2015
DOI: 10.1088/1751-8113/48/24/245202
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The smallest eigenvalue distribution in the real Wishart–Laguerre ensemble with even topology

Abstract: Abstract. We consider rectangular random matrices of size p × n belonging to the real Wishart-Laguerre ensemble also known as the chiral Gaussian orthogonal ensemble. This ensemble appears in many applications like QCD, mesoscopic physics, and time series analysis. We are particularly interested in the distribution of the smallest non-zero eigenvalue and the gap probability to find no eigenvalue in an interval [0, t]. While for odd topology ν = n − p explicit closed results are known for finite and infinite ma… Show more

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Cited by 10 publications
(15 citation statements)
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“…At the same time, for β = 1 a half-integer power in the denominator is involved. To deal with the latter challenge we employ one of very few techniques available in that case, the so-called supersymmetry approach, see [51,32] for concise introductions and also [23,50] for earlier computations involving half-integer powers of characteristic polynomials for real symmetric Gaussian random matrices. We find it convenient to use a (rigorous) variant of the approach proposed originally in [14] and the final expression for D (2) N,1 (λ, p) is given in (3.11) or (3.27).…”
Section: Discussion Of the Methods And Open Problemsmentioning
confidence: 99%
“…At the same time, for β = 1 a half-integer power in the denominator is involved. To deal with the latter challenge we employ one of very few techniques available in that case, the so-called supersymmetry approach, see [51,32] for concise introductions and also [23,50] for earlier computations involving half-integer powers of characteristic polynomials for real symmetric Gaussian random matrices. We find it convenient to use a (rigorous) variant of the approach proposed originally in [14] and the final expression for D (2) N,1 (λ, p) is given in (3.11) or (3.27).…”
Section: Discussion Of the Methods And Open Problemsmentioning
confidence: 99%
“…For any specific N, P the probability distribution of the smallest eigenvalue in the Wishart ensemble can be calculated (either recursively [81,82] or directly [83]). When P − N is held fixed as N tends to infinity, the asymptotics of its mean satisfy λ min (Q Q ) ∼ 1/N as N → ∞, hence the name "hard edge" statistics, as the smallest eigenvalue approaches the constraint that the matrix is positive definite.…”
Section: Unit Metricmentioning
confidence: 99%
“…10 This coincidence should also occur for higher-order correlation functions and the smallest singular-value distribution P (λ min ). The latter was analytically computed for chGOE by various authors [89][90][91][92][93][94]. In the case of QCD, a quantitative agreement between the Dirac spectrum in QCD and the prediction of RMT for ρ(λ) and P (λ min ) has been firmly established through Monte Carlo simulations [95] (see [96,97] for reviews).…”
Section: Random Matrix Theorymentioning
confidence: 94%