Superimposing theta structure on a generalized modular relation

preprint2020arXivOpen access

Abstract

A generalized modular relation of the form F(z,w,α)=F(z,iw,β)F(z, w, α)=F(z, iw,β), where αβ=1αβ=1 and i=−1i=\sqrt{-1}, is obtained in the course of evaluating an integral involving the Riemann ΞΞ-function. It is a two-variable generalization of a transformation found on page 220220 of Ramanujan's Lost Notebook. This modular relation involves a surprising generalization of the Hurwitz zeta function ζ(s,a)ζ(s, a), which we denote by ζw(s,a)ζ_w(s, a). While ζw(s,1)ζ_w(s, 1) is essentially a product of confluent hypergeometric function and the Riemann zeta function, ζw(s,a)ζ_w(s, a) for 0<a<10<a<1 is an interesting new special function. We show that ζw(s,a)ζ_w(s, a) satisfies a beautiful theory generalizing that of ζ(s,a)ζ(s, a) albeit the properties of ζw(s,a)ζ_w(s, a) are much harder to derive than those of ζ(s,a)ζ(s, a). In particular, it is shown that for 0<a<10<a<1 and w∈Cw\in\mathbb{C}, ζw(s,a)ζ_w(s, a) can be analytically continued to Re(s)>−1(s)>-1 except for a simple pole at s=1s=1. This is done by obtaining a generalization of Hermite's formula in the context of ζw(s,a)ζ_w(s, a). The theory of functions reciprocal in the kernel sin⁡(πz)J2z(2xt)−cos⁡(πz)L2z(2xt)\sin(πz) J_{2 z}(2 \sqrt{xt}) -\cos(πz) L_{2 z}(2 \sqrt{xt}), where Lz(x)=−2πKz(x)−Yz(x)L_{z}(x)=-\frac{2}πK_{z}(x)-Y_{z}(x) and Jz(x),Yz(x)J_{z}(x), Y_{z}(x) and Kz(x)K_{z}(x) are the Bessel functions, is worked out. So is the theory of a new generalization of Kz(x)K_{z}(x), namely, 1Kz,w(x){}_1K_{z,w}(x). Both these theories as well as that of ζw(s,a)ζ_w(s, a) are essential to obtain the generalized modular relation.

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