“…16(a), it is similar to the conventional six-beam MOT, except that the detunings (δ x and δ y ) and intensities (I x and I y ) of the transverse lasers can be different from those of the longitudinal ones (δ z and I z ). In the case of usual MOT, one obtains a usual Doppler trap superimposed with a tightly confined SDT at the MOT center, exhibiting bimodal velocity as well as spatial distributions (Dalibard, 1988;Townsend et al, 1995;Drewsen et al, 1994;Wallace et al, 1994;. Under equal detunings but unequal intensities (I x , I y I z ), which typically arise in the nonlinear dynamics study of nonadiabatically driven MOT (Kim et al, 2003;, one still obtains the bimodal distribution.…”