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Revista Técnica de la Facultad de Ingeniería Universidad del Zulia

versión impresa ISSN 0254-0770

Rev. Téc. Ing. Univ. Zulia v.33 n.1 Maracaibo abr. 2010

 

A summation formula concerning the Mellin Transform* 

M.L. Glasser 1,2, Nikos Bagis 3, Grazyna Majchrowska

1 Department of Physics, Clarkson University, Potsdam. New York, USA. laryg@clarkson.edu

2 Departamento de Física Teórica, Atómica y Óptica, Universidad de Valladolid, 47071. Spain.

3 Department of Informatics, Aristotele University of Thessaloniki 54124, Greece. 

Abstract 

We derive a new summation formula involving Mellin transform. We apply this formula to sum various series related to elliptic integrals and theta functions. 

Key words: Mellin Transform, summation formulas, Jacobian functions. 

Una fórmula de adición usando la Transformada de Mellin

Resumen 

En este trabajo una nueva fórmula de adición es derivada usando la transformada de Mellin. Esta fórmula es aplicada para sumar varias series relacionadas con las integrales elípticas y las funciones theta. 

Palabra clave: Transformada de Mellin, fórmulas de adición, función jacobiana.

Received: January 10, 2010  Revised form, March 1, 2010 

1. Introduction 

One of the fundamental results of Fourier analysis is the Poisson Summation Formula, which can be written [1] 

where a  > 0 , ab= 2p and

is the Fourier Transform of f. Equation (1) is valid under relatively weak conditions. For example f(X)=O [(1+ ½X½C) -1, for X Î R and for some C > 0. It is also known that if

is the Cosine Transform of a function f then we have the Poisson Summation Cosine Formula [2] 

where a  > 0 , ab= 2p

In this work using the Poisson Summation Formula we generalize an exponential formula of Ramanujan and arrive at a new Mellin Summation Formula. This formula is like (4) but now the part of Fourier Cosine Transform is replaced by the Mellin Transform. We also give several applications. 

Definition [2] 

The Mellin Transform of a function Y is defined to be

For the applications we will need the following 

2. The Theorems 

Theorem 1 [3] 

Let a  > 0 and the function f  be odd and analytic in the uper half plane Im(z) > 0 and continuous in Im(z) ³ 0 and let there exist C,N > 0 and 0 £ b < p such that

for every z in Im(z) ³ 0, then

where ab= 2p and

The Main Theorem. (The Mellin Summation Formula-MSF) 

Let a, b > 0 and ab= 2p, then

 

where f (x)= Re [(My) (ix) f (-x)], with and f, y, x real, f (o)= 0, provided that all sums

converge.

To prove the MSF we use a Theorem which appeared first in [4]. Here we give a complete proof and the conditions under which this Theorem holds. 

Theorem 2. [4] 

Let y (x) be analytic around 0. Also let f be analytic function in C satisfying

for every z with Im(z) ³ 0, C, l, d > 0 constantst, with the condition |z|= x + N + 1/2, N sufficiently large natural number. Then for x > 0 the integral  


converges absolutely, the series


converges in the Abel sense and

If also


then the series 


converges and we can drop the limit in (10). 

3. The Proofs of Theorems 

The proof of Theorem 1 is in [3]. For the proof of Theorem 2 we need a Lemma. 

Lemma 

Let y have a Taylor Series around 0, with radius of convergence r > 0. Let also x Î R such that

Then the Mellin Transform of  Y can be extended analytically into a meromorphic function in the half plane Re (z) < x with simple poles at the points z= -m for m Î z with m > -x, m ³ 0.

Proof 

Let 0 < a < r. Then if z is not an integer


 

 

 

Thus the function is meromorphic in C whose only poles are z= -m with residue

We also define the function  h2(z) =  ò ¥a y (u)z-1 du which converges absolutely to ananalytic function when Re(z) < x.


                    

And for the derivative we have

This completes the proof of the Lemma. 

