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Titlebook: Computer Simulation Studies in Condensed-Matter Physics V; Proceedings of the F David P. Landau,K. K. Mon,Heinz-Bernd Schüttler Conference

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樓主: Enlightening
21#
發(fā)表于 2025-3-25 06:40:09 | 只看該作者
Monte-Carlo Simulations in Adiabatic Ensemblesample we present the first results from simulations using the new Monte Carlo method to generate the HtN ensemble, where H is the enthalpy, and t the thermodynamic tension. This method is the Monte Carlo counterpart of the Parrinello-Rahman form of molecular dynamics. In particular we discuss HtN Mo
22#
發(fā)表于 2025-3-25 10:42:57 | 只看該作者
Dynamics of Acoustic Phonon Decay: Experiment and Simulationral dynamics associated with anharmonic decay are determined using an absorption vibronic sideband spectrometer. Experimental results are compared with Monte Carlo simulations based upon the isotropic dispersionless model for spontaneous three phonon anharmonic processes.
23#
發(fā)表于 2025-3-25 14:00:41 | 只看該作者
0930-8989 and neophytes to discuss new techniques and results in an evironment which promotes extended discussion. As a consequence of these concerns, The Center for Simulational Physics established an annual workshop on Recent Developments in Computer Simulation Studies in Condensed-Matter Physics. This year
24#
發(fā)表于 2025-3-25 17:19:32 | 只看該作者
25#
發(fā)表于 2025-3-25 22:04:12 | 只看該作者
26#
發(fā)表于 2025-3-26 00:55:41 | 只看該作者
27#
發(fā)表于 2025-3-26 06:19:09 | 只看該作者
Computer Simulation Studies in Condensed-Matter Physics: An Introduction. The invited talks include rather long papers which have some pedagogical content, and at the end of this volume we present a few shorter, contributed papers which present very recent research results.
28#
發(fā)表于 2025-3-26 09:10:09 | 只看該作者
29#
發(fā)表于 2025-3-26 13:13:01 | 只看該作者
The 2d/3D Classical Heisenberg Ferromagnet .. ~ 0.6. The phase transition has unusual features reminiscent of a Kosterlitz-Thouless (topological) phase transition; it is suggested that topological defects may play an important role in the ordering of this system.
30#
發(fā)表于 2025-3-26 17:02:38 | 只看該作者
https://doi.org/10.1007/978-1-4613-0679-5 v and the dynamic critical exponent z at this transition are in good agreement with experiments. In d = 4 dimensions the gauge glass transition is located at T ≈ 0.95. It is concluded that the lack of time reversal symmetry in the model places it into a universality class different from that of the XY spin glass.
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