench, f_old=self.energy,
+                                    x_old=self.x)
+
+        return accept, minres
+
+    def one_cycle(self):
+        """Do one cycle of the basinhopping algorithm
+        """
+        self.nstep += 1
+        new_global_min = False
+
+        accept, minres = self._monte_carlo_step()
+
+        if accept:
+            self.energy = minres.fun
+            self.x = np.copy(minres.x)
+            self.incumbent_minres = minres  # best minimize result found so far
+            new_global_min = self.storage.update(minres)
+
+        # print some information
+        if self.disp:
+            self.print_report(minres.fun, accept)
+            if new_global_min:
+                print("found new global minimum on step %d with function"
+                      " value %g" % (self.nstep, self.energy))
+
+        # save some variables as BasinHoppingRunner attributes
+        self.xtrial = minres.x
+        self.energy_trial = minres.fun
+        self.accept = accept
+
+        return new_global_min
+
+    def print_report(self, energy_trial, accept):
+        """print a status update"""
+        minres = self.storage.get_lowest()
+        print("basinhopping step %d: f %g trial_f %g accepted %d "
+              " lowest_f %g" % (self.nstep, self.energy, energy_trial,
+                                accept, minres.fun))
+
+
+class AdaptiveStepsize:
+    """
+    Class to implement adaptive stepsize.
+
+    This class wraps the step taking class and modifies the stepsize to
+    ensure the true acceptance rate is as close as possible to the target.
+
+    Parameters
+    ----------
+    takestep : callable
+        The step taking routine.  Must contain modifiable attribute
+        takestep.stepsize
+    accept_rate : float, optional
+        The target step acceptance rate
+    interval : int, optional
+        Interval for how often to update the stepsize
+    factor : float, optional
+        The step size is multiplied or divided by this factor upon each
+        update.
+    verbose : bool, optional
+        Print information about each update
+
+    """
+    def __init__(self, takestep, accept_rate=0.5, interval=50, factor=0.9,
+                 verbose=True):
+        self.takestep = takestep
+        self.target_accept_rate = accept_rate
+        self.interval = interval
+        self.factor = factor
+        self.verbose = verbose
+
+        self.nstep = 0
+        self.nstep_tot = 0
+        self.naccept = 0
+
+    def __call__(self, x):
+        return self.take_step(x)
+
+    def _adjust_step_size(self):
+        old_stepsize = self.takestep.stepsize
+        accept_rate = float(self.naccept) / self.nstep
+        if accept_rate > self.target_accept_rate:
+            # We're accepting too many steps. This generally means we're
+            # trapped in a basin. Take bigger steps.
+            self.takestep.stepsize /= self.factor
+        else:
+            # We're not accepting enough steps. Take smaller steps.
+            self.takestep.stepsize *= self.factor
+        if self.verbose:
+            print("adaptive stepsize: acceptance rate {:f} target {:f} new "
+                  "stepsize {:g} old stepsize {:g}".format(accept_rate,
+                  self.target_accept_rate, self.takestep.stepsize,
+                  old_stepsize))
+
+    def take_step(self, x):
+        self.nstep += 1
+        self.nstep_tot += 1
+        if self.nstep % self.interval == 0:
+            self._adjust_step_size()
+        return self.takestep(x)
+
+    def report(self, accept, **kwargs):
+        "called by basinhopping to report the result of the step"
+        if accept:
+            self.naccept += 1
+
+
+class RandomDisplacement:
+    """Add a random displacement of maximum size `stepsize` to each coordinate.
+
+    Calling this updates `x` in-place.
+
+    Parameters
+    ----------
+    stepsize : float, optional
+        Maximum stepsize in any dimension
+    random_gen : {None, int, `numpy.random.Generator`,
+                  `numpy.random.RandomState`}, optional
+
+        If `seed` is None (or `np.random`), the `numpy.random.RandomState`
+        singleton is used.
+        If `seed` is an int, a new ``RandomState`` instance is used,
+        seeded with `seed`.
+        If `seed` is already a ``Generator`` or ``RandomState`` instance then
+        that instance is used.
+
+    """
+
+    def __init__(self, stepsize=0.5, random_gen=None):
+        self.stepsize = stepsize
+        self.random_gen = check_random_state(random_gen)
+
+    def __call__(self, x):
+        x += self.random_gen.uniform(-self.stepsize, self.stepsize,
+                                     np.shape(x))
+        return x
+
+
+class MinimizerWrapper:
+    """
+    wrap a minimizer function as a minimizer class
+    """
+    def __init__(self, minimizer, func=None, **kwargs):
+        self.minimizer = minimizer
+        self.func = func
+        self.kwargs = kwargs
+
+    def __call__(self, x0):
+        if self.func is None:
+            return self.minimizer(x0, **self.kwargs)
+        else:
+            return self.minimizer(self.func, x0, **self.kwargs)
+
+
+class Metropolis:
+    """Metropolis acceptance criterion.
+
+    Parameters
+    ----------
+    T : float
+        The "temperature" parameter for the accept or reject criterion.
+    random_gen : {None, int, `numpy.random.Generator`,
+                  `numpy.random.RandomState`}, optional
+
+        If `seed` is None (or `np.random`), the `numpy.random.RandomState`
+        singleton is used.
+        If `seed` is an int, a new ``RandomState`` instance is used,
+        seeded with `seed`.
+        If `seed` is already a ``Generator`` or ``RandomState`` instance then
+        that instance is used.
+        Random number generator used for acceptance test.
+
+    """
+
+    def __init__(self, T, random_gen=None):
+        # Avoid ZeroDivisionError since "MBH can be regarded as a special case
+        # of the BH framework with the Metropolis criterion, where temperature
+        # T = 0." (Reject all steps that increase energy.)
+        self.beta = 1.0 / T if T != 0 else float('inf')
+        self.random_gen = check_random_state(random_gen)
+
+    def accept_reject(self, res_new, res_old):
+        """
+        Assuming the local search underlying res_new was successful:
+        If new energy is lower than old, it will always be accepted.
+        If new is higher than old, there is a chance it will be accepted,
+        less likely for larger differences.
+        """
+        with np.errstate(invalid='ignore'):
+            # The energy values being fed to Metropolis are 1-length arrays, and if
+            # they are equal, their difference is 0, which gets multiplied by beta,
+            # which is inf, and array([0]) * float('inf') causes
+            #
+            # RuntimeWarning: invalid value encountered in multiply
+            #
+            # Ignore this warning so when the algorithm is on a flat plane, it always
+            # accepts the step, to try to move off the plane.
+            prod = -(res_new.fun - res_old.fun) * self.beta
+            w = math.exp(min(0, prod))
+
+        rand = self.random_gen.uniform()
+        return w >= rand and (res_new.success or not res_old.success)
+
+    def __call__(self, *, res_new, res_old):
+        """
+        f_new and f_old are mandatory in kwargs
+        """
+        return bool(self.accept_reject(res_new, res_old))
+
+
+def basinhopping(func, x0, niter=100, T=1.0, stepsize=0.5,
+                 minimizer_kwargs=None, take_step=None, accept_test=None,
+                 callback=None, interval=50, disp=False, niter_success=None,
+                 seed=None, *, target_accept_rate=0.5, stepwise_factor=0.9):
+    """Find the global minimum of a function using the basin-hopping algorithm.
+
+    Basin-hopping is a two-phase method that combines a global stepping
+    algorithm with local minimization at each step. Designed to mimic
+    the natural process of energy minimization of clusters of atoms, it works
+    well for similar problems with "funnel-like, but rugged" energy landscapes
+    [5]_.
+
+    As the step-taking, step acceptance, and minimization methods are all
+    customizable, this function can also be used to implement other two-phase
+    methods.
+
+    Parameters
+    ----------
+    func : callable ``f(x, *args)``
+        Function to be optimized.  ``args`` can be passed as an optional item
+        in the dict `minimizer_kwargs`
+    x0 : array_like
+        Initial guess.
+    niter : integer, optional
+        The number of basin-hopping iterations. There will be a total of
+        ``niter + 1`` runs of the local minimizer.
+    T : float, optional
+        The "temperature" parameter for the acceptance or rejection criterion.
+        Higher "temperatures" mean that larger jumps in function value will be
+        accepted.  For best results `T` should be comparable to the
+        separation (in function value) between local minima.
+    stepsize : float, optional
+        Maximum step size for use in the random displacement.
+    minimizer_kwargs : dict, optional
+        Extra keyword arguments to be passed to the local minimizer
+        `scipy.optimize.minimize` Some important options could be:
+
+            method : str
+                The minimization method (e.g. ``"L-BFGS-B"``)
+            args : tuple
+                Extra arguments passed to the objective function (`func`) and
+                its derivatives (Jacobian, Hessian).
+
+    take_step : callable ``take_step(x)``, optional
+        Replace the default step-taking routine with this routine. The default
+        step-taking routine is a random displacement of the coordinates, but
+        other step-taking algorithms may be better for some systems.
