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/content/aip/journal/jap/52/12/10.1063/1.328693
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1.E. R. Cowley, G. Jacucci, M. L. Klein, and I. R. McDonald, Phys. Rev. B 14, 1758 (1976).
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2.M. Parrinello and A. Rahman, Phys. Rev. Lett. 45, 1196 (1980).
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6.J. P. Hansen and I. R. McDonald, Theory of Simple Liquids (Academic, London, 1976).
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8.W. G. Hoover, D. J. Evans, R. B. Hickman, A. J. Ladd, W. T. Ashurst, and B. Moran, Phys. Rev. A 22, 1690 (1980).
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9.L. D. Landau and E. M. Lifshitz, Theory of Elasticity (Pergamon, Oxford, 1959).
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10.Note that in the definition of S through Eq. (2.20) we have adopted a certain sign convention: corresponds to a system under hydrostatic pressure p.
11.
11.A. Rahman, in NATO Advanced Study Institute Series: Correlation Functions and Quasiparticle Interactions in Condensed Matter, edited by J. W. Halley (Plenum, New York, 1978).
12.
12.This procedure, used systematically in Ref. 2, is extremely useful for the purpose of resolving peaks in which otherwise would merge in neighboring peaks especially if the corresponding coordination numbers are very different. For example, in an hep structure the third and the fouth shells are very close to each other with a population, respectively, of 2 and 18 neighbors.
13.
13.In an MD calculation the “failure” of a system is manifested by a monotonic change in the and in an obvious disruption of the shell‐like structure of A monotonic drop in the value of the density is simply a consequence of the behavior of the
14.
14.C. Kittel, Introduction to Solid State Physics (Wiley, New York, 1968).
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1981-12-01
2016-07-29
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