"""
Integrate functions by rewriting them as Meijer G-functions.

There are three user-visible functions that can be used by other parts of the
sympy library to solve various integration problems:

- meijerint_indefinite
- meijerint_definite
- meijerint_inversion

They can be used to compute, respectively, indefinite integrals, definite
integrals over intervals of the real line, and inverse laplace-type integrals
(from c-I*oo to c+I*oo). See the respective docstrings for details.

The main references for this are:

[L] Luke, Y. L. (1969), The Special Functions and Their Approximations,
    Volume 1

[R] Kelly B. Roach.  Meijer G Function Representations.
    In: Proceedings of the 1997 International Symposium on Symbolic and
    Algebraic Computation, pages 205-211, New York, 1997. ACM.

[P] A. P. Prudnikov, Yu. A. Brychkov and O. I. Marichev (1990).
    Integrals and Series: More Special Functions, Vol. 3,.
    Gordon and Breach Science Publisher
"""
from __future__ import print_function, division

from sympy.core import oo, S, pi, Expr
from sympy.core.exprtools import factor_terms
from sympy.core.function import expand, expand_mul, expand_power_base
from sympy.core.add import Add
from sympy.core.mul import Mul
from sympy.core.compatibility import range
from sympy.core.cache import cacheit
from sympy.core.symbol import Dummy, Wild
from sympy.simplify import hyperexpand, powdenest, collect
from sympy.logic.boolalg import And, Or, BooleanAtom
from sympy.functions.special.delta_functions import Heaviside
from sympy.functions.elementary.exponential import exp
from sympy.functions.elementary.piecewise import Piecewise, piecewise_fold
from sympy.functions.elementary.hyperbolic import \
    _rewrite_hyperbolics_as_exp, HyperbolicFunction
from sympy.functions.special.hyper import meijerg
from sympy.utilities.iterables import multiset_partitions, ordered
from sympy.utilities.misc import debug as _debug
from sympy.utilities import default_sort_key

# keep this at top for easy reference
z = Dummy('z')


def _has(res, *f):
    # return True if res has f; in the case of Piecewise
    # only return True if *all* pieces have f
    res = piecewise_fold(res)
    if getattr(res, 'is_Piecewise', False):
        return all(_has(i, *f) for i in res.args)
    return res.has(*f)


def _create_lookup_table(table):
    """ Add formulae for the function -> meijerg lookup table. """
    def wild(n):
        return Wild(n, exclude=[z])
    p, q, a, b, c = list(map(wild, 'pqabc'))
    n = Wild('n', properties=[lambda x: x.is_Integer and x > 0])
    t = p*z**q

    def add(formula, an, ap, bm, bq, arg=t, fac=S(1), cond=True, hint=True):
        table.setdefault(_mytype(formula, z), []).append((formula,
                                     [(fac, meijerg(an, ap, bm, bq, arg))], cond, hint))

    def addi(formula, inst, cond, hint=True):
        table.setdefault(
            _mytype(formula, z), []).append((formula, inst, cond, hint))

    def constant(a):
        return [(a, meijerg([1], [], [], [0], z)),
                (a, meijerg([], [1], [0], [], z))]
    table[()] = [(a, constant(a), True, True)]

    # [P], Section 8.

    from sympy import unpolarify, Function, Not

    class IsNonPositiveInteger(Function):

        @classmethod
        def eval(cls, arg):
            arg = unpolarify(arg)
            if arg.is_Integer is True:
                return arg <= 0

    # Section 8.4.2
    from sympy import (gamma, pi, cos, exp, re, sin, sqrt, sinh, cosh,
                       factorial, log, erf, erfc, erfi, polar_lift)
    # TODO this needs more polar_lift (c/f entry for exp)
    add(Heaviside(t - b)*(t - b)**(a - 1), [a], [], [], [0], t/b,
        gamma(a)*b**(a - 1), And(b > 0))
    add(Heaviside(b - t)*(b - t)**(a - 1), [], [a], [0], [], t/b,
        gamma(a)*b**(a - 1), And(b > 0))
    add(Heaviside(z - (b/p)**(1/q))*(t - b)**(a - 1), [a], [], [], [0], t/b,
        gamma(a)*b**(a - 1), And(b > 0))
    add(Heaviside((b/p)**(1/q) - z)*(b - t)**(a - 1), [], [a], [0], [], t/b,
        gamma(a)*b**(a - 1), And(b > 0))
    add((b + t)**(-a), [1 - a], [], [0], [], t/b, b**(-a)/gamma(a),
        hint=Not(IsNonPositiveInteger(a)))
    add(abs(b - t)**(-a), [1 - a], [(1 - a)/2], [0], [(1 - a)/2], t/b,
        pi/(gamma(a)*cos(pi*a/2))*abs(b)**(-a), re(a) < 1)
    add((t**a - b**a)/(t - b), [0, a], [], [0, a], [], t/b,
        b**(a - 1)*sin(a*pi)/pi)

    # 12
    def A1(r, sign, nu):
        return pi**(-S(1)/2)*(-sign*nu/2)**(1 - 2*r)

    def tmpadd(r, sgn):
        # XXX the a**2 is bad for matching
        add((sqrt(a**2 + t) + sgn*a)**b/(a**2 + t)**r,
            [(1 + b)/2, 1 - 2*r + b/2], [],
            [(b - sgn*b)/2], [(b + sgn*b)/2], t/a**2,
            a**(b - 2*r)*A1(r, sgn, b))
    tmpadd(0, 1)
    tmpadd(0, -1)
    tmpadd(S(1)/2, 1)
    tmpadd(S(1)/2, -1)

    # 13
    def tmpadd(r, sgn):
        add((sqrt(a + p*z**q) + sgn*sqrt(p)*z**(q/2))**b/(a + p*z**q)**r,
            [1 - r + sgn*b/2], [1 - r - sgn*b/2], [0, S(1)/2], [],
            p*z**q/a, a**(b/2 - r)*A1(r, sgn, b))
    tmpadd(0, 1)
    tmpadd(0, -1)
    tmpadd(S(1)/2, 1)
    tmpadd(S(1)/2, -1)
    # (those after look obscure)

    # Section 8.4.3
    add(exp(polar_lift(-1)*t), [], [], [0], [])

    # TODO can do sin^n, sinh^n by expansion ... where?
    # 8.4.4 (hyperbolic functions)
    add(sinh(t), [], [1], [S(1)/2], [1, 0], t**2/4, pi**(S(3)/2))
    add(cosh(t), [], [S(1)/2], [0], [S(1)/2, S(1)/2], t**2/4, pi**(S(3)/2))

    # Section 8.4.5
    # TODO can do t + a. but can also do by expansion... (XXX not really)
    add(sin(t), [], [], [S(1)/2], [0], t**2/4, sqrt(pi))
    add(cos(t), [], [], [0], [S(1)/2], t**2/4, sqrt(pi))

    # Section 8.5.5
    def make_log1(subs):
        N = subs[n]
        return [((-1)**N*factorial(N),
                 meijerg([], [1]*(N + 1), [0]*(N + 1), [], t))]

    def make_log2(subs):
        N = subs[n]
        return [(factorial(N),
                 meijerg([1]*(N + 1), [], [], [0]*(N + 1), t))]
    # TODO these only hold for positive p, and can be made more general
    #      but who uses log(x)*Heaviside(a-x) anyway ...
    # TODO also it would be nice to derive them recursively ...
    addi(log(t)**n*Heaviside(1 - t), make_log1, True)
    addi(log(t)**n*Heaviside(t - 1), make_log2, True)

    def make_log3(subs):
        return make_log1(subs) + make_log2(subs)
    addi(log(t)**n, make_log3, True)
    addi(log(t + a),
         constant(log(a)) + [(S(1), meijerg([1, 1], [], [1], [0], t/a))],
         True)
    addi(log(abs(t - a)), constant(log(abs(a))) +
         [(pi, meijerg([1, 1], [S(1)/2], [1], [0, S(1)/2], t/a))],
         True)
    # TODO log(x)/(x+a) and log(x)/(x-1) can also be done. should they
    #      be derivable?
    # TODO further formulae in this section seem obscure

    # Sections 8.4.9-10
    # TODO

    # Section 8.4.11
    from sympy import Ei, I, expint, Si, Ci, Shi, Chi, fresnels, fresnelc
    addi(Ei(t),
         constant(-I*pi) + [(S(-1), meijerg([], [1], [0, 0], [],
                  t*polar_lift(-1)))],
         True)

    # Section 8.4.12
    add(Si(t), [1], [], [S(1)/2], [0, 0], t**2/4, sqrt(pi)/2)
    add(Ci(t), [], [1], [0, 0], [S(1)/2], t**2/4, -sqrt(pi)/2)

    # Section 8.4.13
    add(Shi(t), [S(1)/2], [], [0], [S(-1)/2, S(-1)/2], polar_lift(-1)*t**2/4,
        t*sqrt(pi)/4)
    add(Chi(t), [], [S(1)/2, 1], [0, 0], [S(1)/2, S(1)/2], t**2/4, -
        pi**S('3/2')/2)

    # generalized exponential integral
    add(expint(a, t), [], [a], [a - 1, 0], [], t)

    # Section 8.4.14
    add(erf(t), [1], [], [S(1)/2], [0], t**2, 1/sqrt(pi))
    # TODO exp(-x)*erf(I*x) does not work
    add(erfc(t), [], [1], [0, S(1)/2], [], t**2, 1/sqrt(pi))
    # This formula for erfi(z) yields a wrong(?) minus sign
    #add(erfi(t), [1], [], [S(1)/2], [0], -t**2, I/sqrt(pi))
    add(erfi(t), [S(1)/2], [], [0], [-S(1)/2], -t**2, t/sqrt(pi))

    # Fresnel Integrals
    add(fresnels(t), [1], [], [S(3)/4], [0, S(1)/4], pi**2*t**4/16, S(1)/2)
    add(fresnelc(t), [1], [], [S(1)/4], [0, S(3)/4], pi**2*t**4/16, S(1)/2)