+        `take_step` can optionally have the attribute ``take_step.stepsize``.
+        If this attribute exists, then `basinhopping` will adjust
+        ``take_step.stepsize`` in order to try to optimize the global minimum
+        search.
+    accept_test : callable, ``accept_test(f_new=f_new, x_new=x_new, f_old=fold, x_old=x_old)``, optional
+        Define a test which will be used to judge whether to accept the
+        step. This will be used in addition to the Metropolis test based on
+        "temperature" `T`. The acceptable return values are True,
+        False, or ``"force accept"``. If any of the tests return False
+        then the step is rejected. If the latter, then this will override any
+        other tests in order to accept the step. This can be used, for example,
+        to forcefully escape from a local minimum that `basinhopping` is
+        trapped in.
+    callback : callable, ``callback(x, f, accept)``, optional
+        A callback function which will be called for all minima found. ``x``
+        and ``f`` are the coordinates and function value of the trial minimum,
+        and ``accept`` is whether that minimum was accepted. This can
+        be used, for example, to save the lowest N minima found. Also,
+        `callback` can be used to specify a user defined stop criterion by
+        optionally returning True to stop the `basinhopping` routine.
+    interval : integer, optional
+        interval for how often to update the `stepsize`
+    disp : bool, optional
+        Set to True to print status messages
+    niter_success : integer, optional
+        Stop the run if the global minimum candidate remains the same for this
+        number of iterations.
+    seed : {None, int, `numpy.random.Generator`, `numpy.random.RandomState`}, optional
+
+        If `seed` is None (or `np.random`), the `numpy.random.RandomState`
+        singleton is used.
+        If `seed` is an int, a new ``RandomState`` instance is used,
+        seeded with `seed`.
+        If `seed` is already a ``Generator`` or ``RandomState`` instance then
+        that instance is used.
+        Specify `seed` for repeatable minimizations. The random numbers
+        generated with this seed only affect the default Metropolis
+        `accept_test` and the default `take_step`. If you supply your own
+        `take_step` and `accept_test`, and these functions use random
+        number generation, then those functions are responsible for the state
+        of their random number generator.
+    target_accept_rate : float, optional
+        The target acceptance rate that is used to adjust the `stepsize`.
+        If the current acceptance rate is greater than the target,
+        then the `stepsize` is increased. Otherwise, it is decreased.
+        Range is (0, 1). Default is 0.5.
+
+        .. versionadded:: 1.8.0
+
+    stepwise_factor : float, optional
+        The `stepsize` is multiplied or divided by this stepwise factor upon
+        each update. Range is (0, 1). Default is 0.9.
+
+        .. versionadded:: 1.8.0
+
+    Returns
+    -------
+    res : OptimizeResult
+        The optimization result represented as a `OptimizeResult` object.
+        Important attributes are: ``x`` the solution array, ``fun`` the value
+        of the function at the solution, and ``message`` which describes the
+        cause of the termination. The ``OptimizeResult`` object returned by the
+        selected minimizer at the lowest minimum is also contained within this
+        object and can be accessed through the ``lowest_optimization_result``
+        attribute.  See `OptimizeResult` for a description of other attributes.
+
+    See Also
+    --------
+    minimize :
+        The local minimization function called once for each basinhopping step.
+        `minimizer_kwargs` is passed to this routine.
+
+    Notes
+    -----
+    Basin-hopping is a stochastic algorithm which attempts to find the global
+    minimum of a smooth scalar function of one or more variables [1]_ [2]_ [3]_
+    [4]_. The algorithm in its current form was described by David Wales and
+    Jonathan Doye [2]_ http://www-wales.ch.cam.ac.uk/.
+
+    The algorithm is iterative with each cycle composed of the following
+    features
+
+    1) random perturbation of the coordinates
+
+    2) local minimization
+
+    3) accept or reject the new coordinates based on the minimized function
+       value
+
+    The acceptance test used here is the Metropolis criterion of standard Monte
+    Carlo algorithms, although there are many other possibilities [3]_.
+
+    This global minimization method has been shown to be extremely efficient
+    for a wide variety of problems in physics and chemistry. It is
+    particularly useful when the function has many minima separated by large
+    barriers. See the `Cambridge Cluster Database
+    <https://www-wales.ch.cam.ac.uk/CCD.html>`_ for databases of molecular
+    systems that have been optimized primarily using basin-hopping. This
+    database includes minimization problems exceeding 300 degrees of freedom.
+
+    See the free software program `GMIN <https://www-wales.ch.cam.ac.uk/GMIN>`_
+    for a Fortran implementation of basin-hopping. This implementation has many
+    variations of the procedure described above, including more
+    advanced step taking algorithms and alternate acceptance criterion.
+
+    For stochastic global optimization there is no way to determine if the true
+    global minimum has actually been found. Instead, as a consistency check,
+    the algorithm can be run from a number of different random starting points
+    to ensure the lowest minimum found in each example has converged to the
+    global minimum. For this reason, `basinhopping` will by default simply
+    run for the number of iterations `niter` and return the lowest minimum
+    found. It is left to the user to ensure that this is in fact the global
+    minimum.
+
+    Choosing `stepsize`:  This is a crucial parameter in `basinhopping` and
+    depends on the problem being solved. The step is chosen uniformly in the
+    region from x0-stepsize to x0+stepsize, in each dimension. Ideally, it
+    should be comparable to the typical separation (in argument values) between
+    local minima of the function being optimized. `basinhopping` will, by
+    default, adjust `stepsize` to find an optimal value, but this may take
+    many iterations. You will get quicker results if you set a sensible
+    initial value for ``stepsize``.
+
+    Choosing `T`: The parameter `T` is the "temperature" used in the
+    Metropolis criterion. Basinhopping steps are always accepted if
+    ``func(xnew) < func(xold)``. Otherwise, they are accepted with
+    probability::
+
+        exp( -(func(xnew) - func(xold)) / T )
+
+    So, for best results, `T` should to be comparable to the typical
+    difference (in function values) between local minima. (The height of
+    "walls" between local minima is irrelevant.)
+
+    If `T` is 0, the algorithm becomes Monotonic Basin-Hopping, in which all
+    steps that increase energy are rejected.
+
+    .. versionadded:: 0.12.0
+
+    References
+    ----------
+    .. [1] Wales, David J. 2003, Energy Landscapes, Cambridge University Press,
+        Cambridge, UK.
+    .. [2] Wales, D J, and Doye J P K, Global Optimization by Basin-Hopping and
+        the Lowest Energy Structures of Lennard-Jones Clusters Containing up to
+        110 Atoms.  Journal of Physical Chemistry A, 1997, 101, 5111.
+    .. [3] Li, Z. and Scheraga, H. A., Monte Carlo-minimization approach to the
+        multiple-minima problem in protein folding, Proc. Natl. Acad. Sci. USA,
+        1987, 84, 6611.
+    .. [4] Wales, D. J. and Scheraga, H. A., Global optimization of clusters,
+        crystals, and biomolecules, Science, 1999, 285, 1368.
+    .. [5] Olson, B., Hashmi, I., Molloy, K., and Shehu1, A., Basin Hopping as
+        a General and Versatile Optimization Framework for the Characterization
+        of Biological Macromolecules, Advances in Artificial Intelligence,
+        Volume 2012 (2012), Article ID 674832, :doi:`10.1155/2012/674832`
+
+    Examples
+    --------
+    The following example is a 1-D minimization problem, with many
+    local minima superimposed on a parabola.
+
+    >>> import numpy as np
+    >>> from scipy.optimize import basinhopping
+    >>> func = lambda x: np.cos(14.5 * x - 0.3) + (x + 0.2) * x
+    >>> x0 = [1.]
+
+    Basinhopping, internally, uses a local minimization algorithm. We will use
+    the parameter `minimizer_kwargs` to tell basinhopping which algorithm to
+    use and how to set up that minimizer. This parameter will be passed to
+    `scipy.optimize.minimize`.
+
+    >>> minimizer_kwargs = {"method": "BFGS"}
+    >>> ret = basinhopping(func, x0, minimizer_kwargs=minimizer_kwargs,
+    ...                    niter=200)
+    >>> print("global minimum: x = %.4f, f(x) = %.4f" % (ret.x, ret.fun))
+    global minimum: x = -0.1951, f(x) = -1.0009
+
+    Next consider a 2-D minimization problem. Also, this time, we
+    will use gradient information to significantly speed up the search.
+
+    >>> def func2d(x):
+    ...     f = np.cos(14.5 * x[0] - 0.3) + (x[1] + 0.2) * x[1] + (x[0] +
+    ...                                                            0.2) * x[0]
+    ...     df = np.zeros(2)
+    ...     df[0] = -14.5 * np.sin(14.5 * x[0] - 0.3) + 2. * x[0] + 0.2
+    ...     df[1] = 2. * x[1] + 0.2
+    ...     return f, df
+
+    We'll also use a different local minimization algorithm. Also, we must tell
+    the minimizer that our function returns both energy and gradient (Jacobian).
