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We compute numerically the yrast line for harmonically trapped N-boson systems with a weak repulsive contact interaction, studying the transition to a vortex state as the angular momentum L increases and approaches N. There is a smooth crossover between low and high L with no indication of a quantum phase transition; at L0ex0ex=0ex0exN there is a kink in the slope of the spectrum. Most strikingly, the energy and wave function appear to be analytical functions of L over the entire range 2≤L≤N. We confirm the structure of low- L states proposed by Mottelson as mainly single-particle excitations with two or three units of angular momentum.
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Bertsch et al. (1999) studied this question.
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