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Skyrmions in quantum Hall ferromagnets as spin-waves bound to unbalanced magnetic flux quanta

机译:量子霍尔铁磁体中的skyrmions作为自旋波束缚到不平衡   磁通量子

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摘要

A microscopic description of (baby)skyrmions in quantum Hall ferromagnets isderived from a scattering theory of collective (neutral) spin modes by a barequasiparticle. We start by mapping the low lying spectrum of spin waves in theuniform ferromagnet onto that of free moving spin excitons, and then we studytheir scattering by the defect of charge. In the presence of this disturbance,the local spin stiffness varies in space, and we translate it into aninhomogeneus metric in the Hilbert space supporting the excitons. An attractivepotencial is then required to preserve the symmetry under global spinrotations, and it traps the excitons around the charged defect. Thequasiparticle now carries a spin texture. Textures containing more than oneexciton are described within a mean-field theory, the interaction among theexcitons being taken into account through a new renormalization of the metric.The number of excitons actually bound depends on the Zeeman coupling, thatplays the same role as a chemical potencial. For small Zeeman energies, thedefect binds many excitons which condensate. As the bound excitons have a unitof angular momentum, provided by the quantum of magnetic flux left unbalancedby the defect of charge, the resulting texture turns out to be a topologicalexcitation of charge 1. Its energy is that given by the non-linear sigma modelfor the ground state in this topological sector, i.e. the texture is askyrmion.
机译:量子霍尔铁磁体中(婴儿)斯基米恩斯的微观描述是从准等粒子的集体(中性)自旋模式的散射理论中得出的。我们首先将均匀铁磁体中自旋波的低频谱映射到自由移动自旋激子的频谱上,然后研究由电荷缺陷引起的散射。在存在这种扰动的情况下,局部自旋刚度在空间中会发生变化,我们将其转换为支持激子的希尔伯特空间中的不均匀度量。然后,需要一个有吸引力的电位来保持整体自旋下的对称性,并且它将激子捕获在带电缺陷周围。准粒子现在带有自旋纹理。在均值场理论中描述了包含一个以上激子的纹理,通过重新对度量进行重新归一化来考虑激子之间的相互作用。实际束缚的激子数取决于塞曼耦合,起着与化学势相同的作用。对于小的塞曼能量,该缺陷结合了许多凝聚的激子。由于束缚的激子具有单位角动量,由电荷缺陷使磁通量量子不平衡而提供,因此所产生的织构证明是电荷1的拓扑激发。其能量是由非线性sigma模型给出的。此拓扑区域中的基态,即纹理是askirmion。

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