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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >SU(N) spin-wave theory: Application to spin-orbital Mott insulators
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SU(N) spin-wave theory: Application to spin-orbital Mott insulators

机译:SU(N)自旋波理论:在自旋轨道莫特绝缘子上的应用

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We present the application of the SU(N) spin-wave theory to spin-orbital Mott insulators whose ground states exhibit magnetic orders. When taking both spin and orbital degrees of freedom into account rather than projecting Hilbert space onto the Kramers doublet, which is the lowest spin-orbital locked energy levels, the SV(N) spin-wave theory should take the place of the SU(2) one due to the inevitable spin-orbital multipole exchange interactions. To implement the application, we introduce an efficient general local mean-field method, which involves all local fluctuations, and develop the SU(N) linear spin-wave theory. Our approach is tested firstly by calculating the multipolar spin-wave spectra of the SU(4) antiferromagnetic model. Then, we apply it to spin-orbital Mott insulators. It is revealed that the Hund's coupling would influence the effectiveness of the isospin-1/2 picture when the spin-orbital coupling is not large enough. We further carry out the SU(N) spin-wave calculations of two materials. a-RuCl_3 and Sr_2IrO_4. and find that the magnonic and spin-orbital excitations are consistent with experiments.
机译:我们介绍了SU(N)自旋波理论在自旋轨道Mott绝缘子上的应用,该绝缘子的基态表现出磁阶。当考虑自旋和轨道自由度而不是将希尔伯特空间投影到自旋轨道锁定能级最低的Kramers doublet上时,SV(N)自旋波理论应取代SU(2 )之一是由于不可避免的自旋轨道多极交换相互作用。为了实现该应用,我们引入了一种有效的通用局部均值方法,该方法涉及所有局部波动,并发展了SU(N)线性自旋波理论。首先,通过计算SU(4)反铁磁模型的多极自旋波谱来测试我们的方法。然后,将其应用于自旋轨道Mott绝缘子。揭示了当自旋轨道耦合不够大时,洪德耦合将影响等位旋1/2图片的有效性。我们进一步对两种材料进行SU(N)自旋波计算。 a-RuCl_3和Sr_2IrO_4。并发现强磁和自旋轨道激发与实验一致。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2018年第20期|205106.1-205106.10|共10页
  • 作者单位

    National Laboratory of Solid Slate Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China;

    National Laboratory of Solid Slate Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China;

    National Laboratory of Solid Slate Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China and Collaborative Innovation Center of Advanced Microstructures, Nanjing University, Nanjing 210093, China;

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