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      Gauge-spin-space rotation invariant vortices in spin-orbit coupled Bose-Einstein condensates

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          Abstract

          We revisit ground states of spinor Bose-Einstein condensates with a Rashba spin-orbit coupling, and find that votices show up as a direct consequence of spontaneous symmetry breaking into a combined gauge, spin, and space rotation symmetry, which determines the vortex-core spin state at the rotating center. For the continuous combined symmetry, the total spin rotation about the rotating axis is restricted to \(2\pi\), whereas for the discrete combined symmetry, we further need 2F quantum numbers to characterize the total spin rotation for the spin-\(F\) system. For lattice phases we find that in the ground state the topological charge for each unit cell vanishes. However, we find two types of highly symmetric lattices with a nontrivial topological charge in the spin-\(\frac{1}{2}\) system based on the symmetry classification, and show that they are skyrmion crystals.

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          The topological theory of defects in ordered media

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            A spin-orbit coupled Bose-Einstein condensate

            Spin-orbit (SO) coupling -- the interaction between a quantum particle's spin and its momentum -- is ubiquitous in nature, from atoms to solids. In condensed matter systems, SO coupling is crucial for the spin-Hall effect and topological insulators, which are of extensive interest; it contributes to the electronic properties of materials such as GaAs, and is important for spintronic devices. Ultracold atoms, quantum many-body systems under precise experimental control, would seem to be an ideal platform to study these fascinating SO coupled systems. While an atom's intrinsic SO coupling affects its electronic structure, it does not lead to coupling between the spin and the center-of-mass motion of the atom. Here, we engineer SO coupling (with equal Rashba and Dresselhaus strengths) in a neutral atomic Bose-Einstein condensate by dressing two atomic spin states with a pair of lasers. Not only is this the first SO coupling realized in ultracold atomic gases, it is also the first ever for bosons. Furthermore, in the presence of the laser coupling, the interactions between the two dressed atomic spin states are modified, driving a quantum phase transition from a spatially spin-mixed state (lasers off) to a phase separated state (above a critical laser intensity). The location of this transition is in quantitative agreement with our theory. This SO coupling -- equally applicable for bosons and fermions -- sets the stage to realize topological insulators in fermionic neutral atom systems.
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              Quantized vortices in superfluidHe3

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                Author and article information

                Journal
                16 April 2013
                Article
                10.1103/PhysRevA.88.013621
                1304.4340
                f2b8d689-ce11-48ad-8162-591e7cdd9320

                http://arxiv.org/licenses/nonexclusive-distrib/1.0/

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                Custom metadata
                Phys. Rev. A 88, 013621 (2013)
                10+ pages, 5 figures
                cond-mat.quant-gas

                Quantum gases & Cold atoms
                Quantum gases & Cold atoms

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