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R. Jimenez, G. R. Fleming, P. V. Kumar, and M. Maroncelli, Nature 369, 471 (1994). These papers make clear the need for short timescale theories of dynamics and molecular models for friction in liquid phase chemistry.
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(a) The basic principles and equations of our theory of liquid phase chemical dynamics are developed for monatomic solvents in S. A. Adelman, Adv. Chem. Phys. 53, 61 (1983) and references therein.
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The short time treatment of liquid phase vibrational energy relaxation overviewed in Section VC is developed and applied for monatomic solvents in S. A. Adelman and R. H. Stote, J. Chem. Phys. 88, 4397 (1988);
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For brief reviews of the theory developed in refs. 20-24 see S. A. Adelman, Rev. Chem. Intermed. 8, 321 (1987)
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See, for example, the discussion on p. 581 of ref. 8
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See, for example, the discussion on p. 581 of ref. 8.
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For reviews of liquid phase vibrational energy relaxation see, for example, D. W. Oxtoby, Adv. Chem. Phys. 47, 487 (1981)
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52849123446
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For a comparison of the assumptions underlying our theory of liquid phase VER and those of the Landau-Teller theory see sec. 23 of ref. 19
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For a comparison of the assumptions underlying our theory of liquid phase VER and those of the Landau-Teller theory see sec. 23 of ref. 19.
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86
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52849086755
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See, for example, the comments after eq. (15.18.7) on p. 595 of ref. 37
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See, for example, the comments after eq. (15.18.7) on p. 595 of ref. 37.
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87
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52849122552
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See the first of eqs. (214) of ref. 2
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See the first of eqs. (214) of ref. 2.
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89
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52849138306
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Mori's eq. (3.10) of ref. 5 and Eq. (A.54) in the present chapter are equivalent for the microscopically reversible A's assumed by Onsager
-
Mori's eq. (3.10) of ref. 5 and Eq. (A.54) in the present chapter are equivalent for the microscopically reversible A's assumed by Onsager.
-
-
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90
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0003527976
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Harper & Row, New York, chaps. 21 and 22
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See, for example, D. A. McQuarrie, Statistical Mechanics (Harper & Row, New York, 1976), chaps. 21 and 22 and references therein.
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McQuarrie, D.A.1
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