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δ at δ≤3 (long-range potential) and is finite at δ>3 (short-range potential).
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L+2A =0. This pole is responsible for longitudinal polarization waves generated in a polar solvent by the insertion of the solute. However, this singularity gives a negligible contribution to the integral and is not considered here.
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∝ in which is as strong as in the Marcus formula.
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