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arXiv 1306.2769cond-mat.str-el
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关联铁磁Kondo晶格模型中的磁振子自能:锰氧化物中磁振子激发的自旋-电荷耦合效应

Magnon self energy in the correlated ferromagnetic Kondo lattice model: spin-charge coupling effects on magnon excitations in manganites

Dheeraj Kumar Singh, Avinash Singh

摘要:

利用图解展开法计算了关联铁磁Kondo晶格模型中自旋-电荷耦合引起的磁振子自能。系统地将自能和顶点校正形式的相关效应,扩展计划明确地保留了连续的自旋旋转对称性,因此戈德斯通模式。由于在中等耦合和铁磁锰氧化物相关的最佳带填充下,关联FKLM的重整化磁振子能量几乎与关联项无关。即使在更高的能带填充下,尽管表现出整体的非海森堡行为,但在Γ-X方向上的磁振子色散仍然保持接近海森堡形式。因此,实验观察到的掺杂依赖区界磁振子软化必须归因于自旋轨道耦合效应。

英文摘要:

Magnon self energy due to spin-charge coupling is calculated for the correlated ferromagnetic Kondo lattice model using a diagrammatic expansion scheme. Systematically incorporating correlation effects in the form of self-energy and vertex corrections, the expansion scheme explicitly preserves the continuous spin rotation symmetry and hence the Goldstone mode. Due to a near cancellation of the correlation-induced quantum correction terms at intermediate coupling and optimal band filling relevant for ferromagnetic manganites, the renormalized magnon energies for the correlated FKLM are nearly independent of correlation term. Even at higher band fillings, despite exhibiting overall non-Heisenberg behavior, magnon dispersion in the Γ-X direction retains nearly Heisenberg form. Therefore, the experimentally observed doping dependent zone-boundary magnon softening must be ascribed to spin-orbital coupling effects.

机构、总结、中文摘要均由AI分析而来,可能存在错误,请以论文正文为准。

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