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日本物理学会講演概要集

1a-L-10 Analysis of First-Order Transitions by the Monte Carlo Twist Method : Two-Dimensional Potts Model

Tatsunori Takahashi, Yohtaro Ueno

Published Mar 15, 1996• 0 citations
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We study the three-dimensional generalized six-state clock model at values of the energy parameters at which the system is considered to have the same behavior as the stacked triangular antiferromagnetic Ising model and the three-state antiferromagnetic Potts model. First, we investigate ordered phases by using the Monte Carlo twist method (MCTM). We confirmed the existence of an incompletely ordered phase (IOP1) at intermediate temperature, besides the completely ordered phase at low temperature. In this intermediate phase, two neighboring states of the six-state model mix, while one of them is selected in the low-temperature phase. We examine the fluctuation the mixing rate of the two states in IOP1 and clarify that the mixing rate is very stable around 1:1. The high-temperature phase transition is investigated by using a nonequilibrium relaxation method. We estimate the critical exponents \ensuremath{\beta}=0.34(1) and \ensuremath{\nu}=0.66(4). These values are consistent with the $3\mathrm{D}\ensuremath{-}XY$ universality class. The low temperature phase transition is found to be of first-order by using MCTM and finite-size-scaling analyses.

arXiv:cond-mat/0207665•Physical review. B, Condensed matter•Dec 6, 2002•14 citations
The Wolff cluster Monte Carlo algorithm is used to investigate the effect of frozen nonmagnetic canonically distributed impurities on the phase transitions in a two-dimensional Potts model with the spin state q = 5. Systems with linear dimensions L = 20–160 at spin concentrations p = 1.0 and 0.9 are considered. Using the fourth-order Binder cumulant method and the histogram analysis method it is shown that if a weak quenched disorder in the form of non-magnetic impurities (p = 0.9) is introduced in the system, the first-order phase transition changes to a second-order phase transition.
We study the three-dimensional generalized six-state clock model at values of the energy parameters at which the system is considered to have the same behavior as the stacked triangular antiferromagnetic Ising model and the three-state antiferromagnetic Potts model. First, we investigate ordered phases by using the Monte Carlo twist method (MCTM). We confirmed the existence of an incompletely ordered phase (IOP1) at intermediate temperature, besides the completely ordered phase at low temperature. In this intermediate phase, two neighboring states of the six-state model mix, while one of them is selected in the low-temperature phase. We examine the fluctuation the mixing rate of the two states in IOP1 and clarify that the mixing rate is very stable around 1:1. The high-temperature phase transition is investigated by using a nonequilibrium relaxation method. We estimate the critical exponents \ensuremath{\beta}=0.34(1) and \ensuremath{\nu}=0.66(4). These values are consistent with the $3\mathrm{D}\ensuremath{-}XY$ universality class. The low temperature phase transition is found to be of first-order by using MCTM and finite-size-scaling analyses.