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首页> 外文期刊>Physical review. B, Condensed Matter And Materals Physics >Magnon-phonon coupling effects on the indirect K-edge resonant inelastic x-ray scattering spectrum of a two-dimensional Heisenberg antiferromagnet
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Magnon-phonon coupling effects on the indirect K-edge resonant inelastic x-ray scattering spectrum of a two-dimensional Heisenberg antiferromagnet

机译:磁振子-声子耦合对二维Heisenberg反铁磁体的间接K边共振非弹性X射线散射谱的影响

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摘要

We compute the effects of magnon-phonon coupling on the indirect K-edge bimagnon resonant inelastic x-ray scattering (RIXS) intensity spectrum of a square lattice Heisenberg antiferromagnet. We analyze the effects of competing nearest and next-nearest magnetic and magnon-phonon coupling interaction in the RIXS spectrum, for both the antiferromagnetic (AF) and the collinear antiferromagnetic (CAF) phases of the model. Utilizing the Dyson-Maleev representation of spin operators, the Bethe-Salpeter ladder approximation scheme for the bimagnon interacting channel, and considering the lowest-order magnon-phonon-magnon scattering interaction, we highlight distinct features in the x-ray spectrum. Considering damping effects, arising due to the presence of phonons, we find that in the AF phase the RIXS intensity spectrum attains a maximum value primarily localized around the K (± 2/π, ±2/π) point. For the CAF phase, the intensity is broadly distributed with a significant scattering intensity located around the Y (± 2/π, 0) point. Furthermore, in the CAF phase for suitable anisotropy, nearest-, and next-nearest-neighbor interaction parameters, the phonon effects can manifest as a distinct peak both below and above the bimagnon peak. Such a feature is in contrast to the antiferromagnetic spectrum where the effect due to the phonon peak was located consistently beyond the bimagnon peak in the high-energy end of the spectrum. Additionally, in the CAF phase we find the RIXS bimagnon-phonon spectrum to be more sensitive to anisotropy compared to its antiferromagnetic counterpart. We conclude that the ultimate effect of magnon-phonon effects in the indirect K-edge RIXS spectrum, in both the antiferromagnetic and the collinear antiferromagnetic phases, is an observable effect.
机译:我们计算了方格海森堡反铁磁体的间接K边双磁子共振非弹性X射线散射(RIXS)强度谱上的磁子-声子耦合效应。我们针对模型的反铁磁(AF)和共线反铁磁(CAF)相分析了RIXS光谱中竞争最近和最接近的磁和磁振子耦合相互作用的影响。利用自旋算子的戴森-马列夫(Dyson-Maleev)表示,双磁子相互作用通道的Bethe-Salpeter梯形近似方案,并考虑最低阶的磁子-声子-磁子散射相互作用,我们突出了X射线光谱中的独特特征。考虑到由于声子的存在而产生的阻尼效应,我们发现在AF阶段,RIXS强度谱获得了一个最大值,该最大值主要位于K(±2 /π,±2 /π)点附近。对于CAF阶段,强度分布广泛,且散射强度位于Y(±2 /π,0)点附近。此外,在CAF相中,为了获得适当的各向异性,最近邻和次近邻相互作用参数,声子效应可表现为双磁子峰以下和以上的明显峰。这种特征与反铁磁光谱相反,在反铁磁光谱中,由于声子峰的影响始终位于光谱高能端的双磁子峰之外。此外,在CAF阶段,与反铁磁对应物相比,我们发现RIXS双磁子-声子光谱对各向异性更敏感。我们得出结论,在反铁磁相和共线反铁磁相中,间接K边RIXS谱中的磁子声子效应的最终效应都是可观察到的效应。

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  • 来源
    《Physical review. B, Condensed Matter And Materals Physics》 |2017年第14期|144436.1-144436.13|共13页
  • 作者单位

    State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Sun Yat-Sen University, Guangzhou 510275, China;

    State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Sun Yat-Sen University, Guangzhou 510275, China ,Department of Chemistry and Physics, Augusta University, 1120 15th Street, Augusta, Georgia 30912, USA;

    Department of Chemistry and Physics, Augusta University, 1120 15th Street, Augusta, Georgia 30912, USA;

    State Key Laboratory of Optoelectronic Materials and Technologies, School of Physics, Sun Yat-Sen University, Guangzhou 510275, China;

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