+
+    >>> minimizer_kwargs = {"method":"L-BFGS-B", "jac":True}
+    >>> x0 = [1.0, 1.0]
+    >>> ret = basinhopping(func2d, x0, minimizer_kwargs=minimizer_kwargs,
+    ...                    niter=200)
+    >>> print("global minimum: x = [%.4f, %.4f], f(x) = %.4f" % (ret.x[0],
+    ...                                                           ret.x[1],
+    ...                                                           ret.fun))
+    global minimum: x = [-0.1951, -0.1000], f(x) = -1.0109
+
+    Here is an example using a custom step-taking routine. Imagine you want
+    the first coordinate to take larger steps than the rest of the coordinates.
+    This can be implemented like so:
+
+    >>> class MyTakeStep:
+    ...    def __init__(self, stepsize=0.5):
+    ...        self.stepsize = stepsize
+    ...        self.rng = np.random.default_rng()
+    ...    def __call__(self, x):
+    ...        s = self.stepsize
+    ...        x[0] += self.rng.uniform(-2.*s, 2.*s)
+    ...        x[1:] += self.rng.uniform(-s, s, x[1:].shape)
+    ...        return x
+
+    Since ``MyTakeStep.stepsize`` exists basinhopping will adjust the magnitude
+    of `stepsize` to optimize the search. We'll use the same 2-D function as
+    before
+
+    >>> mytakestep = MyTakeStep()
+    >>> ret = basinhopping(func2d, x0, minimizer_kwargs=minimizer_kwargs,
+    ...                    niter=200, take_step=mytakestep)
+    >>> print("global minimum: x = [%.4f, %.4f], f(x) = %.4f" % (ret.x[0],
+    ...                                                           ret.x[1],
+    ...                                                           ret.fun))
+    global minimum: x = [-0.1951, -0.1000], f(x) = -1.0109
+
+    Now, let's do an example using a custom callback function which prints the
+    value of every minimum found
+
+    >>> def print_fun(x, f, accepted):
+    ...         print("at minimum %.4f accepted %d" % (f, int(accepted)))
+
+    We'll run it for only 10 basinhopping steps this time.
+
+    >>> rng = np.random.default_rng()
+    >>> ret = basinhopping(func2d, x0, minimizer_kwargs=minimizer_kwargs,
+    ...                    niter=10, callback=print_fun, seed=rng)
+    at minimum 0.4159 accepted 1
+    at minimum -0.4317 accepted 1
+    at minimum -1.0109 accepted 1
+    at minimum -0.9073 accepted 1
+    at minimum -0.4317 accepted 0
+    at minimum -0.1021 accepted 1
+    at minimum -0.7425 accepted 1
+    at minimum -0.9073 accepted 1
+    at minimum -0.4317 accepted 0
+    at minimum -0.7425 accepted 1
+    at minimum -0.9073 accepted 1
+
+    The minimum at -1.0109 is actually the global minimum, found already on the
+    8th iteration.
+
+    """ # numpy/numpydoc#87  # noqa: E501
+    if target_accept_rate <= 0. or target_accept_rate >= 1.:
+        raise ValueError('target_accept_rate has to be in range (0, 1)')
+    if stepwise_factor <= 0. or stepwise_factor >= 1.:
+        raise ValueError('stepwise_factor has to be in range (0, 1)')
+
+    x0 = np.array(x0)
+
+    # set up the np.random generator
+    rng = check_random_state(seed)
+
+    # set up minimizer
+    if minimizer_kwargs is None:
+        minimizer_kwargs = dict()
+    wrapped_minimizer = MinimizerWrapper(scipy.optimize.minimize, func,
+                                         **minimizer_kwargs)
+
+    # set up step-taking algorithm
+    if take_step is not None:
+        if not callable(take_step):
+            raise TypeError("take_step must be callable")
+        # if take_step.stepsize exists then use AdaptiveStepsize to control
+        # take_step.stepsize
+        if hasattr(take_step, "stepsize"):
+            take_step_wrapped = AdaptiveStepsize(
+                take_step, interval=interval,
+                accept_rate=target_accept_rate,
+                factor=stepwise_factor,
+                verbose=disp)
+        else:
+            take_step_wrapped = take_step
+    else:
+        # use default
+        displace = RandomDisplacement(stepsize=stepsize, random_gen=rng)
+        take_step_wrapped = AdaptiveStepsize(displace, interval=interval,
+                                             accept_rate=target_accept_rate,
+                                             factor=stepwise_factor,
+                                             verbose=disp)
+
+    # set up accept tests
+    accept_tests = []
+    if accept_test is not None:
+        if not callable(accept_test):
+            raise TypeError("accept_test must be callable")
+        accept_tests = [accept_test]
+
+    # use default
+    metropolis = Metropolis(T, random_gen=rng)
+    accept_tests.append(metropolis)
+
+    if niter_success is None:
+        niter_success = niter + 2
+
+    bh = BasinHoppingRunner(x0, wrapped_minimizer, take_step_wrapped,
+                            accept_tests, disp=disp)
+
+    # The wrapped minimizer is called once during construction of
+    # BasinHoppingRunner, so run the callback
+    if callable(callback):
+        callback(bh.storage.minres.x, bh.storage.minres.fun, True)
+
+    # start main iteration loop
+    count, i = 0, 0
+    message = ["requested number of basinhopping iterations completed"
+               " successfully"]
+    for i in range(niter):
+        new_global_min = bh.one_cycle()
+
+        if callable(callback):
+            # should we pass a copy of x?
+            val = callback(bh.xtrial, bh.energy_trial, bh.accept)
+            if val is not None:
+                if val:
+                    message = ["callback function requested stop early by"
+                               "returning True"]
+                    break
+
+        count += 1
+        if new_global_min:
+            count = 0
+        elif count > niter_success:
+            message = ["success condition satisfied"]
+            break
+
+    # prepare return object
+    res = bh.res
+    res.lowest_optimization_result = bh.storage.get_lowest()
+    res.x = np.copy(res.lowest_optimization_result.x)
+    res.fun = res.lowest_optimization_result.fun
+    res.message = message
+    res.nit = i + 1
+    res.success = res.lowest_optimization_result.success
+    return res

llmeval-env/lib/python3.10/site-packages/scipy/optimize/_dcsrch.py

@@ -0,0 +1,728 @@
+import numpy as np
+
+"""
+# 2023 - ported from minpack2.dcsrch, dcstep (Fortran) to Python
+c     MINPACK-1 Project. June 1983.
+c     Argonne National Laboratory.
+c     Jorge J. More' and David J. Thuente.
+c
+c     MINPACK-2 Project. November 1993.
+c     Argonne National Laboratory and University of Minnesota.
+c     Brett M. Averick, Richard G. Carter, and Jorge J. More'.
+"""
+
+# NOTE this file was linted by black on first commit, and can be kept that way.
+
+
+class DCSRCH:
+    """
+    Parameters
+    ----------
+    phi : callable phi(alpha)
+        Function at point `alpha`
+    derphi : callable phi'(alpha)
+        Objective function derivative. Returns a scalar.
+    ftol : float
+        A nonnegative tolerance for the sufficient decrease condition.
+    gtol : float
+        A nonnegative tolerance for the curvature condition.
+    xtol : float
+        A nonnegative relative tolerance for an acceptable step. The
+        subroutine exits with a warning if the relative difference between
+        sty and stx is less than xtol.
+    stpmin : float
+        A nonnegative lower bound for the step.
+    stpmax :
+        A nonnegative upper bound for the step.
+
+    Notes
+    -----
+
+    This subroutine finds a step that satisfies a sufficient
+    decrease condition and a curvature condition.
+
+    Each call of the subroutine updates an interval with
+    endpoints stx and sty. The interval is initially chosen
+    so that it contains a minimizer of the modified function
+
+           psi(stp) = f(stp) - f(0) - ftol*stp*f'(0).
+
+    If psi(stp) <= 0 and f'(stp) >= 0 for some step, then the
+    interval is chosen so that it contains a minimizer of f.
+
+    The algorithm is designed to find a step that satisfies
+    the sufficient decrease condition
+
+           f(stp) <= f(0) + ftol*stp*f'(0),
+
+    and the curvature condition
+
+           abs(f'(stp)) <= gtol*abs(f'(0)).
+
+    If ftol is less than gtol and if, for example, the function
+    is bounded below, then there is always a step which satisfies
+    both conditions.
+
+    If no step can be found that satisfies both conditions, then
+    the algorithm stops with a warning. In this case stp only
+    satisfies the sufficient decrease condition.
+
+    A typical invocation of dcsrch has the following outline:
+
+    Evaluate the function at stp = 0.0d0; store in f.
+    Evaluate the gradient at stp = 0.0d0; store in g.
+    Choose a starting step stp.
+
+    task = 'START'
+    10 continue
+        call dcsrch(stp,f,g,ftol,gtol,xtol,task,stpmin,stpmax,
+                   isave,dsave)
+        if (task .eq. 'FG') then
+           Evaluate the function and the gradient at stp
+           go to 10
+           end if
+
+    NOTE: The user must not alter work arrays between calls.
