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Mathematics > Probability

Title: Hidden temperature in the KMP model

Abstract: In the KMP model a positive energy $\zeta_i$ is associated with each site $i\in\{0,\frac1n,\dots,\frac{n-1}{n},1\}$. When a Poisson clock rings at the bond $ij$ with energies $\zeta_i,\zeta_j$, those values are substituted by $U(\zeta_i+\zeta_j)$ and $(1-U)(\zeta_i+\zeta_j)$, respectively, where $U$ is a uniform random variable in $(0,1)$. The boundary dynamics is defined in such way that the resulting Markov process $\zeta(t)$, with boundary conditions $T_0,T_{1}$, satisfies that $\zeta_b(t)$ is exponential with mean $T_b$, for $b=0,1$, for all $t$. We show that the invariant measure is the distribution of a vector $\zeta$ with coordinates $\zeta_i=T_iX_i$, where $X_{k/n}$ are iid exponential$(1)$ random variables, the law of $T$ is the invariant measure for an opinion model with the same boundary conditions, and $X,T$ are independent. The result confirms a conjecture based on the large deviations of the model. The discrete derivative of the opinion model behaves as a neural spiking process, which is also analysed. The hydrostatic limit shows that the empirical measure of a configuration chosen with the invariant measure converges to the lineal interpolation of $T_0$ and $T_{1}$.
Comments: 29 pages, 4 figures
Subjects: Probability (math.PR); Statistical Mechanics (cond-mat.stat-mech)
MSC classes: 37B15, 37K40, 60C05
Cite as: arXiv:2310.01672 [math.PR]
  (or arXiv:2310.01672v1 [math.PR] for this version)

Submission history

From: Pablo A. Ferrari [view email]
[v1] Mon, 2 Oct 2023 22:02:59 GMT (81kb,D)

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