半金属/半导体材料中的激子磁化率函数:激子凝聚态的形成

T. Do
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引用次数: 0

摘要

通过分析包含电子-声子相互作用的二维扩展Falicov-Kimbol模型中的激子磁化率函数,研究了半金属/半导体材料中激子的凝聚态。利用Hartree-Fock近似计算了系统的激子磁化率。根据数值结果,建立了激子凝聚态的相图。相图证实了电子-声子耦合和库仑吸引在低温下建立激子凝聚相中起着重要的作用。当电子-声子耦合足够大时,激子的凝聚相在库仑吸引的有限范围内存在。根据电子-声子耦合和库仑吸引,还指出了激子凝聚相的BCS-BEC交叉。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
The Excitonic Susceptibility Function in Semimetal/semiconductor Materials: Formation of the Excitonic Condensate State
The condensate state of excitons in semimetal/semiconductor materials has been considered by analyzing the excitonic susceptibility function in the 2D extended Falicov-Kimbol model including electron-phonon interaction. The excitonic susceptibility in the system has calculated by using the Hartree-Fock approximation. From numerical results, we have set up phase diagrams ofthe excitonic condensate state. Phase diagrams confirm that the electron-phonon coupling plays an important role as well as the Coulomb attraction does in establishing the excitonic condensed phase at low temperature. The condensate phase of excitons is found within a limited range of the Coulomb attraction as the electron-phonon coupling is large enough. Depending on theelectron-phonon coupling and the Coulomb attraction, the BCS-BEC crossover of the excitonic condensation phase has also been pointed out.
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