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By Mohler F.L.

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By Mohler F.L.

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Kornishev, J. Chem. Soc. , 2, 70 (1974) 1121. [22] V. Basilevsky and D. F. Parsons, J. Chem. , 105 (1996) 3734. 28 Continuum Solvation Models in Chemical Physics [23] G. Alagona, c. Ghio, R. Cammi and J. Tomasi, A Reappraisal of the hydrogen bonding interaction obtained by combining energy decomposition analyses and counterpoise corrections, in J. ), Moleculaes in Physics, Chemistry, Biology, Vol. II, Kluwer, Dordrecht, 1988, p. 507. [24] J.

Chem. , 107 (1997) 3032. [21] R. R. Dogonadze and A. A. Kornishev, J. Chem. Soc. , 2, 70 (1974) 1121. [22] V. Basilevsky and D. F. Parsons, J. Chem. , 105 (1996) 3734. 28 Continuum Solvation Models in Chemical Physics [23] G. Alagona, c. Ghio, R. Cammi and J. Tomasi, A Reappraisal of the hydrogen bonding interaction obtained by combining energy decomposition analyses and counterpoise corrections, in J. ), Moleculaes in Physics, Chemistry, Biology, Vol. II, Kluwer, Dordrecht, 1988, p. 507. [24] J.

The same happens for the other states in the manifold created by the sudden perturbation. The conclusion is that the amplitudes of such states must be described by an expression more complex than that used in the standard formulation for molecules in vacuo. The QM description of molecules in condensed phases is rich in problems of this type. We stress that the physical basis of the description is correct: the origin of the differences with respect to the standard picture is due to the use of effective Hamiltonians, a feature we cannot abandon.

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A Photo-Ionization Experiment with Hydrogen by Mohler F.L.


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