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Strong coupling phases of the spin-orbit-coupled spin-1 Bose-Hubbard chain: odd integer Mott lobes and helical magnetic phases

机译:自旋轨道耦合自旋-1 Bose-Hubbard的强耦合相位   链:奇整数mott叶和螺旋磁相

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摘要

We study the odd integer filled Mott phases of a spin-1 Bose-Hubbard chainand determine their fate in the presence of a Raman induced spin-orbit couplingwhich has been achieved in ultracold atomic gases; this system is described bya quantum spin-1 chain with a spiral magnetic field. The spiral magnetic fieldinitially induces helical order with either ferromagnetic or dimer orderparameters, giving rise to a spiral paramagnet at large field. The spiralferromagnet-to-paramagnet phase transition is in a novel universality class,with critical exponents associated with the divergence of the correlationlength $\nu \approx 2/3$ and the order parameter susceptibility $\gamma \approx1/2$. We solve the effective spin model exactly using the density matrixrenormalization group, and compare with both a large-$S$ classical solution anda phenomenological Landau theory. We discuss how these exotic bosonic magneticphases can be produced and probed in ultracold atomic experiments in opticallattices.
机译:我们研究了自旋1 Bose-Hubbard链的奇数整数填充Mott相,并确定了在超冷原子气体中实现的拉曼感应自旋轨道耦合存在下它们的命运;该系统由具有螺旋磁场的量子自旋1链描述。螺旋磁场首先以铁磁或二聚体顺序参数感应出螺旋顺序,从而在大磁场下产生螺旋顺磁。螺旋铁磁体到顺磁体的相变属于新颖的通用性类别,其临界指数与相关长度$ \ nu \约2/3 $和阶数参数磁化率$ \ gamma \ approx1 / 2 $的发散有关。我们使用密度矩阵重新归一化组精确地求解了有效的自旋模型,并与大型S $经典解和现象学Landau理论进行了比较。我们讨论了如何在光学晶格的超冷原子实验中产生并探测这些奇异的玻色子磁相。

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