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厚壳 CuInS/ZnS 量子点,具有抑制的“闪烁”和窄的单粒子发射线宽。

Thick-Shell CuInS/ZnS Quantum Dots with Suppressed "Blinking" and Narrow Single-Particle Emission Line Widths.

机构信息

Center for High Technology Materials, University of New Mexico , Albuquerque, New Mexico 87131, United States.

出版信息

Nano Lett. 2017 Mar 8;17(3):1787-1795. doi: 10.1021/acs.nanolett.6b05118. Epub 2017 Feb 14.

Abstract

Quantum dots (QDs) of ternary I-III-VI compounds such as CuInS and CuInSe have been actively investigated as heavy-metal-free alternatives to cadmium- and lead-containing semiconductor nanomaterials. One serious limitation of these nanostructures, however, is a large photoluminescence (PL) line width (typically >300 meV), the origin of which is still not fully understood. It remains even unclear whether the observed broadening results from considerable sample heterogeneities (due, e.g., to size polydispersity) or is an unavoidable intrinsic property of individual QDs. Here, we answer this question by conducting single-particle measurements on a new type of CuInS (CIS) QDs with an especially thick ZnS shell. These QDs show a greatly enhanced photostability compared to core-only or thin-shell samples and, importantly, exhibit a strongly suppressed PL blinking at the single-dot level. Spectrally resolved measurements reveal that the single-dot, room-temperature PL line width is much narrower (down to ∼60 meV) than that of the ensemble samples. To explain this distinction, we invoke a model wherein PL from CIS QDs arises from radiative recombination of a delocalized band-edge electron and a localized hole residing on a Cu-related defect and also account for the effects of electron-hole Coulomb coupling. We show that random positioning of the emitting center in the QD can lead to more than 300 meV variation in the PL energy, which represents at least one of the reasons for large PL broadening of the ensemble samples. These results suggest that in addition to narrowing size dispersion, future efforts on tightening the emission spectra of these QDs might also attempt decreasing the "positional" heterogeneity of the emitting centers.

摘要

量子点(QD)的三元 I-III-VI 化合物,如 CuInS 和 CuInSe,作为不含镉和铅的半导体纳米材料的替代品得到了广泛的研究。然而,这些纳米结构的一个严重限制是光致发光(PL)线宽较大(通常>300 毫电子伏特),其起源尚未完全理解。甚至不清楚观察到的展宽是由于样品的显著不均匀性(例如由于尺寸多分散性)还是单个 QD 的不可避免的固有特性。在这里,我们通过对具有特别厚的 ZnS 壳的新型 CuInS(CIS)QD 进行单粒子测量来回答这个问题。与仅包含核或薄壳的样品相比,这些 QD 表现出大大增强的光稳定性,重要的是,在单粒子水平上表现出强烈抑制的 PL 闪烁。光谱分辨测量表明,单粒子,室温 PL 线宽要窄得多(低至约 60 毫电子伏特)比集合样品。为了解释这一区别,我们援引了一个模型,其中 CIS QD 的 PL 源自局域化在与 Cu 相关的缺陷上的带边电子和局域化空穴的辐射复合,并且还考虑了电子-空穴库仑耦合的影响。我们表明,发射中心在 QD 中的随机定位会导致 PL 能量发生超过 300 毫电子伏特的变化,这至少是集合样品中 PL 展宽的原因之一。这些结果表明,除了缩小尺寸分散度之外,未来在这些 QD 的发射光谱变窄方面的努力也可能尝试减小发射中心的“位置”不均匀性。

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