By D. P. Landau, S. P. Lewis, H.-B. Schüttler
Greater than a decade in the past, as a result of the exceptional progress within the energy of laptop simulations, The college of Georgia shaped the 1st institutional unit dedicated to using simulations in learn and educating: the heart for Simulational Physics. because the simulations group multiplied additional, we sensed a necessity for a gathering position for either skilled simulators and neophytes to debate new innovations and up to date leads to an atmosphere which promoted prolonged dialogue. accordingly, the guts for Sim ulational Physics confirmed an annual workshop on contemporary advancements in laptop Simulation stories in Condensed subject Physics. This year's workshop was once the 12th during this sequence. It was once held on the college of Geor gia, March 8-12, 1999 as an unofficial satellite tv for pc convention to the Centennial assembly of the yankee actual Society in Atlanta, GA. the continuing curiosity proven through the medical group demonstrates rather sincerely the necessary goal which the sequence has served. those complaints supply a "sta tus file" on a few vital themes. This quantity is released with the aim of well timed dissemination of the fabric to a much broader viewers. we want to supply distinctive due to IBM company for his or her beneficiant aid of this year's workshop. This quantity includes either invited papers and contributed shows on difficulties in either classical and quantum condensed subject physics. we are hoping that every reader will take advantage of really expert effects in addition to cash in on publicity to new algorithms, equipment of study, and conceptual devel opments.
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Additional resources for Computer Simulation Studies in Condensed-Matter Physics
Ei → Ei+1 → . . 7) where the density of states g(E) is ﬁxed for the simulated system. One choice of generalized weights is the multicanonical ensemble  where the weight of a conﬁguration c is deﬁned as Wmulticanonical(c) ∝ 1/g(E(c)). The multicanonical ensemble then leads to a ﬂat histogram in energy space Hmulticanonical(E) ∝ g(E)Wmulticanonical(E) = g(E) 1 = const. 8) removing the exponentially small minimum in the canonical distribution. After performing a simulation, measurements in the multicanonical ensemble are reweighted by a factor WBoltzmann (E)/Wmulticanonical(E) to obtain averages in the canonical ensemble.
Simulation box was 1 × 1 × Lz , and Lz was changed from 2 to 20. Boundary condition to Lz directions were thermal walls, that is, a sphere forgot its velocity and is assigned new velocity randomly from Boltzmann distribution of the wall temperature at every collision with thermal walls. The perpendicular directions have periodic boundary conditions. System density was less than the freezing density all over the system. 2) was also observed in heat-ﬂux autocorrelation function. Heat conductivity of system with Lz = 7 was already within 10% of the converging value.
Ito, Computer Simulation Studies in Condensed-Matter Physics XI. P. -B. ) (Springer, Berlin Heidelberg New York 1999) p. 130. 5. N. Ito, Physica A 196, 569 (1993). 6. P. Landau, K. Binder, A Guide to Monte Carlo Simulations in Statistical Physics. 2nd Edn. (Cambridge University Press, 2005). 7. org/lists/2005/11/basic 8. K. ), Monte Carlo Methods in Statistical Physics. (Springer, Berlin Heidelberg New York, 1979). 9. K. ), Applications of the Monte Carlo Methods in Statistical Physics. 2nd Edn.