On germs of constriction curves in model of overdamped Josephson junction, dynamical isomonodromic foliation and Painlev\'e 3 equation

Abstract

B.Josephson (Nobel Prize, 1973) predicted tunnelling effect for a system (called Josephson junction) of two superconductors separated by a narrow dielectric: existence of a supercurrent through it and equations governing it. The overdamped Josephson junction is modeled by a family of differential equations on 2-torus depending on 3 parameters: BB, AA, Ο‰\omega. We study its rotation number ρ(B,A;Ο‰)\rho(B,A;\omega) as a function of parameters. The three-dimensional phase-lock areas are the level sets Lr:={ρ=r}L_r:=\{\rho=r\} with non-empty interiors; they exist for r∈Zr\in\mathbb Z (Buchstaber, Karpov, Tertychnyi). For every fixed Ο‰>0\omega>0 and r∈Zr\in\mathbb Z the planar slice Lr∩(RB,A2Γ—{Ο‰})L_r\cap(\mathbb R^2_{B,A}\times\{\omega\}) is a garland of domains going vertically to infinity and separated by points; those separating points for which Aβ‰ 0A\neq0 are called constrictions. In a joint paper by Yu.Bibilo and the author, it was shown that 1) at each constriction the rescaled abscissa β„“:=BΟ‰\ell:=\frac B\omega is equal to ρ\rho; 2) the family of constrictions with given β„“βˆˆZ\ell\in\mathbb Z is an analytic submanifold Constrβ„“Constr_\ell in (R+2)a,s(\mathbb R^2_+)_{a,s}, a=Ο‰βˆ’1a=\omega^{-1}, s=AΟ‰s=\frac A\omega. Here we show that the limit points of Constrβ„“Constr_\ell are Ξ²β„“,k=(0,sβ„“,k)\beta_{\ell,k}=(0,s_{\ell,k}), where sβ„“,k>0s_{\ell,k}>0 are zeros of the Bessel function Jβ„“(s)J_\ell(s), and it lands at them regularly. Known numerical pictures show that high components of Int(Lr)Int(L_r) look similar. In his paper with Bibilo, the author introduced a candidate to the self-similarity map between neighbor components: the Poincar\'e map of the dynamical isomonodromic foliation governed by Painlev\'e 3 equation. Whenever well-defined, it preserves ρ\rho. We show that the Poincar\'e map is well-defined on a neighborhood of the plane {a=0}βŠ‚Rβ„“,a2Γ—(R+)s\{ a=0\}\subset\mathbb R^2_{\ell,a}\times(\mathbb R_+)_s, and it sends Ξ²β„“,k\beta_{\ell,k} to Ξ²β„“,k+1\beta_{\ell,k+1} for integer β„“\ell.Comment: 41 page, 5 figure

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