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

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3 Vortex arrays in mean-field Thomas-Fermi<br />

regime<br />

Feynman’s mean vortex density in a <strong>rotating</strong> superfluid<br />

• solid-body rotation has v sb = Ω × r<br />

• v sb has constant vorticity ∇ × v sb = 2Ω<br />

• each quantized vortex at r j has localized vorticity<br />

∇ × v = 2π<br />

M δ(2) (r − r j ) ẑ<br />

• assume N v vortices uniformly distributed in area A<br />

bounded by contour C<br />

• circulation around C is N v × 2π/M<br />

• but circulation in A is also 2ΩA<br />

• hence vortex density is n v = N v /A = MΩ/π<br />

• area per vortex 1/n v is π/MΩ ≡ πl 2 which defines<br />

radius l = √ /MΩ of circular cell<br />

• intervortex spacing ∼ 2l decreases like 1/ √ Ω<br />

• analogous to quantized flux lines (charged vortices) in<br />

type-II superconductors<br />

18

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