1994
DOI: 10.1103/physreve.49.2711
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Finite-range-scaling analysis of metastability in an Ising model with long-range interactions

Abstract: We apply both a scalar field theory and a recently developed transfer-matrix method to study the stationary properties of metastability in a two-state model with weak, long-range interactions: the N ×∞ quasi-one-dimensional Ising model. Using the field theory, we find the analytic continuationf of the free energy across the first-order transition, assuming that the system escapes the metastable state by nucleation of noninteracting droplets. We find that corrections to the field-dependence are substantial, and… Show more

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Cited by 12 publications
(29 citation statements)
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“…In systems with effective long-range interactions we expect the change from metastability to instability of the LS phase to take place at a sharply defined mean-field spinodal point. 4 This leads to a threshold behavior with respect to the irradiation intensity, 4,19,20 which is qualitatively different from the gradual crossover seen in short-range models. 21 Here, we therefore investigate the LS-to-HS transition time and its dependence on the system size as functions of the irradiation intensity.…”
Section: Introductionmentioning
confidence: 82%
“…In systems with effective long-range interactions we expect the change from metastability to instability of the LS phase to take place at a sharply defined mean-field spinodal point. 4 This leads to a threshold behavior with respect to the irradiation intensity, 4,19,20 which is qualitatively different from the gradual crossover seen in short-range models. 21 Here, we therefore investigate the LS-to-HS transition time and its dependence on the system size as functions of the irradiation intensity.…”
Section: Introductionmentioning
confidence: 82%
“…For the Q1DI model R=N and d=1 [152,156]. By solving the Euler-Lagrange equation numerically, one can also take into account the corrections to the expansion, as well as discrete lattice effects [94]. The prefactor to the Van't Hoff-Arrhenius term in |Im f | can be calculated by expanding the free-energy density functional about the stationary points corresponding to the metastable phase and the critical droplet.…”
Section: Nucleationmentioning
confidence: 99%
“…where B(T ) is a nonuniversal function of T , V is the system volume, and V ′ is the volume of the subspace in which the droplet itself is free to move without a cost in free energy. For the Q1DI model, [94]. From Eqs.…”
Section: Nucleationmentioning
confidence: 99%
“…The application of such ideas to a fieldtheoretical droplet model with Fokker-Planck dynamics has shown that close to coexistence, the nucleation rate for droplets of the equilibrium phase is proportional to the imaginary part of a complex-valued constrained free energy obtained by analytic continuation from the equilibrium phase into the metastable phase [8][9][10]. long-range forces [13][14][15] by a constrained-transfer-matrix method introduced by one of us [16]. Although no dynamical aspects were explicitly considered to obtain the constrained free energies, the average free-energy cost of a critical droplet was obtained over a wide range of fields and temperatures, in good agreement with the predictions of field-theoretical droplet models [8][9][10]14,15,17] and Monte Carlo (MC) simulations [1,[4][5][6].…”
Section: Introductionmentioning
confidence: 99%
“…long-range forces [13][14][15] by a constrained-transfer-matrix method introduced by one of us [16]. Although no dynamical aspects were explicitly considered to obtain the constrained free energies, the average free-energy cost of a critical droplet was obtained over a wide range of fields and temperatures, in good agreement with the predictions of field-theoretical droplet models [8][9][10]14,15,17] and Monte Carlo (MC) simulations [1,[4][5][6]. These results indicate the relevance of purely static properties, such as the free energy, to the relaxation behavior of metastable phases.…”
Section: Introductionmentioning
confidence: 99%