+
+    The subroutine statement is
+
+        subroutine dcsrch(f,g,stp,ftol,gtol,xtol,stpmin,stpmax,
+                         task,isave,dsave)
+        where
+
+    stp is a double precision variable.
+        On entry stp is the current estimate of a satisfactory
+            step. On initial entry, a positive initial estimate
+            must be provided.
+        On exit stp is the current estimate of a satisfactory step
+            if task = 'FG'. If task = 'CONV' then stp satisfies
+            the sufficient decrease and curvature condition.
+
+    f is a double precision variable.
+        On initial entry f is the value of the function at 0.
+        On subsequent entries f is the value of the
+            function at stp.
+        On exit f is the value of the function at stp.
+
+    g is a double precision variable.
+        On initial entry g is the derivative of the function at 0.
+        On subsequent entries g is the derivative of the
+           function at stp.
+        On exit g is the derivative of the function at stp.
+
+    ftol is a double precision variable.
+        On entry ftol specifies a nonnegative tolerance for the
+           sufficient decrease condition.
+        On exit ftol is unchanged.
+
+    gtol is a double precision variable.
+        On entry gtol specifies a nonnegative tolerance for the
+           curvature condition.
+        On exit gtol is unchanged.
+
+    xtol is a double precision variable.
+        On entry xtol specifies a nonnegative relative tolerance
+          for an acceptable step. The subroutine exits with a
+          warning if the relative difference between sty and stx
+          is less than xtol.
+
+        On exit xtol is unchanged.
+
+    task is a character variable of length at least 60.
+        On initial entry task must be set to 'START'.
+        On exit task indicates the required action:
+
+           If task(1:2) = 'FG' then evaluate the function and
+           derivative at stp and call dcsrch again.
+
+           If task(1:4) = 'CONV' then the search is successful.
+
+           If task(1:4) = 'WARN' then the subroutine is not able
+           to satisfy the convergence conditions. The exit value of
+           stp contains the best point found during the search.
+
+          If task(1:5) = 'ERROR' then there is an error in the
+          input arguments.
+
+        On exit with convergence, a warning or an error, the
+           variable task contains additional information.
+
+    stpmin is a double precision variable.
+        On entry stpmin is a nonnegative lower bound for the step.
+        On exit stpmin is unchanged.
+
+    stpmax is a double precision variable.
+        On entry stpmax is a nonnegative upper bound for the step.
+        On exit stpmax is unchanged.
+
+    isave is an integer work array of dimension 2.
+
+    dsave is a double precision work array of dimension 13.
+
+    Subprograms called
+
+      MINPACK-2 ... dcstep
+    MINPACK-1 Project. June 1983.
+    Argonne National Laboratory.
+    Jorge J. More' and David J. Thuente.
+
+    MINPACK-2 Project. November 1993.
+    Argonne National Laboratory and University of Minnesota.
+    Brett M. Averick, Richard G. Carter, and Jorge J. More'.
+    """
+
+    def __init__(self, phi, derphi, ftol, gtol, xtol, stpmin, stpmax):
+        self.stage = None
+        self.ginit = None
+        self.gtest = None
+        self.gx = None
+        self.gy = None
+        self.finit = None
+        self.fx = None
+        self.fy = None
+        self.stx = None
+        self.sty = None
+        self.stmin = None
+        self.stmax = None
+        self.width = None
+        self.width1 = None
+
+        # leave all assessment of tolerances/limits to the first call of
+        # this object
+        self.ftol = ftol
+        self.gtol = gtol
+        self.xtol = xtol
+        self.stpmin = stpmin
+        self.stpmax = stpmax
+
+        self.phi = phi
+        self.derphi = derphi
+
+    def __call__(self, alpha1, phi0=None, derphi0=None, maxiter=100):
+        """
+        Parameters
+        ----------
+        alpha1 : float
+            alpha1 is the current estimate of a satisfactory
+            step. A positive initial estimate must be provided.
+        phi0 : float
+            the value of `phi` at 0 (if known).
+        derphi0 : float
+            the derivative of `derphi` at 0 (if known).
+        maxiter : int
+
+        Returns
+        -------
+        alpha : float
+            Step size, or None if no suitable step was found.
+        phi : float
+            Value of `phi` at the new point `alpha`.
+        phi0 : float
+            Value of `phi` at `alpha=0`.
+        task : bytes
+            On exit task indicates status information.
+
+           If task[:4] == b'CONV' then the search is successful.
+
+           If task[:4] == b'WARN' then the subroutine is not able
+           to satisfy the convergence conditions. The exit value of
+           stp contains the best point found during the search.
+
+           If task[:5] == b'ERROR' then there is an error in the
+           input arguments.
+        """
+        if phi0 is None:
+            phi0 = self.phi(0.0)
+        if derphi0 is None:
+            derphi0 = self.derphi(0.0)
+
+        phi1 = phi0
+        derphi1 = derphi0
+
+        task = b"START"
+        for i in range(maxiter):
+            stp, phi1, derphi1, task = self._iterate(
+                alpha1, phi1, derphi1, task
+            )
+
+            if not np.isfinite(stp):
+                task = b"WARN"
+                stp = None
+                break
+
+            if task[:2] == b"FG":
+                alpha1 = stp
+                phi1 = self.phi(stp)
+                derphi1 = self.derphi(stp)
+            else:
+                break
+        else:
+            # maxiter reached, the line search did not converge
+            stp = None
+            task = b"WARNING: dcsrch did not converge within max iterations"
+
+        if task[:5] == b"ERROR" or task[:4] == b"WARN":
+            stp = None  # failed
+
+        return stp, phi1, phi0, task
+
+    def _iterate(self, stp, f, g, task):
+        """
+        Parameters
+        ----------
+        stp : float
+            The current estimate of a satisfactory step. On initial entry, a
+            positive initial estimate must be provided.
+        f : float
+            On first call f is the value of the function at 0. On subsequent
+            entries f should be the value of the function at stp.
+        g : float
+            On initial entry g is the derivative of the function at 0. On
+            subsequent entries g is the derivative of the function at stp.
+        task : bytes
+            On initial entry task must be set to 'START'.
+
+        On exit with convergence, a warning or an error, the
+           variable task contains additional information.
+
+
+        Returns
+        -------
+        stp, f, g, task: tuple
+
+            stp : float
+                the current estimate of a satisfactory step if task = 'FG'. If
+                task = 'CONV' then stp satisfies the sufficient decrease and
+                curvature condition.
+            f : float
+                the value of the function at stp.
+            g : float
+                the derivative of the function at stp.
+            task : bytes
+                On exit task indicates the required action:
+
+               If task(1:2) == b'FG' then evaluate the function and
+               derivative at stp and call dcsrch again.
+
+               If task(1:4) == b'CONV' then the search is successful.
+
+               If task(1:4) == b'WARN' then the subroutine is not able
+               to satisfy the convergence conditions. The exit value of
+               stp contains the best point found during the search.
+
+              If task(1:5) == b'ERROR' then there is an error in the
+              input arguments.
+        """
+        p5 = 0.5
+        p66 = 0.66
+        xtrapl = 1.1
+        xtrapu = 4.0
+
+        if task[:5] == b"START":
+            if stp < self.stpmin:
+                task = b"ERROR: STP .LT. STPMIN"
+            if stp > self.stpmax:
+                task = b"ERROR: STP .GT. STPMAX"
+            if g >= 0:
+                task = b"ERROR: INITIAL G .GE. ZERO"
+            if self.ftol < 0:
+                task = b"ERROR: FTOL .LT. ZERO"
+            if self.gtol < 0:
+                task = b"ERROR: GTOL .LT. ZERO"
+            if self.xtol < 0:
+                task = b"ERROR: XTOL .LT. ZERO"
+            if self.stpmin < 0:
+                task = b"ERROR: STPMIN .LT. ZERO"
+            if self.stpmax < self.stpmin:
+                task = b"ERROR: STPMAX .LT. STPMIN"
+
+            if task[:5] == b"ERROR":
+                return stp, f, g, task
+
+            # Initialize local variables.
+
+            self.brackt = False
+            self.stage = 1
+            self.finit = f
+            self.ginit = g
+            self.gtest = self.ftol * self.ginit
+            self.width = self.stpmax - self.stpmin
+            self.width1 = self.width / p5
+
+            # The variables stx, fx, gx contain the values of the step,
+            # function, and derivative at the best step.
+            # The variables sty, fy, gy contain the value of the step,
+            # function, and derivative at sty.
+            # The variables stp, f, g contain the values of the step,
+            # function, and derivative at stp.
+
+            self.stx = 0.0
+            self.fx = self.finit
+            self.gx = self.ginit
+            self.sty = 0.0
+            self.fy = self.finit
+            self.gy = self.ginit
+            self.stmin = 0
+            self.stmax = stp + xtrapu * stp
+            task = b"FG"
+            return stp, f, g, task
+
+        # in the original Fortran this was a location to restore variables
+        # we don't need to do that because they're attributes.