    ##### bessel-type functions #####
    from sympy import besselj, bessely, besseli, besselk

    # Section 8.4.19
    add(besselj(a, t), [], [], [a/2], [-a/2], t**2/4)

    # all of the following are derivable
    #add(sin(t)*besselj(a, t), [S(1)/4, S(3)/4], [], [(1+a)/2],
    #    [-a/2, a/2, (1-a)/2], t**2, 1/sqrt(2))
    #add(cos(t)*besselj(a, t), [S(1)/4, S(3)/4], [], [a/2],
    #    [-a/2, (1+a)/2, (1-a)/2], t**2, 1/sqrt(2))
    #add(besselj(a, t)**2, [S(1)/2], [], [a], [-a, 0], t**2, 1/sqrt(pi))
    #add(besselj(a, t)*besselj(b, t), [0, S(1)/2], [], [(a + b)/2],
    #    [-(a+b)/2, (a - b)/2, (b - a)/2], t**2, 1/sqrt(pi))

    # Section 8.4.20
    add(bessely(a, t), [], [-(a + 1)/2], [a/2, -a/2], [-(a + 1)/2], t**2/4)

    # TODO all of the following should be derivable
    #add(sin(t)*bessely(a, t), [S(1)/4, S(3)/4], [(1 - a - 1)/2],
    #    [(1 + a)/2, (1 - a)/2], [(1 - a - 1)/2, (1 - 1 - a)/2, (1 - 1 + a)/2],
    #    t**2, 1/sqrt(2))
    #add(cos(t)*bessely(a, t), [S(1)/4, S(3)/4], [(0 - a - 1)/2],
    #    [(0 + a)/2, (0 - a)/2], [(0 - a - 1)/2, (1 - 0 - a)/2, (1 - 0 + a)/2],
    #    t**2, 1/sqrt(2))
    #add(besselj(a, t)*bessely(b, t), [0, S(1)/2], [(a - b - 1)/2],
    #    [(a + b)/2, (a - b)/2], [(a - b - 1)/2, -(a + b)/2, (b - a)/2],
    #    t**2, 1/sqrt(pi))
    #addi(bessely(a, t)**2,
    #     [(2/sqrt(pi), meijerg([], [S(1)/2, S(1)/2 - a], [0, a, -a],
    #                           [S(1)/2 - a], t**2)),
    #      (1/sqrt(pi), meijerg([S(1)/2], [], [a], [-a, 0], t**2))],
    #     True)
    #addi(bessely(a, t)*bessely(b, t),
    #     [(2/sqrt(pi), meijerg([], [0, S(1)/2, (1 - a - b)/2],
    #                           [(a + b)/2, (a - b)/2, (b - a)/2, -(a + b)/2],
    #                           [(1 - a - b)/2], t**2)),
    #      (1/sqrt(pi), meijerg([0, S(1)/2], [], [(a + b)/2],
    #                           [-(a + b)/2, (a - b)/2, (b - a)/2], t**2))],
    #     True)

    # Section 8.4.21 ?
    # Section 8.4.22
    add(besseli(a, t), [], [(1 + a)/2], [a/2], [-a/2, (1 + a)/2], t**2/4, pi)
    # TODO many more formulas. should all be derivable

    # Section 8.4.23
    add(besselk(a, t), [], [], [a/2, -a/2], [], t**2/4, S(1)/2)
    # TODO many more formulas. should all be derivable

    # Complete elliptic integrals K(z) and E(z)
    from sympy import elliptic_k, elliptic_e
    add(elliptic_k(t), [S.Half, S.Half], [], [0], [0], -t, S.Half)
    add(elliptic_e(t), [S.Half, 3*S.Half], [], [0], [0], -t, -S.Half/2)


####################################################################
# First some helper functions.
####################################################################

from sympy.utilities.timeutils import timethis
timeit = timethis('meijerg')


def _mytype(f, x):
    """ Create a hashable entity describing the type of f. """
    if x not in f.free_symbols:
        return ()
    elif f.is_Function:
        return (type(f),)
    else:
        types = [_mytype(a, x) for a in f.args]
        res = []
        for t in types:
            res += list(t)
        res.sort()
        return tuple(res)


class _CoeffExpValueError(ValueError):
    """
    Exception raised by _get_coeff_exp, for internal use only.
    """
    pass


def _get_coeff_exp(expr, x):
    """
    When expr is known to be of the form c*x**b, with c and/or b possibly 1,
    return c, b.

    >>> from sympy.abc import x, a, b
    >>> from sympy.integrals.meijerint import _get_coeff_exp
    >>> _get_coeff_exp(a*x**b, x)
    (a, b)
    >>> _get_coeff_exp(x, x)
    (1, 1)
    >>> _get_coeff_exp(2*x, x)
    (2, 1)
    >>> _get_coeff_exp(x**3, x)
    (1, 3)
    """
    from sympy import powsimp
    (c, m) = expand_power_base(powsimp(expr)).as_coeff_mul(x)
    if not m:
        return c, S(0)
    [m] = m
    if m.is_Pow:
        if m.base != x:
            raise _CoeffExpValueError('expr not of form a*x**b')
        return c, m.exp
    elif m == x:
        return c, S(1)
    else:
        raise _CoeffExpValueError('expr not of form a*x**b: %s' % expr)


def _exponents(expr, x):
    """
    Find the exponents of ``x`` (not including zero) in ``expr``.

    >>> from sympy.integrals.meijerint import _exponents
    >>> from sympy.abc import x, y
    >>> from sympy import sin
    >>> _exponents(x, x)
    set([1])
    >>> _exponents(x**2, x)
    set([2])
    >>> _exponents(x**2 + x, x)
    set([1, 2])
    >>> _exponents(x**3*sin(x + x**y) + 1/x, x)
    set([-1, 1, 3, y])
    """
    def _exponents_(expr, x, res):
        if expr == x:
            res.update([1])
            return
        if expr.is_Pow and expr.base == x:
            res.update([expr.exp])
            return
        for arg in expr.args:
            _exponents_(arg, x, res)
    res = set()
    _exponents_(expr, x, res)
    return res


def _functions(expr, x):
    """ Find the types of functions in expr, to estimate the complexity. """
    from sympy import Function
    return set(e.func for e in expr.atoms(Function) if x in e.free_symbols)


def _find_splitting_points(expr, x):
    """
    Find numbers a such that a linear substitution x -> x + a would
    (hopefully) simplify expr.

    >>> from sympy.integrals.meijerint import _find_splitting_points as fsp
    >>> from sympy import sin
    >>> from sympy.abc import a, x
    >>> fsp(x, x)
    set([0])
    >>> fsp((x-1)**3, x)
    set([1])
    >>> fsp(sin(x+3)*x, x)
    set([-3, 0])
    """
    p, q = [Wild(n, exclude=[x]) for n in 'pq']

    def compute_innermost(expr, res):
        if not isinstance(expr, Expr):
            return
        m = expr.match(p*x + q)
        if m and m[p] != 0:
            res.add(-m[q]/m[p])
            return
        if expr.is_Atom:
            return
        for arg in expr.args:
            compute_innermost(arg, res)
    innermost = set()
    compute_innermost(expr, innermost)
    return innermost


def _split_mul(f, x):
    """
    Split expression ``f`` into fac, po, g, where fac is a constant factor,
    po = x**s for some s independent of s, and g is "the rest".

    >>> from sympy.integrals.meijerint import _split_mul
    >>> from sympy import sin
    >>> from sympy.abc import s, x
    >>> _split_mul((3*x)**s*sin(x**2)*x, x)
    (3**s, x*x**s, sin(x**2))
    """
    from sympy import polarify, unpolarify
    fac = S(1)
    po = S(1)
    g = S(1)
    f = expand_power_base(f)

    args = Mul.make_args(f)
    for a in args:
        if a == x:
            po *= x
        elif x not in a.free_symbols:
            fac *= a
        else:
            if a.is_Pow and x not in a.exp.free_symbols:
                c, t = a.base.as_coeff_mul(x)
                if t != (x,):
                    c, t = expand_mul(a.base).as_coeff_mul(x)
                if t == (x,):
                    po *= x**a.exp
                    fac *= unpolarify(polarify(c**a.exp, subs=False))
                    continue
            g *= a

    return fac, po, g


def _mul_args(f):
    """
    Return a list ``L`` such that Mul(*L) == f.

    If f is not a Mul or Pow, L=[f].
    If f=g**n for an integer n, L=[g]*n.
    If f is a Mul, L comes from applying _mul_args to all factors of f.
    """
    args = Mul.make_args(f)
    gs = []
    for g in args:
        if g.is_Pow and g.exp.is_Integer:
            n = g.exp
            base = g.base
            if n < 0:
                n = -n
                base = 1/base
            gs += [base]*n
        else:
            gs.append(g)
    return gs


def _mul_as_two_parts(f):
    """
    Find all the ways to split f into a product of two terms.
    Return None on failure.

    Although the order is canonical from multiset_partitions, this is
    not necessarily the best order to process the terms. For example,
    if the case of len(gs) == 2 is removed and multiset is allowed to
    sort the terms, some tests fail.

    >>> from sympy.integrals.meijerint import _mul_as_two_parts
    >>> from sympy import sin, exp, ordered
    >>> from sympy.abc import x
    >>> list(ordered(_mul_as_two_parts(x*sin(x)*exp(x))))
    [(x, exp(x)*sin(x)), (x*exp(x), sin(x)), (x*sin(x), exp(x))]
    """

    gs = _mul_args(f)
    if len(gs) < 2:
        return None
    if len(gs) == 2:
        return [tuple(gs)]
    return [(Mul(*x), Mul(*y)) for (x, y) in multiset_partitions(gs, 2)]


def _inflate_g(g, n):
    """ Return C, h such that h is a G function of argument z**n and
        g = C*h. """
    # TODO should this be a method of meijerg?
    # See: [L, page 150, equation (5)]
    def inflate(params, n):
        """ (a1, .., ak) -> (a1/n, (a1+1)/n, ..., (ak + n-1)/n) """
        res = []
        for a in params:
            for i in range(n):
                res.append((a + i)/n)
        return res
    v = S(len(g.ap) - len(g.bq))
    C = n**(1 + g.nu + v/2)
    C /= (2*pi)**((n - 1)*g.delta)
    return C, meijerg(inflate(g.an, n), inflate(g.aother, n),
                      inflate(g.bm, n), inflate(g.bother, n),
                      g.argument**n * n**(n*v))


def _flip_g(g):
    """ Turn the G function into one of inverse argument
        (i.e. G(1/x) -> G'(x)) """
    # See [L], section 5.2
    def tr(l):
        return [1 - a for a in l]
    return meijerg(tr(g.bm), tr(g.bother), tr(g.an), tr(g.aother), 1/g.argument)


def _inflate_fox_h(g, a):
    r"""
    Let d denote the integrand in the definition of the G function ``g``.
    Consider the function H which is defined in the same way, but with
    integrand d/Gamma(a*s) (contour conventions as usual).

