English

Integrable systems and effectivisation of Riemann theorem about domaims of the complex plane

Complex Variables 2007-05-23 v2 High Energy Physics - Theory Mathematical Physics Combinatorics math.MP Exactly Solvable and Integrable Systems

Abstract

Consider a closed analytic curve γ\gamma in the complex plane and denote by > D+D_+ and DD_- the interior and exterior domains with respect to the curve. The point z=0z=0 is assumed to be in D+D_+. Then according to Riemann theorem there exists a function w(z)=1rz+j=0pjzjw(z)=\frac 1r z+\sum_{j=0}^\infty p_j z^{-j}, mapping DD_- to the exterior of the unit disk {wCw>1}\{w\in C|| w | >1\}. It is follow from [arXiv : hep-th /0005259] that this function is described by formula logw=logzt0(12t0+k1zkktk)v\log w=\log z-\partial_{t_0} (\frac 12\partial_{t_0}+\sum\limits_{k\geqslant 1}\frac{z^{-k}}{k} \partial_{t_k})v, where v=v(t0,t1,tˉ1,t2,tˉ2,...)v=v(t_0, t_1, \bar t_1, t_2, \bar t_2,...) is a function from the area t0t_0 of D+D_+ and the momemts tkt_k of DD_-. Moreover, this function satisfies the dispersionless Hirota equation for 2D Toda lattice hierarchy. Thus for an effectivisation of Riemann theorem it is sufficiently to find a representation of vv in the form of Taylor series v=N(i0i1,...,ikiˉ1,...,iˉkˉ)t0ti1,...,tktˉiˉ1,...,tˉiˉkˉv=\sum N(i_0 | i_1,...,i_k| \bar i_1,...,\bar i_{\bar k})t_0 t_{i_1},...,t_k \bar t_{\bar i_1},...,\bar t_{\bar i_{\bar k}}. The numbers N(i0i1,...,ikiˉ1,...,iˉkˉ)N(i_0 | i_1,...,i_k | \bar i_1, ..., \bar i_{\bar k}) for iα,iˉβ2i_\alpha, \bar i_\beta\leqslant 2 is found in [arXiv: hep-th/0005259]. In this paper we find some recurrence relations that give a possible to find all N(i0i1,...,ikiˉ1,...,iˉkˉ)N(i_0\bigl| i_1,...,i_k|\bar i_1,...,\bar i_{\bar k}).

Keywords

Cite

@article{arxiv.math/0103136,
  title  = {Integrable systems and effectivisation of Riemann theorem about domaims of the complex plane},
  author = {S. M. Natanzon},
  journal= {arXiv preprint arXiv:math/0103136},
  year   = {2007}
}

Comments

9 pages, AmsTex