“…This restriction can be avoided by introducing an additional quartic potential, so that the combined trapping potential in the xy plane becomes V ex (r) = (1/2)mω 2 ⊥ (r 2 + λr 4 /a 2 ho ), where the dimensionless parameter λ characterizes the relative strength of the quartic potential. The properties of a rotating condensate in an anharmonic potential have recently attracted a lot of theoretical attention (Fetter 2001b, Lundh 2002, Fischer 2003, Kasamatsu 2002a, Kavoulakis 2003, Aftalion 2004, Jackson 2004a,b, Fetter 2005, Danaila 2005, Kim 2005, Bargi 2006, Fu 2006. The vortex phases in an anharmonic trap are quite different from those in a harmonic trap, since it is possible to rotate the system arbitrarily fast.…”