By Alessio F., Zelati V.C., Montechiarri P.
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Extra info for Chaotic behavior of rapidly oscillating Lagrangian systems
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 ) 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.
Chaotic behavior of rapidly oscillating Lagrangian systems by Alessio F., Zelati V.C., Montechiarri P.