+
+        # If psi(stp) <= 0 and f'(stp) >= 0 for some step, then the
+        # algorithm enters the second stage.
+        ftest = self.finit + stp * self.gtest
+
+        if self.stage == 1 and f <= ftest and g >= 0:
+            self.stage = 2
+
+        # test for warnings
+        if self.brackt and (stp <= self.stmin or stp >= self.stmax):
+            task = b"WARNING: ROUNDING ERRORS PREVENT PROGRESS"
+        if self.brackt and self.stmax - self.stmin <= self.xtol * self.stmax:
+            task = b"WARNING: XTOL TEST SATISFIED"
+        if stp == self.stpmax and f <= ftest and g <= self.gtest:
+            task = b"WARNING: STP = STPMAX"
+        if stp == self.stpmin and (f > ftest or g >= self.gtest):
+            task = b"WARNING: STP = STPMIN"
+
+        # test for convergence
+        if f <= ftest and abs(g) <= self.gtol * -self.ginit:
+            task = b"CONVERGENCE"
+
+        # test for termination
+        if task[:4] == b"WARN" or task[:4] == b"CONV":
+            return stp, f, g, task
+
+        # A modified function is used to predict the step during the
+        # first stage if a lower function value has been obtained but
+        # the decrease is not sufficient.
+        if self.stage == 1 and f <= self.fx and f > ftest:
+            # Define the modified function and derivative values.
+            fm = f - stp * self.gtest
+            fxm = self.fx - self.stx * self.gtest
+            fym = self.fy - self.sty * self.gtest
+            gm = g - self.gtest
+            gxm = self.gx - self.gtest
+            gym = self.gy - self.gtest
+
+            # Call dcstep to update stx, sty, and to compute the new step.
+            # dcstep can have several operations which can produce NaN
+            # e.g. inf/inf. Filter these out.
+            with np.errstate(invalid="ignore", over="ignore"):
+                tup = dcstep(
+                    self.stx,
+                    fxm,
+                    gxm,
+                    self.sty,
+                    fym,
+                    gym,
+                    stp,
+                    fm,
+                    gm,
+                    self.brackt,
+                    self.stmin,
+                    self.stmax,
+                )
+                self.stx, fxm, gxm, self.sty, fym, gym, stp, self.brackt = tup
+
+            # Reset the function and derivative values for f
+            self.fx = fxm + self.stx * self.gtest
+            self.fy = fym + self.sty * self.gtest
+            self.gx = gxm + self.gtest
+            self.gy = gym + self.gtest
+
+        else:
+            # Call dcstep to update stx, sty, and to compute the new step.
+            # dcstep can have several operations which can produce NaN
+            # e.g. inf/inf. Filter these out.
+
+            with np.errstate(invalid="ignore", over="ignore"):
+                tup = dcstep(
+                    self.stx,
+                    self.fx,
+                    self.gx,
+                    self.sty,
+                    self.fy,
+                    self.gy,
+                    stp,
+                    f,
+                    g,
+                    self.brackt,
+                    self.stmin,
+                    self.stmax,
+                )
+            (
+                self.stx,
+                self.fx,
+                self.gx,
+                self.sty,
+                self.fy,
+                self.gy,
+                stp,
+                self.brackt,
+            ) = tup
+
+        # Decide if a bisection step is needed
+        if self.brackt:
+            if abs(self.sty - self.stx) >= p66 * self.width1:
+                stp = self.stx + p5 * (self.sty - self.stx)
+            self.width1 = self.width
+            self.width = abs(self.sty - self.stx)
+
+        # Set the minimum and maximum steps allowed for stp.
+        if self.brackt:
+            self.stmin = min(self.stx, self.sty)
+            self.stmax = max(self.stx, self.sty)
+        else:
+            self.stmin = stp + xtrapl * (stp - self.stx)
+            self.stmax = stp + xtrapu * (stp - self.stx)
+
+        # Force the step to be within the bounds stpmax and stpmin.
+        stp = np.clip(stp, self.stpmin, self.stpmax)
+
+        # If further progress is not possible, let stp be the best
+        # point obtained during the search.
+        if (
+            self.brackt
+            and (stp <= self.stmin or stp >= self.stmax)
+            or (
+                self.brackt
+                and self.stmax - self.stmin <= self.xtol * self.stmax
+            )
+        ):
+            stp = self.stx
+
+        # Obtain another function and derivative
+        task = b"FG"
+        return stp, f, g, task
+
+
+def dcstep(stx, fx, dx, sty, fy, dy, stp, fp, dp, brackt, stpmin, stpmax):
+    """
+    Subroutine dcstep
+
+    This subroutine computes a safeguarded step for a search
+    procedure and updates an interval that contains a step that
+    satisfies a sufficient decrease and a curvature condition.
+
+    The parameter stx contains the step with the least function
+    value. If brackt is set to .true. then a minimizer has
+    been bracketed in an interval with endpoints stx and sty.
+    The parameter stp contains the current step.
+    The subroutine assumes that if brackt is set to .true. then
+
+        min(stx,sty) < stp < max(stx,sty),
+
+    and that the derivative at stx is negative in the direction
+    of the step.
+
+    The subroutine statement is
+
+      subroutine dcstep(stx,fx,dx,sty,fy,dy,stp,fp,dp,brackt,
+                        stpmin,stpmax)
+
+    where
+
+    stx is a double precision variable.
+        On entry stx is the best step obtained so far and is an
+          endpoint of the interval that contains the minimizer.
+        On exit stx is the updated best step.
+
+    fx is a double precision variable.
+        On entry fx is the function at stx.
+        On exit fx is the function at stx.
+
+    dx is a double precision variable.
+        On entry dx is the derivative of the function at
+          stx. The derivative must be negative in the direction of
+          the step, that is, dx and stp - stx must have opposite
+          signs.
+        On exit dx is the derivative of the function at stx.
+
+    sty is a double precision variable.
+        On entry sty is the second endpoint of the interval that
+          contains the minimizer.
+        On exit sty is the updated endpoint of the interval that
+          contains the minimizer.
+
+    fy is a double precision variable.
+        On entry fy is the function at sty.
+        On exit fy is the function at sty.
+
+    dy is a double precision variable.
+        On entry dy is the derivative of the function at sty.
+        On exit dy is the derivative of the function at the exit sty.
+
+    stp is a double precision variable.
+        On entry stp is the current step. If brackt is set to .true.
+          then on input stp must be between stx and sty.
+        On exit stp is a new trial step.
+
+    fp is a double precision variable.
+        On entry fp is the function at stp
+        On exit fp is unchanged.
+
+    dp is a double precision variable.
+        On entry dp is the derivative of the function at stp.
+        On exit dp is unchanged.
+
+    brackt is an logical variable.
+        On entry brackt specifies if a minimizer has been bracketed.
+            Initially brackt must be set to .false.
+        On exit brackt specifies if a minimizer has been bracketed.
+            When a minimizer is bracketed brackt is set to .true.
+
+    stpmin is a double precision variable.
+        On entry stpmin is a lower bound for the step.
+        On exit stpmin is unchanged.
+
+    stpmax is a double precision variable.
+        On entry stpmax is an upper bound for the step.
+        On exit stpmax is unchanged.
+
+    MINPACK-1 Project. June 1983
+    Argonne National Laboratory.
+    Jorge J. More' and David J. Thuente.
+
+    MINPACK-2 Project. November 1993.
+    Argonne National Laboratory and University of Minnesota.
+    Brett M. Averick and Jorge J. More'.
+
+    """
+    sgn_dp = np.sign(dp)
+    sgn_dx = np.sign(dx)
+
+    # sgnd = dp * (dx / abs(dx))
+    sgnd = sgn_dp * sgn_dx
+
+    # First case: A higher function value. The minimum is bracketed.
+    # If the cubic step is closer to stx than the quadratic step, the
+    # cubic step is taken, otherwise the average of the cubic and
+    # quadratic steps is taken.
+    if fp > fx:
+        theta = 3.0 * (fx - fp) / (stp - stx) + dx + dp
+        s = max(abs(theta), abs(dx), abs(dp))
+        gamma = s * np.sqrt((theta / s) ** 2 - (dx / s) * (dp / s))
+        if stp < stx:
+            gamma *= -1
+        p = (gamma - dx) + theta
+        q = ((gamma - dx) + gamma) + dp
+        r = p / q
+        stpc = stx + r * (stp - stx)
+        stpq = stx + ((dx / ((fx - fp) / (stp - stx) + dx)) / 2.0) * (stp - stx)
+        if abs(stpc - stx) <= abs(stpq - stx):
+            stpf = stpc
+        else:
+            stpf = stpc + (stpq - stpc) / 2.0
+        brackt = True
+    elif sgnd < 0.0:
+        # Second case: A lower function value and derivatives of opposite
+        # sign. The minimum is bracketed. If the cubic step is farther from
+        # stp than the secant step, the cubic step is taken, otherwise the
+        # secant step is taken.
