Titlebook: Computer Simulation Studies in Condensed-Matter Physics XV; Proceedings of the F David P. Landau,Steven P. Lewis,Heinz-Bernd Schütt Confere

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Nonequilibrium Relaxation Analysis of Frustrated , Models in Two Dimensionswo different transitions, the chiral transition and the Kosterlitz-Thouless one, have been discussed. Further, we calculate the NER functions of fluctuations for these models, and analyze the universality class of them

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First Principles Calculations of the Magnetic Structure in FeMn/Co Bilayers magnetization in the ground state. We find that the magnetic configuration does not differ significantly from bulk Co in the Co, however it changes from a bulk 3Q configuration to a 1Q like antiferromagnetic configuration in Fe.Mn.. Additionally, the Fe.Mn. moments are found to be mostly perpendicular to Co

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Melting of Stripes in a Two-Dimensional Hard-Core Boson Hubbard Modeling quantum Monte Carlo simulations. We find that the stripe melting is realized in a first order transition at low temperatures. In addition we conjecture that a nematic phase does not exist in this model

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Is Language a General Principle of Nature?,We investigate structural properties of pore condensates in cylindrical pores as well as phase transition and quantum effects by path integral Monte Carlo simulations

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Simulation for Licensure and Certificationwo different transitions, the chiral transition and the Kosterlitz-Thouless one, have been discussed. Further, we calculate the NER functions of fluctuations for these models, and analyze the universality class of them

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Algorithms on Compressed Words, magnetization in the ground state. We find that the magnetic configuration does not differ significantly from bulk Co in the Co, however it changes from a bulk 3Q configuration to a 1Q like antiferromagnetic configuration in Fe.Mn.. Additionally, the Fe.Mn. moments are found to be mostly perpendicular to Co

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Lecture Notes in Computer Scienceing quantum Monte Carlo simulations. We find that the stripe melting is realized in a first order transition at low temperatures. In addition we conjecture that a nematic phase does not exist in this model