    If a is rational, the function H can be written as C*G, for a constant C
    and a G-function G.

    This function returns C, G.
    """
    if a < 0:
        return _inflate_fox_h(_flip_g(g), -a)
    p = S(a.p)
    q = S(a.q)
    # We use the substitution s->qs, i.e. inflate g by q. We are left with an
    # extra factor of Gamma(p*s), for which we use Gauss' multiplication
    # theorem.
    D, g = _inflate_g(g, q)
    z = g.argument
    D /= (2*pi)**((1 - p)/2)*p**(-S(1)/2)
    z /= p**p
    bs = [(n + 1)/p for n in range(p)]
    return D, meijerg(g.an, g.aother, g.bm, list(g.bother) + bs, z)

_dummies = {}


def _dummy(name, token, expr, **kwargs):
    """
    Return a dummy. This will return the same dummy if the same token+name is
    requested more than once, and it is not already in expr.
    This is for being cache-friendly.
    """
    d = _dummy_(name, token, **kwargs)
    if d in expr.free_symbols:
        return Dummy(name, **kwargs)
    return d


def _dummy_(name, token, **kwargs):
    """
    Return a dummy associated to name and token. Same effect as declaring
    it globally.
    """
    global _dummies
    if not (name, token) in _dummies:
        _dummies[(name, token)] = Dummy(name, **kwargs)
    return _dummies[(name, token)]


def _is_analytic(f, x):
    """ Check if f(x), when expressed using G functions on the positive reals,
        will in fact agree with the G functions almost everywhere """
    from sympy import Heaviside, Abs
    return not any(x in expr.free_symbols for expr in f.atoms(Heaviside, Abs))


def _condsimp(cond):
    """
    Do naive simplifications on ``cond``.

    Note that this routine is completely ad-hoc, simplification rules being
    added as need arises rather than following any logical pattern.

    >>> from sympy.integrals.meijerint import _condsimp as simp
    >>> from sympy import Or, Eq, unbranched_argument as arg, And
    >>> from sympy.abc import x, y, z
    >>> simp(Or(x < y, z, Eq(x, y)))
    Or(x <= y, z)
    >>> simp(Or(x <= y, And(x < y, z)))
    x <= y
    """
    from sympy import (
        symbols, Wild, Eq, unbranched_argument, exp_polar, pi, I,
        periodic_argument, oo, polar_lift)
    from sympy.logic.boolalg import BooleanFunction
    if not isinstance(cond, BooleanFunction):
        return cond
    cond = cond.func(*list(map(_condsimp, cond.args)))
    change = True
    p, q, r = symbols('p q r', cls=Wild)
    rules = [
        (Or(p < q, Eq(p, q)), p <= q),
        # The next two obviously are instances of a general pattern, but it is
        # easier to spell out the few cases we care about.
        (And(abs(unbranched_argument(p)) <= pi,
           abs(unbranched_argument(exp_polar(-2*pi*I)*p)) <= pi),
       Eq(unbranched_argument(exp_polar(-I*pi)*p), 0)),
        (And(abs(unbranched_argument(p)) <= pi/2,
           abs(unbranched_argument(exp_polar(-pi*I)*p)) <= pi/2),
       Eq(unbranched_argument(exp_polar(-I*pi/2)*p), 0)),
        (Or(p <= q, And(p < q, r)), p <= q)
    ]
    while change:
        change = False
        for fro, to in rules:
            if fro.func != cond.func:
                continue
            for n, arg in enumerate(cond.args):
                if r in fro.args[0].free_symbols:
                    m = arg.match(fro.args[1])
                    num = 1
                else:
                    num = 0
                    m = arg.match(fro.args[0])
                if not m:
                    continue
                otherargs = [x.subs(m) for x in fro.args[:num] + fro.args[num + 1:]]
                otherlist = [n]
                for arg2 in otherargs:
                    for k, arg3 in enumerate(cond.args):
                        if k in otherlist:
                            continue
                        if arg2 == arg3:
                            otherlist += [k]
                            break
                        if arg3.func is And and arg2.args[1] == r and \
                                arg2.func is And and arg2.args[0] in arg3.args:
                            otherlist += [k]
                            break
                        if arg3.func is And and arg2.args[0] == r and \
                                arg2.func is And and arg2.args[1] in arg3.args:
                            otherlist += [k]
                            break
                if len(otherlist) != len(otherargs) + 1:
                    continue
                newargs = [arg for (k, arg) in enumerate(cond.args)
                           if k not in otherlist] + [to.subs(m)]
                cond = cond.func(*newargs)
                change = True
                break
    # final tweak

    def repl_eq(orig):
        if orig.lhs == 0:
            expr = orig.rhs
        elif orig.rhs == 0:
            expr = orig.lhs
        else:
            return orig
        m = expr.match(unbranched_argument(polar_lift(p)**q))
        if not m:
            if expr.func is periodic_argument and not expr.args[0].is_polar \
                    and expr.args[1] == oo:
                return (expr.args[0] > 0)
            return orig
        return (m[p] > 0)
    return cond.replace(
        lambda expr: expr.is_Relational and expr.rel_op == '==',
        repl_eq)


def _eval_cond(cond):
    """ Re-evaluate the conditions. """
    if isinstance(cond, bool):
        return cond
    return _condsimp(cond.doit())

####################################################################
# Now the "backbone" functions to do actual integration.
####################################################################


def _my_principal_branch(expr, period, full_pb=False):
    """ Bring expr nearer to its principal branch by removing superfluous
        factors.
        This function does *not* guarantee to yield the principal branch,
        to avoid introducing opaque principal_branch() objects,
        unless full_pb=True. """
    from sympy import principal_branch
    res = principal_branch(expr, period)
    if not full_pb:
        res = res.replace(principal_branch, lambda x, y: x)
    return res


def _rewrite_saxena_1(fac, po, g, x):
    """
    Rewrite the integral fac*po*g dx, from zero to infinity, as
    integral fac*G, where G has argument a*x. Note po=x**s.
    Return fac, G.
    """
    _, s = _get_coeff_exp(po, x)
    a, b = _get_coeff_exp(g.argument, x)
    period = g.get_period()
    a = _my_principal_branch(a, period)

    # We substitute t = x**b.
    C = fac/(abs(b)*a**((s + 1)/b - 1))
    # Absorb a factor of (at)**((1 + s)/b - 1).

    def tr(l):
        return [a + (1 + s)/b - 1 for a in l]
    return C, meijerg(tr(g.an), tr(g.aother), tr(g.bm), tr(g.bother),
                      a*x)


def _check_antecedents_1(g, x, helper=False):
    """
    Return a condition under which the mellin transform of g exists.
    Any power of x has already been absorbed into the G function,
    so this is just int_0^\infty g dx.

    See [L, section 5.6.1]. (Note that s=1.)

    If ``helper`` is True, only check if the MT exists at infinity, i.e. if
    int_1^\infty g dx exists.
    """
    # NOTE if you update these conditions, please update the documentation as well
    from sympy import Eq, Not, ceiling, Ne, re, unbranched_argument as arg
    delta = g.delta
    eta, _ = _get_coeff_exp(g.argument, x)
    m, n, p, q = S([len(g.bm), len(g.an), len(g.ap), len(g.bq)])
    xi = m + n - p

    if p > q:
        def tr(l):
            return [1 - x for x in l]
        return _check_antecedents_1(meijerg(tr(g.bm), tr(g.bother),
                                            tr(g.an), tr(g.aother), x/eta),
                                    x)

    tmp = []
    for b in g.bm:
        tmp += [-re(b) < 1]
    for a in g.an:
        tmp += [1 < 1 - re(a)]
    cond_3 = And(*tmp)

    for b in g.bother:
        tmp += [-re(b) < 1]
    for a in g.aother:
        tmp += [1 < 1 - re(a)]
    cond_3_star = And(*tmp)

    cond_4 = (-re(g.nu) + (q + 1 - p)/2 > q - p)

    def debug(*msg):
        _debug(*msg)

    debug('Checking antecedents for 1 function:')
    debug('  delta=%s, eta=%s, m=%s, n=%s, p=%s, q=%s'
          % (delta, eta, m, n, p, q))
    debug('  ap = %s, %s' % (list(g.an), list(g.aother)))
    debug('  bq = %s, %s' % (list(g.bm), list(g.bother)))
    debug('  cond_3=%s, cond_3*=%s, cond_4=%s' % (cond_3, cond_3_star, cond_4))

    conds = []

    # case 1
    case1 = []
    tmp1 = [1 <= n, p < q, 1 <= m]
    tmp2 = [1 <= p, 1 <= m, Eq(q, p + 1), Not(And(Eq(n, 0), Eq(m, p + 1)))]
    tmp3 = [1 <= p, Eq(q, p)]
    for k in range(ceiling(delta/2) + 1):
        tmp3 += [Ne(abs(arg(eta)), (delta - 2*k)*pi)]
    tmp = [delta > 0, abs(arg(eta)) < delta*pi]
    extra = [Ne(eta, 0), cond_3]
    if helper:
        extra = []
    for t in [tmp1, tmp2, tmp3]:
        case1 += [And(*(t + tmp + extra))]
    conds += case1
    debug('  case 1:', case1)

    # case 2
    extra = [cond_3]
    if helper:
        extra = []
    case2 = [And(Eq(n, 0), p + 1 <= m, m <= q,
                 abs(arg(eta)) < delta*pi, *extra)]
    conds += case2
    debug('  case 2:', case2)

    # case 3
    extra = [cond_3, cond_4]
    if helper:
        extra = []
    case3 = [And(p < q, 1 <= m, delta > 0, Eq(abs(arg(eta)), delta*pi),
                 *extra)]
    case3 += [And(p <= q - 2, Eq(delta, 0), Eq(abs(arg(eta)), 0), *extra)]
    conds += case3
    debug('  case 3:', case3)

    # TODO altered cases 4-7

    # extra case from wofram functions site:
    # (reproduced verbatim from Prudnikov, section 2.24.2)
    # http://functions.wolfram.com/HypergeometricFunctions/MeijerG/21/02/01/
    case_extra = []
    case_extra += [Eq(p, q), Eq(delta, 0), Eq(arg(eta), 0), Ne(eta, 0)]
    if not helper:
        case_extra += [cond_3]
    s = []
    for a, b in zip(g.ap, g.bq):
        s += [b - a]
    case_extra += [re(Add(*s)) < 0]
    case_extra = And(*case_extra)
    conds += [case_extra]
    debug('  extra case:', [case_extra])

    case_extra_2 = [And(delta > 0, abs(arg(eta)) < delta*pi)]
    if not helper:
        case_extra_2 += [cond_3]
    case_extra_2 = And(*case_extra_2)
    conds += [case_extra_2]
    debug('  second extra case:', [case_extra_2])

    # TODO This leaves only one case from the three listed by Prudnikov.
    #      Investigate if these indeed cover everything; if so, remove the rest.

    return Or(*conds)


def _int0oo_1(g, x):
    """
    Evaluate int_0^\infty g dx using G functions,
    assuming the necessary conditions are fulfilled.

