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Ramanujan's master theorem

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Ramanujan's master theorem

In mathematics, Ramanujan's master theorem (named after mathematician Srinivasa Ramanujan) is a technique that provides an analytic expression for the Mellin transform of an analytic function.

Contents

The result is stated as follows:

If a complex-valued function f ( x ) has an expansion of the form

f ( x ) = ∑ k = 0 ∞ ϕ ( k ) k ! ( − x ) k

then the Mellin transform of f ( x ) is given by

∫ 0 ∞ x s − 1 f ( x ) d x = Γ ( s ) ϕ ( − s )

where Γ ( s ) is the gamma function.

It was widely used by Ramanujan to calculate definite integrals and infinite series.

Higher-dimensional versions of this theorem also appear in quantum physics (through Feynman diagrams).

A similar result was also obtained by J. W. L. Glaisher.

Alternative formalism

An alternative formulation of Ramanujan's master theorem is as follows:

∫ 0 ∞ x s − 1 ( λ ( 0 ) − x λ ( 1 ) + x 2 λ ( 2 ) − ⋯ ) d x = π sin ⁡ ( π s ) λ ( − s )

which gets converted to the above form after substituting λ ( n ) = ϕ ( n ) Γ ( 1 + n ) and using the functional equation for the gamma function.

The integral above is convergent for 0 < Re ⁡ ( s ) < 1 .

Proof

The proof of Ramanujan's Master Theorem provided by G. H. Hardy employs the Cauchy's residue theorem and the well-known Mellin inversion theorem.

Application to Bernoulli polynomials

The generating function of the Bernoulli polynomials B k ( x ) is given by:

z e x z e z − 1 = ∑ k = 0 ∞ B k ( x ) z k k !

These polynomials are given in terms of Hurwitz zeta function:

ζ ( s , a ) = ∑ n = 0 ∞ 1 ( n + a ) s

by ζ ( 1 − n , a ) = − B n ( a ) n for n ≥ 1 . By means of Ramanujan master theorem and generating function of Bernoulli polynomials one will have following integral representation:

∫ 0 ∞ x s − 1 ( e − a x 1 − e − x − 1 x ) d x = Γ ( s ) ζ ( s , a )

valid for 0 < Re ⁡ ( s ) < 1 .

Application to the Gamma function

Weierstrass's definition of the Gamma function

Γ ( x ) = e − γ x x ∏ n = 1 ∞ ( 1 + x n ) − 1 e x / n

is equivalent to expression

log ⁡ Γ ( 1 + x ) = − γ x + ∑ k = 2 ∞ ζ ( k ) k ( − x ) k

where ζ ( k ) is the Riemann zeta function.

Then applying Ramanujan master theorem we have:

∫ 0 ∞ x s − 1 γ x + log ⁡ Γ ( 1 + x ) x 2 d x = π sin ⁡ ( π s ) ζ ( 2 − s ) 2 − s

valid for 0 < R e ( s ) < 1 .

Special cases of s = 1 2 and s = 3 4 are

∫ 0 ∞ γ x + log ⁡ Γ ( 1 + x ) x 5 / 2 d x = 2 π 3 ζ ( 3 2 ) ∫ 0 ∞ γ x + log ⁡ Γ ( 1 + x ) x 9 / 4 d x = 2 4 π 5 ζ ( 5 4 )

Mathematica 7 is unable to compute these examples.

References

Ramanujan's master theorem Wikipedia
(Text) CC BY-SA


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