We investigate the totally asymmetric exclusion process on Z, with the jump rate at site i given by ri = 1 for i 6= 0, r0 = r. It is easy to see that the maximal stationary current j(r) is nondecreasing in r and that j(r) = 1/4 for r ≥ 1; it is a long outstanding problem to determine whether or not the critical value rc of r such that j(r) = 1/4 for r > rc is strictly less than 1. Here we present a heuristic argument, based on the analysis of the first sixteen terms in a formal power series expansion of j(r) obtained from finite volume systems, that rc = 1 and that for r / 1, j(r) ≃ 1/4 − γ exp[−a/(1 − r)] with a ≈ 2. We also give some new exact results about this system; in particular we prove that j(r) = Jmax(r), with Jmax(r) the hydrodynamic maximal current defined by Sepp¨al¨ainen, and thus establish continuity of j(r). Finally we describe a related exactly solvable model, a semi-infinite system in which the site i = 0 is always occupied. For that system, r s-i c = 1/2 and the analogue j s-i(r) of j(r) satisfies j s-i(r) = r(1 − r) for r ≤ r s-i c ; j s-i(r) is the limit of finite volume currents inside the curve |r(1 − r)| = 1/4 in the complex r plane and we suggest that analogous behavior may hold for the original system.
The blockage problem
A. Troiani
2013
Abstract
We investigate the totally asymmetric exclusion process on Z, with the jump rate at site i given by ri = 1 for i 6= 0, r0 = r. It is easy to see that the maximal stationary current j(r) is nondecreasing in r and that j(r) = 1/4 for r ≥ 1; it is a long outstanding problem to determine whether or not the critical value rc of r such that j(r) = 1/4 for r > rc is strictly less than 1. Here we present a heuristic argument, based on the analysis of the first sixteen terms in a formal power series expansion of j(r) obtained from finite volume systems, that rc = 1 and that for r / 1, j(r) ≃ 1/4 − γ exp[−a/(1 − r)] with a ≈ 2. We also give some new exact results about this system; in particular we prove that j(r) = Jmax(r), with Jmax(r) the hydrodynamic maximal current defined by Sepp¨al¨ainen, and thus establish continuity of j(r). Finally we describe a related exactly solvable model, a semi-infinite system in which the site i = 0 is always occupied. For that system, r s-i c = 1/2 and the analogue j s-i(r) of j(r) satisfies j s-i(r) = r(1 − r) for r ≤ r s-i c ; j s-i(r) is the limit of finite volume currents inside the curve |r(1 − r)| = 1/4 in the complex r plane and we suggest that analogous behavior may hold for the original system.I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.