Now let the function Y be as in Lemma and let x Î R be such that (11) holds. We define the function

Then from the Lemma g is meromorphic in Im(z) > 0 and continuous in Im(z) ³ 0 with simple poles at z= i(m + x), where m Î z , m ³ 0, m + x > 0 and

Let gR be the upper half circle with diameter [-R,R] where R = RN = x + N +1/2, N a natural number. Then

and thus

So, if the integral ò ¥- ¥ f(t) (MY)(x + it)dt exists and also

the series converges and we have 

The condition m > -x not needed if x > 0

Having in mind the above and the Lemma we can proceed to the following 

Proof of Theorem 2 

From (9) the integral 

ò ¥- ¥ f (t) (MY)(x + it)eita dt

is absolutely convergent for a > 0. Also if 0 < a £ d we will have

for RN ® ¥ when 0 £ q £ p

Hence for every a > 0 one as

from which (10) follows. 

Proof of the Main Theorem 

If f (x) = Re [(MY)(ix) f (-ix)], with f, y, x real, then f (x) is an even function. The reason is that we can write according Theorem 2 

From the above we have 


 

 

 

also 

 

where ab= 2p, and . This completes the proof. 

Notes 

1. In the same way one can prove a formula of Ramajunan [5] (which we give here a more general form) 

If ab= 2p, then

 

where

2. The use of Theorem 2 for finding Self Reciprocal functions. 

From [2] we have that whenever fc (x) = f (x) then


and


 

where , fe (s) being an even function. Using Theorem 2 with Y(x)= e-x we have


 

 

which is more convenient to calculate. 

Similar expansions hold for the Fourier sine transform and Hankel transforms. 

4. Applications 

1. Let and f(k) = knk, then Y(x)= e-x and (MY)(S) = G(S). Hence if ab= 2p

2. Let and f(k) = k, then we have . Hence if a,n > 0, noting that 

we have from the MSF.

It is known from tables that [6]

Thus we arrive at

3. From the relations [7]

and 

from the Main Theorem we get

whenever

4. Also we have 

5. If  a,n > 0 and , denotes the Polylogarithm function then

Proof 

Let and f(k)= k, then if   we have  

In the same way we have

where   is the Riemann Zeta function. 

Or, if ab= 2p then

6. A consequence of Jacobi’s triple identity. Note that the calculations of sums in Application 5 depend on finding the values 

where we have set

To find C1 (a) we differentiate X (n, a) twice with respect to v to get


 

 

 

 

where qj (0, q)= qj (q)

Note use Theorem 1 with along with Jacobi’s triple identity [6] to arrive at

But it is known from tables that

where kb is the solution of (note that when b Î Q*+ then the kb are algebraic numbers) and

 

Hence we have 

Proposition 2.1

For Y we can find in the same way that

and B2(b)= 0, where is the q-product. Thus what remains is to find the value of A2(b). In this way we are led to 

Proposition 2.2. 

References 

1. C.K.Chui. ’An Introduction to Wavelets’. Academic Press. New York. 1992.         [ Links ]

2. E.C. Tichmarsh. ’Introduction to the theory of Fourier integrals’. Oxford University Press, Amen House, London, 1948.         [ Links ]

3. M.L. Glasser and N. Bagis, arXiv: 0812.0990.         [ Links ]

4. N. Bagis and M.L. Glasser.’ Integrals and Series Resulting from Two Sampling Theorems’. Journal of Sampling Theory in Signal and Image Processing. Vol. 5, No. 1, Jan. 2006, pp.89-97.         [ Links ]

5. B.C. Berndt and J.L. Hafner. ’Two remarkable boubly exponential series transformations of Ramanujan’. J. Proceedings Mathematical Sciences Jan 2008, pp. 245-252.         [ Links ]

6. E.T. Whittaker and G.N. Watson. ’A course on Modern Analysis’. Cambridge U.P. 1927         [ Links ]

7. I.J. Zucker. ’The Summation of Series of Hyperbolic functions’. SIAM J. Math. Anal. 10. (1979). 192-206.        [ Links ]