Low-Lying Superfluid States in a Rotating Annulus

Abstract
The low-lying states of rotating liquid He II in an annulus (R1<r<R2) are studied with the model of a classical inviscid fluid. An exact hydrodynamic solution is obtained with the method of images for a system consisting of rectilinear vortices with circulation κ combined with circulation Γ1 about the inner cylinder. The energy and angular momentum are calculated, both for an arbitrary configuration of vortices and for the particular configuration of a symmetric ring of l vortices. If Γ1 is treated as a variational parameter, the critical angular velocity Ω0 for the appearance of vortices in a narrow annulus is (κπd2)ln(2dπa), where d is the width of the annulus and a is the radius of the vortex core. For Ω<Ω0, the equilibrium state is an irrotational (vortex-free) flow with quantized circulation nκ(n=1,2,); these levels are equally spaced, and a given quantum state represents the lowest free energy only in a narrow angular-velocity interval of κ2πR2, where R is the mean radius of the annulus. The maximum quantum number of irrotational circulation is 2πR2Ω0κ=2(Rd)2ln(2dπa)1. For Ω>Ω0, the vortices lie on the circumference of a ring midway between the walls, and the number of vortices increases rapidly with Ω. If Γ1 is constrained to vanish identically, the critical angular velocity Ωc for the appearance of vortices in a narrow annulus is of order κ2πRd; this is equivalent to Feynman's critical velocity vc=O(md) for singly quantized vortices with κ=hm. In the opposite limit of a wide annulus (R1R2), the equilibrium state is shown to agree with Vinen's earlier calculations.