By Krauth W.
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W. Rosenbluth, M. N. Rosenbluth, A. H. Teller, E. Teller, J. chem. Phys 21 1087 (1953) [2] Monte Carlo Methods in Statistical Physics, edited by K. Binder, 2nd ed. (Springer Verlag, Berlin, 1986) [3] S. Caracciolo, A. Pelissetto, A. D. Sokal, Phys. Rev. Lett 72 179 (1994) [4] R. H. -S. Wang Phys. Rev. Lett. 63, 86 (1987) [5] U. Wolff Phys. Rev. Lett. 62, 361 (1989) [6] A. B. Bortz, M. H. Kalos, J. L. Lebowitz; J. Comput. Phys. 17, 10 (1975) cf also : K. 1 [7] J. D. Shore, M. Holzer, J. P. Sethna; Phys Rev.
Lett 72 179 (1994) [4] R. H. -S. Wang Phys. Rev. Lett. 63, 86 (1987) [5] U. Wolff Phys. Rev. Lett. 62, 361 (1989) [6] A. B. Bortz, M. H. Kalos, J. L. Lebowitz; J. Comput. Phys. 17, 10 (1975) cf also : K. 1 [7] J. D. Shore, M. Holzer, J. P. Sethna; Phys Rev. B 46 11376 (1992) [8] W. H. Press, S. A. Teukolsky, W. T. Vetterling, B. P. Flannery, Numerical Recipes, 2nd edition, Cambridge University Press (1992). [9] E. L. Pollock, D. M. Ceperley Phys. Rev. B 30, 2555 (1984), 36 8343 (1987); D. M. Ceperley Rev.
There are endless possibilities to improve the dynamical algorithms for some systems. Of course, the more powerful a method the less frequently it can be applied. 5). A large class of systems for which none of these conditions hold are the spin glasses with a socalled continuous replica symmetry breaking transition, as the Sherrington-Kirkpatrick model. In these cases, the ergodicity breaking takes place very “gracefully”, there are very many configurations accessible for any given initial condition.
Introduction to monte-carlo algorithms by Krauth W.
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