    >>> from sympy.abc import a, b, c, d, x, y
    >>> from sympy import meijerg
    >>> from sympy.integrals.meijerint import _int0oo_1
    >>> _int0oo_1(meijerg([a], [b], [c], [d], x*y), x)
    gamma(-a)*gamma(c + 1)/(y*gamma(-d)*gamma(b + 1))
    """
    # See [L, section 5.6.1]. Note that s=1.
    from sympy import gamma, combsimp, unpolarify
    eta, _ = _get_coeff_exp(g.argument, x)
    res = 1/eta
    # XXX TODO we should reduce order first
    for b in g.bm:
        res *= gamma(b + 1)
    for a in g.an:
        res *= gamma(1 - a - 1)
    for b in g.bother:
        res /= gamma(1 - b - 1)
    for a in g.aother:
        res /= gamma(a + 1)
    return combsimp(unpolarify(res))


def _rewrite_saxena(fac, po, g1, g2, x, full_pb=False):
    """
    Rewrite the integral fac*po*g1*g2 from 0 to oo in terms of G functions
    with argument c*x.
    Return C, f1, f2 such that integral C f1 f2 from 0 to infinity equals
    integral fac po g1 g2 from 0 to infinity.

    >>> from sympy.integrals.meijerint import _rewrite_saxena
    >>> from sympy.abc import s, t, m
    >>> from sympy import meijerg
    >>> g1 = meijerg([], [], [0], [], s*t)
    >>> g2 = meijerg([], [], [m/2], [-m/2], t**2/4)
    >>> r = _rewrite_saxena(1, t**0, g1, g2, t)
    >>> r[0]
    s/(4*sqrt(pi))
    >>> r[1]
    meijerg(((), ()), ((-1/2, 0), ()), s**2*t/4)
    >>> r[2]
    meijerg(((), ()), ((m/2,), (-m/2,)), t/4)
    """
    from sympy.core.numbers import ilcm

    def pb(g):
        a, b = _get_coeff_exp(g.argument, x)
        per = g.get_period()
        return meijerg(g.an, g.aother, g.bm, g.bother,
                       _my_principal_branch(a, per, full_pb)*x**b)

    _, s = _get_coeff_exp(po, x)
    _, b1 = _get_coeff_exp(g1.argument, x)
    _, b2 = _get_coeff_exp(g2.argument, x)
    if (b1 < 0) == True:
        b1 = -b1
        g1 = _flip_g(g1)
    if (b2 < 0) == True:
        b2 = -b2
        g2 = _flip_g(g2)
    if not b1.is_Rational or not b2.is_Rational:
        return
    m1, n1 = b1.p, b1.q
    m2, n2 = b2.p, b2.q
    tau = ilcm(m1*n2, m2*n1)
    r1 = tau//(m1*n2)
    r2 = tau//(m2*n1)

    C1, g1 = _inflate_g(g1, r1)
    C2, g2 = _inflate_g(g2, r2)
    g1 = pb(g1)
    g2 = pb(g2)

    fac *= C1*C2
    a1, b = _get_coeff_exp(g1.argument, x)
    a2, _ = _get_coeff_exp(g2.argument, x)

    # arbitrarily tack on the x**s part to g1
    # TODO should we try both?
    exp = (s + 1)/b - 1
    fac = fac/(abs(b) * a1**exp)

    def tr(l):
        return [a + exp for a in l]
    g1 = meijerg(tr(g1.an), tr(g1.aother), tr(g1.bm), tr(g1.bother), a1*x)
    g2 = meijerg(g2.an, g2.aother, g2.bm, g2.bother, a2*x)

    return powdenest(fac, polar=True), g1, g2


def _check_antecedents(g1, g2, x):
    """ Return a condition under which the integral theorem applies. """
    from sympy import re, Eq, Ne, cos, I, exp, sin, sign, unpolarify
    from sympy import arg as arg_, unbranched_argument as arg
    #  Yes, this is madness.
    # XXX TODO this is a testing *nightmare*
    # NOTE if you update these conditions, please update the documentation as well

    # The following conditions are found in
    # [P], Section 2.24.1
    #
    # They are also reproduced (verbatim!) at
    # http://functions.wolfram.com/HypergeometricFunctions/MeijerG/21/02/03/
    #
    # Note: k=l=r=alpha=1
    sigma, _ = _get_coeff_exp(g1.argument, x)
    omega, _ = _get_coeff_exp(g2.argument, x)
    s, t, u, v = S([len(g1.bm), len(g1.an), len(g1.ap), len(g1.bq)])
    m, n, p, q = S([len(g2.bm), len(g2.an), len(g2.ap), len(g2.bq)])
    bstar = s + t - (u + v)/2
    cstar = m + n - (p + q)/2
    rho = g1.nu + (u - v)/2 + 1
    mu = g2.nu + (p - q)/2 + 1
    phi = q - p - (v - u)
    eta = 1 - (v - u) - mu - rho
    psi = (pi*(q - m - n) + abs(arg(omega)))/(q - p)
    theta = (pi*(v - s - t) + abs(arg(sigma)))/(v - u)
    lambda_c = (q - p)*abs(omega)**(1/(q - p))*cos(psi) \
        + (v - u)*abs(sigma)**(1/(v - u))*cos(theta)

    def lambda_s0(c1, c2):
        return c1*(q - p)*abs(omega)**(1/(q - p))*sin(psi) \
            + c2*(v - u)*abs(sigma)**(1/(v - u))*sin(theta)
    lambda_s = Piecewise(
        ((lambda_s0(+1, +1)*lambda_s0(-1, -1)),
         And(Eq(arg(sigma), 0), Eq(arg(omega), 0))),
        (lambda_s0(sign(arg(omega)), +1)*lambda_s0(sign(arg(omega)), -1),
         And(Eq(arg(sigma), 0), Ne(arg(omega), 0))),
        (lambda_s0(+1, sign(arg(sigma)))*lambda_s0(-1, sign(arg(sigma))),
         And(Ne(arg(sigma), 0), Eq(arg(omega), 0))),
        (lambda_s0(sign(arg(omega)), sign(arg(sigma))), True))

    _debug('Checking antecedents:')
    _debug('  sigma=%s, s=%s, t=%s, u=%s, v=%s, b*=%s, rho=%s'
           % (sigma, s, t, u, v, bstar, rho))
    _debug('  omega=%s, m=%s, n=%s, p=%s, q=%s, c*=%s, mu=%s,'
           % (omega, m, n, p, q, cstar, mu))
    _debug('  phi=%s, eta=%s, psi=%s, theta=%s' % (phi, eta, psi, theta))

    def _c1():
        for g in [g1, g2]:
            for i in g.an:
                for j in g.bm:
                    diff = i - j
                    if diff.is_integer and diff.is_positive:
                        return False
        return True
    c1 = _c1()
    c2 = And(*[re(1 + i + j) > 0 for i in g1.bm for j in g2.bm])
    c3 = And(*[re(1 + i + j) < 1 + 1 for i in g1.an for j in g2.an])
    c4 = And(*[(p - q)*re(1 + i - 1) - re(mu) > -S(3)/2 for i in g1.an])
    c5 = And(*[(p - q)*re(1 + i) - re(mu) > -S(3)/2 for i in g1.bm])
    c6 = And(*[(u - v)*re(1 + i - 1) - re(rho) > -S(3)/2 for i in g2.an])
    c7 = And(*[(u - v)*re(1 + i) - re(rho) > -S(3)/2 for i in g2.bm])
    c8 = (abs(phi) + 2*re((rho - 1)*(q - p) + (v - u)*(q - p) + (mu -
          1)*(v - u)) > 0)
    c9 = (abs(phi) - 2*re((rho - 1)*(q - p) + (v - u)*(q - p) + (mu -
          1)*(v - u)) > 0)
    c10 = (abs(arg(sigma)) < bstar*pi)
    c11 = Eq(abs(arg(sigma)), bstar*pi)
    c12 = (abs(arg(omega)) < cstar*pi)
    c13 = Eq(abs(arg(omega)), cstar*pi)

    # The following condition is *not* implemented as stated on the wolfram
    # function site. In the book of Prudnikov there is an additional part
    # (the And involving re()). However, I only have this book in russian, and
    # I don't read any russian. The following condition is what other people
    # have told me it means.
    # Worryingly, it is different from the condition implemented in REDUCE.
    # The REDUCE implementation:
    #   https://reduce-algebra.svn.sourceforge.net/svnroot/reduce-algebra/trunk/packages/defint/definta.red
    #   (search for tst14)
    # The Wolfram alpha version:
    #   http://functions.wolfram.com/HypergeometricFunctions/MeijerG/21/02/03/03/0014/
    z0 = exp(-(bstar + cstar)*pi*I)
    zos = unpolarify(z0*omega/sigma)
    zso = unpolarify(z0*sigma/omega)
    if zos == 1/zso:
        c14 = And(Eq(phi, 0), bstar + cstar <= 1,
                  Or(Ne(zos, 1), re(mu + rho + v - u) < 1,
                     re(mu + rho + q - p) < 1))
    else:
        c14 = And(Eq(phi, 0), bstar - 1 + cstar <= 0,
                  Or(And(Ne(zos, 1), abs(arg_(1 - zos)) < pi),
                     And(re(mu + rho + v - u) < 1, Eq(zos, 1))))

        c14_alt = And(Eq(phi, 0), cstar - 1 + bstar <= 0,
                  Or(And(Ne(zso, 1), abs(arg_(1 - zso)) < pi),
                     And(re(mu + rho + q - p) < 1, Eq(zso, 1))))

