Abstract

We derive a fully quantum-mechanical equation of motion for a vortex in a 2-dimensional Bose superfluid, in the temperature regime where the normal fluid density ρn(T)ρ_n(T) is small. The coupling between the vortex "zero mode" and the quasiparticles has no term linear in the quasiparticle variables -- the lowest-order coupling is quadratic. We find that as a function of the dimensionless frequency Ω~=ℏΩ/kBT\tilde Ω= \hbar Ω/k_BT, the standard Hall-Vinen/Iordanskii equations are valid when Ω~≪1\tilde Ω\ll 1 (the "classical regime"), but elsewhere, the equations of motion become highly retarded, with significant experimental implications when Ω~≳1\tilde Ω\gtrsim 1.

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