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| Content Provider | Springer Nature Link |
|---|---|
| Author | Arndt, Peter F. Heinzel, Thomas Rittenberg, Vladimir |
| Copyright Year | 1998 |
| Abstract | The steady states of the two-species (positive and negative particles) asymmetric exclusion model of Evans, Foster, Godrèche, and Mukamel are studied using Monte Carlo simulations. We show that mean-field theory does not give the correct phase diagram. On the first-order phase transition line which separates the CP-symmetric phase from the broken phase, the density profiles can be understood through an unexpected pattern of shocks. In the broken phase the free energy functional is not a convex function, but looks like a standard Ginzburg–Landau picture. If a symmetry-breaking term is introduced in the boundaries, the Ginzburg–Landau picture remains and one obtains spinodal points. The spectrum of the Hamiltonian associated with the master equation was studied using numerical diagonalization. There are massless excitations on the first-order phase transition fine with a dynamical critical exponent z = 2, as expected from the existence of shocks, and at the spinodal points, where we find z = 1. It is the first time that this value, which characterizes conformal invariant equilibrium problems, appears in stochastic processes. |
| Starting Page | 783 |
| Ending Page | 815 |
| Page Count | 33 |
| File Format | |
| ISSN | 00224715 |
| Journal | Journal of Statistical Physics |
| Volume Number | 90 |
| Issue Number | 3-4 |
| e-ISSN | 15729613 |
| Language | English |
| Publisher | Kluwer Academic Publishers-Plenum Publishers |
| Publisher Date | 1998-01-01 |
| Publisher Place | New York |
| Access Restriction | One Nation One Subscription (ONOS) |
| Subject Keyword | Physical Chemistry Quantum Physics Mathematical and Computational Physics Statistical Physics |
| Content Type | Text |
| Resource Type | Article |
| Subject | Statistical and Nonlinear Physics Mathematical Physics |
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