Abstract

We obtain an exact analytic expression for the average distribution, in the thermodynamic limit, of overlaps between two copies of the same random energy model (REM) at different temperatures. We quantify the non-self averaging effects and provide an exact approach to the computation of the fluctuations in the distribution of overlaps in the thermodynamic limit. We show that the overlap probabilities satisfy recurrence relations that generalise Ghirlanda–Guerra identities to two temperatures. We also analyse the two temperature REM using the replica method. The replica expressions for the overlap probabilities satisfy the same recurrence relations as the exact form. We show how a generalisation of Parisi’s replica symmetry breaking ansatz is consistent with our replica expressions. A crucial aspect to this generalisation is that we must allow for fluctuations in the replica block sizes even in the thermodynamic limit. This contrasts with the single temperature case where the extremal condition leads to a fixed block size in the thermodynamic limit. Finally, we analyse the fluctuations of the block sizes in our generalised Parisi ansatz and show that in general they may have a negative variance.

Highlights

  • Since replica symmetry breaking (RSB) was invented by Parisi, 40 years ago [1], it has been used in many different contexts and the subtle physical meaning of the scheme he used has been elucidated [2,3,4]

  • One of the achievements of Parisi’s theory of spin glasses was to predict that P(q) remains sample dependent even in the thermodynamic limit, and to allow the calculation of various averages and moments which characterize its sample to sample fluctuations [3, 4, 8, 9]

  • The Parisi ansatz is used in the single temperature case and we show how it can be generalised to two temperatures in the case of the random energy model (REM)

Read more

Summary

Introduction

Since replica symmetry breaking (RSB) was invented by Parisi, 40 years ago [1], it has been used in many different contexts and the subtle physical meaning of the scheme he used has been elucidated [2,3,4] (for reviews see [5] or [6]). There are models for which these multiple temperature overlaps do not vanish and the question of how the Parisi theory has to be modified in these cases is, to our knowledge, not fully understood (see for example the multi-p-spin models analysed in [12]) We attack this question in the simplest model which exhibits RSB, the random energy model (REM, see [13, 14]) which has the advantage of being open to both exact and replica analysis. This will allow us to propose a way to adapt Parisi’s scheme for the two temperature case, in order to be compatible with our exact results of section 2.

The direct calculation of the overlaps
The replica method
The REM at a single temperature
The REM at two temperatures
Parisi overlap matrices
Single temperature case
Two temperature case
When the numbers n and n of replicas become non integer
The generating function of μi and μi
Conclusion
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call