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AIP conference proceedings

Integrable case of two vortices in a perfect fluid in a cylindrical domain

S.V. Sokolov, Рамоданов Сергей Михайлович

Published Jan 1, 2022• 0 citations
Publisher

Abstract

This paper is concerned with a system of two vortex filaments in a Bose-Einstein condensate enclosed in a harmonic trap. Such a problem is a restriction for the more complicated case of a circular cylinder rigid body and two rectilinear vortex filaments. For these conditions we propose that rigid body has a infinitely big mass. Here we present the Hamiltonian form of equations of motion and explicitly show that system is integrable in Liouville sense. Some bifurcation diagram is constructed, and analysis of bifurcations of Liouville tori is carried out for the case of opposite-signed vortices.

DOI
10.1063/5.0119934

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This paper is concerned with a system of two vortex filaments in a Bose-Einstein condensate enclosed in a harmonic trap. Such a problem is a restriction for the more complicated case of a circular cylinder rigid body and two rectilinear vortex filaments. For these conditions we propose that rigid body has a infinitely big mass. Here we present the Hamiltonian form of equations of motion and explicitly show that system is integrable in Liouville sense. Some bifurcation diagram is constructed, and analysis of bifurcations of Liouville tori is carried out for the case of opposite-signed vortices.
The equation of motion of a quantized vortex filament in a trapped Bose–Einstein condensate [A. A. Svidzinsky and A. L. Fetter, Phys. Rev. A 62, 063617 (2000)] has been generalized to the case of an arbitrary anharmonic anisotropic rotating trap and presented in the variational form. For condensate density profiles of the form ρ = f(x 2 + y 2 + ReΨ(x + iy)) in the presence of the plane of symmetry y = 0, the solutions x(z) describing stationary vortices of U and S types coming to the surface and solitary waves have been found in quadratures. Analogous three-dimensional configurations of the vortex filament uniformly moving along the z axis have also been found in strictly cylindrical geometry. The dependence of solutions on the form of the function f(q) has been analyzed.
We have studied numerically the Hamiltonian dynamics of two same-sign point vortices in an effectively two-dimensional, harmonically trapped Bose-Einstein condensate. We have found in the phase space of the system an impenetrable wall that divides the dynamics into two distinct and exhaustive types. In the two-dimensional position-coordinate space, the first type corresponds to intersecting single-vortex orbits and the second type to orbits that have no points in common. The two types are also easily distinguished in the two-dimensional space spanned by the radial and angular velocities of the vortices: In the first type, both single-vortex orbits are the same simple loop in this two-dimensional space, whereas in the second type the two orbits constitute two nonintersecting loops. The phase-space-dividing wall is distinct from the bifurcation curve of rigidly rotating states found by Navarro et al. [Phys. Rev. Lett. 110, 225301 (2013)].
In this paper, we consider the dynamics of two interacting point vortex rings in a Bose – Einstein condensate. The existence of an invariant manifold corresponding to vortex rings is proved. Equations of motion on this invariant manifold are obtained for an arbitrary number of rings from an arbitrary number of vortices. A detailed analysis is made of the case of two vortex rings each of which consists of two point vortices where all vortices have same topological charge. For this case, partial solutions are found and a complete bifurcation analysis is carried out. It is shown that, depending on the parameters of the Bose – Einstein condensate, there are three different types of bifurcation diagrams. For each type, typical phase portraits are presented.