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层状六方氮化硼中的巨大激子效应。

Huge excitonic effects in layered hexagonal boron nitride.

作者信息

Arnaud B, Lebègue S, Rabiller P, Alouani M

机构信息

Groupe Matière condensée et Matériaux (GMCM), Campus de Beaulieu - Bat 11 A, 35042 Rennes Cedex, France, EU.

出版信息

Phys Rev Lett. 2006 Jan 20;96(2):026402. doi: 10.1103/PhysRevLett.96.026402. Epub 2006 Jan 18.

Abstract

The all-electron GW approximation energy band gap of bulk hexagonal boron nitride is shown to be of indirect type. The resulting computed in-plane polarized optical spectrum, obtained by solving the Bethe-Salpeter equation for the electron-hole two-particle Green function, is in excellent agreement with experiment and has a strong anisotropy compared to out-of-plane polarized spectrum. A detailed analysis of the excitonic structures within the band gap shows that the low-lying excitons belong to the Frenkel class and are tightly confined within the layers. The calculated exciton binding energy is much larger than that obtained by Watanabe et al. [Nat. Mater. 3, 404 (2004).] based on a Wannier model assuming h-BN to be a direct-band-gap semiconductor.

摘要

块状六方氮化硼的全电子GW近似能带隙被证明是间接型的。通过求解电子-空穴双粒子格林函数的贝特-萨尔皮特方程得到的计算出的面内偏振光谱与实验结果非常吻合,并且与面外偏振光谱相比具有很强的各向异性。对带隙内激子结构的详细分析表明,低能激子属于弗伦克尔类,并且被紧密限制在层内。计算得到的激子结合能比渡边等人[《自然·材料》3, 404 (2004年)]基于假设h-BN为直接带隙半导体的万尼尔模型所得到的结果大得多。

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