Volume 2011, Article ID 132081,7pages doi:10.1155/2011/132081
Research Article
On a New Summation Formula for
2
ψ
2
Basic Bilateral Hypergeometric Series
and Its Applications
D. D. Somashekara, K. Narasimha Murthy, and S. L. Shalini
Department of Studies in Mathematics, University of Mysore, Manasagangotri, Mysore 570006, India
Correspondence should be addressed to K. Narasimha Murthy,[email protected]
Received 7 December 2010; Accepted 24 January 2011
Academic Editor: J. Dydak
Copyrightq2011 D. D. Somashekara et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
We have obtained a new summation formula for2ψ2 bilateral basic hypergeometric series by the method of parameter augmentation and demonstrated its various uses leading to some development of etafunctions,q-gamma, andq-beta function identities.
1. Introduction
The summation formulae for hypergeometric series form a very interesting and useful component of the theory ofbasichypergeometric series. Theq-binomial theorem of Cauchy
1is perhaps the first identity in the class of the summation formulae, which can be stated as
∞
k0
ak
qkzk
az∞
z∞ , |z|<1, q<1, 1.1
where
a∞:a;q∞:
∞
k0
1−aqk,
ak:a;qk: a∞ aqk ∞
, k is an integer.
For more details about theq-binomial theorem and about the identities which fall in this sequel, one may refer to the book by Gasper and Rahman2. Another famous identity in the sequel is the Ramanujan’s 1ψ1summation formula3
∞
k−∞
ak bkzk
az∞q∞q/az∞b/a∞ z∞b∞b/az∞q/a∞ ,
ba<|z|<1, q<1. 1.3
There are a number of proofs of the1ψ1 summation formula1.3in the literature. For more
details, one refers to the book by Berndt4and a recent paper of Johnson5.
In this paper, we derive a new summation formula for2ψ2basic bilateral
hypergeomet-ric series using the1ψ1summation formula1.3by the method of parameter augmentation.
We then use the formula to derive theq-analogue of Gauss summation formula and to obtain a number of etafunction, q-gamma, and q-beta function identities, which complement the works of Bhargava and Somashekara6, Bhargava et al.7, Somashekara and Mamta8, Srivastava9, and Bhargava and Adiga10.
First, we recall thatq-difference operator and theq-shift operator are defined by
Dqfa fa−f
aq
a , ζ
fafaq, 1.4
respectively. In11, Chen and Liu have constructed an operatorθas
θζ−1D
q, 1.5
and thereby they defined the operatorEbθas
Ebθ ∞
k0
bθkqkk−1/2
q;qk . 1.6
Then, we have the following operator identities12, Theorem 1:
Ebθ at;q∞at, bt;q∞,
Ebθ as, at;q∞
as, at, bs, bt;q∞
abst/q;q∞ ,
abstq <1.
Further, the Dedekind etafunction is defined by
ητ:eπiτ/12
∞
k1
1−e2πikτ:q1/24q;q∞, 1.8
whereqe2πiτ, and Imτ>0.
Jackson13defined theq-analogue of the gamma function by
Γqx
q;q∞
qx;q ∞
1−q1−x, 0< q <1. 1.9
In his paper on the q-gamma andq-beta function, Askey14has obtainedq-analogues of several classical results about the gamma function. Further, he has given the definition for q-beta function as
Bqx, y1−q ∞
n0
qnx
qn 1 ∞
qx y ∞
. 1.10
In fact, he has shown that
Bqx, y ΓqxΓq
y
Γqx y . 1.11
InSection 2, we prove our main result. In Section 3, we deduce the well-known q-analogue of the Gauss summation formula and some etafunction, q-gamma, and q-beta function identities.
2. Main Result
Theorem 2.1. If 0<|z|<1, |q|<1, then
∞
k−∞
akbc/azqk
bkck zk
az∞q∞q/az∞b/a∞c/a∞bc/azq∞
z∞b∞c∞b/az∞c/az∞q/a∞ . 2.1
Proof. Ramanujan’s1ψ1summation formula1.3can be written as
∞
k0
ak bkzk
∞
k1
q/bk
q/ak
b
az
k
az∞
q∞q/az∞b/a∞
This is the same as
∞
k0
akzkbqk ∞
b
az
∞
∞
k1
−1kqkk 1/2
q/ak
1 az
k
bq−k ∞
b
az
∞
az∞
q∞q/az∞
z∞q/a∞
b
a
∞
.
2.3
On applyingEcθto both sides with respect tob, we obtain
∞
k0
akzk
bqk
∞b/az ∞cqk∞c/az∞
bcqk/azq ∞
∞
k1
−1kqkk 1/2
q/ak
1 az
kbq−k
∞b/az ∞cq−k∞c/az∞
bcq−k/azq ∞
az∞
q∞q/az∞
z∞q/a∞
b
a
∞
c
a
∞
.
