Search arXiv⌕ Search

arXiv · 2610.18527

Phases of a rotating Bose-Einstein condensate trapped in a hard-wall potential

Abstract

We investigate the rotational properties of a zero-temperature Bose-Einstein condensed gas, which is confined in a hard-wall potential. For weak interactions the gas carries its angular momentum via vortices of multiple quantization. As the coupling increases and for sufficiently slow rotational frequencies of the trap, the multiply-quantized vortex states become unstable against a mixed state. For stronger couplings, as the angular frequency of the trap increases, there is a transition from a vortex lattice, to a vortex lattice with a hole at the trap center, and finally to a giant vortex. For weak effective attractive interactions we still have vortices of multiple quantization. These states become unstable towards states which break the axial symmetry of the problem and resemble center-of-mass excitation, as the coupling becomes more negative. Finally, for even more attractive forces, the system becomes unstable against collapse.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Hélène Perrin, G. M. Kavoulakis. 2026-10-13. Phases of a rotating Bose-Einstein condensate trapped in a hard-wall potential. https://arxiv.org/abs/2610.18527

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

Sound Wave in the Backreaction Affected Spacetime in Analogue Gravity Based on Number-Conserving Approach

Adopting a number-conserving approach, we show that the sound wave in the backreaction-affected dynamical spacetime obeys the equations of motion for a massive scalar field in an analogue spacetime. Even with backreaction, the analogue metric has the same form as that without backreaction, except that the sound velocity, fluid density, and fluid velocity incorporate small corrections that account for backreaction. Moreover, the modification of the classical fluid-dynamical equations by backreaction introduces a spacetime-dependent mass. We also present a linear form of the modified Bogoliubov-de Gennes equation with number conservation, which allows us to solve it numerically. Using a finite-size homogeneous quasi-one-dimensional Bose gas as an example, we find that backreaction enhances the canonically normal-ordered correlation function at the same point, by about $10\%$ in the bulk and up to about $20\%$ near the edges. The bulk enhancement persists when the finite imaging resolution of cold-atom experiments is taken into account.

cond-mat.quant-gas↗

Skin phase transition of a skyrmion in a ferromagnetic superfluid

Compared with a scalar Bose-Einstein condensate (BEC), a spinor BEC supports richer phenomena because of its internal spin degrees of freedom, including topological solitons such as domain walls or skyrmions. Here, we theoretically reveal three distinct axisymmetric soliton structures formed as a circular domain wall in a spin-1 BEC, connected within fixed winding numbers. We refer to these structures as the broken-axisymmetry (BA)-skin, antiferromagnetic (AF)-skin and normal-core phases. Their occurrence is controlled by the two dimensionless parameters in the absence of linear Zeeman coefficient $p=0$: $q/μ$, the ratio of the quadratic Zeeman coefficient to the chemical potential, and $c_s/c_n$, the ratio of spin interaction to the density interaction. The BA-skin and AF-skin phases exhibit local easy-plane magnetic order and local easy-plane spin-nematic order, respectively, while the normal-core phase is similar to a doubly quantized vortex analogous to that of a scalar BEC with a density depletion at the center. We obtain semi-analytical estimates of selected transition boundaries separating these phases by analyzing the Bogoliubov-de Gennes equation and also numerically confirm them by solving the Gross-Pitaevskii equation. We estimate the skyrmion radius using a hydrostatic approximation and compare the result with numerical solutions. We envision our results on skyrmions in a spin-1 BEC can trigger further investigation on novel soliton structures in a magnetic superfluid.

cond-mat.quant-gas↗

Competing delocalisation and localisation induced by the dipolar tail in fragmented lattice gases

We investigate how the long-range tail of dipole-dipole interactions modifies the dynamics of strongly interacting hard-core bosons in a one-dimensional lattice. In the nearest-neighbour model, large interactions generate an emergent Hilbert-space fragmentation into manifolds labelled by the number of nearest-neighbour bonds \(N_{\mathrm{NN}}\). The dipolar tail has a non-monotonic effect on this fragmented dynamics as the interaction-to-tunnelling ratio \(V/t\) is increased. At intermediate \(V/t\), it enhances delocalisation relative to the nearest-neighbour model by reducing the energetic detuning between neighbouring \(N_{\mathrm{NN}}\) manifolds and sustaining their hybridisation by hopping. At larger \(V/t\), the same tail lifts degeneracies within each manifold, beginning with the splitting associated with the next-nearest-neighbour bond number \(N_{\mathrm{NNN}}\), and promotes intra-manifold localisation and Hilbert-space shattering. The competition between these two effects produces a crossover from a delocalising to a localising role of the dipolar tail, visible in the late-time spatial inhomogeneity. This crossover occurs for nearly all initial states considered and persists at different fillings. Transverse confinement strengthens the short-range part of the dipolar tail and shifts the crossover to lower \(V/t\), bringing it into the regime relevant to current experiments with magnetic atoms and polar molecules.

cond-mat.quant-gas↗