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Emergent gauge field and the Lifshitz transition of spin-orbit coupled bosons in one dimension

机译:一维自旋轨道耦合玻色子的新兴尺度场和Lifshitz跃迁

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In the presence of strong spin-independent interactions and spin-orbit coupling, we show that the spinor Bose liquid confined to one spatial dimension undergoes an interaction- or density-tuned quantum phase transition similar to one theoretically proposed for itinerant magnetic solid-state systems. The order parameter describes broken Zsub2/sub inversion symmetry, with the ordered phase accompanied by non-vanishing momentum which is generated by fluctuations of an emergent dynamical gauge field at the phase transition. This quantum phase transition has dynamical critical exponent z???2, typical of a Lifshitz transition, but is described by a nontrivial interacting fixed point. From direct numerical simulation of the microscopic model, we extract previously unknown critical exponents for this fixed point. Our model describes a realistic situation of 1D ultracold atoms with Raman-induced spin-orbit coupling, establishing this system as a platform for studying exotic critical behavior of the Hertz-Millis type.
机译:在强自旋无关的相互作用和自旋轨道耦合的存在下,我们表明,受限于一个空间维度的自旋玻色子液体经历了相互作用或密度调节的量子相变,类似于理论上为迭代磁性固体系统提出的。阶次参数描述了破碎的Z 2 反演对称性,阶次相伴随着不消失的动量,动量是由相变时出现的动态规范场的波动产生的。该量子相变具有典型的Lifshitz跃迁的动态临界指数z≈2,但是由非平凡的相互作用固定点描述。从微观模型的直接数值模拟中,我们提取了该固定点先前未知的临界指数。我们的模型描述了一维超冷原子与拉曼诱导的自旋-轨道耦合的现实情况,从而将该系统建立为研究Hertz-Millis型奇异临界行为的平台。

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