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Singular Values of Products of Ginibre Random Matrices
Author(s) -
Witte N. S.,
Forrester P. J.
Publication year - 2017
Publication title -
studies in applied mathematics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 1.164
H-Index - 46
eISSN - 1467-9590
pISSN - 0022-2526
DOI - 10.1111/sapm.12147
Subject(s) - mathematics , biorthogonal system , resolvent , hypergeometric function , bessel function , singular value , nonlinear system , random matrix , singularity , singular solution , mathematical analysis , orthogonal polynomials , differential equation , hermite polynomials , eigenvalues and eigenvectors , physics , quantum mechanics , wavelet transform , artificial intelligence , computer science , wavelet
The squared singular values of the product of M complex Ginibre matrices form a biorthogonal ensemble, and thus their distribution is fully determined by a correlation kernel. The kernel permits a hard edge scaling to a form specified in terms of certain Meijer G‐functions, or equivalently hypergeometric functions0 F M , also referred to as hyper‐Bessel functions. In the case M = 1 , it is well known that the corresponding gap probability for no squared singular values in (0, s ) can be evaluated in terms of a solution of a particular sigma form of the Painlevé III' system. One approach to this result is a formalism due to Tracy and Widom, involving the reduction of a certain integrable system. Strahov has generalized this formalism to general M ≥ 1 , but has not exhibited its reduction. After detailing the necessary working in the case M = 1 , we consider the problem of reducing the 12 coupled differential equations in the case M = 2 to a single differential equation for the resolvent. An explicit fourth‐order nonlinear is found for general hard edge parameters. For a particular choice of parameters, evidence is given that this simplifies to a much simpler third‐order nonlinear equation. The small and large s asymptotics of the fourth‐order equation are discussed, as is a possible relationship of the M = 2 systems to so‐called four‐dimensional Painlevé‐type equations.