        # Since r=k=l=1, in our case there is c14_alt which is the same as calling
        # us with (g1, g2) = (g2, g1). The conditions below enumerate all cases
        # (i.e. we don't have to try arguments reversed by hand), and indeed try
        # all symmetric cases. (i.e. whenever there is a condition involving c14,
        # there is also a dual condition which is exactly what we would get when g1,
        # g2 were interchanged, *but c14 was unaltered*).
        # Hence the following seems correct:
        c14 = Or(c14, c14_alt)

    tmp = [lambda_c > 0,
           And(Eq(lambda_c, 0), Ne(lambda_s, 0), re(eta) > -1),
           And(Eq(lambda_c, 0), Eq(lambda_s, 0), re(eta) > 0)]
    c15 = Or(*tmp)
    if _eval_cond(lambda_c > 0) != False:
        c15 = (lambda_c > 0)

    for cond, i in [(c1, 1), (c2, 2), (c3, 3), (c4, 4), (c5, 5), (c6, 6),
                    (c7, 7), (c8, 8), (c9, 9), (c10, 10), (c11, 11),
                    (c12, 12), (c13, 13), (c14, 14), (c15, 15)]:
        _debug('  c%s:' % i, cond)

    # We will return Or(*conds)
    conds = []

    def pr(count):
        _debug('  case %s:' % count, conds[-1])
    conds += [And(m*n*s*t != 0, bstar.is_positive is True, cstar.is_positive is True, c1, c2, c3, c10,
                  c12)]  # 1
    pr(1)
    conds += [And(Eq(u, v), Eq(bstar, 0), cstar.is_positive is True, sigma.is_positive is True, re(rho) < 1,
                  c1, c2, c3, c12)]  # 2
    pr(2)
    conds += [And(Eq(p, q), Eq(cstar, 0), bstar.is_positive is True, omega.is_positive is True, re(mu) < 1,
                  c1, c2, c3, c10)]  # 3
    pr(3)
    conds += [And(Eq(p, q), Eq(u, v), Eq(bstar, 0), Eq(cstar, 0),
                  sigma.is_positive is True, omega.is_positive is True, re(mu) < 1, re(rho) < 1,
                  Ne(sigma, omega), c1, c2, c3)]  # 4
    pr(4)
    conds += [And(Eq(p, q), Eq(u, v), Eq(bstar, 0), Eq(cstar, 0),
                  sigma.is_positive is True, omega.is_positive is True, re(mu + rho) < 1,
                  Ne(omega, sigma), c1, c2, c3)]  # 5
    pr(5)
    conds += [And(p > q, s.is_positive is True, bstar.is_positive is True, cstar >= 0,
                  c1, c2, c3, c5, c10, c13)]  # 6
    pr(6)
    conds += [And(p < q, t.is_positive is True, bstar.is_positive is True, cstar >= 0,
                  c1, c2, c3, c4, c10, c13)]  # 7
    pr(7)
    conds += [And(u > v, m.is_positive is True, cstar.is_positive is True, bstar >= 0,
                  c1, c2, c3, c7, c11, c12)]  # 8
    pr(8)
    conds += [And(u < v, n.is_positive is True, cstar.is_positive is True, bstar >= 0,
                  c1, c2, c3, c6, c11, c12)]  # 9
    pr(9)
    conds += [And(p > q, Eq(u, v), Eq(bstar, 0), cstar >= 0, sigma.is_positive is True,
                  re(rho) < 1, c1, c2, c3, c5, c13)]  # 10
    pr(10)
    conds += [And(p < q, Eq(u, v), Eq(bstar, 0), cstar >= 0, sigma.is_positive is True,
                  re(rho) < 1, c1, c2, c3, c4, c13)]  # 11
    pr(11)
    conds += [And(Eq(p, q), u > v, bstar >= 0, Eq(cstar, 0), omega.is_positive is True,
                  re(mu) < 1, c1, c2, c3, c7, c11)]  # 12
    pr(12)
    conds += [And(Eq(p, q), u < v, bstar >= 0, Eq(cstar, 0), omega.is_positive is True,
                  re(mu) < 1, c1, c2, c3, c6, c11)]  # 13
    pr(13)
    conds += [And(p < q, u > v, bstar >= 0, cstar >= 0,
                  c1, c2, c3, c4, c7, c11, c13)]  # 14
    pr(14)
    conds += [And(p > q, u < v, bstar >= 0, cstar >= 0,
                  c1, c2, c3, c5, c6, c11, c13)]  # 15
    pr(15)
    conds += [And(p > q, u > v, bstar >= 0, cstar >= 0,
                  c1, c2, c3, c5, c7, c8, c11, c13, c14)]  # 16
    pr(16)
    conds += [And(p < q, u < v, bstar >= 0, cstar >= 0,
                  c1, c2, c3, c4, c6, c9, c11, c13, c14)]  # 17
    pr(17)
    conds += [And(Eq(t, 0), s.is_positive is True, bstar.is_positive is True, phi.is_positive is True, c1, c2, c10)]  # 18
    pr(18)
    conds += [And(Eq(s, 0), t.is_positive is True, bstar.is_positive is True, phi.is_negative is True, c1, c3, c10)]  # 19
    pr(19)
    conds += [And(Eq(n, 0), m.is_positive is True, cstar.is_positive is True, phi.is_negative is True, c1, c2, c12)]  # 20
    pr(20)
    conds += [And(Eq(m, 0), n.is_positive is True, cstar.is_positive is True, phi.is_positive is True, c1, c3, c12)]  # 21
    pr(21)
    conds += [And(Eq(s*t, 0), bstar.is_positive is True, cstar.is_positive is True,
                  c1, c2, c3, c10, c12)]  # 22
    pr(22)
    conds += [And(Eq(m*n, 0), bstar.is_positive is True, cstar.is_positive is True,
                  c1, c2, c3, c10, c12)]  # 23
    pr(23)

    # The following case is from [Luke1969]. As far as I can tell, it is *not*
    # covered by Prudnikov's.
    # Let G1 and G2 be the two G-functions. Suppose the integral exists from
    # 0 to a > 0 (this is easy the easy part), that G1 is exponential decay at
    # infinity, and that the mellin transform of G2 exists.
    # Then the integral exists.
    mt1_exists = _check_antecedents_1(g1, x, helper=True)
    mt2_exists = _check_antecedents_1(g2, x, helper=True)
    conds += [And(mt2_exists, Eq(t, 0), u < s, bstar.is_positive is True, c10, c1, c2, c3)]
    pr('E1')
    conds += [And(mt2_exists, Eq(s, 0), v < t, bstar.is_positive is True, c10, c1, c2, c3)]
    pr('E2')
    conds += [And(mt1_exists, Eq(n, 0), p < m, cstar.is_positive is True, c12, c1, c2, c3)]
    pr('E3')
    conds += [And(mt1_exists, Eq(m, 0), q < n, cstar.is_positive is True, c12, c1, c2, c3)]
    pr('E4')

    # Let's short-circuit if this worked ...
    # the rest is corner-cases and terrible to read.
    r = Or(*conds)
    if _eval_cond(r) != False:
        return r

    conds += [And(m + n > p, Eq(t, 0), Eq(phi, 0), s.is_positive is True, bstar.is_positive is True, cstar.is_negative is True,
                  abs(arg(omega)) < (m + n - p + 1)*pi,
                  c1, c2, c10, c14, c15)]  # 24
    pr(24)
    conds += [And(m + n > q, Eq(s, 0), Eq(phi, 0), t.is_positive is True, bstar.is_positive is True, cstar.is_negative is True,
                  abs(arg(omega)) < (m + n - q + 1)*pi,
                  c1, c3, c10, c14, c15)]  # 25
    pr(25)
    conds += [And(Eq(p, q - 1), Eq(t, 0), Eq(phi, 0), s.is_positive is True, bstar.is_positive is True,
                  cstar >= 0, cstar*pi < abs(arg(omega)),
                  c1, c2, c10, c14, c15)]  # 26
    pr(26)
    conds += [And(Eq(p, q + 1), Eq(s, 0), Eq(phi, 0), t.is_positive is True, bstar.is_positive is True,
                  cstar >= 0, cstar*pi < abs(arg(omega)),
                  c1, c3, c10, c14, c15)]  # 27
    pr(27)
    conds += [And(p < q - 1, Eq(t, 0), Eq(phi, 0), s.is_positive is True, bstar.is_positive is True,
                  cstar >= 0, cstar*pi < abs(arg(omega)),
                  abs(arg(omega)) < (m + n - p + 1)*pi,
                  c1, c2, c10, c14, c15)]  # 28
    pr(28)
    conds += [And(
        p > q + 1, Eq(s, 0), Eq(phi, 0), t.is_positive is True, bstar.is_positive is True, cstar >= 0,
                  cstar*pi < abs(arg(omega)),
                  abs(arg(omega)) < (m + n - q + 1)*pi,
                  c1, c3, c10, c14, c15)]  # 29
    pr(29)
    conds += [And(Eq(n, 0), Eq(phi, 0), s + t > 0, m.is_positive is True, cstar.is_positive is True, bstar.is_negative is True,
                  abs(arg(sigma)) < (s + t - u + 1)*pi,
                  c1, c2, c12, c14, c15)]  # 30
    pr(30)
    conds += [And(Eq(m, 0), Eq(phi, 0), s + t > v, n.is_positive is True, cstar.is_positive is True, bstar.is_negative is True,
                  abs(arg(sigma)) < (s + t - v + 1)*pi,
                  c1, c3, c12, c14, c15)]  # 31
    pr(31)
    conds += [And(Eq(n, 0), Eq(phi, 0), Eq(u, v - 1), m.is_positive is True, cstar.is_positive is True,
                  bstar >= 0, bstar*pi < abs(arg(sigma)),
                  abs(arg(sigma)) < (bstar + 1)*pi,
                  c1, c2, c12, c14, c15)]  # 32
    pr(32)
    conds += [And(Eq(m, 0), Eq(phi, 0), Eq(u, v + 1), n.is_positive is True, cstar.is_positive is True,
                  bstar >= 0, bstar*pi < abs(arg(sigma)),
                  abs(arg(sigma)) < (bstar + 1)*pi,
                  c1, c3, c12, c14, c15)]  # 33
    pr(33)
    conds += [And(
        Eq(n, 0), Eq(phi, 0), u < v - 1, m.is_positive is True, cstar.is_positive is True, bstar >= 0,
        bstar*pi < abs(arg(sigma)),
        abs(arg(sigma)) < (s + t - u + 1)*pi,
        c1, c2, c12, c14, c15)]  # 34
    pr(34)
    conds += [And(
        Eq(m, 0), Eq(phi, 0), u > v + 1, n.is_positive is True, cstar.is_positive is True, bstar >= 0,
        bstar*pi < abs(arg(sigma)),
        abs(arg(sigma)) < (s + t - v + 1)*pi,
        c1, c3, c12, c14, c15)]  # 35
    pr(35)

    return Or(*conds)

    # NOTE An alternative, but as far as I can tell weaker, set of conditions
    #      can be found in [L, section 5.6.2].


def _int0oo(g1, g2, x):
    """
    Express integral from zero to infinity g1*g2 using a G function,
    assuming the necessary conditions are fulfilled.

