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The Extended Variational Principle for Mean-Field, Classical Spin Systems
Mathematical Physics · Submitted 30 Apr 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim This is a new connection, and it permits a generalization of the EVP.
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The abstract, sentence by sentence
The purpose of this article is to obtain a better understanding of the extended variational principle (EVP). The EVP is a formula for the thermodynamic pressure of a statistical mechanical system as a limit of a sequence of minimization problems. It was developed for disordered mean-field spin systems, spin systems where the underlying Hamiltonian is itself random, and whose distribution is permutation invariant. We present the EVP in the simpler setting of classical mean-field spin systems, where the Hamiltonian is non-random and symmetric. The EVP essentially solves these models. We compare the EVP with another method for mean-field spin systems: the self-consistent mean-field equations. The two approaches lead to dual convex optimization problems. This is a new connection, and it permits a generalization of the EVP.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | The purpose of this article is to obtain a better understanding of the extended variational principle (EVP). | contribution 0.53 | 0.39 | 0.04 | asserted 0.77 |
| s1 | The EVP is a formula for the thermodynamic pressure of a statistical mechanical system as a limit of a sequence of minimization problems. | background 1.00 | 0.10 | 0.06 | asserted 1.00 |
| s2 | It was developed for disordered mean-field spin systems, spin systems where the underlying Hamiltonian is itself random, and whose distribution is permutation invariant. | background 1.00 | 0.07 | 0.03 | asserted 1.00 |
| s3 | We present the EVP in the simpler setting of classical mean-field spin systems, where the Hamiltonian is non-random and symmetric. | contribution 0.84 | 0.86 | 0.07 | asserted 0.99 |
| s4 | The EVP essentially solves these models. | interpretation 0.60 | 0.31 | 0.33 | asserted 0.99 |
| s5 | We compare the EVP with another method for mean-field spin systems: the self-consistent mean-field equations. | contribution 0.67 | 0.74 | 0.05 | asserted 0.97 |
| s6 | The two approaches lead to dual convex optimization problems. | result 0.90 | 0.76 | 0.14 | asserted 1.00 |
| s7 | This is a new connection, and it permits a generalization of the EVP. | contribution 0.39 | 0.86 | 0.33 | asserted 0.99 |
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Original abstract
The purpose of this article is to obtain a better understanding of the extended variational principle (EVP). The EVP is a formula for the thermodynamic pressure of a statistical mechanical system as a limit of a sequence of minimization problems. It was developed for disordered mean-field spin systems, spin systems where the underlying Hamiltonian is itself random, and whose distribution is permutation invariant. We present the EVP in the simpler setting of classical mean-field spin systems, where the Hamiltonian is non-random and symmetric. The EVP essentially solves these models. We compare the EVP with another method for mean-field spin systems: the self-consistent mean-field equations. The two approaches lead to dual convex optimization problems. This is a new connection, and it permits a generalization of the EVP.
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