ASEPsc particle-position Tracy–Widom GOE conjecture

From papers

Let XNASEPsc(t)X_N^{{\rm ASEPsc}}(t) be the position of particle NN in ASEPsc with flat initial condition, and use the functions J(β,E)J(\beta,E) and Γ(β,E)\Gamma(\beta,E) defined by the model parameters. Define

XNresc(t)=XNASEPsc(t)XNASEPsc(0)2J(β,E)t2Γ(β,E)1/3t1/3.X^{\rm resc}_N(t)=\frac{X_N^{{\rm ASEPsc}}(t)-X_N^{{\rm ASEPsc}}(0)-2J(\beta,E)t}{-2\Gamma(\beta,E)^{1/3}t^{1/3}}.

ASEPsc particle-position conjecture. For any NZN\in\mathbb{Z} and every sRs\in\mathbb{R},

limtP(XNresc(t)s)=FGOE(2s),\lim_{t\to\infty}\mathbb{P}\left(X^{\rm resc}_N(t)\le s\right)=F_{\rm GOE}(2s),

where FGOEF_{\rm GOE} is the Tracy–Widom GOE distribution. This predicts the GOE fluctuation law for particle positions in ASEPsc under KPZ t1/3t^{1/3} scaling; the source does not state that it has been proved.

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Sources & referencesView supporting material

Primary source

Patrik L. Ferrari and Min Liu, “Quasi-geodesics in integrable and non-integrable exclusion processes”, arXiv:2412.11626 (2024).

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