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17 q-Hypergeometric and Related FunctionsProperties

Β§17.8 Special Cases of {{}_{r}\psi_{r}} Functions

Jacobi’s Triple Product

17.8.1 \sum_{n=-\infty}^{\infty}(-z)^{n}q^{n(n-1)/2}=\left(q,z,q/z;q\right)_{\infty};

compare (20.5.9).

Analytic Continuation

Note that for the equations below, the constraints are included to guarantee that the infinite series representation (17.4.3) of the {{}_{r}\psi_{r}} functions converges. These equations can also be used as analytic continuation of these {{}_{r}\psi_{r}} functions.

Ramanujan’s {{}_{1}\psi_{1}} Summation

17.8.2 {{}_{1}\psi_{1}}\left({a\atop b};q,z\right)=\frac{\left(q,b/a,az,q/(az);q%
\right)_{\infty}}{\left(b,q/a,z,b/(az);q\right)_{\infty}},\left|b/a\right|<\left|z\right|<1.

Quintuple Product Identity

Apart from Jacobi’s triple product identity (17.8.1) and the quintuple product identity (17.8.3) (see Cooper (2006) for a review), there also exist higher-order tuple product identities. One may see Pascadi (2021) for discussions and derivations of sextuple, septuple, octuple, nonuple and undecuple product identities. These identities are all given in terms of sums and products of basic bilateral hypergeometric series.

Bailey’s Bilateral Summations

17.8.4 {{}_{2}\psi_{2}}\left(b,c;aq/b,aq/c;q,-aq/(bc)\right)=\frac{\left(aq/(bc);q%
\right)_{\infty}\left(aq^{2}/b^{2},aq^{2}/c^{2},q^{2},aq,q/a;q^{2}\right)_{%
\infty}}{\left(aq/b,aq/c,q/b,q/c,-aq/(bc);q\right)_{\infty}},\left|qa\right|<\left|bc\right|,
17.8.5 {{}_{3}\psi_{3}}\left({b,c,d\atop q/b,q/c,q/d};q,\frac{q}{bcd}\right)=\frac{%
\left(q,q/(bc),q/(bd),q/(cd);q\right)_{\infty}}{\left(q/b,q/c,q/d,q/(bcd);q%
\right)_{\infty}},\left|q\right|<\left|bcd\right|,
17.8.6 {{}_{4}\psi_{4}}\left({-qa^{\frac{1}{2}},b,c,d\atop-a^{\frac{1}{2}},aq/b,aq/c,%
aq/d};q,\frac{qa^{\frac{3}{2}}}{bcd}\right)=\frac{\left(aq,aq/(bc),aq/(bd),aq/%
(cd),qa^{\frac{1}{2}}/b,qa^{\frac{1}{2}}/c,qa^{\frac{1}{2}}/d,q,q/a;q\right)_{%
\infty}}{\left(aq/b,aq/c,aq/d,q/b,q/c,q/d,qa^{\frac{1}{2}},qa^{-\frac{1}{2}},%
qa^{\frac{3}{2}}/(bcd);q\right)_{\infty}},\left|qa^{\frac{3}{2}}\right|<\left|bcd\right|,
17.8.7 {{}_{6}\psi_{6}}\left({qa^{\frac{1}{2}},-qa^{\frac{1}{2}},b,c,d,e\atop a^{%
\frac{1}{2}},-a^{\frac{1}{2}},aq/b,aq/c,aq/d,aq/e};q,\frac{qa^{2}}{bcde}\right%
)=\frac{\left(aq,aq/(bc),aq/(bd),aq/(be),aq/(cd),aq/(ce),aq/(de),q,q/a;q\right%
)_{\infty}}{\left(aq/b,aq/c,aq/d,aq/e,q/b,q/c,q/d,q/e,qa^{2}/(bcde);q\right)_{%
\infty}},\left|qa^{2}\right|<\left|bcde\right|.

Sum Related to (17.6.4)

17.8.8 {{}_{2}\psi_{2}}\left({b^{2},\ifrac{b^{2}}{c}\atop q,cq};q^{2},\ifrac{cq^{2}}{%
b^{2}}\right)=\frac{1}{2}\frac{\left(q^{2},qb^{2},\ifrac{q}{b^{2}},\ifrac{cq}{%
b^{2}};q^{2}\right)_{\infty}}{\left(cq,\ifrac{cq^{2}}{b^{2}},\ifrac{q^{2}}{b^{%
2}},\ifrac{c}{b^{2}};q^{2}\right)_{\infty}}\left(\frac{\left(\ifrac{c\sqrt{q}}%
{b};q\right)_{\infty}}{\left(b\sqrt{q};q\right)_{\infty}}+\frac{\left(\ifrac{-%
c\sqrt{q}}{b};q\right)_{\infty}}{\left(-b\sqrt{q};q\right)_{\infty}}\right),\left|cq^{2}\right|<\left|b^{2}\right|.

For similar formulas see Verma and Jain (1983).