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Related papers: On Painleve VI transcendents related to the Dirac …

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Correlation functions for holonomic fields on the Poincare' disk are analyzed. The two point functions are shown to be expressible in terms of Painleve' functions of type VI.

High Energy Physics - Theory · Physics 2009-07-11 John Palmer , Morris Beatty , Craig A. Tracy

A result from Palmer, Beatty and Tracy suggests that the two-point function of certain spinless scaling fields in a free Dirac theory on the Poincare disk can be described in terms of Painleve VI transcendents. We complete and verify this…

High Energy Physics - Theory · Physics 2015-06-26 Benjamin Doyon

We study a Fredholm determinant of the hypergeometric kernel arising in the representation theory of the infinite-dimensional unitary group. It is shown that this determinant coincides with the Palmer-Beatty-Tracy tau function of a Dirac…

Mathematical Physics · Physics 2011-03-25 O. Lisovyy

Painleve's transcendental differential equation P_{VI} may be expressed as the consistency condition for a pair of linear differential equations with 2 by 2 matrix coefficients with rational entries. By a construction due to Tracy and…

Functional Analysis · Mathematics 2024-09-24 Gordon Blower

We represent and analyze the general solution of the sixth Painleve transcendent in the Picard-Hitchin-Okamoto class in the Painleve form as the logarithmic derivative of the ratio of certain $\tau$-functions. These functions are…

Classical Analysis and ODEs · Mathematics 2010-11-18 Yurii V. Brezhnev

The goal of the present paper is to calculate the determinant of the Dirac operator with a mass in the cylindrical geometry. The domain of this operator consists of functions that realize a unitary one-dimensional representation of the…

High Energy Physics - Theory · Physics 2009-11-10 O. Lisovyy

We prove that certain polynomials previously introduced by the author can be identified with tau functions of Painlev\'e VI, obtained from one of Picard's algebraic solutions by acting with a four-dimensional lattice of B\"acklund…

Mathematical Physics · Physics 2014-06-16 Hjalmar Rosengren

The Painlev\'e transcendents $P_{\rom{I}}$--$P_{\rom{V}}$ and their representations as isomonodromic deformation equations are derived as nonautonomous Hamiltonian systems from the classical $R$--matrix Poisson bracket structure on the dual…

High Energy Physics - Theory · Physics 2009-10-28 J. Harnad , M. Routhier

Equivalence is established between a special class of Painleve VI equations parametrized by a conformal dimension $\mu$, time dependent Euler top equations, isomonodromic deformations and three-dimensional Frobenius manifolds. The…

Exactly Solvable and Integrable Systems · Physics 2007-05-23 Henrik Aratyn , Johan van de Leur

We prove a Fredholm determinant and short-distance series representation of the Painlev\'e V tau function $\tau(t)$ associated to generic monodromy data. Using a relation of $\tau(t)$ to two different types of irregular $c=1$ Virasoro…

Mathematical Physics · Physics 2018-10-10 O. Lisovyy , H. Nagoya , J. Roussillon

The isomonodromic deformations underlying the Painlev\'e transcendants are interpreted as nonautonomous Hamiltonian systems in the dual $\gR^*$ of a loop algebra $\tilde\grg$ in the classical $R$-matrix framework. It is shown how canonical…

High Energy Physics - Theory · Physics 2008-02-03 J. Harnad , M. -A. Wisse

In this paper, we analyze the asymptotic behaviour of the poles of certain rational solutions of the fifth Painlev\'e equation. These solutions are constructed by relating the corresponding tau function to a Hankel determinant of a certain…

Exactly Solvable and Integrable Systems · Physics 2025-11-18 Malik Balogoun , Marco Bertola

We study the global analytic properties of the solutions of a particular family of Painleve' VI equations with the parameters $\beta=\gamma=0$, $\delta={1\over2}$ and $\alpha$ arbitrary. We introduce a class of solutions having critical…

Algebraic Geometry · Mathematics 2007-05-23 B. Dubrovin , M. Mazzocco

We reformulate the $q$-difference linear system corresponding to the $q$-Painlev\'e equation of type $A_7^{(1)'}$ as a Riemann-Hilbert problem on a circle. Then, we consider the Fredholm determinant built from the jump of this…

Mathematical Physics · Physics 2025-01-03 Pavlo Gavrylenko

In this paper we obtain explicit expressions for tau-functions related to Picard type solutions of the Painlev\'e VI equation in terms of theta functions and their derivatives.

Classical Analysis and ODEs · Mathematics 2010-02-12 Vladimir V. Mangazeev

We use the $\zeta$-function regularization and an integral representation of the complex power of a pseudo differential operator, to give an unambiguous definition of the determinant of the Dirac operator. We bring this definition to a…

High Energy Physics - Theory · Physics 2009-10-28 L. L. Salcedo , E. Ruiz Arriola

For smooth hyperbolic dynamical systems and smooth weights, we relate Ruelle transfer operators with dynamical Fredholm determinants and dynamical zeta functions: First, we establish bounds for the essential spectral radii of the transfer…

Dynamical Systems · Mathematics 2008-01-17 Viviane Baladi , Masato Tsujii

An ergodic study of Painleve VI is developed. The chaotic nature of its Poincare return map is established for almost all loops. The exponential growth of the numbers of periodic solutions is also shown. Principal ingredients of the…

Algebraic Geometry · Mathematics 2007-05-23 Katsunori Iwasaki , Takato Uehara

Generic c=1 four-point conformal blocks on the Riemann sphere can be seen as the coefficients of Fourier expansion of the tau function of Painlev\'e VI equation with respect to one of its integration constants. Based on this relation, we…

High Energy Physics - Theory · Physics 2013-12-19 N. Iorgov , O. Lisovyy , Yu. Tykhyy

We introduce certain B\"acklund transformations for rational solutions of the Painlev\'e VI equation. These transformations act ona family of Painlev\'e VI tau functions. They are obtained from reducing the Hirota bilinear equations that…

Mathematical Physics · Physics 2012-08-23 Henrik Aratyn , Johan van de Leur
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