2019
DOI: 10.1103/physreva.100.063633
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Coherent spin mixing via spin-orbit coupling in Bose gases

Abstract: We study beyond-mean-field properties of interacting spin-1 Bose gases with synthetic Rashba-Dresselhaus spin-orbit coupling at low energies. We derive a many-body Hamiltonian following a tight-binding approximation in quasi-momentum space, where the effective spin dependence of the collisions that emerges from spin-orbit coupling leads to dominant correlated tunneling processes that couple the different bound states. We discuss the properties of the spectrum of the derived Hamiltonian and its experimental sig… Show more

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Cited by 7 publications
(10 citation statements)
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“…Several authors have suggested a connection between spinor gases with spin-changing collisions and SOC BECs [37][38][39][40][41][42][43][44]. In this work, we show analytically that the Raman-dressed spin-1 SOC gas at low energy is equivalent, for weak Raman coupling and interactions, and zero total magnetization, to an artificial spin-1 gas with tunable spin-changing collisions.…”
mentioning
confidence: 56%
“…Several authors have suggested a connection between spinor gases with spin-changing collisions and SOC BECs [37][38][39][40][41][42][43][44]. In this work, we show analytically that the Raman-dressed spin-1 SOC gas at low energy is equivalent, for weak Raman coupling and interactions, and zero total magnetization, to an artificial spin-1 gas with tunable spin-changing collisions.…”
mentioning
confidence: 56%
“…Several authors have suggested a connection between spinor gases with spin-changing collisions and SOC BECs [12,[25][26][27][28][29][30][31]. In this work, we show analytically that the Raman-dressed spin-1 SOC gas at low energy is equivalent, for weak Raman coupling and interactions, and zero total magnetization, to an artificial spin-1 gas with tun- able spin-changing collisions.…”
mentioning
confidence: 57%
“…⟩ g is the ground state energy per particle for the single-particle Hamiltonian (17). At zero temperature, this energy corresponds to the minimum of the band (18). For non-interacting fermions, the currents are given by j (f ) 1…”
Section: B Current Distribution In the Triangular Laddermentioning
confidence: 99%
“…In the bulk SOC can stabilize exotic phases like the stripe phase [11,12], where translation invariance is spontaneously broken [13], in analogy with supersolids very recently realized in dipolar gases [14][15][16] (see also [17] for the realization supersolid-like state in a cavity). Under suitable conditions SOC gives also access to beyond-mean-field dynamics in weakly interacting dilute gases [18] (for experimental demonstrations of beyondmean-field effects due to competing interactions see [19][20][21]) by inducing spin changing collisions in F = 1 BEC (see [22]) from SU(3)-symmetric density-density interactions that are controllable. Interestingly, SOC combined with radio-frequency dressing offers a novel mechanism to achieve subwavelength optical lattices [23].…”
Section: Introductionmentioning
confidence: 99%