R E S E A R C H
Open Access
A reduction formula for a
q
-beta integral
Zeinab Sayed Mansour
1,2and Maryam Ahmed Al-Towailb
3**Correspondence:
mtowaileb@ksu.edu.sa
3Department of Natural and
Engineering Science, Faculty of Applied Studies and Community Service, King Saud University, Riyadh, KSA
Full list of author information is available at the end of the article
Abstract
In this paper, we give a reduction formula for a specificq-integral. Our formula is expressed as a three term recurrence relations for basic hypergeometric3
φ
2series. This is aq-analog of work by Watson and by Bailey of 1953.Keywords: q-beta integral; basic hypergeometric series; contiguous relations
1 Introduction and preliminaries
In [], Watson constructed a reduction formula for the integral
In=
xα( –x)βdn{x
γ( –x)δ}
dxn dx.
In fact, he proved that
In=
(α+γ –n+ )(β+δ–n+ )
(σ–n+ ) Hn,
where
Hn= n
r=
(–)n–r
n r
(–γ)n–r(β+δ–n+ )n–r(–δ)r(α+γ –n+ )r,
and the notation (x)rdenotes the product
(x)≡ and (x)r≡x(x+ )· · ·(x+r– ), r≥.
Furthermore, Watson proved thatHnsatisfies the following three term recurrence
rela-tion:
(σ–n)(σ–n)Hn+–QnHn++SnHn= , (.)
where
Sn= (n+ )(σ–n– )(α+β–n)(γ+δ–n)(β+δ–n),
Qn= (σ– n– )
(βγ–αδ)(σ+ ) +θ(n+ )(σ–n)
,
and σ=α+β+γ+δ, θ=α–β–γ+δ. Also, he remarkedHncan be expressed in terms
of a hypergeometric series of the typeFwith last element unity which implies that (.)
gives a three term contiguous relation for terminatingFseries.
The proof introduced by Watson depends on constructing a second order linear differ-ential equation satisfied by the integrand ofIn. On the other hand, in [], Bailey derived
relations between contiguous hypergeometric functions of the typeF(), and by using
these relations, he obtained another proof of Watson’s reduction formula. In this paper, we introduce aq-analog of the integralInby
In,q=
xα(qx;q)βDnq–
xγ qβ+x;qδdqx, n= , , , . . . ,
whereα,β,γ, andδare complex numbers, andqis a positive number less than one. Our aim to obtain a reduction formula forIn,q.
It turns out to us that Watson technique for introducing (.) is too hard to applied to our work. Therefore, we follow Bailey’s approach for deriving the reduction formula.
We recall the following definitions (see,e.g., [–]): Theq-shifted fractional is defined by
(a;q)∞= ∞
j=
–aqj, and (a;q)n:=
(a;q)∞
(aqn;q)∞ forn∈Z,a∈C.
Theq-derivativeDqf of an arbitrary functionf is given by
(Dqf)(x) :=
f(x) –f(qx)
( –q)x , x= .
We follow Gasper and Rahman [] for the definitions of Jacksonq-integrals, and the
q-gamma andq-beta functions (see also [–]). Theq-integration by parts rule (see []) is
a
f(qt)Dqg(t)dqt=f(a)g(a) – lim n→∞f q
ng qn–
a
Dqf(t)g(t)dqt.
Leta, . . . ,ar,b, . . . ,bsbe complex numbers, theq-hypergeometric seriesrφsdefined by
rφs(a, . . . ,ar,b, . . . ,bs;q,z) = ∞
n=
(a, . . . ,ar;q)n
(q,b, . . . ,bs;q)n
zn –q(n–)/n(s–r+)
The series representation of the functionrφsconverges absolutely for allz∈Cifr≤s, and
converges only for|z|< ifr=s+ (for more details and results see [–] and []). Observe that
I,q=
xα+γ(qx;q)β+δdqx=Bq(α+γ + ,β+δ+ )
=q(α+γ + )q(β+δ+ )
q(α+γ +β+δ+ )
and, by using theq-integration by parts, one can verify that
I,q=
xα(qx;q)βDq–
xγ qβ+x;qδdqx
=q–γ q(α+γ)q(β+δ)
q(α+γ +β+δ+ )
[γ][β+δ] –qβ[δ][α+γ],
where the notation [z] is defined by
[z] := –q
z
–q.
Note that the above values of the integralsI,qandI,qcoincide withIandI, respectively,
which are given by Watson in the limitq→.
