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arXiv 1707.03071cond-mat.mes-hall
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铅卤钙钛矿中的亮三重态激子

Bright triplet excitons in lead halide perovskites

Michael A. Becker, Roman Vaxenburg, Georgian Nedelcu, Peter C. Sercel, Andrew Shabaev, Michael J. Mehl, John G. Michopoulos, Samuel G. Lambrakos, Noam Bernstein… 展开作者

Michael A. Becker, Roman Vaxenburg, Georgian Nedelcu, Peter C. Sercel, Andrew Shabaev, Michael J. Mehl, John G. Michopoulos, Samuel G. Lambrakos, Noam Bernstein, John L. Lyons, Thilo Stöferle, Rainer F. Mahrt, Maksym V. Kovalenko, David J. Norris, Gabriele Rainò, Alexander L. Efros

AI总结:

本文证明准立方铅卤钙钛矿的最低激子是光学活跃的亮激子,结合有效质量模型、群论及单纳米晶荧光测量,解释了其反常的高发射速率,并为光电子器件材料筛选提供判据。

摘要:

纳米结构半导体从被称为激子的电子态发光[1]。根据洪德规则[2],有机材料中能量最低的激子应当是发光很弱的三重态。类似地,在所有已知无机半导体中,最低激子能级也被认为在光学上是不活跃的。这些系统可以弛豫进入的“暗”激子阻碍了基于半导体纳米结构的发光器件。尽管已经发展出削弱其影响的策略[3-5],但尚未发现任何材料中最低激子是亮的。本文我们证明准立方铅卤钙钛矿中的最低激子在光学上是活跃的。我们首先利用有效质量模型和群论探索这种可能性,当钙钛矿导带中的强自旋轨道耦合与Rashba效应[6-10]相结合时,这种情况就可能出现。随后我们将模型应用于CsPbX3(X=Cl,Br,I)纳米晶[11],并在单纳米晶水平上测量了依赖于尺寸和组分的荧光。最低激子的亮特性直接解释了这些材料反常的光子发射速率,它们在室温[13-16]和低温[17]下分别比任何其他半导体纳米晶快20倍和1000倍[12]。通过对低温荧光光谱精细结构的详细分析,亮激子得到进一步证实。对于已经用于照明[19,20]、激光器[21,22]和显示器[23]的半导体纳米晶[18]而言,这些光学活跃的激子可以带来发射更亮、吸收更强的材料。更一般地,我们的结果为识别其他表现出亮激子的半导体提供了判据,对光电子器件具有潜在的广泛意义。

英文摘要:

Nanostructured semiconductors emit light from electronic states known as excitons[1]. According to Hund's rules[2], the lowest energy exciton in organic materials should be a poorly emitting triplet state. Analogously, the lowest exciton level in all known inorganic semiconductors is believed to be optically inactive. These 'dark' excitons (into which the system can relax) hinder light-emitting devices based on semiconductor nanostructures. While strategies to diminish their influence have been developed[3-5], no materials have been identified in which the lowest exciton is bright. Here we show that the lowest exciton in quasi-cubic lead halide perovskites is optically active. We first use the effective-mass model and group theory to explore this possibility, which can occur when the strong spin-orbit coupling in the perovskite conduction band is combined with the Rashba effect [6-10]. We then apply our model to CsPbX3 (X=Cl,Br,I) nanocrystals[11], for which we measure size- and composition-dependent fluorescence at the single-nanocrystal level. The bright character of the lowest exciton immediately explains the anomalous photon-emission rates of these materials, which emit 20 and 1,000 times faster[12] than any other semiconductor nanocrystal at room[13-16] and cryogenic[17] temperatures, respectively. The bright exciton is further confirmed by detailed analysis of the fine structure in low-temperature fluorescence spectra. For semiconductor nanocrystals[18], which are already used in lighting[19,20], lasers[21,22], and displays[23], these optically active excitons can lead to materials with brighter emission and enhanced absorption. More generally, our results provide criteria for identifying other semiconductors exhibiting bright excitons with potentially broad implications for optoelectronic devices.

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