Functional equations and Weierstrass sigma-functions
- Authors: Illarionov A.A.1
-
Affiliations:
- Khabarovsk Division of the Institute of Applied Mathematics, Far Eastern Branch of the Russian Academy of Sciences
- Issue: Vol 50, No 4 (2016)
- Pages: 281-290
- Section: Article
- URL: https://journals.rcsi.science/0016-2663/article/view/234241
- DOI: https://doi.org/10.1007/s10688-016-0159-7
- ID: 234241
Cite item
Abstract
It is proved that if an entire function f: ℂ → ℂ satisfies an equation of the form α1(x)β1(y) + α2(x)β2(y) + α3(x)β3(y), x,y ∈ C, for some αj, βj: ℂ → ℂ and there exist no \({\widetilde \alpha _j}\) and ˜\({\widetilde \beta _j}\) for which \(f\left( {x + y} \right)f\left( {x - y} \right) = {\overline \alpha _1}\left( x \right){\widetilde \beta _1}\left( y \right) + {\overline \alpha _2}\left( x \right){\widetilde \beta _2}\left( y \right)\), then f(z) = exp(Az2 + Bz + C) ∙ σΓ(z - z1) ∙ σΓ(z - z2), where Γ is a lattice in ℂ; σΓ is the Weierstrass sigma-function associated with Γ; A,B,C, z1, z2 ∈ ℂ; and \({z_1} - {z_2} \notin \left( {\frac{1}{2}\Gamma } \right)\backslash \Gamma \).
About the authors
A. A. Illarionov
Khabarovsk Division of the Institute of Applied Mathematics, Far Eastern Branch of the Russian Academy of Sciences
Author for correspondence.
Email: illar_a@list.ru
Russian Federation, Khabarovsk
Supplementary files
