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Connecting Eigenvalue Rigidity with Polymer Geometry: Diffusive Transversal Fluctuations under Large Deviation

Probability 2019-02-26 v1 Mathematical Physics math.MP

Abstract

We consider the exactly solvable model of exponential directed last passage percolation on Z2\mathbb{Z}^2 in the large deviation regime. Conditional on the upper tail large deviation event Uδ:={Tn(4+δ)n}\mathcal{U}_{\delta}:=\{T_{n}\geq (4+\delta)n\} where TnT_{n} denotes the last passage time from (1,1)(1,1) to (n,n)(n,n), we study the geometry of the polymer/geodesic Γn\Gamma_{n}, i.e., the optimal path attaining TnT_{n}. We show that conditioning on Uδ\mathcal{U}_{\delta} changes the transversal fluctuation exponent from the characteristic 2/32/3 of the KPZ universality class to 1/21/2, i.e., conditionally, the smallest strip around the diagonal that contains Γn\Gamma_{n} has width n1/2+o(1)n^{1/2+o(1)} with high probability. This sharpens a result of Deuschel and Zeitouni (1999) who proved a o(n)o(n) bound on the transversal fluctuation in the context of Poissonian last passage percolation, and complements (Basu, Ganguly, Sly, 2017), where the transversal fluctuation was shown to be Θ(n)\Theta(n) in the lower tail large deviation event. Our proof exploits the correspondence between last passage times in the exponential LPP model and the largest eigenvalue of the Laguerre Unitary Ensemble (LUE) together with the determinantal structure of the spectrum of the latter. A key ingredient in our proof is a sharp refinement of the large deviation result for the largest eigenvalue (Sepp\"al\"ainen '98, Johansson '99), using rigidity properties of the spectrum, which could be of independent interest.

Keywords

Cite

@article{arxiv.1902.09510,
  title  = {Connecting Eigenvalue Rigidity with Polymer Geometry: Diffusive Transversal Fluctuations under Large Deviation},
  author = {Riddhipratim Basu and Shirshendu Ganguly},
  journal= {arXiv preprint arXiv:1902.09510},
  year   = {2019}
}

Comments

35 pages, 4 figures

R2 v1 2026-06-23T07:50:36.143Z