2.4
Multiplying2.4throughout by{bc/azq∞/b∞c∞}, we obtain
∞
k0
akbc/azqk
bkck zk
∞
k1
a−kbc/azq−k
b−kc−k z−k
az∞
q∞q/az∞b/a∞c/a∞bc/azq∞
z∞b∞c∞b/az∞c/az∞q/a∞ ,
2.5
which yields2.1.
3. Some Applications of the Main Identity
The following identity is the well-knownq-analogue of the Gauss summation formula.
Corollary 3.1see15. If|q|<1,|γ/αβ|<1, then
∞
k0
αkβk
qkγk
γ
αβ
k
γ/α∞γ/β∞
γ∞γ/αβ∞ . 3.1
Corollary 3.2. If|q|<1, then
∞
k−∞
q2;q4 k
1−q4k 1q3;q4 k
qkq−1/8 η72τ
η3τη24τ, 3.2
∞
k−∞
−q2;q2
k
1 q2k 12−q;q2 k
qk2q−3/4η64τ
η32τ, 3.3
∞
k−∞
−q;q2
k
−q2;q2
k
1−q2k 12q;q22 n
qk2q−3/4η84τ
η72τ, 3.4
∞
k−∞
1 q−q;q2 k
−q2;q2
k
1−q2k 2q2;q22 k
qk η2τ
η2τ, 3.5
∞
k−∞
q2;q6 k
1−q6k 1q5;q6 k
q3kq−1/4η42τ
η2τ , 3.6
∞
k−∞
1 q22−q2;q2 k−1
−q2;q2
k 1
1−q2k 22q2;q22 k
qk η24τ
η42τ. 3.7
Proof. Puttingazq1/4,bq3/4,cq5/4, and then changingqtoq4in2.1, we obtain
∞
k−∞
q;q4 k
q2;q4 k
q;q4 k 1
q3;q4 k
qk
q2;q44 ∞
q4;q42 ∞
q;q43 ∞
q3;q43 ∞
. 3.8
Simplifying the right hand side and then using1.8, we obtain3.2.
Similarly, puttinga −q1/2,zq1/2,b−q3/2,c −q3/2, and then changingqtoq2,
we obtain3.3. Puttinga−q1/2,zq1/2,bcq3/2, and then changingqtoq2, we obtain
3.4. Puttinga −q1/2,z q1/2,b q,c q2, and then changingqtoq2, we obtain3.5.
Puttingaq1/6,zq1/2,bq7/6,cq5/6, and then changingqtoq6, we obtain3.6. Finally,
puttinga−1,zq,bcq2, and then changingqtoq2, we obtain3.7.
Corollary 3.3. If 0< q <1, 0< x,y <1, and 0< x y <1, then
B3 q
x, y Γq
1−x yΓqx−y1−q2
1−qy2
∞ k−∞ q1−x k
qx y k
q1 y2 k
qky. 3.9
Proof. Puttingaq1−x,zqy, andb c q1 yin2.1, we get
∞ k−∞ q1−x k
qx y k
q1 y2 k
qky
q1−x y
∞
q∞qx−y ∞
qy ∞
q1 y ∞
q1 y ∞
qx y ∞
qx ∞
3
. 3.10
Corollary 3.4. If 0< q <1, 0< x,y <1, and 1< x y <2, then
B2
qx, y
Γqy−xΓqx−y 1Γqx y−1
ΓqyΓq1 x
∞
k−∞
q−x k
qx y−1
k
qy2 k
qky. 3.11
Proof. Puttinga q−x,z b c qy, in2.1, and then using 1.9,1.10, and1.11, we
obtain3.11.
Corollary 3.5. If 0< x,y <1, and 0< x y <1, then
B3x, y Γ
1−x yΓx−y y2
⎡
⎣∞
k0
1−xkx yk
1 y2k
∞
k1
−y2k
xk1−x−yk
⎤
⎦. 3.12
Proof. Lettingq → 1 in3.9, we obtain3.12.
Corollary 3.6. If 0< x,y <1, and 1< x y <2, then
B2x, y Γ
y−xΓx−y 1Γx y−1
ΓyΓ1 x
× ⎡
⎣∞
k0
−xkx y−1k
y2 k
∞
k1
1−y2k
1 xk2−x−yk
⎤
⎦.
3.13
Proof. Lettingq → 1 in3.11, we obtain3.13.
Corollary 3.7. If 0< q <1, 0< x,y <1, and 0< x y <1, then
Bqx, y ΓqyΓq1−y ∞
k0
q1−x−y
k
qy k
q2 k
qkx. 3.14
Proof. Puttingaq1−x−y,zqx, andbcqin2.1, we obtain3.14.
Acknowledgment
The authors would like to thank the referees for their valuable suggestions which consi-derably improved the quality of the paper.
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