Download Computer Simulation Studies in Condensed-Matter Physics XVI: by D.P. Landau, S.P. Lewis, H.-B. Schüttler PDF

By D.P. Landau, S.P. Lewis, H.-B. Schüttler

This prestige file positive aspects the newest advancements within the box, spanning a variety of topical parts within the desktop simulation of condensed matter/materials physics. either validated and new subject matters are incorporated, starting from the statistical mechanics of classical magnetic spin types to digital constitution calculations, quantum simulations, and simulations of sentimental condensed subject. The ebook provides new actual effects in addition to novel equipment of simulation and information research. Highlights of this quantity contain quite a few elements of non-equilibrium statistical mechanics, experiences of homes of genuine fabrics utilizing either classical version simulations and digital constitution calculations, and using desktop simulations in instructing.

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Read Online or Download Computer Simulation Studies in Condensed-Matter Physics XVI: Proceedings of the Seventeenth Workshop, Athens, GA, USA, February 16-20, 2004 (Springer Proceedings in Physics) (v. 17) PDF

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Additional info for Computer Simulation Studies in Condensed-Matter Physics XVI: Proceedings of the Seventeenth Workshop, Athens, GA, USA, February 16-20, 2004 (Springer Proceedings in Physics) (v. 17)

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For the models with many meta-stable states such as systems with disorder, frustration or KT transitions, however, corrections to scaling could be strong. For accurate estimate of critical exponents, one needs to take into account corrections to scaling. 1 The 2D F F XY Model In this subsection, we study the second order phase transition in the 2D F F XY model [12]. e. the Kosterlitz–Thouless phase transition (XY -like) and the second order phase transition (Ising-like). Numerical simulations of the 2D F F XY model suffer severely from critical slowing down.

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Most of the recent works on the 2D F F XY model support that these two phase transitions take place at two different temperatures, however, it is not very clear whether the chiral degree of freedom of the F F XY model is in the same universality class of the Ising model [47–50]. 15) ij where θi is the angle of the spin (a planar unit vector) located on site i, Aij determine the frustration and the sum is over the nearest neighbors on a square lattice. 5 100 t 1000 −4 100 2000 t 1000 2000 Fig. 1.

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