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Uniform sine-kernel determinant asymptotics, tail-side quantiles, and prolate eigenvalue bounds

Ahmadreza Azimifard

math.FAarXiv:2608.15808

Abstract

Let Sc=P(0,c)QP(0,c) be the one-dimensional sinc-kernel concentration operator, let Na(c)=\#n:λn(c)>a, and set L=((1-δ)/δ). We prove, uniformly for each fixed A>0, the tail-side quantile formula Nδ(c)=c+π-2 L(4π2c/ L)+OA( c+ L) for 6 L A c. It yields corresponding additive formulas for the lower half and full plunge, with main terms respectively π-2 L(4π2c/ L) and twice this quantity. An exact one-tail-coordinate selection gives, for fixed A>0, d1, and q∈(1/2,1), the one-sided tensor-product bound Λδ(c;d)π-2d cd-1 L(4π2c/ L)-OA,d,q(cd-1( c+ L)) for Ld,q L A c, where Ld,q=(q-(d-1)(e6+1)-1); the tensor content is nontrivial for d2. The analytic input is a signed growing-parameter sine-kernel determinant asymptotic: uniformly for 0ω A s, (I+(e2ω-1)Ks)=4ωs/π+2π-2ω2(4s)+2|G(1+iω/π)|2+OA((1+ω)42s/s), where G is the Barnes G-function. We prove this negative-coupling counterpart of the Bothner--Deift--Its--Krasovsky theorem by direct IIKS steepest descent. We also retain the uniform head-side results and use a two-way determinant reduction to obtain the moving-depth lower-half bridge bound with constant 1/(32π2); extending it to the deeper range uses Kulikov--Dam Larsen and may require a smaller constant. These counting formulas are additive. Their errors become uniformly relative when L tends uniformly to infinity; fixed thresholds are covered separately by Landau--Widom. A Lambert-W-1 formula is recorded only for the continuous main term, not for individual eigenvalues.

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