T-4: Difference between revisions
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=== RSB and the free-entry landscape === | === RSB and the free-entry landscape === | ||
We have seen | We have seen an example of mean-field model, the spherical p-spin, in which the low-T phase is glassy, described by a 1-RSB ansatz of the overlap matrix. The thermodynamics in the glassy phase is described by three quantities: the typical overlap <math> q_1^{SP} </math> between configurations belonging to the same pure state, the typical overlap <math> q_0^{SP} </math> between configurations belonging to different pure states, and the probability <math> (1-m^{SP}) </math> that two configurations extracted at equilibrium belong to the same state. It can be shown that the low-T, frozen phase of the REM is also described by this 1-RSB ansatz with <math> q_0^{SP}=0, q_1^{SP}=1</math> and <math> m^{SP}=T/T_c </math>. |
Revision as of 16:43, 24 December 2023
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RSB and the free-entry landscape
We have seen an example of mean-field model, the spherical p-spin, in which the low-T phase is glassy, described by a 1-RSB ansatz of the overlap matrix. The thermodynamics in the glassy phase is described by three quantities: the typical overlap between configurations belonging to the same pure state, the typical overlap between configurations belonging to different pure states, and the probability that two configurations extracted at equilibrium belong to the same state. It can be shown that the low-T, frozen phase of the REM is also described by this 1-RSB ansatz with and .