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Dynamics of Modular Matings

Abstract

In the paper 'Mating quadratic maps with the modular group II' the current authors proved that each member of the family of holomorphic (2:2)(2:2) correspondences Fa\mathcal{F}_a: (az+1z+1)2+(az+1z+1)(awβˆ’1wβˆ’1)+(awβˆ’1wβˆ’1)2=3,\left(\frac{az+1}{z+1}\right)^2+\left(\frac{az+1}{z+1}\right)\left(\frac{aw-1}{w-1}\right) +\left(\frac{aw-1}{w-1}\right)^2=3, introduced by the first author and C. Penrose in 'Mating quadratic maps with the modular group', is a mating between the modular group and a member of the parabolic family of quadratic rational maps PA:zβ†’z+1/z+AP_A:z\to z+1/z+A whenever the limit set of Fa\mathcal{F}_a is connected. Here we provide a dynamical description for the correspondences Fa\mathcal{F}_a which parallels the Douady and Hubbard description for quadratic polynomials. We define a B\"ottcher map and a Green's function for Fa\mathcal{F}_a, and we show how in this setting periodic geodesics play the role played by external rays for quadratic polynomials. Finally, we prove a Yoccoz inequality which implies that for the parameter aa to be in the connectedness locus MΞ“M_{\Gamma} of the family Fa\mathcal{F}_a, the value of the log-multiplier of an alpha fixed point which has combinatorial rotation number 1/q1/q lies in a strip whose width goes to zero at rate proportional to (log⁑q)/q2(\log q)/q^2

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