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Low Temperature Physics

Effect of an external field on the thermodynamics of the free-fermion model

S. B. Rutkevich

Published Dec 1, 1993• 0 citations
Publisher

Abstract

The effect of an external field on the phase transition is studied in the continuous version of the model of free fermions without dislocations. The critical indices δ = ∞, β = + 0, γ = 3/2 and the phase diagram are obtained as well as an exact expression for the free energy in the strong field limit. The results are compared with scaling properties in the six-vertex model. While the similarity of scaling in zero field and a coincidence of the values of β and δ indicate that both models have the same class of universality, considerable differences are observed in other characteristics like the index γ, phase diagram, and scaling function. This “discrepancy” is explained by the fact that the external field violates the symmetry in fermion and six-vertex models in different ways. The possibility of experimental observation of the obtained scaling dependences in two-dimensional crystals undergoing a transition to the incommensurate phase is discussed.

DOI
10.1063/10.0033556

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The effect of an external field on the phase transition is studied in the continuous version of the model of free fermions without dislocations. The critical indices δ = ∞, β = + 0, γ = 3/2 and the phase diagram are obtained as well as an exact expression for the free energy in the strong field limit. The results are compared with scaling properties in the six-vertex model. While the similarity of scaling in zero field and a coincidence of the values of β and δ indicate that both models have the same class of universality, considerable differences are observed in other characteristics like the index γ, phase diagram, and scaling function. This “discrepancy” is explained by the fact that the external field violates the symmetry in fermion and six-vertex models in different ways. The possibility of experimental observation of the obtained scaling dependences in two-dimensional crystals undergoing a transition to the incommensurate phase is discussed.
The q-state Potts model on a square lattice and in the presence of an external magnetic field that couples to only one state is studied by using extensive Monte Carlo simulations. A hybrid algorithm that combines the single spin-flip Metropolis method with Wolff cluster updates is employed. Single-histogram reweighting techniques and the field-mixing approach are also used to obtain the corresponding universal probability distributions. By analyzing the finite-size scaling behavior of the order parameters and universal probability distributions, the phase diagram in the temperature-versus-external field plane is obtained in the thermodynamic limit for some values of state q≥5. For positive fields and higher values of q, there is a clear first-order transition line that starts at the zero-field transition point and ends at an isolated critical point, which is in the two-dimensional Ising universality class. As the value of state q decreases, the corresponding critical field also decreases. The present results strongly suggest that the critical field vanishes when q→5^{+}. However, for negative fields, another first-order transition line occurs without any critical or multicritical behavior for q≥6. The special case with q=5 undergoes a weak first-order transition at zero field and a line of second-order transitions for negative fields. This second-order transition line is in the same universality class as the q=4 Potts model.
A general lattice-statistical model which includes all soluble two-dimensional model of phase transitions is proposed. Besides the well-known Ising and "ice" models, other soluble cases are also considered. After discussing some general symmetry properties of this model, we consider in detail a particular class of the soluble cases, the "free-fermion" model. The explicit expressions for all thermodynamic functions with the inclusion of an external electric field are obtained. It is shown that both the specific heat and the polarizability of the free-fermion model exhibit in general a logarithmic singularity. An inverse-square-root singularity results, however, if the free-fermion model also satisfies the ice condition. The results are illustrated with a specific example.
We investigate the critical behavior of the two-dimensional spin-1 Baxter-Wu model in the presence of a crystal-field coupling Δ with the goal of determining the universality class of transitions along the second-order part of the transition line as one approaches the putative location of the multicritical point. We employ extensive Monte Carlo simulations using two different methodologies: (i) a study of the zeros of the energy probability distribution, closely related to the Fisher zeros of the partition function, and (ii) the well-established multicanonical approach employed to study the probability distribution of the crystal-field energy. A detailed finite-size scaling analysis in the regime of second-order phase transitions in the (Δ,T) phase diagram supports previous claims that the transition belongs to the universality class of the four-state Potts model. For positive values of Δ, we observe the presence of strong finite-size effects, indicative of crossover effects due to the proximity of the first-order part of the transition line. Finally, we demonstrate how a combination of cluster and heat-bath updates allows one to equilibrate larger systems, and we demonstrate the potential of this approach for resolving the ambiguities observed in the regime of Δ≳0.
The theory of fermion phase transitions is reviewed from a unified field theoretic standpoint, based on the diagrammatic perturbation expansion of a generalized matrix propagator. Transitions from a normal to a condensed phase are characterized by the spontaneous appearance of long-range order and (in the presence of a suitable infinitesimal external field) broken symmetry. This is illustrated by the ferromagnetic, solid, superconducting and spindensity wave ground states. The phenomenon is explained qualitatively as caused by the creation of a long-range internal field, F, due to the interactions between particles. This field establishes long-range order in the system, and is in turn itself established by the long-range order, in a self-consistent fashion. The mechanism here is expressed quantitatively in terms of a self-consistent Dyson equation relating a generalized matrix propagator, G, to a proper self-energy matrix, Σ. The off-diagonal elements of G describe ‘anomalous’ propagation processes which are characteristic for the condensed phase, and they yield directly the long-range order parameters. The Σ-matrix is just the potential of the internal field. The method is illustrated by applying it to the ferromagnetic phase of a system with δ-function interaction between particles. Finally, the technique is used to derive the vertex part equation for the transition point.