A Monte Carlo study of the entropy, the pressure, and the critical behavior of the hard-square lattice gas

An approximate technique for estimating the entropyS with computer simulation methods, suggested recently by Meirovitch, is applied here to the Metropolis Monte Carlo (MC) simulation of the hard-square lattice gas in both the grand canonical and the canonical ensembles. The chemical potentialμ, calculated by Widom's method, andS enable one to obtain also the pressureP. The MC results are compared with results obtained with Padé approximants (PA) and are found to be very accurate; for example, at the critical activityzc the MC and the PA estimates forS deviate by 0.5%. Beyondzc this deviation decreases to 0.01% and comparable accuracy is detected forP. We argue that close tozc our results forS, μ, andP are more accurate than the PA estimates. Independent of the entropy study, we also calculate the critical exponents by applying Fisher's finite-size scaling theory to the results for the long-range order, the compressibility and the staggered compressibility, obtained for several lattices of different size at zc. The data are consistent with the critical exponents of the plane Ising latticeβ=1/8,ν=1,γ=7/4, andα=0. Our values forβ and ν agree with series expansion and renormalization group results, respectively,α=0 has been obtained also by matrix method studies; it differs, however, from the estimate of Baxteret al. α=0.09 ± 0.05. As far as we knowγ has not been calculated yet.

[1]  W. Fickett,et al.  Application of the Monte Carlo Method to the Lattice‐Gas Model. I. Two‐Dimensional Triangular Lattice , 1959 .

[2]  Michael E. Fisher,et al.  Scaling Theory for Finite-Size Effects in the Critical Region , 1972 .

[3]  Kurt Binder,et al.  Phase diagrams and critical behavior in Ising square lattices with nearest- and next-nearest-neighbor interactions , 1980 .

[4]  F. Ree,et al.  Phase Transition of a Hard‐Core Lattice Gas. The Square Lattice with Nearest‐Neighbor Exclusion , 1966 .

[5]  Z. Alexandrowicz,et al.  Estimation of the pressure with computer simulation , 1977 .

[6]  H. Temperley Application of the Mayer Method to the Melting Problem , 1959 .

[7]  K. K. Mon,et al.  Monte Carlo study of multicriticality in finite Baxter models , 1975 .

[8]  D. Burley A Lattice Model of a Classical Hard Sphere Gas: II , 1960 .

[9]  B. Jancovici Theory of freezing , 1965 .

[10]  L. Verlet,et al.  Integral equation for classical fluids and the lattice gas , 1964 .

[11]  L. K. Runnels,et al.  Exact Finite Method of Lattice Statistics. I. Square and Triangular Lattice Gases of Hard Molecules , 1966 .

[12]  D. S. Gaunt,et al.  Hard‐Sphere Lattice Gases. I. Plane‐Square Lattice , 1965 .

[13]  D. N. Card,et al.  Monte Carlo Estimation of the Free Energy by Multistage Sampling , 1972 .

[14]  H. Temperley Improvements in the Lattice Model of a Liquid , 1961 .

[15]  C. Domb Self-avoiding walks and the Ising and Heisenberg models , 1970 .

[16]  Robert H. Swendsen,et al.  Monte Carlo Renormalization Group , 1979 .

[17]  H. Meirovitch An approximate stochastic process for computer simulation of the Ising model at equilibrium , 1982 .

[18]  Kurt Binder,et al.  Monte Carlo study of entropy for face-centered cubic Ising antiferromagnets , 1981 .

[19]  D. J. Adams,et al.  Chemical potential of hard-sphere fluids by Monte Carlo methods , 1974 .

[20]  N. Metropolis,et al.  Equation of State Calculations by Fast Computing Machines , 1953, Resonance.

[21]  M. Fisher The theory of equilibrium critical phenomena , 1967 .

[22]  D. W. Wood,et al.  Vertex models for the hard-square and hard-hexagon gases, and critical parameters from the scaling transformation , 1980 .

[23]  M. P. Nightingale,et al.  Scaling theory and finite systems , 1976 .

[24]  B. Widom,et al.  Some Topics in the Theory of Fluids , 1963 .

[25]  R. Swendsen Monte Carlo renormalization-group studies of the d=2 Ising model , 1979 .

[26]  S. K. Tsang,et al.  Hard-square lattice gas , 1980 .

[27]  J. Gunton Finite size effects at the critical point , 1968 .

[28]  W. Kinzel,et al.  Extent of exponent variation in a hard-square lattice gas with second-neighbor repulsion , 1981 .

[29]  L. K. Runnels Hard-Square Lattice Gas , 1965 .

[30]  H. Müller-Krumbhaar,et al.  A „self consistent” monte carlo method for the heisenberg ferromagnet , 1972 .

[31]  H. Temperley Statistics of a Two-dimensional Lattice Gas. I , 1962 .

[32]  Z. Alexandrowicz Entropy calculated from the frequency of states of individual particles , 1976 .

[33]  H. Meirovitch Computer simulation of a lattice model of nematic liquid crystal , 1977 .

[34]  Z. Alexandrowicz,et al.  Irreversible adiabatic demagnetization: Entropy and discrimination of a model stochastic process , 1975 .

[35]  Hagai Meirovitch,et al.  The stochastic models method applied to the critical behavior of Ising lattices , 1977 .

[36]  Z. Rácz Phase boundary of Ising antiferromagnets near H=Hc and T=0: Results from hard-core lattice gas calculations , 1980 .

[37]  C. Domb,et al.  Some theoretical aspects of melting , 1958 .

[38]  J. L. Jackson,et al.  Potential Distribution Method in Equilibrium Statistical Mechanics , 1964 .

[39]  C. Domb On co-operative effects in finite assemblies , 1965 .

[40]  Z. Alexandrowicz Stochastic Models for the Statistical Description of Lattice Systems , 1971 .

[41]  H. Meirovitch Calculation of entropy with computer simulation methods , 1977 .

[42]  E. Domany,et al.  Classification of continuous order-disorder transitions in adsorbed monolayers , 1978 .

[43]  Jean-Pierre Hansen,et al.  Phase Transitions of the Lennard-Jones System , 1969 .