Computer Simulation Studies in Condensed-Matter Physics XVI: by David P. Landau, Steven P. Lewis, Heinz-Bernd Schüttler

By David P. Landau, Steven P. Lewis, Heinz-Bernd Schüttler

This prestige document good points the latest advancements within the box, spanning a variety of topical parts within the desktop simulation of condensed matter/materials physics. either demonstrated and new themes are integrated, starting from the statistical mechanics of classical magnetic spin types to digital constitution calculations, quantum simulations, and simulations of sentimental condensed topic. The e-book offers new actual effects in addition to novel tools of simulation and information research. Highlights of this quantity contain a variety of elements of non-equilibrium statistical mechanics, reviews of houses of actual fabrics utilizing either classical version simulations and digital constitution calculations, and using desktop simulation in teaching.

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Extra resources for Computer Simulation Studies in Condensed-Matter Physics XVI: Proceedings of the Fifteenth Workshop, Athens, GA, USA, February 24–28, 2003

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B 13, 547 (2000) M. Gitterman: J. Phys. J. : Phys. Rev. E 64, 056135 (2001) H. J. Y. Choi: Phys. Rev. E 66, 018101 (2002) H. Y. J. Kim: Phys. Rev. H. Strogatz: Nature 410, 268 (2001) Y. Kuramoto: in International Symposium on Mathematical Problems in Theoretical Physics, Lecture Notes in Physics, Vol 39 ed by H. 420-422 R. Fujimoto: Commun. D. Lubachevsky: J. Comput. Phys. 75, 103 (1988) G. Korniss, Z. A. A. Rikvold: Phys. Rev. Lett. 84, 1351 (2000) G. A. Novotny, H. Guclu, Z. A. Rikvold: Science 299, 677 (2003) R.

Moriya also used J = 1MX1M = -1M [82Ej8B~xtl 1M. Xexc is close (but strictly speaking is not the same) to the "bare" susceptibility X = 8mj8B tot = _8 2Ej8Btot8Bext. The usual assumption of weak enhancement J q - o = Jg is valid due to well known X~1 = J q = I. As a consequence, the spectrum of elementary excitations is not affected by exchange-correlation enhancement effects in linear response regime. 16) is directly related to several very strong approximations: rigid spin, smallness of SW dispersion compared to the effective exchange splitting (atomic limit) and Kq = 1 (smallness of "kinetic" gradients).

For a perfect strip along the y-direction, (<1>(1,0)) = 1, while a random configuration gives Except where noted, all simulations are run on 40 x 40 lattices, starting from random initial configurations. One MC step (MCS) is defined as 2LxLy update attempts. The first 2 x 105 MCS are discarded, and measurements are taken every 200 MCS for the next 8 x 105 MCS. 3 Monte Carlo Results: Phase Diagram Although most detailed studies of the KLS model have considered the limit of infinite E to accentuate nonequilibrium properties, we are forced to consider finite values of E.

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