    >>> from sympy.integrals.meijerint import _int0oo
    >>> from sympy.abc import s, t, m
    >>> from sympy import meijerg, S
    >>> g1 = meijerg([], [], [-S(1)/2, 0], [], s**2*t/4)
    >>> g2 = meijerg([], [], [m/2], [-m/2], t/4)
    >>> _int0oo(g1, g2, t)
    4*meijerg(((1/2, 0), ()), ((m/2,), (-m/2,)), s**(-2))/s**2
    """
    # See: [L, section 5.6.2, equation (1)]
    eta, _ = _get_coeff_exp(g1.argument, x)
    omega, _ = _get_coeff_exp(g2.argument, x)

    def neg(l):
        return [-x for x in l]
    a1 = neg(g1.bm) + list(g2.an)
    a2 = list(g2.aother) + neg(g1.bother)
    b1 = neg(g1.an) + list(g2.bm)
    b2 = list(g2.bother) + neg(g1.aother)
    return meijerg(a1, a2, b1, b2, omega/eta)/eta


def _rewrite_inversion(fac, po, g, x):
    """ Absorb ``po`` == x**s into g. """
    _, s = _get_coeff_exp(po, x)
    a, b = _get_coeff_exp(g.argument, x)

    def tr(l):
        return [t + s/b for t in l]
    return (powdenest(fac/a**(s/b), polar=True),
            meijerg(tr(g.an), tr(g.aother), tr(g.bm), tr(g.bother), g.argument))


def _check_antecedents_inversion(g, x):
    """ Check antecedents for the laplace inversion integral. """
    from sympy import re, im, Or, And, Eq, exp, I, Add, nan, Ne
    _debug('Checking antecedents for inversion:')
    z = g.argument
    _, e = _get_coeff_exp(z, x)
    if e < 0:
        _debug('  Flipping G.')
        # We want to assume that argument gets large as |x| -> oo
        return _check_antecedents_inversion(_flip_g(g), x)

    def statement_half(a, b, c, z, plus):
        coeff, exponent = _get_coeff_exp(z, x)
        a *= exponent
        b *= coeff**c
        c *= exponent
        conds = []
        wp = b*exp(I*re(c)*pi/2)
        wm = b*exp(-I*re(c)*pi/2)
        if plus:
            w = wp
        else:
            w = wm
        conds += [And(Or(Eq(b, 0), re(c) <= 0), re(a) <= -1)]
        conds += [And(Ne(b, 0), Eq(im(c), 0), re(c) > 0, re(w) < 0)]
        conds += [And(Ne(b, 0), Eq(im(c), 0), re(c) > 0, re(w) <= 0,
                      re(a) <= -1)]
        return Or(*conds)

    def statement(a, b, c, z):
        """ Provide a convergence statement for z**a * exp(b*z**c),
             c/f sphinx docs. """
        return And(statement_half(a, b, c, z, True),
                   statement_half(a, b, c, z, False))

    # Notations from [L], section 5.7-10
    m, n, p, q = S([len(g.bm), len(g.an), len(g.ap), len(g.bq)])
    tau = m + n - p
    nu = q - m - n
    rho = (tau - nu)/2
    sigma = q - p
    if sigma == 1:
        epsilon = S(1)/2
    elif sigma > 1:
        epsilon = 1
    else:
        epsilon = nan
    theta = ((1 - sigma)/2 + Add(*g.bq) - Add(*g.ap))/sigma
    delta = g.delta
    _debug('  m=%s, n=%s, p=%s, q=%s, tau=%s, nu=%s, rho=%s, sigma=%s' % (
        m, n, p, q, tau, nu, rho, sigma))
    _debug('  epsilon=%s, theta=%s, delta=%s' % (epsilon, theta, delta))

    # First check if the computation is valid.
    if not (g.delta >= e/2 or (p >= 1 and p >= q)):
        _debug('  Computation not valid for these parameters.')
        return False

    # Now check if the inversion integral exists.

    # Test "condition A"
    for a in g.an:
        for b in g.bm:
            if (a - b).is_integer and a > b:
                _debug('  Not a valid G function.')
                return False

    # There are two cases. If p >= q, we can directly use a slater expansion
    # like [L], 5.2 (11). Note in particular that the asymptotics of such an
    # expansion even hold when some of the parameters differ by integers, i.e.
    # the formula itself would not be valid! (b/c G functions are cts. in their
    # parameters)
    # When p < q, we need to use the theorems of [L], 5.10.

    if p >= q:
        _debug('  Using asymptotic Slater expansion.')
        return And(*[statement(a - 1, 0, 0, z) for a in g.an])

    def E(z):
        return And(*[statement(a - 1, 0, z) for a in g.an])

    def H(z):
        return statement(theta, -sigma, 1/sigma, z)

    def Hp(z):
        return statement_half(theta, -sigma, 1/sigma, z, True)

    def Hm(z):
        return statement_half(theta, -sigma, 1/sigma, z, False)

    # [L], section 5.10
    conds = []
    # Theorem 1
    conds += [And(1 <= n, p < q, 1 <= m, rho*pi - delta >= pi/2, delta > 0,
                  E(z*exp(I*pi*(nu + 1))))]
    # Theorem 2, statements (2) and (3)
    conds += [And(p + 1 <= m, m + 1 <= q, delta > 0, delta < pi/2, n == 0,
                  (m - p + 1)*pi - delta >= pi/2,
                  Hp(z*exp(I*pi*(q - m))), Hm(z*exp(-I*pi*(q - m))))]
    # Theorem 2, statement (5)
    conds += [And(p < q, m == q, n == 0, delta > 0,
                  (sigma + epsilon)*pi - delta >= pi/2, H(z))]
    # Theorem 3, statements (6) and (7)
    conds += [And(Or(And(p <= q - 2, 1 <= tau, tau <= sigma/2),
                     And(p + 1 <= m + n, m + n <= (p + q)/2)),
                  delta > 0, delta < pi/2, (tau + 1)*pi - delta >= pi/2,
                  Hp(z*exp(I*pi*nu)), Hm(z*exp(-I*pi*nu)))]
    # Theorem 4, statements (10) and (11)
    conds += [And(p < q, 1 <= m, rho > 0, delta > 0, delta + rho*pi < pi/2,
                  (tau + epsilon)*pi - delta >= pi/2,
                  Hp(z*exp(I*pi*nu)), Hm(z*exp(-I*pi*nu)))]
    # Trivial case
    conds += [m == 0]

    # TODO
    # Theorem 5 is quite general
    # Theorem 6 contains special cases for q=p+1

    return Or(*conds)


def _int_inversion(g, x, t):
    """
    Compute the laplace inversion integral, assuming the formula applies.
    """
    b, a = _get_coeff_exp(g.argument, x)
    C, g = _inflate_fox_h(meijerg(g.an, g.aother, g.bm, g.bother, b/t**a), -a)
    return C/t*g


####################################################################
# Finally, the real meat.
####################################################################

_lookup_table = None


@cacheit
@timeit
def _rewrite_single(f, x, recursive=True):
    """
    Try to rewrite f as a sum of single G functions of the form
    C*x**s*G(a*x**b), where b is a rational number and C is independent of x.
    We guarantee that result.argument.as_coeff_mul(x) returns (a, (x**b,))
    or (a, ()).
    Returns a list of tuples (C, s, G) and a condition cond.
    Returns None on failure.
    """
    from sympy import polarify, unpolarify, oo, zoo, Tuple
    global _lookup_table
    if not _lookup_table:
        _lookup_table = {}
        _create_lookup_table(_lookup_table)

    if isinstance(f, meijerg):
        from sympy import factor
        coeff, m = factor(f.argument, x).as_coeff_mul(x)
        if len(m) > 1:
            return None
        m = m[0]
        if m.is_Pow:
            if m.base != x or not m.exp.is_Rational:
                return None
        elif m != x:
            return None
        return [(1, 0, meijerg(f.an, f.aother, f.bm, f.bother, coeff*m))], True

    f_ = f
    f = f.subs(x, z)
    t = _mytype(f, z)
    if t in _lookup_table:
        l = _lookup_table[t]
        for formula, terms, cond, hint in l:
            subs = f.match(formula, old=True)
            if subs:
                subs_ = {}
                for fro, to in subs.items():
                    subs_[fro] = unpolarify(polarify(to, lift=True),
                                            exponents_only=True)
                subs = subs_
                if not isinstance(hint, bool):
                    hint = hint.subs(subs)
                if hint == False:
                    continue
                if not isinstance(cond, (bool, BooleanAtom)):
                    cond = unpolarify(cond.subs(subs))
                if _eval_cond(cond) == False:
                    continue
                if not isinstance(terms, list):
                    terms = terms(subs)
                res = []
                for fac, g in terms:
                    r1 = _get_coeff_exp(unpolarify(fac.subs(subs).subs(z, x),
                                                   exponents_only=True), x)
                    g = g.subs(subs).subs(z, x)
                    # NOTE these substitutions can in principle introduce oo,
                    #      zoo and other absurdities. It shouldn't matter,
                    #      but better be safe.
                    if Tuple(*(r1 + (g,))).has(oo, zoo, -oo):
                        continue
                    g = meijerg(g.an, g.aother, g.bm, g.bother,
                                unpolarify(g.argument, exponents_only=True))
                    res.append(r1 + (g,))
                if res:
                    return res, cond

