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70) 12 This indicates a marked increase in the7 interaction energy when com­ pared with the Casimir-Polder (1/R ) form when the molecules are between parallel conducting plates. DISPERSION FORCES FROM THE FIELD POINT OF VIEW asymptotic Ko. = X a = 0 z / z z - z2 + . . 5 = > = r. uC 5 , 54 DISPERSION FORCES The approach outlined here can easily be generalized to take account of other types of boundaries, such as dielectric boundaries. We shall not dwell on this point further at this stage, except to make a general observation that when two molecules are near a dielectric surface, the non-retarded dispersion interactions between them will be diminished from its free space value.

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