
In mathematics, basic hypergeometric series, or q-hypergeometric series, are q-analogue generalizations of generalized hypergeometric series, and are in turn generalized by elliptic hypergeometric series. A series xn is called hypergeometric if the ratio of successive terms xn+1/xn is a rational function of n. If the ratio of successive terms is a rational function of qn, then the series is called a basic hypergeometric series. The number q is called the base.
The basic hypergeometric series
{}2\phi
| \alpha | |
| 1(q |
,q\beta;q\gamma;q,x)
F(\alpha,\beta;\gamma;x)
q=1
There are two forms of basic hypergeometric series, the unilateral basic hypergeometric series φ, and the more general bilateral basic hypergeometric series ψ.The unilateral basic hypergeometric series is defined as
j\phik\left[\begin{matrix}a1&a2&\ldots&aj\ b1&b2&\ldots&bk\end{matrix};q,z\right]=
| infty | |
| \sum | |
| n=0 |
| (a1,a2,\ldots,aj;q)n | |
| (b1,b2,\ldots,bk,q;q)n |
\left((-1)nqn\choose\right)1+k-jzn
(a1,a2,\ldots,am;q)n=(a1;q)n(a2;q)n\ldots(am;q)n
(a;q)n=
| n-1 | |
| \prod | |
| k=0 |
(1-aqk)=(1-a)(1-aq)(1-aq2) … (1-aqn-1)
k+1\phik\left[\begin{matrix}a1&a2&\ldots&ak&ak+1\ b1&b2&\ldots&bk\end{matrix};q,z\right]=
| infty | |
| \sum | |
| n=0 |
| (a1,a2,\ldots,ak+1;q)n | |
| (b1,b2,\ldots,bk,q;q)n |
zn.
\limq\to j\phik\left[\begin{matrix}
| a1 | |
| q |
&
| a2 | |
| q |
&\ldots&
| aj | |
| q |
| b1 | |
| \ q |
&
| b2 | |
| q |
&\ldots&
| bk | |
| q |
\end{matrix};q,(q-1)1+k-jz\right]= jFk\left[\begin{matrix}a1&a2&\ldots&aj\ b1&b2&\ldots&bk\end{matrix};z\right]
j\psik\left[\begin{matrix}a1&a2&\ldots&aj\ b1&b2&\ldots&bk\end{matrix};q,z\right]=
| infty | |
| \sum | |
| n=-infty |
| (a1,a2,\ldots,aj;q)n | |
| (b1,b2,\ldots,bk;q)n |
\left((-1)nqn\choose\right)k-jzn.
The most important special case is when j = k, when it becomes
k\psik\left[\begin{matrix}a1&a2&\ldots&ak\ b1&b2&\ldots&bk\end{matrix};q,z\right]=
| infty | |
| \sum | |
| n=-infty |
| (a1,a2,\ldots,ak;q)n | |
| (b1,b2,\ldots,bk;q)n |
zn.
The unilateral series can be obtained as a special case of the bilateral one by setting one of the b variables equal to q, at least when none of the a variables is a power of q, as all the terms with n < 0 then vanish.
Some simple series expressions include
| z | |
| 1-q |
2\phi1\left[\begin{matrix}q q\ q2\end{matrix} ;q,z\right]=
| z | |
| 1-q |
+
| z2 | |
| 1-q2 |
+
| z3 | |
| 1-q3 |
+\ldots
and
| z | |
| 1-q1/2 |
2\phi1\left[\begin{matrix}q q1/2\ q3/2\end{matrix} ;q,z\right]=
| z | |
| 1-q1/2 |
+
| z2 | |
| 1-q3/2 |
+
| z3 | |
| 1-q5/2 |
+\ldots
and
2\phi1\left[\begin{matrix}q -1\ -q\end{matrix} ;q,z\right]=1+
| 2z | |
| 1+q |
+
| 2z2 | |
| 1+q2 |
+
| 2z3 | |
| 1+q3 |
+\ldots.
The q-binomial theorem (first published in 1811 by Heinrich August Rothe)[1] [2] states thatIt can be proved by repeatedly applying the identityWhen is a negative integer power of q, the hypergeometric sum is finite and one recovers the finite form of the q-binomial theorem (also sometimes known as the Cauchy binomial theorem).[3] Here is a q-binomial coefficient.
The special case of a = 0 is closely related to the q-exponential.
Srinivasa Ramanujan gave the identityvalid for |q| < 1 and |b/a| < |z| < 1. Similar identities for
6\psi6
| infty | |
| \sum | |
| n=-infty |
qn(n+1)/2zn=(q;q)infty (-1/z;q)infty (-zq;q)infty.
Gwynneth Coogan and Ken Ono give a related formal power series
A(z;q)\stackrel{\rm{def}}{=}
| 1 | |
| 1+z |
| infty | |
| \sum | |
| n=0 |
| (z;q)n | |
| (-zq;q)n |
zn=
| infty | |
| \sum | |
| n=0 |
(-1)nz2n
| n2 | |
| q |
.
As an analogue of the Barnes integral for the hypergeometric series, Watson showed that
{}2\phi1(a,b;c;q,z)=
| -1 | |
| 2\pii |
| (a,b;q)infty | |
| (q,c;q)infty |
| iinfty | |
| \int | |
| -iinfty |
| |||||||||||||
|
| \pi(-z)s | |
| \sin\pis |
ds
(aqs,bq
| s;q) | |
| infty |
The basic hypergeometric matrix function can be defined as follows:
{}2\phi1(A,B;C;q,z):=
| ||||
| \sum | ||||
| n=0 |
zn, (A;q)0:=1, (A;q)n:=\prod
| n-1 | |
| k=0 |
(1-Aqk).
1\psi1