    # try recursive mellin transform
    if not recursive:
        return None
    _debug('Trying recursive Mellin transform method.')
    from sympy.integrals.transforms import (mellin_transform,
                                    inverse_mellin_transform, IntegralTransformError,
                                    MellinTransformStripError)
    from sympy import oo, nan, zoo, simplify, cancel

    def my_imt(F, s, x, strip):
        """ Calling simplify() all the time is slow and not helpful, since
            most of the time it only factors things in a way that has to be
            un-done anyway. But sometimes it can remove apparent poles. """
        # XXX should this be in inverse_mellin_transform?
        try:
            return inverse_mellin_transform(F, s, x, strip,
                                            as_meijerg=True, needeval=True)
        except MellinTransformStripError:
            return inverse_mellin_transform(
                simplify(cancel(expand(F))), s, x, strip,
                as_meijerg=True, needeval=True)
    f = f_
    s = _dummy('s', 'rewrite-single', f)
    # to avoid infinite recursion, we have to force the two g functions case

    def my_integrator(f, x):
        from sympy import Integral, hyperexpand
        r = _meijerint_definite_4(f, x, only_double=True)
        if r is not None:
            res, cond = r
            res = _my_unpolarify(hyperexpand(res, rewrite='nonrepsmall'))
            return Piecewise((res, cond),
                             (Integral(f, (x, 0, oo)), True))
        return Integral(f, (x, 0, oo))
    try:
        F, strip, _ = mellin_transform(f, x, s, integrator=my_integrator,
                                       simplify=False, needeval=True)
        g = my_imt(F, s, x, strip)
    except IntegralTransformError:
        g = None
    if g is None:
        # We try to find an expression by analytic continuation.
        # (also if the dummy is already in the expression, there is no point in
        #  putting in another one)
        a = _dummy_('a', 'rewrite-single')
        if a not in f.free_symbols and _is_analytic(f, x):
            try:
                F, strip, _ = mellin_transform(f.subs(x, a*x), x, s,
                                               integrator=my_integrator,
                                               needeval=True, simplify=False)
                g = my_imt(F, s, x, strip).subs(a, 1)
            except IntegralTransformError:
                g = None
    if g is None or g.has(oo, nan, zoo):
        _debug('Recursive Mellin transform failed.')
        return None
    args = Add.make_args(g)
    res = []
    for f in args:
        c, m = f.as_coeff_mul(x)
        if len(m) > 1:
            raise NotImplementedError('Unexpected form...')
        g = m[0]
        a, b = _get_coeff_exp(g.argument, x)
        res += [(c, 0, meijerg(g.an, g.aother, g.bm, g.bother,
                               unpolarify(polarify(
                                   a, lift=True), exponents_only=True)
                               *x**b))]
    _debug('Recursive Mellin transform worked:', g)
    return res, True


def _rewrite1(f, x, recursive=True):
    """
    Try to rewrite f using a (sum of) single G functions with argument a*x**b.
    Return fac, po, g such that f = fac*po*g, fac is independent of x
    and po = x**s.
    Here g is a result from _rewrite_single.
    Return None on failure.
    """
    fac, po, g = _split_mul(f, x)
    g = _rewrite_single(g, x, recursive)
    if g:
        return fac, po, g[0], g[1]


def _rewrite2(f, x):
    """
    Try to rewrite f as a product of two G functions of arguments a*x**b.
    Return fac, po, g1, g2 such that f = fac*po*g1*g2, where fac is
    independent of x and po is x**s.
    Here g1 and g2 are results of _rewrite_single.
    Returns None on failure.
    """
    fac, po, g = _split_mul(f, x)
    if any(_rewrite_single(expr, x, False) is None for expr in _mul_args(g)):
        return None
    l = _mul_as_two_parts(g)
    if not l:
        return None
    l = list(ordered(l, [
        lambda p: max(len(_exponents(p[0], x)), len(_exponents(p[1], x))),
        lambda p: max(len(_functions(p[0], x)), len(_functions(p[1], x))),
        lambda p: max(len(_find_splitting_points(p[0], x)),
                      len(_find_splitting_points(p[1], x)))]))

    for recursive in [False, True]:
        for fac1, fac2 in l:
            g1 = _rewrite_single(fac1, x, recursive)
            g2 = _rewrite_single(fac2, x, recursive)
            if g1 and g2:
                cond = And(g1[1], g2[1])
                if cond != False:
                    return fac, po, g1[0], g2[0], cond


def meijerint_indefinite(f, x):
    """
    Compute an indefinite integral of ``f`` by rewriting it as a G function.

    Examples
    ========

    >>> from sympy.integrals.meijerint import meijerint_indefinite
    >>> from sympy import sin
    >>> from sympy.abc import x
    >>> meijerint_indefinite(sin(x), x)
    -cos(x)
    """
    from sympy import hyper, meijerg

    results = []
    for a in sorted(_find_splitting_points(f, x) | set([S(0)]), key=default_sort_key):
        res = _meijerint_indefinite_1(f.subs(x, x + a), x)
        if not res:
            continue
        res = res.subs(x, x - a)
        if _has(res, hyper, meijerg):
            results.append(res)
        else:
            return res
    if f.has(HyperbolicFunction):
        _debug('Try rewriting hyperbolics in terms of exp.')
        rv = meijerint_indefinite(
            _rewrite_hyperbolics_as_exp(f), x)
        if rv:
            if not type(rv) is list:
                return collect(factor_terms(rv), rv.atoms(exp))
            results.extend(rv)
    if results:
        return next(ordered(results))


def _meijerint_indefinite_1(f, x):
    """ Helper that does not attempt any substitution. """
    from sympy import Integral, piecewise_fold
    _debug('Trying to compute the indefinite integral of', f, 'wrt', x)

    gs = _rewrite1(f, x)
    if gs is None:
        # Note: the code that calls us will do expand() and try again
        return None

    fac, po, gl, cond = gs
    _debug(' could rewrite:', gs)
    res = S(0)
    for C, s, g in gl:
        a, b = _get_coeff_exp(g.argument, x)
        _, c = _get_coeff_exp(po, x)
        c += s

        # we do a substitution t=a*x**b, get integrand fac*t**rho*g
        fac_ = fac * C / (b*a**((1 + c)/b))
        rho = (c + 1)/b - 1

        # we now use t**rho*G(params, t) = G(params + rho, t)
        # [L, page 150, equation (4)]
        # and integral G(params, t) dt = G(1, params+1, 0, t)
        #   (or a similar expression with 1 and 0 exchanged ... pick the one
        #    which yields a well-defined function)
        # [R, section 5]
        # (Note that this dummy will immediately go away again, so we
        #  can safely pass S(1) for ``expr``.)
        t = _dummy('t', 'meijerint-indefinite', S(1))

        def tr(p):
            return [a + rho + 1 for a in p]
        if any(b.is_integer and (b <= 0) == True for b in tr(g.bm)):
            r = -meijerg(
                tr(g.an), tr(g.aother) + [1], tr(g.bm) + [0], tr(g.bother), t)
        else:
            r = meijerg(
                tr(g.an) + [1], tr(g.aother), tr(g.bm), tr(g.bother) + [0], t)
        r = hyperexpand(r.subs(t, a*x**b))

        # now substitute back
        # Note: we really do want the powers of x to combine.
        res += powdenest(fac_*r, polar=True)

    def _clean(res):
        """This multiplies out superfluous powers of x we created, and chops off
        constants:

            >> _clean(x*(exp(x)/x - 1/x) + 3)
            exp(x)

        cancel is used before mul_expand since it is possible for an
        expression to have an additive constant that doesn't become isolated
        with simple expansion. Such a situation was identified in issue 6369:


        >>> from sympy import sqrt, cancel
        >>> from sympy.abc import x
        >>> a = sqrt(2*x + 1)
        >>> bad = (3*x*a**5 + 2*x - a**5 + 1)/a**2
        >>> bad.expand().as_independent(x)[0]
        0
        >>> cancel(bad).expand().as_independent(x)[0]
        1
        """
        from sympy import cancel
        res = expand_mul(cancel(res), deep=False)
        return Add._from_args(res.as_coeff_add(x)[1])

    res = piecewise_fold(res)
    if res.is_Piecewise:
        newargs = []
        for expr, cond in res.args:
            expr = _my_unpolarify(_clean(expr))
            newargs += [(expr, cond)]
        res = Piecewise(*newargs)
    else:
        res = _my_unpolarify(_clean(res))
    return Piecewise((res, _my_unpolarify(cond)), (Integral(f, x), True))


@timeit
def meijerint_definite(f, x, a, b):
    """
    Integrate ``f`` over the interval [``a``, ``b``], by rewriting it as a product
    of two G functions, or as a single G function.

    Return res, cond, where cond are convergence conditions.

