By Alessio F., Zelati V.C., Montechiarri P.

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1c). 17. The slab is initialized at zero temperature. 0. The spring constant k1 is associated with displacements from the equilibrium distance r0 , and the second spring constant k2 is associated with large bond stretching for r > ron . 1550, respectively. 9165 for atomic mass m = 1. 8. 012. 029, corresponding to the respective ron . The dynamic crack instabilities for the various α = k2 /k1 are associated with the precipitous drops in crack speed, as indicated by the arrows, and are a consequence of the crack deviating from straight line motion (see Fig.

1 1/L Fig. 4. Static structure factors S(π,π) for 2 ≤ N ≤ 8. The straight line representing the power law L−2 is drawn for comparison. Estimated statistical errors are not shown, because they are equal to or smaller than the symbol size. The inset presents the data for N = 3, 4, 5, 6 in the linear scale, together with the best fitting curves obtained by the method of least squares. (Adopted from Harada and Kawashima [11]) On the other hand, Fig. 5 shows a clear evidence for a dimer order in N ≥ 5.

54, 966 (1985) 10. G. Santoro, S. Sorella, L. Guidoni, A. Parola, E. Tosatti: Phys. Rev. Lett. 83, 3065 (1999) 11. K. Harada, N. Kawashima: Phys. Rev. Lett. 90, 117203 (2003) 4 Event-by-Event Simulation of Quantum Phenomena H. De Raedt1 , K. De Raedt2 , and K. Michielsen1 1 2 Applied Physics – Computational Physics, Materials Science Centre, University of Groningen, Nijenborgh 4, NL-9747 AG,Groningen, The Netherlands Department of Computer Science, University of Groningen, Blauwborgje 3, NL-9747 AC Groningen, The Netherlands Abstract.

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Chaotic behavior of rapidly oscillating Lagrangian systems by Alessio F., Zelati V.C., Montechiarri P.

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