+        theta = 3 * (fx - fp) / (stp - stx) + dx + dp
+        s = max(abs(theta), abs(dx), abs(dp))
+        gamma = s * np.sqrt((theta / s) ** 2 - (dx / s) * (dp / s))
+        if stp > stx:
+            gamma *= -1
+        p = (gamma - dp) + theta
+        q = ((gamma - dp) + gamma) + dx
+        r = p / q
+        stpc = stp + r * (stx - stp)
+        stpq = stp + (dp / (dp - dx)) * (stx - stp)
+        if abs(stpc - stp) > abs(stpq - stp):
+            stpf = stpc
+        else:
+            stpf = stpq
+        brackt = True
+    elif abs(dp) < abs(dx):
+        # Third case: A lower function value, derivatives of the same sign,
+        # and the magnitude of the derivative decreases.
+
+        # The cubic step is computed only if the cubic tends to infinity
+        # in the direction of the step or if the minimum of the cubic
+        # is beyond stp. Otherwise the cubic step is defined to be the
+        # secant step.
+        theta = 3 * (fx - fp) / (stp - stx) + dx + dp
+        s = max(abs(theta), abs(dx), abs(dp))
+
+        # The case gamma = 0 only arises if the cubic does not tend
+        # to infinity in the direction of the step.
+        gamma = s * np.sqrt(max(0, (theta / s) ** 2 - (dx / s) * (dp / s)))
+        if stp > stx:
+            gamma = -gamma
+        p = (gamma - dp) + theta
+        q = (gamma + (dx - dp)) + gamma
+        r = p / q
+        if r < 0 and gamma != 0:
+            stpc = stp + r * (stx - stp)
+        elif stp > stx:
+            stpc = stpmax
+        else:
+            stpc = stpmin
+        stpq = stp + (dp / (dp - dx)) * (stx - stp)
+
+        if brackt:
+            # A minimizer has been bracketed. If the cubic step is
+            # closer to stp than the secant step, the cubic step is
+            # taken, otherwise the secant step is taken.
+            if abs(stpc - stp) < abs(stpq - stp):
+                stpf = stpc
+            else:
+                stpf = stpq
+
+            if stp > stx:
+                stpf = min(stp + 0.66 * (sty - stp), stpf)
+            else:
+                stpf = max(stp + 0.66 * (sty - stp), stpf)
+        else:
+            # A minimizer has not been bracketed. If the cubic step is
+            # farther from stp than the secant step, the cubic step is
+            # taken, otherwise the secant step is taken.
+            if abs(stpc - stp) > abs(stpq - stp):
+                stpf = stpc
+            else:
+                stpf = stpq
+            stpf = np.clip(stpf, stpmin, stpmax)
+
+    else:
+        # Fourth case: A lower function value, derivatives of the same sign,
+        # and the magnitude of the derivative does not decrease. If the
+        # minimum is not bracketed, the step is either stpmin or stpmax,
+        # otherwise the cubic step is taken.
+        if brackt:
+            theta = 3.0 * (fp - fy) / (sty - stp) + dy + dp
+            s = max(abs(theta), abs(dy), abs(dp))
+            gamma = s * np.sqrt((theta / s) ** 2 - (dy / s) * (dp / s))
+            if stp > sty:
+                gamma = -gamma
+            p = (gamma - dp) + theta
+            q = ((gamma - dp) + gamma) + dy
+            r = p / q
+            stpc = stp + r * (sty - stp)
+            stpf = stpc
+        elif stp > stx:
+            stpf = stpmax
+        else:
+            stpf = stpmin
+
+    # Update the interval which contains a minimizer.
+    if fp > fx:
+        sty = stp
+        fy = fp
+        dy = dp
+    else:
+        if sgnd < 0:
+            sty = stx
+            fy = fx
+            dy = dx
+        stx = stp
+        fx = fp
+        dx = dp
+
+    # Compute the new step.
+    stp = stpf
+
+    return stx, fx, dx, sty, fy, dy, stp, brackt

llmeval-env/lib/python3.10/site-packages/scipy/optimize/_differentiable_functions.py

@@ -0,0 +1,646 @@
+import numpy as np
+import scipy.sparse as sps
+from ._numdiff import approx_derivative, group_columns
+from ._hessian_update_strategy import HessianUpdateStrategy
+from scipy.sparse.linalg import LinearOperator
+from scipy._lib._array_api import atleast_nd, array_namespace
+
+
+FD_METHODS = ('2-point', '3-point', 'cs')
+
+
+class ScalarFunction:
+    """Scalar function and its derivatives.
+
+    This class defines a scalar function F: R^n->R and methods for
+    computing or approximating its first and second derivatives.
+
+    Parameters
+    ----------
+    fun : callable
+        evaluates the scalar function. Must be of the form ``fun(x, *args)``,
+        where ``x`` is the argument in the form of a 1-D array and ``args`` is
+        a tuple of any additional fixed parameters needed to completely specify
+        the function. Should return a scalar.
+    x0 : array-like
+        Provides an initial set of variables for evaluating fun. Array of real
+        elements of size (n,), where 'n' is the number of independent
+        variables.
+    args : tuple, optional
+        Any additional fixed parameters needed to completely specify the scalar
+        function.
+    grad : {callable, '2-point', '3-point', 'cs'}
+        Method for computing the gradient vector.
+        If it is a callable, it should be a function that returns the gradient
+        vector:
+
+            ``grad(x, *args) -> array_like, shape (n,)``
+
+        where ``x`` is an array with shape (n,) and ``args`` is a tuple with
+        the fixed parameters.
+        Alternatively, the keywords  {'2-point', '3-point', 'cs'} can be used
+        to select a finite difference scheme for numerical estimation of the
+        gradient with a relative step size. These finite difference schemes
+        obey any specified `bounds`.
+    hess : {callable, '2-point', '3-point', 'cs', HessianUpdateStrategy}
+        Method for computing the Hessian matrix. If it is callable, it should
+        return the  Hessian matrix:
+
+            ``hess(x, *args) -> {LinearOperator, spmatrix, array}, (n, n)``
+
+        where x is a (n,) ndarray and `args` is a tuple with the fixed
+        parameters. Alternatively, the keywords {'2-point', '3-point', 'cs'}
+        select a finite difference scheme for numerical estimation. Or, objects
+        implementing `HessianUpdateStrategy` interface can be used to
+        approximate the Hessian.
+        Whenever the gradient is estimated via finite-differences, the Hessian
+        cannot be estimated with options {'2-point', '3-point', 'cs'} and needs
+        to be estimated using one of the quasi-Newton strategies.
+    finite_diff_rel_step : None or array_like
+        Relative step size to use. The absolute step size is computed as
+        ``h = finite_diff_rel_step * sign(x0) * max(1, abs(x0))``, possibly
+        adjusted to fit into the bounds. For ``method='3-point'`` the sign
+        of `h` is ignored. If None then finite_diff_rel_step is selected
+        automatically,
+    finite_diff_bounds : tuple of array_like
+        Lower and upper bounds on independent variables. Defaults to no bounds,
+        (-np.inf, np.inf). Each bound must match the size of `x0` or be a
+        scalar, in the latter case the bound will be the same for all
+        variables. Use it to limit the range of function evaluation.
+    epsilon : None or array_like, optional
+        Absolute step size to use, possibly adjusted to fit into the bounds.
+        For ``method='3-point'`` the sign of `epsilon` is ignored. By default
+        relative steps are used, only if ``epsilon is not None`` are absolute
+        steps used.
+
+    Notes
+    -----
+    This class implements a memoization logic. There are methods `fun`,
+    `grad`, hess` and corresponding attributes `f`, `g` and `H`. The following
+    things should be considered:
+
+        1. Use only public methods `fun`, `grad` and `hess`.
+        2. After one of the methods is called, the corresponding attribute
+           will be set. However, a subsequent call with a different argument
+           of *any* of the methods may overwrite the attribute.
+    """
+    def __init__(self, fun, x0, args, grad, hess, finite_diff_rel_step,
+                 finite_diff_bounds, epsilon=None):
+        if not callable(grad) and grad not in FD_METHODS:
+            raise ValueError(
+                f"`grad` must be either callable or one of {FD_METHODS}."
+            )
+
+        if not (callable(hess) or hess in FD_METHODS
+                or isinstance(hess, HessianUpdateStrategy)):
+            raise ValueError(
+                f"`hess` must be either callable, HessianUpdateStrategy"
+                f" or one of {FD_METHODS}."
+            )
+
+        if grad in FD_METHODS and hess in FD_METHODS:
+            raise ValueError("Whenever the gradient is estimated via "
+                             "finite-differences, we require the Hessian "
+                             "to be estimated using one of the "
+                             "quasi-Newton strategies.")
