Advances in Pure Mathematics
Vol.06 No.03(2016), Article ID:63987,9 pages
10.4236/apm.2016.63013
Modified Double Zeta Function and Its Properties
Arif M. Khan
Department of Mathematics, Jodhpur Institute of Engineering & Technology, Jodhpur, India

Copyright © 2016 by author and Scientific Research Publishing Inc.
This work is licensed under the Creative Commons Attribution International License (CC BY).
http://creativecommons.org/licenses/by/4.0/


Received 4 November 2015; accepted 24 February 2016; published 29 February 2016
ABSTRACT
The present paper aims at introducing and investigating a new class of generalized double zeta function i.e. modified double zeta function which involves the Riemann, Hurwitz, Hurwitz-Lerch, Barnes double zeta function and Bin-Saad generalized double zeta function as particular cases. The results are obtained by suitably applying Riemann-Liouville type and Tremblay fractional integral and differential operators. We derive the expansion formula for the proposed function with some of its properties via fractional operators and discuss the link with known results.
Keywords:
Modified Zeta Function, Riemann-Liouville Operator, Tremblay Fractional Operators, Hypergeometric Function

1. Introduction and Preliminaries
The Hurwitz-Lerch zeta function [1] is defined by
(1)
is an analytic function in both variables y and z in suitable region.
The further generalization of Hurwitz-Lerch zeta function
is defined by [2]
(2)
where
denotes the Pochhammer’s symbol,
, 
In [3] [4] Bin-Saad and Al-Gonah introduced two hypergeometric type generating functions of generalized zeta function as follows
(3)
and
(4)
The generalized double zeta function of Bin-Saad [5] is defined by
(5)
where
;
, 
The alternate representation is
(6)
where
is the generalized zeta function defined by (2).
The generalized hypergeometric function in classical form has been defined [6] as

where
Bin-Saad [5] discussed following relationships.




where F1 is the Appell’s function of two variables [7] defined as

We further recall the following well known expansion formula of Hurwitz-Lerch zeta function [1]

where



is Hurwitz zeta function which is generalization of the Riemann zeta function given as

Due to great potential and significant role of special functions especially hypergeometric functions in various problems occurring in mathematical physics, engineering [8] [9] , the author has motivated to further investigate the topic. Several generalizations of hypergeometric functions have been made by many authors [10] [11] . Recently Rao [12] defined Wright type generalized hypergeometric function via fractional calculus. Many authors investigated the fractional calculus approach in study of generalized hypergeometric type function [13] [14] . The subject fractional calculus has gained much attention amongst researchers due to its vast potential of demonstrated mathematical models in various fields of science and engineering such as diffusion, oscillation, dynamical process in porous structures, propagation of waves, diffusive transport, fluid flow, etc. The present paper aims at introducing and investigating a new kind of hypergeometric type function that is modified double zeta function via fractional calculus. The layout of the paper is as follows
In section 2 we introduce and discuss some properties of the modified double zeta function. Section 3 devoted to discuss the Trembley [15] well poised fractional calculus operator together with its properties. In section 4, we establish some interesting results of modified double zeta function through fractional operators and also derive its summation formula. In section 5, we develop some properties of fractional operators. Many Lemmas and particular cases have been discussed to relate known results.
2. Modified Double Zeta Function
In a sequel of result (5) here we introduce a modified double zeta function as follows

where


We can readily obtain following relationship




Integration and differentiation of fractional order are traditionally defined by the left side Riemann fractional integral operator 





Further for 


A generalization of Riemann-Liouville fractional derivatives 

(throughout this paper we apply all operators with respect to x variable).


Lemma 2.1. (Mathai and Haubold [16] ) If


Lemma 2.2. (Srivastava and Tomovski [14] ) If



Lemma 2.3. If




Proof. On using definition (16), we get
Simplify and using definition (16) again, yields the proof of (29).
Now we define the integral operator as follows:

where


3. The Well Poised Fractional Calculus Operator
The fractional calculus operator 

where 

We can easily obtain the following result of




where 
The operator 
4. The Main Results
Theorem 4.1 If






If 

Proof. L.H.S of (38) after using (21) gives
Using definition (16) suitably changing the order of summation and integration, we have

By virtue of (27)

Finally by using definition (16), yields result (38).
Further to prove (39), we use (16) and (23)

Using (38) we get

Finally using lemma 2.3 yields R.H.S of (39).
To prove (40), we have

Using Equation (28), yields proof of (40).
Theorem 4.2 If



Proof. We have

On using (35) we get

After little simplification and using definition (16), yields the results (46).
Remark 4.1. For

Remark 4.2. On putting y = 0 in Equation (49), we get

Remark 4.3. Further if we set b = c in Equation (46), it reduces to known identity due to Trembley [15]

Theorem 4.3. If


then

Proof. Expressing modified zeta function in L.H.S as series and changing the order of integration and summation, gives

employing (37), yields
which completes the proof.
Corollary 4.1. On putting 

Theorem 4.4. If


where

Proof. From (16) we have
Now employing series representation of 

Clearly
After little simplification

This completes the proof of (55).
Remark 4.4. For b = c equation (55) yields the result [Bin-Saad [5] : p. 273, Equation (2.18), theorem 2.1].
5. Some Properties of the Operator
Theorem 5.1. With all conditions on parameters as stated in Equations (27) and (30), the following properties holds true

Proof. From (21) and (30), we have
Therefore
Interchanging the order of integration and using Dirichlet formula [17] , we obtain
and substituting

Making use of (21) leads
this leads the proof of L.H.S of (58).
again
Using the Dirichlet formula [17] and interchanging the order of integration we get
Substituting

making use of (59) readily leads to the proof of R.H.S of (58).
6. Conclusion
Recently fractional operator’s theory was recognized to be a good tool for modeling complex problems, kinetic equations, fractional reaction, diffusion equations, etc. In this work we introduce and study the new class of generalized zeta function through Riemann Liouville type and Tremblay fractional integral and differential operators. In section 4, interesting images of modified double zeta function have been obtained and useful link between generalized and modified zeta function has been established through Trembley fractional operator. Series expansion of the new class of generalized zeta function is a significant contribution in the direction along that developed in [5] . In section 5, interesting properties of operator 
Cite this paper
Arif M.Khan, (2016) Modified Double Zeta Function and Its Properties. Advances in Pure Mathematics,06,159-167. doi: 10.4236/apm.2016.63013
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