This paper is organized as follows. In Section , we derive three term contiguous rela-tions for the basic hypergeometric functionφ(a,b,c;d,e;q,q). In Section , we show that
In,qcan be represented asφ(q) and a direct substation in the derived contiguous relation
yields the result of this paper.
2 Contiguous relations of3
φ
2Throughout this section, we simply usedato denotes the valueq–nwherenis an arbitrary
nonnegative integer. We denote byφthe function
φ(a,b,c;d,e;q,q),
and by φ(a+), φ(a–) the same function when ais changed toaq,a/q, respectively. We
use a similar notation when the other parameters are so changed. Also, letφ+,φ–be the
functions defined by
φ+=φ(aq,bq,cq;dq,eq;q,q) and φ–=φ(a/q,b/q,c/q;d/q,e/q;q,q).
By the definition ofφ, one can verify the following:
φ a+–φ=qa( –b)( –c)
( –d)( –e)φ+, (.)
φ a––φ= –a( –b)( –c)
( –d)( –e)φ+ a
–, (.)
φ d+–φ= –qd ( –a)( –b)( –c)
( –d)( –qd)( –e)φ+ d
+, (.)
φ d––φ=d ( –a)( –b)( –c)
( –d/q)( –d)( –e)φ+. (.)
These equations, and the symmetries of theφ, give us
c( –a)φ a+–φ=a( –c)φ c+–φ, (.)
a( –b)φ b+–φ=b( –a)φ a+–φ, (.)
d( –e/q)φ e––φ=e( –d/q)φ d––φ. (.) Now, applying the transformation (see [])
φ(a,b,c;d,e;q,q) =
(de/bc;q)n
(e;q)n
(bc/d)nφ(a,d/b,d/c;d,de/bc;q,q), (.)
toψ=φ(a,d/b,d/c;qd,de/bc;q,q) yields the following relations:
φ=(de/bc;q)n (e;q)n
(bc/d)nψ d–,
φ+=
(de/bc;q)n–
(qe;q)n–
(qbc/d)n–ψ a+,
φ+ a–
=(de/bc;q)n (qe;q)n
(qbc/d)nψ.
(.)
Thus, from (.), changingφintoψ, and using (.) we get
d( –a)
(qe;q)n–
(de/bc;q)n–
(d/qbc)n–φ+–
(qe;q)n
(de/bc;q)n
(d/qbc)nφ+ a–
–a( –d)
(e;q)n
(de/bc;q)n
(d/bc)nφ– (qe;q)n (de/bc;q)n
(d/qbc)nφ+ a–
= .
After some simplification this yields
a( –d)( –e)φ– (a–e)(a–d)φ+ a–
– ( –a)(qabc–de)φ+= . (.)
From the symmetries of theφ, we have
b( –d)( –e)φ– (b–e)(b–d)φ+ b–
– ( –b)(qabc–de)φ+= . (.)
Using (.), (.), and (.), we obtain the following contiguous relations:
ab(a–b)( –c)φ+b(a–e)(a–d)φ a––φ
–a(b–e)(b–d)φ b––φ= , (.)
qa( –b)( –c)φ+q(a–e)(a–d)φ a––φ
– ( –a)(qabc–de)φ a+–φ= , (.)
qb( –b)( –c)φ+q(b–e)(b–d)φ b––φ
– ( –b)(qabc–de)φ b+–φ= . (.)
Now, replacingbbyb/qin (.) andbbybqin (.) we get
(b–aq)φ b––φ+b( –a)φ–b( –a)φ a+,b–= , (.)
(a–qb)(ed–qabc)φ b+–φ+bq(a–e)(a–d)φ a–,b+
Hence, combining (.) and (.) yields the three term contiguous relation
In this section, we state and prove the reduction formula for theq-integralIn,qstated in
the introduction. We start with the following result.
Denoting theq-integral in the left-hand-side of (.) byJn, we obtain
Substituting (.) into (.), using (.), yields
In,q=
Using the transformation (.) yields the required result and completes the proof.
Corollary . Ifγ = then In,q vanishes for all values of n where n–β –δ andβ are
wherem,mare arbitrary nonnegative integers (see []), the proof follows directly from
Watson remarkedInvanishes for odd values ofnin two special cases, (i)α=γandβ=δ
and (ii)α=βandγ =δ.
Now, we can derive the reduction formula forIn,q.