+
+        self.xp = xp = array_namespace(x0)
+        _x = atleast_nd(x0, ndim=1, xp=xp)
+        _dtype = xp.float64
+        if xp.isdtype(_x.dtype, "real floating"):
+            _dtype = _x.dtype
+
+        # promotes to floating
+        self.x = xp.astype(_x, _dtype)
+        self.x_dtype = _dtype
+        self.n = self.x.size
+        self.nfev = 0
+        self.ngev = 0
+        self.nhev = 0
+        self.f_updated = False
+        self.g_updated = False
+        self.H_updated = False
+
+        self._lowest_x = None
+        self._lowest_f = np.inf
+
+        finite_diff_options = {}
+        if grad in FD_METHODS:
+            finite_diff_options["method"] = grad
+            finite_diff_options["rel_step"] = finite_diff_rel_step
+            finite_diff_options["abs_step"] = epsilon
+            finite_diff_options["bounds"] = finite_diff_bounds
+        if hess in FD_METHODS:
+            finite_diff_options["method"] = hess
+            finite_diff_options["rel_step"] = finite_diff_rel_step
+            finite_diff_options["abs_step"] = epsilon
+            finite_diff_options["as_linear_operator"] = True
+
+        # Function evaluation
+        def fun_wrapped(x):
+            self.nfev += 1
+            # Send a copy because the user may overwrite it.
+            # Overwriting results in undefined behaviour because
+            # fun(self.x) will change self.x, with the two no longer linked.
+            fx = fun(np.copy(x), *args)
+            # Make sure the function returns a true scalar
+            if not np.isscalar(fx):
+                try:
+                    fx = np.asarray(fx).item()
+                except (TypeError, ValueError) as e:
+                    raise ValueError(
+                        "The user-provided objective function "
+                        "must return a scalar value."
+                    ) from e
+
+            if fx < self._lowest_f:
+                self._lowest_x = x
+                self._lowest_f = fx
+
+            return fx
+
+        def update_fun():
+            self.f = fun_wrapped(self.x)
+
+        self._update_fun_impl = update_fun
+        self._update_fun()
+
+        # Gradient evaluation
+        if callable(grad):
+            def grad_wrapped(x):
+                self.ngev += 1
+                return np.atleast_1d(grad(np.copy(x), *args))
+
+            def update_grad():
+                self.g = grad_wrapped(self.x)
+
+        elif grad in FD_METHODS:
+            def update_grad():
+                self._update_fun()
+                self.ngev += 1
+                self.g = approx_derivative(fun_wrapped, self.x, f0=self.f,
+                                           **finite_diff_options)
+
+        self._update_grad_impl = update_grad
+        self._update_grad()
+
+        # Hessian Evaluation
+        if callable(hess):
+            self.H = hess(np.copy(x0), *args)
+            self.H_updated = True
+            self.nhev += 1
+
+            if sps.issparse(self.H):
+                def hess_wrapped(x):
+                    self.nhev += 1
+                    return sps.csr_matrix(hess(np.copy(x), *args))
+                self.H = sps.csr_matrix(self.H)
+
+            elif isinstance(self.H, LinearOperator):
+                def hess_wrapped(x):
+                    self.nhev += 1
+                    return hess(np.copy(x), *args)
+
+            else:
+                def hess_wrapped(x):
+                    self.nhev += 1
+                    return np.atleast_2d(np.asarray(hess(np.copy(x), *args)))
+                self.H = np.atleast_2d(np.asarray(self.H))
+
+            def update_hess():
+                self.H = hess_wrapped(self.x)
+
+        elif hess in FD_METHODS:
+            def update_hess():
+                self._update_grad()
+                self.H = approx_derivative(grad_wrapped, self.x, f0=self.g,
+                                           **finite_diff_options)
+                return self.H
+
+            update_hess()
+            self.H_updated = True
+        elif isinstance(hess, HessianUpdateStrategy):
+            self.H = hess
+            self.H.initialize(self.n, 'hess')
+            self.H_updated = True
+            self.x_prev = None
+            self.g_prev = None
+
+            def update_hess():
+                self._update_grad()
+                self.H.update(self.x - self.x_prev, self.g - self.g_prev)
+
+        self._update_hess_impl = update_hess
+
+        if isinstance(hess, HessianUpdateStrategy):
+            def update_x(x):
+                self._update_grad()
+                self.x_prev = self.x
+                self.g_prev = self.g
+                # ensure that self.x is a copy of x. Don't store a reference
+                # otherwise the memoization doesn't work properly.
+
+                _x = atleast_nd(x, ndim=1, xp=self.xp)
+                self.x = self.xp.astype(_x, self.x_dtype)
+                self.f_updated = False
+                self.g_updated = False
+                self.H_updated = False
+                self._update_hess()
+        else:
+            def update_x(x):
+                # ensure that self.x is a copy of x. Don't store a reference
+                # otherwise the memoization doesn't work properly.
+                _x = atleast_nd(x, ndim=1, xp=self.xp)
+                self.x = self.xp.astype(_x, self.x_dtype)
+                self.f_updated = False
+                self.g_updated = False
+                self.H_updated = False
+        self._update_x_impl = update_x
+
+    def _update_fun(self):
+        if not self.f_updated:
+            self._update_fun_impl()
+            self.f_updated = True
+
+    def _update_grad(self):
+        if not self.g_updated:
+            self._update_grad_impl()
+            self.g_updated = True
+
+    def _update_hess(self):
+        if not self.H_updated:
+            self._update_hess_impl()
+            self.H_updated = True
+
+    def fun(self, x):
+        if not np.array_equal(x, self.x):
+            self._update_x_impl(x)
+        self._update_fun()
+        return self.f
+
+    def grad(self, x):
+        if not np.array_equal(x, self.x):
+            self._update_x_impl(x)
+        self._update_grad()
+        return self.g
+
+    def hess(self, x):
+        if not np.array_equal(x, self.x):
+            self._update_x_impl(x)
+        self._update_hess()
+        return self.H
+
+    def fun_and_grad(self, x):
+        if not np.array_equal(x, self.x):
+            self._update_x_impl(x)
+        self._update_fun()
+        self._update_grad()
+        return self.f, self.g
+
+
+class VectorFunction:
+    """Vector function and its derivatives.
+
+    This class defines a vector function F: R^n->R^m and methods for
+    computing or approximating its first and second derivatives.
+
+    Notes
+    -----
+    This class implements a memoization logic. There are methods `fun`,
+    `jac`, hess` and corresponding attributes `f`, `J` and `H`. The following
+    things should be considered:
+
+        1. Use only public methods `fun`, `jac` and `hess`.
+        2. After one of the methods is called, the corresponding attribute
+           will be set. However, a subsequent call with a different argument
+           of *any* of the methods may overwrite the attribute.
+    """
+    def __init__(self, fun, x0, jac, hess,
+                 finite_diff_rel_step, finite_diff_jac_sparsity,
+                 finite_diff_bounds, sparse_jacobian):
+        if not callable(jac) and jac not in FD_METHODS:
+            raise ValueError(f"`jac` must be either callable or one of {FD_METHODS}.")
+
+        if not (callable(hess) or hess in FD_METHODS
+                or isinstance(hess, HessianUpdateStrategy)):
+            raise ValueError("`hess` must be either callable,"
+                             f"HessianUpdateStrategy or one of {FD_METHODS}.")
+
+        if jac in FD_METHODS and hess in FD_METHODS:
+            raise ValueError("Whenever the Jacobian is estimated via "
+                             "finite-differences, we require the Hessian to "
+                             "be estimated using one of the quasi-Newton "
+                             "strategies.")
+
+        self.xp = xp = array_namespace(x0)
+        _x = atleast_nd(x0, ndim=1, xp=xp)
+        _dtype = xp.float64
+        if xp.isdtype(_x.dtype, "real floating"):
+            _dtype = _x.dtype
+
+        # promotes to floating
+        self.x = xp.astype(_x, _dtype)
+        self.x_dtype = _dtype
+
+        self.n = self.x.size
+        self.nfev = 0
+        self.njev = 0
+        self.nhev = 0
+        self.f_updated = False
+        self.J_updated = False
+        self.H_updated = False
+
+        finite_diff_options = {}
+        if jac in FD_METHODS:
+            finite_diff_options["method"] = jac
+            finite_diff_options["rel_step"] = finite_diff_rel_step
+            if finite_diff_jac_sparsity is not None:
+                sparsity_groups = group_columns(finite_diff_jac_sparsity)
+                finite_diff_options["sparsity"] = (finite_diff_jac_sparsity,
+                                                   sparsity_groups)
+            finite_diff_options["bounds"] = finite_diff_bounds
+            self.x_diff = np.copy(self.x)
+        if hess in FD_METHODS:
+            finite_diff_options["method"] = hess
+            finite_diff_options["rel_step"] = finite_diff_rel_step
+            finite_diff_options["as_linear_operator"] = True
+            self.x_diff = np.copy(self.x)
+        if jac in FD_METHODS and hess in FD_METHODS:
+            raise ValueError("Whenever the Jacobian is estimated via "
+                             "finite-differences, we require the Hessian to "
+                             "be estimated using one of the quasi-Newton "
+                             "strategies.")
