### Abstract

We compute the probability distribution of the number of metastable states at a given applied field in the mean-field random-field Ising model at T = 0. Remarkably, there is a non-zero probability in the thermodynamic limit of observing metastable states on the so-called 'unstable' branch of the magnetization curve. This implies that the branch can be reached when the magnetization is controlled instead of the magnetic field, in contrast to the situation for the pure system.

Original language | English |
---|---|

Article number | P10004 |

Number of pages | 10 |

Journal | Journal of statistical mechanics-Theory and experiment |

Volume | 2008 |

DOIs | |

Publication status | Published - Oct 2008 |

### Keywords

- energy landsacpes (theory)
- disordered systems (theory)
- classical phase transitions theory
- metastable states

### Cite this

*Journal of statistical mechanics-Theory and experiment*,

*2008*, [P10004]. https://doi.org/10.1088/1742-5468/2008/10/P10004

**Stable, metastable and unstable states in the mean-field random-field Ising model at T=0.** / Rosinberg, M. L.; Tarjus, G.; Perez-Reche, F. J.

Research output: Contribution to journal › Article

*Journal of statistical mechanics-Theory and experiment*, vol. 2008, P10004. https://doi.org/10.1088/1742-5468/2008/10/P10004

}

TY - JOUR

T1 - Stable, metastable and unstable states in the mean-field random-field Ising model at T=0

AU - Rosinberg, M. L.

AU - Tarjus, G.

AU - Perez-Reche, F. J.

PY - 2008/10

Y1 - 2008/10

N2 - We compute the probability distribution of the number of metastable states at a given applied field in the mean-field random-field Ising model at T = 0. Remarkably, there is a non-zero probability in the thermodynamic limit of observing metastable states on the so-called 'unstable' branch of the magnetization curve. This implies that the branch can be reached when the magnetization is controlled instead of the magnetic field, in contrast to the situation for the pure system.

AB - We compute the probability distribution of the number of metastable states at a given applied field in the mean-field random-field Ising model at T = 0. Remarkably, there is a non-zero probability in the thermodynamic limit of observing metastable states on the so-called 'unstable' branch of the magnetization curve. This implies that the branch can be reached when the magnetization is controlled instead of the magnetic field, in contrast to the situation for the pure system.

KW - energy landsacpes (theory)

KW - disordered systems (theory)

KW - classical phase transitions theory

KW - metastable states

U2 - 10.1088/1742-5468/2008/10/P10004

DO - 10.1088/1742-5468/2008/10/P10004

M3 - Article

VL - 2008

JO - Journal of statistical mechanics-Theory and experiment

JF - Journal of statistical mechanics-Theory and experiment

SN - 1742-5468

M1 - P10004

ER -