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Magnon Spin-Momentum Locking: Various Spin Vortices and Dirac magnons in Noncollinear Antiferromagnets

机译:磁振子自旋动量锁定:非共线反铁磁体中的各种自旋涡和狄拉克磁振子

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摘要

We generalize the concept of the spin-momentum locking to magnonic systems and derive the formula to calculate the spin expectation value for one-magnon states of general two-body spin Hamiltonians. We give no-go conditions for magnon spin to be independent of momentum. As examples of the magnon spinmomentum locking, we analyze a one-dimensional antiferromagnet with the Neel order and two-dimensional kagome lattice antiferromagnets with the 120 degrees structure. We find that the magnon spin depends on its momentum even when the Hamiltonian has the z-axis spin rotational symmetry, which can be explained in the context of a singular band point or a U(1) symmetry breaking. A spin vortex in momentum space generated in a kagome lattice antiferromagnet has the winding number Q = -2, while the typical one observed in topological insulator surface states is characterized by Q = +1. A magnonic analogue of the surface states, the Dirac magnon with Q = +1, is found in another kagome lattice antiferromagnet. We also derive the sum rule for Q by using the Poincare-Hopf index theorem.
机译:我们将自旋动量锁定的概念推广到了强子系统,并推导了用于计算一般两体自旋哈密顿量的一磁子态的自旋期望值的公式。我们给出了使磁振子自旋独立于动量的通过条件。作为磁振子自旋动锁的例子,我们分析了具有Neel阶的一维反铁磁体和具有120度结构的二维Kagome晶格反铁磁体。我们发现,即使哈密顿量具有z轴自旋旋转对称性,磁振子自旋也取决于其动量,这可以在奇异带点或U(1)对称性破裂的情况下得到解释。在kagome晶格反铁磁体中产生的动量空间中的自旋涡旋的绕组数为Q = -2,而在拓扑绝缘子表面状态下观察到的典型自旋涡旋的特征为Q = +1。在另一个kagome晶格反铁磁体中发现了一种表面状态的强磁模拟物,即狄拉克磁振,其Q = +1。我们还使用Poincare-Hopf指数定理推导Q的求和规则。

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  • 来源
    《Physical review letters》 |2017年第10期|107205.1-107205.6|共6页
  • 作者

    Okuma Nobuyuki;

  • 作者单位

    Univ Tokyo, Dept Phys, Hongo 7-3-1, Tokyo 1130033, Japan;

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  • 正文语种 eng
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