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

無王時(shí)期,

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

大炮

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.

腫塊

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

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刀鋒

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.

Homocystinuria

紅腫

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.

弓箭

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.