    Examples
    ========

    >>> from sympy.integrals.meijerint import meijerint_definite
    >>> from sympy import exp, oo
    >>> from sympy.abc import x
    >>> meijerint_definite(exp(-x**2), x, -oo, oo)
    (sqrt(pi), True)

    This function is implemented as a succession of functions
    meijerint_definite, _meijerint_definite_2, _meijerint_definite_3,
    _meijerint_definite_4. Each function in the list calls the next one
    (presumably) several times. This means that calling meijerint_definite
    can be very costly.
    """
    # This consists of three steps:
    # 1) Change the integration limits to 0, oo
    # 2) Rewrite in terms of G functions
    # 3) Evaluate the integral
    #
    # There are usually several ways of doing this, and we want to try all.
    # This function does (1), calls _meijerint_definite_2 for step (2).
    from sympy import arg, exp, I, And, DiracDelta, count_ops
    _debug('Integrating', f, 'wrt %s from %s to %s.' % (x, a, b))

    if f.has(DiracDelta):
        _debug('Integrand has DiracDelta terms - giving up.')
        return None

    f_, x_, a_, b_ = f, x, a, b

    # Let's use a dummy in case any of the boundaries has x.
    d = Dummy('x')
    f = f.subs(x, d)
    x = d

    if a == b:
        return (S.Zero, True)

    results = []
    if a == -oo and b != oo:
        return meijerint_definite(f.subs(x, -x), x, -b, -a)

    elif a == -oo:
        # Integrating -oo to oo. We need to find a place to split the integral.
        _debug('  Integrating -oo to +oo.')
        innermost = _find_splitting_points(f, x)
        _debug('  Sensible splitting points:', innermost)
        for c in sorted(innermost, key=default_sort_key, reverse=True) + [S(0)]:
            _debug('  Trying to split at', c)
            if not c.is_real:
                _debug('  Non-real splitting point.')
                continue
            res1 = _meijerint_definite_2(f.subs(x, x + c), x)
            if res1 is None:
                _debug('  But could not compute first integral.')
                continue
            res2 = _meijerint_definite_2(f.subs(x, c - x), x)
            if res2 is None:
                _debug('  But could not compute second integral.')
                continue
            res1, cond1 = res1
            res2, cond2 = res2
            cond = _condsimp(And(cond1, cond2))
            if cond == False:
                _debug('  But combined condition is always false.')
                continue
            res = res1 + res2
            return res, cond

    elif a == oo:
        return -meijerint_definite(f, x, b, oo)

    elif (a, b) == (0, oo):
        # This is a common case - try it directly first.
        res = _meijerint_definite_2(f, x)
        if res:
            if _has(res[0], meijerg):
                results.append(res)
            else:
                return res

    else:
        if b == oo:
            for split in _find_splitting_points(f, x):
                if (a - split >= 0) == True:
                    _debug('Trying x -> x + %s' % split)
                    res = _meijerint_definite_2(f.subs(x, x + split)
                                                *Heaviside(x + split - a), x)
                    if res:
                        if _has(res[0], meijerg):
                            results.append(res)
                        else:
                            return res

        f = f.subs(x, x + a)
        b = b - a
        a = 0
        if b != oo:
            phi = exp(I*arg(b))
            b = abs(b)
            f = f.subs(x, phi*x)
            f *= Heaviside(b - x)*phi
            b = oo

        _debug('Changed limits to', a, b)
        _debug('Changed function to', f)
        res = _meijerint_definite_2(f, x)
        if res:
            if _has(res[0], meijerg):
                results.append(res)
            else:
                return res
    if f_.has(HyperbolicFunction):
        _debug('Try rewriting hyperbolics in terms of exp.')
        rv = meijerint_definite(
            _rewrite_hyperbolics_as_exp(f_), x_, a_, b_)
        if rv:
            if not type(rv) is list:
                rv = (collect(factor_terms(rv[0]), rv[0].atoms(exp)),) + rv[1:]
                return rv
            results.extend(rv)
    if results:
        return next(ordered(results))


def _guess_expansion(f, x):
    """ Try to guess sensible rewritings for integrand f(x). """
    from sympy import expand_trig
    from sympy.functions.elementary.trigonometric import TrigonometricFunction
    res = [(f, 'original integrand')]

    orig = res[-1][0]
    saw = set([orig])
    expanded = expand_mul(orig)
    if expanded not in saw:
        res += [(expanded, 'expand_mul')]
        saw.add(expanded)

    expanded = expand(orig)
    if expanded not in saw:
        res += [(expanded, 'expand')]
        saw.add(expanded)

    if orig.has(TrigonometricFunction, HyperbolicFunction):
        expanded = expand_mul(expand_trig(orig))
        if expanded not in saw:
            res += [(expanded, 'expand_trig, expand_mul')]
            saw.add(expanded)

    return res


def _meijerint_definite_2(f, x):
    """
    Try to integrate f dx from zero to infinty.

    The body of this function computes various 'simplifications'
    f1, f2, ... of f (e.g. by calling expand_mul(), trigexpand()
    - see _guess_expansion) and calls _meijerint_definite_3 with each of
    these in succession.
    If _meijerint_definite_3 succeedes with any of the simplified functions,
    returns this result.
    """
    # This function does preparation for (2), calls
    # _meijerint_definite_3 for (2) and (3) combined.

    # use a positive dummy - we integrate from 0 to oo
    # XXX if a nonnegative symbol is used there will be test failures
    dummy = _dummy('x', 'meijerint-definite2', f, positive=True)
    f = f.subs(x, dummy)
    x = dummy

    if f == 0:
        return S(0), True

    for g, explanation in _guess_expansion(f, x):
        _debug('Trying', explanation)
        res = _meijerint_definite_3(g, x)
        if res:
            return res


def _meijerint_definite_3(f, x):
    """
    Try to integrate f dx from zero to infinity.

    This function calls _meijerint_definite_4 to try to compute the
    integral. If this fails, it tries using linearity.
    """
    res = _meijerint_definite_4(f, x)
    if res and res[1] != False:
        return res
    if f.is_Add:
        _debug('Expanding and evaluating all terms.')
        ress = [_meijerint_definite_4(g, x) for g in f.args]
        if all(r is not None for r in ress):
            conds = []
            res = S(0)
            for r, c in ress:
                res += r
                conds += [c]
            c = And(*conds)
            if c != False:
                return res, c


def _my_unpolarify(f):
    from sympy import unpolarify
    return _eval_cond(unpolarify(f))


@timeit
def _meijerint_definite_4(f, x, only_double=False):
    """
    Try to integrate f dx from zero to infinity.

    This function tries to apply the integration theorems found in literature,
    i.e. it tries to rewrite f as either one or a product of two G-functions.

    The parameter ``only_double`` is used internally in the recursive algorithm
    to disable trying to rewrite f as a single G-function.
    """
    # This function does (2) and (3)
    _debug('Integrating', f)
    # Try single G function.
    if not only_double:
        gs = _rewrite1(f, x, recursive=False)
        if gs is not None:
            fac, po, g, cond = gs
            _debug('Could rewrite as single G function:', fac, po, g)
            res = S(0)
            for C, s, f in g:
                if C == 0:
                    continue
                C, f = _rewrite_saxena_1(fac*C, po*x**s, f, x)
                res += C*_int0oo_1(f, x)
                cond = And(cond, _check_antecedents_1(f, x))
                if cond == False:
                    break
            cond = _my_unpolarify(cond)
            if cond == False:
                _debug('But cond is always False.')
            else:
                _debug('Result before branch substitutions is:', res)
                return _my_unpolarify(hyperexpand(res)), cond

    # Try two G functions.
    gs = _rewrite2(f, x)
    if gs is not None:
        for full_pb in [False, True]:
            fac, po, g1, g2, cond = gs
            _debug('Could rewrite as two G functions:', fac, po, g1, g2)
            res = S(0)
            for C1, s1, f1 in g1:
                for C2, s2, f2 in g2:
                    r = _rewrite_saxena(fac*C1*C2, po*x**(s1 + s2),
                                        f1, f2, x, full_pb)
                    if r is None:
                        _debug('Non-rational exponents.')
                        return
                    C, f1_, f2_ = r
                    _debug('Saxena subst for yielded:', C, f1_, f2_)
                    cond = And(cond, _check_antecedents(f1_, f2_, x))
                    if cond == False:
                        break
                    res += C*_int0oo(f1_, f2_, x)
                else:
                    continue
                break
            cond = _my_unpolarify(cond)
            if cond == False:
                _debug('But cond is always False (full_pb=%s).' % full_pb)
            else:
                _debug('Result before branch substitutions is:', res)
                if only_double:
                    return res, cond
                return _my_unpolarify(hyperexpand(res)), cond


def meijerint_inversion(f, x, t):
    """
    Compute the inverse laplace transform
    :math:\int_{c+i\infty}^{c-i\infty} f(x) e^{tx) dx,
    for real c larger than the real part of all singularities of f.
    Note that ``t`` is always assumed real and positive.

    Return None if the integral does not exist or could not be evaluated.

    Examples
    ========

    >>> from sympy.abc import x, t
    >>> from sympy.integrals.meijerint import meijerint_inversion
    >>> meijerint_inversion(1/x, x, t)
    Heaviside(t)
    """
    from sympy import I, Integral, exp, expand, log, Add, Mul, Heaviside
    f_ = f
    t_ = t
    t = Dummy('t', polar=True)  # We don't want sqrt(t**2) = abs(t) etc
    f = f.subs(t_, t)
    c = Dummy('c')
    _debug('Laplace-inverting', f)
    if not _is_analytic(f, x):
        _debug('But expression is not analytic.')
        return None
    # We filter out exponentials here. If we are given an Add this will not
    # work, but the calling code will take care of that.
    shift = 0
    if f.is_Mul:
        args = list(f.args)
        newargs = []
        exponentials = []
        while args:
            arg = args.pop()
            if isinstance(arg, exp):
                arg2 = expand(arg)
                if arg2.is_Mul:
                    args += arg2.args
                    continue
                try:
                    a, b = _get_coeff_exp(arg.args[0], x)
                except _CoeffExpValueError:
                    b = 0
                if b == 1:
                    exponentials.append(a)
                else:
                    newargs.append(arg)
            elif arg.is_Pow:
                arg2 = expand(arg)
                if arg2.is_Mul:
                    args += arg2.args
                    continue
                if x not in arg.base.free_symbols:
                    try:
                        a, b = _get_coeff_exp(arg.exp, x)
                    except _CoeffExpValueError:
                        b = 0
                    if b == 1:
                        exponentials.append(a*log(arg.base))
                newargs.append(arg)
            else:
                newargs.append(arg)
        shift = Add(*exponentials)
        f = Mul(*newargs)

    gs = _rewrite1(f, x)
    if gs is not None:
        fac, po, g, cond = gs
        _debug('Could rewrite as single G function:', fac, po, g)
        res = S(0)
        for C, s, f in g:
            C, f = _rewrite_inversion(fac*C, po*x**s, f, x)
            res += C*_int_inversion(f, x, t)
            cond = And(cond, _check_antecedents_inversion(f, x))
            if cond == False:
                break
        cond = _my_unpolarify(cond)
        if cond == False:
            _debug('But cond is always False.')
        else:
            _debug('Result before branch substitution:', res)
            res = _my_unpolarify(hyperexpand(res))
            if not res.has(Heaviside):
                res *= Heaviside(t)
            res = res.subs(t, t + shift)
            if not isinstance(cond, bool):
                cond = cond.subs(t, t + shift)
            return Piecewise((res.subs(t, t_), cond),
                             (Integral(f_*exp(x*t), (x, c - oo*I, c + oo*I)).subs(t, t_), True))
