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On the Lax pairs of the sixth Painleve' equation

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arxiv nlin/0701049 v1 pith:LL6O6RGI submitted 2007-01-24 nlin.SI

classification nlin.SI
keywords thetadependenceequationholomorphicinftyorderpainlevepair
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abstract

The dependence of the sixth equation of Painleve' on its four parameters $(2 \alpha,-2 \beta,2 \gamma,1-2 \delta) =(\theta_{\infty}^2,\theta_{0}^2,\theta_{1}^2,\theta_{x}^2)$ is holomorphic, therefore one expects all its Lax pairs to display such a dependence. This is indeed the case of the second order scalar ``Lax'' pair of Fuchs, but the second order matrix Lax pair of Jimbo and Miwa presents a meromorphic dependence on $\theta_\infty$ (and a holomorphic dependence on the three other $\theta_j$). We analyze the reason for this feature and make suggestions to suppress it.

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Cited by 1 Pith paper

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  1. Geometry of the Ising persistence problem and the universal Bonnet-Manin Painlev\'e VI distribution

    math-ph 2026-03 conditional novelty 7.0 of 10

    The full persistence distribution in 1D Ising coarsening equals a Pfaffian Fredholm determinant of the sech kernel and is controlled by a Painlevé VI equation that is the mean curvature of a Bonnet surface.

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