Complex BBM phase-diagram conjecture

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Let β=σ+iτC\beta=\sigma+i\tau\in\mathbb C, let ρ[1,1]\rho\in[-1,1], and let pt(β)p_t(\beta) be the log-partition function per unit time for the complex BBM energy model. Let B1,B2,B3B_1,B_2,B_3 denote the three regions of the complex REM phase diagram. Complex BBM phase-diagram conjecture. For every ρ[1,1]\rho\in[-1,1], the complex BBM energy model has the same free energy and phase diagram as the complex REM:

limtpt(β)=:p(β)={1+12(σ2τ2),βB1,2σ,βB2,12+σ2,βB3,\lim_{t\uparrow\infty}p_t(\beta)=:p(\beta)=\begin{cases}1+\frac{1}{2}(\sigma^2-\tau^2),&\beta\in\overline{B_1},\sqrt{2}|\sigma|,&\beta\in\overline{B_2},\frac{1}{2}+\sigma^2,&\beta\in\overline{B_3},\end{cases}

and the convergence holds in probability and in L1L^1. This conjecture asserts that correlations parametrized by ρ\rho do not change the limiting free energy or phase boundaries from those of the complex REM.

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Primary source

Lisa Hartung and Anton Klimovsky, “The glassy phase of the complex branching Brownian motion energy model”, arXiv:1504.05097 (2015).

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