Abstract
It is shown that the Gartenhaus-Schwartz-transformation of the electric multipole operator Ω[L], i.e. expressing it in lab frame coordinates, not only leads to the well known concept of kinematic effective charges but in addition gives 2-, 3-,...,N-particle operator contributions whereN=min(A, L). In particular forE2 transitions the electric quadrupole operator contains one- and two-particle operators which contribute to the single particle transition rate and which will lead to two particle transitions.
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