2000
DOI: 10.1002/(sici)1097-0312(200006)53:6<736::aid-cpa2>3.0.co;2-5
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Generic behavior of the density of states in random matrix theory and equilibrium problems in the presence of real analytic external fields

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Cited by 112 publications
(156 citation statements)
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“…We require V to be such that the following generic conditions hold: the density ψ V is strictly positive on (a, b), it vanishes like a square root at the endpoints a, b (in other words, h(x) > 0 for x ∈ [a, b]), and the variational inequality (1.8) is strict on R\ [a, b]. If all those assumptions hold, we say that V is one-cut regular (see [26] for a general classification of singularities). In addition, we require zero to be contained in the interior of the support of µ V , i.e., a < 0 < b.…”
Section: Statement Of Resultsmentioning
confidence: 99%
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“…We require V to be such that the following generic conditions hold: the density ψ V is strictly positive on (a, b), it vanishes like a square root at the endpoints a, b (in other words, h(x) > 0 for x ∈ [a, b]), and the variational inequality (1.8) is strict on R\ [a, b]. If all those assumptions hold, we say that V is one-cut regular (see [26] for a general classification of singularities). In addition, we require zero to be contained in the interior of the support of µ V , i.e., a < 0 < b.…”
Section: Statement Of Resultsmentioning
confidence: 99%
“…As n → ∞ and simultaneously t → 0 in such a way that τ n,t → τ = 0, there exists a limiting kernel K PV α such that 26) for any u, v ∈ R if τ < 0, and for any u, v ∈ R\{± √ τ /4} if τ > 0.…”
mentioning
confidence: 99%
“…For unitarily invariant random matrix ensembles (1.16) the local correlations near edge points are expressed in the limit n → ∞ in terms of the Airy kernel 21) provided that the limiting mean eigenvalue density vanishes like a square root, which is generically the case [19]. In our non-unitarily invariant random matrix model, the limiting mean eigenvalue density vanishes like a square root, (1.12), and indeed we recover the kernel (1.21) in the limit n → ∞.…”
Section: Remarkmentioning
confidence: 99%
“…Consider the disk D(z 1 , r). In the regions I and IV, we have by (7.7), (8.1) and (8.6) 19) hence by (4.1), (7.14), and (7.15) By restricting equation (10.20) to the (1, 1) entry, and using the first expression of (7.13) (in region I) or the fourth expression of (7.13) (in region IV) to evaluate Φ(n 2/3 β(z)), and (6.16) to evaluate M(z), we obtain that P n (z)e − n 2 z 2 = √ π n 1/6 B(z)Ai(n 2/3 β(z))(1 + O(n −1 )) +n −1/6 C(z)Ai ′ (n 2/3 β(z))(1 + O(n −1 )) e −nα(z)+nl 1 , The same asymptotics, (10.22), holds in regions II and III as well. Thus, (10.22) holds in the full disk D(z 1 , r).…”
Section: Large N Asymptotics Of the Multiple Hermite Polynomialsmentioning
confidence: 99%
“…If one of these conditions is not valid, V s,t is called singular. The singular points x * are classified as follows, see [10,21]: (i) x * ∈ R \ S s,t is a type I singular point if equality in (1.9) holds. Then, x * is a zero of q + s,t of multiplicity 4m with m ∈ N.…”
Section: Unitary Random Matrix Ensemblesmentioning
confidence: 99%