Phase diagram of vortices in the polar phase of spin-1 Bose-Einstein condensates

TL;DR

This paper theoretically explores the phase diagram of lowest-energy vortices in the polar phase of spin-1 Bose-Einstein condensates, identifying three vortex types and analyzing their stability, transitions, and core structures.

Contribution

It classifies and characterizes the three types of lowest-energy vortices in the polar phase, including their core structures and phase transitions, using Bogoliubov and Ginzburg--Landau theories.

Findings

Identified three vortex types: elliptic AF-core, axisymmetric F-core, and N-core.

Determined stability conditions based on quadratic Zeeman energy and interactions.

Analyzed phase transitions and critical behavior of vortex core changes.

Abstract

The phase diagram of lowest-energy vortices in the polar phase of spin-1 Bose--Einstein condensates is investigated theoretically. Singly quantized vortices are categorized by the local ordered state in the vortex core and three types of vortices are found as lowest-energy vortices, which are elliptic AF-core vortices, axisymmetric F-core vortices, and N-core vortices. These vortices are named after the local ordered state, ferromagnetic (F), antiferromagnetic (AF), broken-axisymmetry (BA), and normal (N) states apart from the bulk polar (P) state. The N-core vortex is a conventional vortex, in the core of which the superfluid order parameter vanishes. The other two types of vortices are stabilized when the quadratic Zeeman energy is smaller than a critical value. The axisymmetric F-core vortex is the lowest-energy vortex for ferromagnetic interaction, and it has an F core surrounded by a BA skin that forms a ferromagnetic-spin texture, as exemplified by the localized Mermin--Ho texture. The elliptic AF-core vortex is stabilized for antiferromagnetic interaction; the vortex core has both nematic-spin and ferromagnetic orders locally and is composed of the AF-core soliton spanned between two BA edges. The phase transition from the N-core vortex to the other two vortices is continuous, whereas that between the AF-core and F-core vortices is discontinuous. The critical point of the continuous vortex-core transition is computed by the perturbation analysis of the Bogoliubov theory and the Ginzburg--Landau formalism describes the critical behavior. The influence of trapping potential on the core structure is also investigated.