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非中心对称宽禁带半导体中激子共振处强烈增强的位移电流。

Strongly enhanced shift current at exciton resonances in a noncentrosymmetric wide-gap semiconductor.

作者信息

Nakamura Masao, Chan Yang-Hao, Yasunami Takahiro, Huang Yi-Shiuan, Guo Guang-Yu, Hu Yajian, Ogawa Naoki, Chiew Yiling, Yu Xiuzhen, Morimoto Takahiro, Nagaosa Naoto, Tokura Yoshinori, Kawasaki Masashi

机构信息

RIKEN Center for Emergent Matter Science (CEMS), Wako, Japan.

Institute of Atomic and Molecular Sciences, Academia Sinica, Taipei, Taiwan.

出版信息

Nat Commun. 2024 Nov 16;15(1):9672. doi: 10.1038/s41467-024-53541-6.

Abstract

Excitons are fundamental quasiparticles that are ubiquitous in photoexcited semiconductors and insulators. Despite causing a sharp and strong photoabsorption near the interband absorption edge, charge-neutral excitons do not yield photocurrent in conventional photovoltaic processes unless dissociated into free charge carriers. Here, we experimentally demonstrate that excitons can directly contribute to photocurrent generation through a nonlinear light-matter interaction in a noncentrosymmetric semiconductor CuI. Epitaxial thin films of CuI exhibit a substantial enhancement of photocurrent at exciton resonance energies even below the bandgap. From the light polarization dependence, this photocurrent is identified to be shift current, a nonlinear photocurrent driven by the change in the geometric Berry phase of electron wave functions upon the optical transition. The shift current at the exciton resonance is much larger than that induced above the band gap by free electron-hole excitation, and their signs are opposite. First-principles calculations elucidate that the sign and magnitude of the exciton shift current are strongly dependent on the strain in the thin film. The present study reveals the crucial role of excitons in enhancing the shift current magnitude and its strain sensitivity, and will open an unprecedented route for efficient manipulation of nonlinear optical effects.

摘要

激子是光激发半导体和绝缘体中普遍存在的基本准粒子。尽管电荷中性激子在带间吸收边缘附近会引起强烈的光吸收,但在传统的光伏过程中,除非解离成自由电荷载流子,否则它们不会产生光电流。在这里,我们通过实验证明,在非中心对称半导体CuI中,激子可以通过非线性光与物质相互作用直接对光电流产生做出贡献。即使在低于带隙的激子共振能量下,CuI外延薄膜的光电流也会显著增强。从光偏振依赖性来看,这种光电流被确定为移位电流,即由光跃迁时电子波函数的几何贝里相位变化驱动的非线性光电流。激子共振处的移位电流比自由电子-空穴激发在带隙以上诱导的移位电流大得多,且它们的符号相反。第一性原理计算表明,激子移位电流的符号和大小强烈依赖于薄膜中的应变。本研究揭示了激子在增强移位电流大小及其应变敏感性方面的关键作用,并将为有效操纵非线性光学效应开辟一条前所未有的途径。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/8995/11569220/8522641f3b13/41467_2024_53541_Fig1_HTML.jpg

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