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Glauber dynamics of the Sherrington--Kirkpatrick spin-glass model: a dynamical cavity method

Abstract

We present a closed theory, exact in the N→∞ limit, of the equilibrium spin correlations of the Sherrington--Kirkpatrick spin-glass model evolving with Glauber dynamics, above and at the transition temperature Tc. The derivation uses a dynamic cavity approach: in the evolution equation for the selected spin the other spins are represented by a fluctuating field. The influence of the selected spin on this field is included at the linear response level; it is given as a sum of the spin's past flips weighted by the correlations of the unperturbed fluctuating field. The self-consistency condition relates the time-dependent correlations of the selected spin and those of the fluctuating field. The theory predicts a (T−Tc)−2 divergence of the relaxation time upon approaching the transition and an At−1/2 decay of spin correlations at Tc. A numerical solution of the theory gives the amplitude, A=0.964± 0.007. The theoretical predictions are in excellent agreement with Glauber dynamics computer simulations.

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BibTeX
@misc{szamel2026glauber,
  title = {{Glauber dynamics of the Sherrington--Kirkpatrick spin-glass model: a dynamical cavity method}},
  author = {Grzegorz Szamel},
  howpublished = {arXiv},
  year = {2026},
  month = nov,
  doi = {10.48550/arxiv.2611.04078},
  eprint = {2611.04078},
  archivePrefix = {arXiv},
  url = {https://arxiv.org/abs/2611.04078},
}
RIS
TY  - UNPB
TI  - Glauber dynamics of the Sherrington--Kirkpatrick spin-glass model: a dynamical cavity method
AU  - Grzegorz Szamel
PY  - 2026
DA  - 2026/11/02
PB  - arXiv
DO  - 10.48550/arxiv.2611.04078
UR  - https://arxiv.org/abs/2611.04078
AB  - We present a closed theory, exact in the N→∞ limit, of the equilibrium spin correlations of the Sherrington--Kirkpatrick spin-glass model evolving with Glauber dynamics, above and at the transition temperature T_c. The derivation uses a dynamic cavity approach: in the evolution equation for the selected spin the other spins are represented by a fluctuating field. The influence of the selected spin on this field is included at the linear response level; it is given as a sum of the spin's past flips weighted by the correlations of the unperturbed fluctuating field. The self-consistency condition relates the time-dependent correlations of the selected spin and those of the fluctuating field. The theory predicts a (T−T_c)^−2 divergence of the relaxation time upon approaching the transition and an At^−1/2 decay of spin correlations at T_c. A numerical solution of the theory gives the amplitude, A=0.964± 0.007. The theoretical predictions are in excellent agreement with Glauber dynamics computer simulations.
ER  -