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4
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0004138120
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Examples include Ref. 2; Springer, New York
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Examples include Ref. 2; M. Toda, R. Kubo, and N. Saitô, Statistical Physics 1 (Springer, New York, 1995); M. P. Allen and D. J. Tildesley, Computer Simulation of Liquids (Clarendon, Oxford, 1996).
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Toda, M.1
Kubo, R.2
Saitô, N.3
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5
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85052507481
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Clarendon, Oxford
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Examples include Ref. 2; M. Toda, R. Kubo, and N. Saitô, Statistical Physics 1 (Springer, New York, 1995); M. P. Allen and D. J. Tildesley, Computer Simulation of Liquids (Clarendon, Oxford, 1996).
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(1996)
Computer Simulation of Liquids
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Allen, M.P.1
Tildesley, D.J.2
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9
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P. C. Ohara, D. V. Leff, J. R. Heat, and W. M. Gelbart, Phys. Rev. Lett. 75, 3466 (1995).
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(1995)
Phys. Rev. Lett.
, vol.75
, pp. 3466
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Ohara, P.C.1
Leff, D.V.2
Heat, J.R.3
Gelbart, W.M.4
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12
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36449003573
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H. M. Ellerby, C. L. Weakliem, and H. Reiss, J. Chem. Phys. 95, 9209 (1991); C. L. Weakliem and H. Reiss, ibid. 99, 5374 (1993); 101, 2389 (1994); P. Schaaf, B. Senger, and H. Reiss, J. Phys. Chem. B 101, 8740 (1997).
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J. Chem. Phys.
, vol.95
, pp. 9209
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Ellerby, H.M.1
Weakliem, C.L.2
Reiss, H.3
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13
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0000496716
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H. M. Ellerby, C. L. Weakliem, and H. Reiss, J. Chem. Phys. 95, 9209 (1991); C. L. Weakliem and H. Reiss, ibid. 99, 5374 (1993); 101, 2389 (1994); P. Schaaf, B. Senger, and H. Reiss, J. Phys. Chem. B 101, 8740 (1997).
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J. Chem. Phys.
, vol.99
, pp. 5374
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Weakliem, C.L.1
Reiss, H.2
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14
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36449003573
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H. M. Ellerby, C. L. Weakliem, and H. Reiss, J. Chem. Phys. 95, 9209 (1991); C. L. Weakliem and H. Reiss, ibid. 99, 5374 (1993); 101, 2389 (1994); P. Schaaf, B. Senger, and H. Reiss, J. Phys. Chem. B 101, 8740 (1997).
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J. Chem. Phys.
, vol.101
, pp. 2389
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15
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0031245699
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H. M. Ellerby, C. L. Weakliem, and H. Reiss, J. Chem. Phys. 95, 9209 (1991); C. L. Weakliem and H. Reiss, ibid. 99, 5374 (1993); 101, 2389 (1994); P. Schaaf, B. Senger, and H. Reiss, J. Phys. Chem. B 101, 8740 (1997).
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J. Phys. Chem. B
, vol.101
, pp. 8740
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Schaaf, P.1
Senger, B.2
Reiss, H.3
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21
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85034282282
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In certain cases, such as a system under tension (e.g., one-dimensional polymer chain), the number of new configurations for v + dv is less than for v, but again redundancies are removed if a shell particle is present in v + dv
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In certain cases, such as a system under tension (e.g., one-dimensional polymer chain), the number of new configurations for v + dv is less than for v, but again redundancies are removed if a shell particle is present in v + dv.
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