Computer Simulation Studies in Condensed-Matter Physics XIV: by D. P. Landau, S. P. Lewis, H.-B. Schüttler (auth.),

By D. P. Landau, S. P. Lewis, H.-B. Schüttler (auth.), Professor David P. Landau Ph.D., Professor Steven P. Lewis Ph.D., Professor Heinz-Bernd Schüttler Ph.D. (eds.)

This is a "status record" according to the displays and discussions which happened throughout the 14th Annual Workshop on machine Simulation reports in Condensed subject Physics on the heart for Simulational Physics on the college of Georgia in February 2001. It presents a large review of the newest advances within the box, spanning a variety of topical components in simulational condensed topic physics. those contain fresh advancements in simulations of classical statistical mechanics versions, digital constitution calculations, quantum Monte Carlo simulations, and simulations of polymers. New actual effects and novel simulational and information research tools are presented.

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Extra resources for Computer Simulation Studies in Condensed-Matter Physics XIV: Proceedings of the Fourteenth Workshop, Athens, GA, USA, February 19–24, 2001

Example text

This figure shows the KT scaling plot for the transition at the higher density. The horizontal axis shows log[dGj and the vertical axis shows e'T](t,p). 91 where N denotes the number of particles, the second summation takes over particles adjacent to the particle k, and Okl denotes the angle between the directions of an arbitrarily fixed axis and the relative position vector of particle l from particle k. 3) in the disordered phase assuming the KT transition at density Pc. Hexatic ordering state is taken as the initial configuration.

37 7. M. Suzuki: Phys. Lett. A58, 435 (1976) and Prog. Theor. Phys. 58, 1142 (1977) 8. T. Nakamura, private communication 9. S. Fukushima, Master Thesis (The Univ. of Tokyo, 2001) 10. K Ogawa, Master Thesis (Tokyo Inst. , 2000) 11. H. Watanabe, Master Thesis (The Univ. of Tokyo, 2001) 12. KJ. Strandburg: Rev. Mod. Phys. 60, 161 (1988) 13. N. P. -B. 130 14. Y. Nonomura: J. Phys. Soc. Jpn. 67, 5 (1998) 15. Y. Nonomura: J. Phys. A31, 7939 (1998) 5 Dynamic Phase Diagram for a Periodically Driven Kinetic Square-lattice Ising Ferromagnet: Finite-size Scaling Evidence for the Absence of a Tri-critical Point G.

The crossover from the MD to the SD regime is formed by the dynamic spinodal (DSP) [8] and can be estimated by equating tn and tg. This yields an implicit equation for the temperature corresponding to the DSP as a function of Land H, e e Ti DSP = F(TDSP, H) fV (d + 1) lnL -In{C(TDSP' H)[2ild(TDSP )]1/dv(TDsP' H)} . (51) . 1), is shown as a dashed curve in Fig. 1a. In the large-system limit TDSP logarithmically approaches zero. Reducing T at fixed tl/2 and H results in fundamentally different behavior for small and large systems.

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