+
+        # Function evaluation
+        def fun_wrapped(x):
+            self.nfev += 1
+            return np.atleast_1d(fun(x))
+
+        def update_fun():
+            self.f = fun_wrapped(self.x)
+
+        self._update_fun_impl = update_fun
+        update_fun()
+
+        self.v = np.zeros_like(self.f)
+        self.m = self.v.size
+
+        # Jacobian Evaluation
+        if callable(jac):
+            self.J = jac(self.x)
+            self.J_updated = True
+            self.njev += 1
+
+            if (sparse_jacobian or
+                    sparse_jacobian is None and sps.issparse(self.J)):
+                def jac_wrapped(x):
+                    self.njev += 1
+                    return sps.csr_matrix(jac(x))
+                self.J = sps.csr_matrix(self.J)
+                self.sparse_jacobian = True
+
+            elif sps.issparse(self.J):
+                def jac_wrapped(x):
+                    self.njev += 1
+                    return jac(x).toarray()
+                self.J = self.J.toarray()
+                self.sparse_jacobian = False
+
+            else:
+                def jac_wrapped(x):
+                    self.njev += 1
+                    return np.atleast_2d(jac(x))
+                self.J = np.atleast_2d(self.J)
+                self.sparse_jacobian = False
+
+            def update_jac():
+                self.J = jac_wrapped(self.x)
+
+        elif jac in FD_METHODS:
+            self.J = approx_derivative(fun_wrapped, self.x, f0=self.f,
+                                       **finite_diff_options)
+            self.J_updated = True
+
+            if (sparse_jacobian or
+                    sparse_jacobian is None and sps.issparse(self.J)):
+                def update_jac():
+                    self._update_fun()
+                    self.J = sps.csr_matrix(
+                        approx_derivative(fun_wrapped, self.x, f0=self.f,
+                                          **finite_diff_options))
+                self.J = sps.csr_matrix(self.J)
+                self.sparse_jacobian = True
+
+            elif sps.issparse(self.J):
+                def update_jac():
+                    self._update_fun()
+                    self.J = approx_derivative(fun_wrapped, self.x, f0=self.f,
+                                               **finite_diff_options).toarray()
+                self.J = self.J.toarray()
+                self.sparse_jacobian = False
+
+            else:
+                def update_jac():
+                    self._update_fun()
+                    self.J = np.atleast_2d(
+                        approx_derivative(fun_wrapped, self.x, f0=self.f,
+                                          **finite_diff_options))
+                self.J = np.atleast_2d(self.J)
+                self.sparse_jacobian = False
+
+        self._update_jac_impl = update_jac
+
+        # Define Hessian
+        if callable(hess):
+            self.H = hess(self.x, self.v)
+            self.H_updated = True
+            self.nhev += 1
+
+            if sps.issparse(self.H):
+                def hess_wrapped(x, v):
+                    self.nhev += 1
+                    return sps.csr_matrix(hess(x, v))
+                self.H = sps.csr_matrix(self.H)
+
+            elif isinstance(self.H, LinearOperator):
+                def hess_wrapped(x, v):
+                    self.nhev += 1
+                    return hess(x, v)
+
+            else:
+                def hess_wrapped(x, v):
+                    self.nhev += 1
+                    return np.atleast_2d(np.asarray(hess(x, v)))
+                self.H = np.atleast_2d(np.asarray(self.H))
+
+            def update_hess():
+                self.H = hess_wrapped(self.x, self.v)
+        elif hess in FD_METHODS:
+            def jac_dot_v(x, v):
+                return jac_wrapped(x).T.dot(v)
+
+            def update_hess():
+                self._update_jac()
+                self.H = approx_derivative(jac_dot_v, self.x,
+                                           f0=self.J.T.dot(self.v),
+                                           args=(self.v,),
+                                           **finite_diff_options)
+            update_hess()
+            self.H_updated = True
+        elif isinstance(hess, HessianUpdateStrategy):
+            self.H = hess
+            self.H.initialize(self.n, 'hess')
+            self.H_updated = True
+            self.x_prev = None
+            self.J_prev = None
+
+            def update_hess():
+                self._update_jac()
+                # When v is updated before x was updated, then x_prev and
+                # J_prev are None and we need this check.
+                if self.x_prev is not None and self.J_prev is not None:
+                    delta_x = self.x - self.x_prev
+                    delta_g = self.J.T.dot(self.v) - self.J_prev.T.dot(self.v)
+                    self.H.update(delta_x, delta_g)
+
+        self._update_hess_impl = update_hess
+
+        if isinstance(hess, HessianUpdateStrategy):
+            def update_x(x):
+                self._update_jac()
+                self.x_prev = self.x
+                self.J_prev = self.J
+                _x = atleast_nd(x, ndim=1, xp=self.xp)
+                self.x = self.xp.astype(_x, self.x_dtype)
+                self.f_updated = False
+                self.J_updated = False
+                self.H_updated = False
+                self._update_hess()
+        else:
+            def update_x(x):
+                _x = atleast_nd(x, ndim=1, xp=self.xp)
+                self.x = self.xp.astype(_x, self.x_dtype)
+                self.f_updated = False
+                self.J_updated = False
+                self.H_updated = False
+
+        self._update_x_impl = update_x
+
+    def _update_v(self, v):
+        if not np.array_equal(v, self.v):
+            self.v = v
+            self.H_updated = False
+
+    def _update_x(self, x):
+        if not np.array_equal(x, self.x):
+            self._update_x_impl(x)
+
+    def _update_fun(self):
+        if not self.f_updated:
+            self._update_fun_impl()
+            self.f_updated = True
+
+    def _update_jac(self):
+        if not self.J_updated:
+            self._update_jac_impl()
+            self.J_updated = True
+
+    def _update_hess(self):
+        if not self.H_updated:
+            self._update_hess_impl()
+            self.H_updated = True
+
+    def fun(self, x):
+        self._update_x(x)
+        self._update_fun()
+        return self.f
+
+    def jac(self, x):
+        self._update_x(x)
+        self._update_jac()
+        return self.J
+
+    def hess(self, x, v):
+        # v should be updated before x.
+        self._update_v(v)
+        self._update_x(x)
+        self._update_hess()
+        return self.H
+
+
+class LinearVectorFunction:
+    """Linear vector function and its derivatives.
+
+    Defines a linear function F = A x, where x is N-D vector and
+    A is m-by-n matrix. The Jacobian is constant and equals to A. The Hessian
+    is identically zero and it is returned as a csr matrix.
+    """
+    def __init__(self, A, x0, sparse_jacobian):
+        if sparse_jacobian or sparse_jacobian is None and sps.issparse(A):
+            self.J = sps.csr_matrix(A)
+            self.sparse_jacobian = True
+        elif sps.issparse(A):
+            self.J = A.toarray()
+            self.sparse_jacobian = False
+        else:
+            # np.asarray makes sure A is ndarray and not matrix
+            self.J = np.atleast_2d(np.asarray(A))
+            self.sparse_jacobian = False
+
+        self.m, self.n = self.J.shape
+
+        self.xp = xp = array_namespace(x0)
+        _x = atleast_nd(x0, ndim=1, xp=xp)
+        _dtype = xp.float64
+        if xp.isdtype(_x.dtype, "real floating"):
+            _dtype = _x.dtype
+
+        # promotes to floating
+        self.x = xp.astype(_x, _dtype)
+        self.x_dtype = _dtype
+
+        self.f = self.J.dot(self.x)
+        self.f_updated = True
+
+        self.v = np.zeros(self.m, dtype=float)
+        self.H = sps.csr_matrix((self.n, self.n))
+
+    def _update_x(self, x):
+        if not np.array_equal(x, self.x):
+            _x = atleast_nd(x, ndim=1, xp=self.xp)
+            self.x = self.xp.astype(_x, self.x_dtype)
+            self.f_updated = False
+
+    def fun(self, x):
+        self._update_x(x)
+        if not self.f_updated:
+            self.f = self.J.dot(x)
+            self.f_updated = True
+        return self.f
+
+    def jac(self, x):
+        self._update_x(x)
+        return self.J
+
+    def hess(self, x, v):
+        self._update_x(x)
+        self.v = v
+        return self.H
+
+
+class IdentityVectorFunction(LinearVectorFunction):
+    """Identity vector function and its derivatives.
+
+    The Jacobian is the identity matrix, returned as a dense array when
+    `sparse_jacobian=False` and as a csr matrix otherwise. The Hessian is
+    identically zero and it is returned as a csr matrix.
+    """
+    def __init__(self, x0, sparse_jacobian):
+        n = len(x0)
+        if sparse_jacobian or sparse_jacobian is None:
+            A = sps.eye(n, format='csr')
+            sparse_jacobian = True
+        else:
+            A = np.eye(n)
+            sparse_jacobian = False
+        super().__init__(A, x0, sparse_jacobian)