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Rapidly rotating Bose-Einstein condensates∗ Alexander Fetter ...

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Quantitative description of <strong>rotating</strong> TF condensate<br />

Kinetic energy of condensate involves<br />

2 ∫ ∫<br />

dV |∇Ψ| 2 = dV 1 2M<br />

2 Mv2 |Ψ| 2<br />

} {{ }<br />

superflow energy<br />

∫<br />

dV (∇|Ψ|) 2<br />

}<br />

2M<br />

{{ }<br />

density variation<br />

+ 2<br />

where Ψ = exp(iS)|Ψ| and v = ∇S/M is flow velocity<br />

• generalized TF approximation: retain the energy of<br />

superflow but ignore the energy from density variation<br />

• this approximation will fail eventually when vortex<br />

lattice becomes dense and cores start to overlap<br />

• in <strong>rotating</strong> frame, generalized TF energy functional is<br />

∫<br />

E ′ [Ψ] = dV [( 1<br />

2 Mv2 + V tr − MΩ · r × v ) |Ψ| 2<br />

+ 1 2 g|Ψ|4]<br />

• here, v is flow velocity generated by all the vortices<br />

20

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