Markov Form of the Method of Nonequilibrium Statistical Operator

M. D. Zviadadze; A. G. Kvirikadze; M. M. Sozashvili; L. O. Tkeshelashvili

Home/Archive/arXiv

arXiv · cond-mat/0306311

Markov Form of the Method of Nonequilibrium Statistical Operator

M. D. Zviadadze·A. G. Kvirikadze·M. M. Sozashvili·L. O. Tkeshelashvili

View original source ↗Read source document ↗Export metadata ↓

Abstract

The general principles of the choice of the reduced description parameters of nonequilibrium states γα(t) and the construction of the nonequilibrium statistical operator (NSO) ρ(t) are discussed. On the basis of Kavasaki - Gunton projection operator an explicit non-Markov form of NSO with respect to parameters is obtained and the equivalence of the method to the other methods using boundary conditions for ρ(t) or "mixing" operator is shown. An exact NSO transformation to γα(t) Markov form with respect to γα(t) at arbitrary dependence of Vt perturbation on time is made. The generalized kinetic equations not containing the memory with respect to γα(t) are obtained being convenient for practical application.

Explore related subjects

cond-mat.stat-mech

Keep this discovery

BibTeX RIS

M. D. Zviadadze, A. G. Kvirikadze, M. M. Sozashvili, L. O. Tkeshelashvili. 2003-06-12. Markov Form of the Method of Nonequilibrium Statistical Operator. https://arxiv.org/abs/cond-mat/0306311

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

arXiv2026

Universal sampling of spin systems across quenched disorder

Statistical physics extracts macroscopic laws by averaging over the many microscopic degrees of freedom of a system. Disordered systems demand a second and far harder average, one over the quenched randomness itself. The classic analytical routes, the replica and cavity methods, become uncontrolled outside mean-field or tree-like limits, and conventional numerical algorithms like parallel tempering require expensive, independent equilibration for every disorder realization. In this work, we introduce a universal neural variational framework that amortizes inference across the disorder ensemble, eliminating both the need for per-instance Markov chain equilibration and the cost of retraining instance-specific variational ansatzes. Built on an encoder-decoder Transformer architecture, after training once, it produces an explicit approximation to the Boltzmann distribution given previously unseen disorder realizations without further optimization. We validate this framework on 2D Edwards-Anderson models, and apply it to the random-bond Ising model, successfully capturing the Binder cumulant crossings near the Nishimori multicritical point. These results shift the object of variational inference from the single instance to the disorder ensemble, opening a route to frustrated many-body systems where instance-by-instance computation is prohibitive.

cond-mat.stat-mech↗

arXiv2026

Information-Theoretic Characterization of Macroscopic Chaos Emerging from the Chemical Master Equation

Open chemical reaction networks exhibit stochastic concentration dynamics at finite system sizes, whereas their macroscopic limit is governed by deterministic rate equations that can display chaos. In this Letter, we show theoretically that a rate of information loss constructed from two-time mutual information recovers the Kolmogorov-Sinai entropy in the deterministic limit. We verify this result through numerical simulations of a Markov jump process for a three-species system involving seven reactions.

cond-mat.stat-mech↗

arXiv2026

Orientational order on non-orientable domains

We study the statistical properties of passive and active many-body systems with orientational degrees of freedom on non-orientable domains. By rephrasing topological constraints as non-local symmetry relations on an orientable double-cover, we show that non-orientability eliminates global rotational soft modes without acting like an external field. In a passive XY model, this results in topological caging, where orientational fluctuations that exhibit conventional diffusive behavior on a torus saturate on a Klein bottle to a finite value that we compute exactly in the thermodynamic limit. In models of active self-propelled particles with orientational degrees of freedom, topological caging persists despite continuously changing interaction neighborhoods. In an active Ising spin model, non-orientability enforces the coexistence of ordered anti-parallel domains with vanishing global polar order, a state that is absent on orientable domains.

cond-mat.stat-mech↗