By David P. Landau, Steven P. Lewis, Heinz-Bernd Schüttler
This prestige document gains the newest advancements within the box, spanning a variety of topical parts within the computing device simulation of condensed matter/materials physics. either verified and new subject matters are incorporated, starting from the statistical mechanics of classical magnetic spin versions to digital constitution calculations, quantum simulations, and simulations of sentimental condensed subject. The ebook provides new actual effects in addition to novel tools of simulation and information research. Highlights of this quantity comprise quite a few facets of non-equilibrium statistical mechanics, reports of homes of actual fabrics utilizing either classical version simulations and digital constitution calculations, and using machine simulation in teaching.
Read Online or Download Computer Simulation Studies in Condensed-Matter Physics XVI: Proceedings of the Fifteenth Workshop, Athens, GA, USA, February 24–28, 2003 PDF
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Extra info for Computer Simulation Studies in Condensed-Matter Physics XVI: Proceedings of the Fifteenth Workshop, Athens, GA, USA, February 24–28, 2003
Magn. Mater. 67, 65 (1987) 6. M. P. Antropov: J. Appl. Phys. 85, 4827 (1999) 7. V. Antropov: The exchange coupling and spin waves in metallic magnets: removal of the long-wave approximation. cond-mat/0211144 (2002); J. Magn. Magn. Mat. April 2003 (in press) 7 Finite Temperature Simulation Based on Lanczos Algorithm for Low-Dimensional Quantum Systems T. jp Abstract. The Lanczos algorithm is applied to calculate some finite-temperature physical quantities, as well as the ground-state ones. We introduce the finitetemperature Lanczos algorithm and apply it for some current problems in the low-dimensional quantum systems; the magnetization plateau in the frustrated spin ladder and the pseudogap phenomena in the high-Tc cuprates.
8 x 106 MeS were needed to ensure good statistics. 2 x 106 MeS were discarded and measurements were taken every 400 MeS thereafter. 1575, for both E = 20 (effectively infinite) and E = 2. 28 E. Lyman and B. 20(2). Notice the systematic deviations from scaling in the T < Tc branch, which may be due to a small critical region or corrections to scaling from the marginal operator. Though we have not investigated this anomaly in detail, it occurs in the E = 00 model as well  and has been observed in other nonequilibrium Ising models .
J. j. j. j. 'V'l/Jkt] . j. 5). 12) which is just the well-known connection between the inverse static susceptibilityand the parameter P2 in the Landau theory of phase transitions (T. Moriya also always used the inverse susceptibility in the Heisenberg model). Now the goal of following chapter is to consider the relationship between this definition and those currently used in magnetism research. P. 13) is small (long-wave approximation). 16) is the matrix of the exchange parameter in the local (long-wave) approximation.