Discrete Painlevé equations, Orthogonal Polynomials on the Unit Circle and $N$-recurrences for averages over U(N) -- \PVI $τ$-functions

Details Discrete Painlevé equations, Orthogonal Polynomials on the Unit Circle and $N$-recurrences for averages over U(N) -- \PVI $τ$-functions Discrete Painlevé equations, Orthogonal Polynomials on the Unit Circle and $N$-recurrences for averages over U(N) -- \PVI $τ$-functions

2003-08-28

arxiv.org/abs/math-ph/0308036v1

Physics

Mathematical Physics

46 pages, AMSLatex

Scientific paper

The theory of orthogonal polynomials on the unit circle is developed for a general class of weights leading to systems of recurrence relations and derivatives of the polynomials and their associated functions, and to functional-difference equations of certain coefficient functions appearing in the theory. A natural formulation of the Riemann-Hilbert problem is presented which has as its solution the above system of orthogonal polynomials and associated functions. In particular for the case of regular semi-classical weights on the unit circle $ w(z) = \prod^m_{j=1}(z-z_j(t))^{\rho_j} $, consisting of $ m \in \mathbb{Z}_{> 0} $ singularities, difference equations with respect to the orthogonal polynomial degree $ n $ (Laguerre-Freud equations) and differential equations with respect to the deformation variables $ z_j(t) $ (Schlesinger equations) are derived completely characterising the system. It is shown in the simplest non-trivial case of $ m=3 $ that quite generally and simply the difference equations are equivalent to the discrete Painlev\'e equation associated with the degeneration of the rational surface $ D^{(1)}_4 \to D^{(1)}_5 $ and no other. In a three way comparison with other methods employed on this problem - the Toeplitz lattice and Virasoro constraints, the isomonodromic deformation of $ 2\times 2 $ linear Fuchsian differential equations, and the algebraic approach based upon the affine Weyl group symmetry - it is shown all are entirely equivalent, when reduced in order by exact summation, to the above discrete Painlev\'e equation through explicit transformation formulae. The fundamental matrix integrals over the unitary group $ U(N) $ arising in the theory are given by the generalised hypergeometric function $ {{}^{\vphantom{(1)}}_2}F^{(1)}_1 $.

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