Theorem . The reduction formula satisfies a three term recurrence relations of In,q. More precisely,the following holds:
If
Wn=φ q–n,q–β–δ–α–γ+n–,q–β;q–β–δ,q–α–β;q,q
,
then
LnWn+–QnWn–+MnWn= , (.)
where
Ln= q–n–qθ q–n–qθ –qθ+n qθ+n–q–n
,
Qn= –q–n qθ+n–qθ qθ+n–qθ q–n–qθ+n+
,
Mn=qθ –q–n
q–n qθ–qθ+n+q(θ+n)++q(θ+n) q–n–q–β
– []qθ+n qθ+θ+q+θ+q+θ–n [] –q–n–qθ+q–n q–n–β–qθ +q qθ+n–q–n q+θ–β+qθ qθ+n+q–n+qθ+θ q–n+q(θ+n) + []qθ qθ–q–β q–n–qθ+n,
andθ= –α–β,θ= –δ–β,θ= –α–β–δ–γ – .
Proof This result follows by applying Proposition . and using equation (.) with
b=q–β–δ–α–γ+n–, c=q–β, d=q–β–δ and e=q–α–β.
Recall that the littleq-Jacobi polynomials, see [], are defined by
Pn(x;a,b;q) =φ q–n,abqn+;aq;q,qx
, (.)
and the formula
Pn(x;c,d;q) = n
k=
ak,nPk(x;a,b;q)
holds with
ak,n=Ckφ qk–n,cdqn+k+,aqk+;cqk+,abqk+;q,q
,
Ck= (–)kq
(q–n,aq,cdqn+;q)
k
(q,cq,abqk+;q)
k
.
Remark . In (.), if we takea=q–β–,b=q–α–,c=q–β–δ–andd=q–α–γ–, we get
a,n=SnIn,q. Thus, the littleq-Jacobi polynomials and theq-integralsIn,qare related in the
following way:
Pn(x;c,d;q) =
Sn In,q+
n
k=
ak,nPk(x;a,b;q).
Competing interests
The authors declare that they have no competing interests.
Authors’ contributions
The authors have made equal and significant contributions in writing this paper. They read and approved the final manuscript.
Author details
1Present address: Department of Mathematics, Faculty of Science, King Saud University, Riyadh, KSA.2Permanent address:
Department of Mathematics, Faculty of Science, Cairo University, Giza, Egypt.3Department of Natural and Engineering
Science, Faculty of Applied Studies and Community Service, King Saud University, Riyadh, KSA.
Acknowledgements
The authors would like to thank Prof. Mourad Ismail for pointing out the relation betweenIn,qand the littleq-Jacobi
polynomials. They are very grateful to the reviewers and editors for their suggestions and comments which improved final version of this paper. This research is supported by the DSFP program of the King Saud University in Riyadh through grant DSFP/MATH 01.
Received: 25 October 2015 Accepted: 13 March 2016
References
1. Watson, GN: A reduction formula. Proc. Glasgow Math. Assoc.2, 57-61 (1954)
2. Bailey, WN: Contiguous hypergeometric functions of the type3F2(1). Proc. Glasgow Math. Assoc.2, 62-65 (1954)
3. Annaby, MH, Mansour, ZS:q-Fractional Calculus and Equations, vol. 2056. Springer, Berlin (2012) 4. Rainville, ED: Special Functions. The MacMillan Company, New York (1960)
5. Andrews, GE, Askey, R, Roy, R: Special Functions. Cambridge University Press, Cambridge (1999) 6. Gasper, G, Rahman, M: Basic Hypergeometric Series. Cambridge University Press, Cambridge (2004) 7. Jackson, FH: The basic gamma function and elliptic functions. Proc. R. Soc. A76, 127-144 (1905) 8. Jackson, FH: Onq-definite integrals. Q. J. Pure and Appl. Math.41, 193-203 (1910)
9. Askey, R: Theq-gamma andq-beta functions. Appl. Anal.8(2), 125-141 (1979)
10. Wilson, JA: Hypergeometric series, recurrence relations and some orthogonal functions. Ph.D. diss., University of Wisconsin, Madison (1978)
11. Gupta, DP, Ismail, ME, Masson, DR: Contiguous relations, basic hypergeometric functions, and orthogonal polynomials. II. Associated bigq-Jacobi polynomials. J. Math. Anal. Appl.2, 477-497 (1992)
12. Gautschi, W: Computational aspects of three-term recurrence relations. SIAM Rev.9, 24-82 (1967)
13. Rakha, MA, Ibrahim, AK: On the contiguous relations of hypergeometric series. J. Comput. Appl. Math.192(2), 396-410 (2006)
14. Ismail, ME, Masson, DR: Generalized orthogonal and continued fractions. J. Approx. Theory83, 1-40 (1995) 15. Vid ¯unas, R: Contiguous relations of hypergeometric series. J. Math. Anal. Appl.135, 507-519 (2003)