In mathematics, Ramanujan's master theorem (named after mathematician Srinivasa Ramanujan[1]) is a technique which provides an analytic expression for the Mellin transform of a function.
The result is stated as follows:
Assume function
has an expansion of the form

then Mellin transform of
is given by

where
is the Gamma function.
It was widely used by Ramanujan to calculate definite integrals and infinite series.
Multidimensional version of this theorem also appear in quantum physics (through Feynman diagrams).[2]
A similar result was also obtained by J. W. L. Glaisher.[3]
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An alternative formulation of Ramanujan's master theorem is as follows:

which gets converted to original form after substituting
and using functional equation for Gamma function.
The integral above is convergent for
.
The proof of Ramanujan's Master Theorem provided by G. H. Hardy[4] employs Cauchy's residue theorem as well as the well-known Mellin inversion theorem.
The generating function of the Bernoulli polynomials
is given by:

These polynomials are given in terms of Hurwitz zeta function:

by
for
. By means of Ramanujan master theorem and generating function of Bernoulli polynomials one will have following integral representation[5]:

valid for
.
Weierstrass's definition of the Gamma function

is equivalent to expression

where
is the Riemann zeta function.
Then applying Ramanujan master theorem we have:

for valid for
.
Special cases of
and
are


Mathematica 7 is unable to compute these examples.[6]
It is well known for the evaluation of

which is a well known quartic integral.[7]
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