Abstract

We present the phase diagram, the underlying stability and magnetic properties as well as the dynamics of nonlinear solitary wave excitations arising in the distinct phases of a harmonically confined spinor F = 1 Bose–Einstein condensate. Particularly, it is found that nonlinear excitations in the form of dark–dark–bright solitons exist in the antiferromagnetic and in the easy-axis phase of a spinor gas, being generally unstable in the former while possessing stability intervals in the latter phase. Dark–bright–bright solitons can be realized in the polar and the easy-plane phases as unstable and stable configurations respectively; the latter phase can also feature stable dark–dark–dark solitons. Importantly, the persistence of these types of states upon transitioning, by means of tuning the quadratic Zeeman coefficient from one phase to the other is unravelled. Additionally, the spin-mixing dynamics of stable and unstable matter waves is analyzed, revealing among others the coherent evolution of magnetic dark–bright, nematic dark–bright–bright and dark–dark–dark solitons. Moreover, for the unstable cases unmagnetized or magnetic droplet-like configurations and spin-waves consisting of regular and magnetic solitons are seen to dynamically emerge remaining thereafter robust while propagating for extremely large evolution times. Interestingly, exposing spinorial solitons to finite temperatures, their anti-damping in trap oscillation is showcased. It is found that the latter is suppressed for stronger bright soliton component ‘fillings’. Our investigations pave the wave for a systematic production and analysis involving spin transfer processes of such waveforms which have been recently realized in ultracold experiments.

Highlights

  • Ultracold atoms constitute ideal platforms for investigating the nonlinear behavior of quantum many- body systems due to their high degree of controllability and isolation from the environment [1,2,3]

  • We present the phase diagram, the underlying stability and magnetic properties as well as the dynamics of nonlinear solitary wave excitations arising in the distinct phases of a harmonically confined spinor F = 1 Bose-Einstein condensate

  • Owing to the far richer phase diagram exhibited by such gases [37] already several works have been devoted in studying a variety of nonlinear excitations that arise in them [40,41,42,43,44,45]

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Summary

INTRODUCTION

Ultracold atoms constitute ideal platforms for investigating the nonlinear behavior of quantum many- body systems due to their high degree of controllability and isolation from the environment [1,2,3]. Owing to the far richer phase diagram exhibited by such gases [37] (see, [38] for a recent discussion and [39] for the impact of many-body effects) already several works have been devoted in studying a variety of nonlinear excitations that arise in them [40,41,42,43,44,45] These include for instance spin domains [46, 47], spin textures [48, 49], the very recently experimentally observed dark-dark-bright (DDB) and dark-bright-bright (DBB) solitons [50] (and variants [51, 52], as well as interactions [22] thereof) and even twisted magnetic solitons [53].

SPINOR SETUP AND MAGNETIZATION MEASURES
PHASE DIAGRAM OF NONLINEAR EXCITATIONS
Ground state phase diagram
Phase diagram of solitonic excitations
STABILITY ANALYSIS AND DYNAMICS OF SPINOR SOLITONS
Antiferromagnetic DDB matter waves
Polar DBB solitons
Easy-Axis symmetry broken DDB solitons
Nematic DBB and DDD solitons
FINITE TEMPERATURE EFFECTS ON SPINOR SOLITONS
CONCLUSIONS
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