A new type of polarization potential, which is real and local, is derived from classical dynamics based on the linear response theory. The potential is represented by -α( v / r )/2 r 4 , where α( v / r ) is a “polarizability function” of the initial velocity v and the distance r . This function can be obtained if the distribution of oscillator strength is known. The potential tends to the usual adiabatic polarization potential as v / r tends to zero and to be proportional to r -2 as v / r tends to infinity. The phase shift function for the quasi-adiabatic polarization potential is also derived in an analogous form.
No takes yet. Share an insight, caveat, or question.
Hayashi et al. (1977) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: