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卤化物钙钛矿纳米晶体中的反斯托克斯光致发光:从理解机制到全固态光冷却应用

Anti-Stokes Photoluminescence in Halide Perovskite Nanocrystals: From Understanding the Mechanism towards Application in Fully Solid-State Optical Cooling.

作者信息

Pokryshkin Nikolay S, Mantsevich Vladimir N, Timoshenko Victor Y

机构信息

Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia.

Phys-Bio Institute, University "MEPhI", 115409 Moscow, Russia.

出版信息

Nanomaterials (Basel). 2023 Jun 9;13(12):1833. doi: 10.3390/nano13121833.

DOI:10.3390/nano13121833
PMID:37368263
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC10301285/
Abstract

Anti-Stokes photoluminescence (ASPL) is an up-conversion phonon-assisted process of radiative recombination of photoexcited charge carriers when the ASPL photon energy is above the excitation one. This process can be very efficient in nanocrystals (NCs) of metalorganic and inorganic semiconductors with perovskite (Pe) crystal structure. In this review, we present an analysis of the basic mechanisms of ASPL and discuss its efficiency depending on the size distribution and surface passivation of Pe-NCs as well as the optical excitation energy and temperature. When the ASPL process is sufficiently efficient, it can result in an escape of most of the optical excitation together with the phonon energy from the Pe-NCs. It can be used in optical fully solid-state cooling or optical refrigeration.

摘要

反斯托克斯光致发光(ASPL)是一种光激发电荷载流子辐射复合的上转换声子辅助过程,当ASPL光子能量高于激发能量时发生。在具有钙钛矿(Pe)晶体结构的金属有机和无机半导体纳米晶体(NCs)中,这一过程可能非常高效。在本综述中,我们对ASPL的基本机制进行了分析,并讨论了其效率与Pe-NCs的尺寸分布、表面钝化以及光激发能量和温度的关系。当ASPL过程足够高效时,它会导致大部分光激发以及声子能量从Pe-NCs中逸出。它可用于光学全固态冷却或光制冷。

https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f1fa9aeadba2/nanomaterials-13-01833-g013.jpg
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https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/8c3a95b5b511/nanomaterials-13-01833-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/bf814cf433de/nanomaterials-13-01833-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f5d7ba8ff307/nanomaterials-13-01833-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f61be3e82d5d/nanomaterials-13-01833-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/853085bfd76a/nanomaterials-13-01833-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/ee7951f4bffa/nanomaterials-13-01833-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/e1620d85e65c/nanomaterials-13-01833-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f1fa9aeadba2/nanomaterials-13-01833-g013.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/3c19a1609e1b/nanomaterials-13-01833-g001.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/c5792594ed85/nanomaterials-13-01833-g002.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/139ce5096ae1/nanomaterials-13-01833-g003.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/8d0113fb03b3/nanomaterials-13-01833-g004.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/6dcaccb7141f/nanomaterials-13-01833-g005.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/8c3a95b5b511/nanomaterials-13-01833-g006.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/bf814cf433de/nanomaterials-13-01833-g007.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f5d7ba8ff307/nanomaterials-13-01833-g008.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f61be3e82d5d/nanomaterials-13-01833-g009.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/853085bfd76a/nanomaterials-13-01833-g010.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/ee7951f4bffa/nanomaterials-13-01833-g011.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/e1620d85e65c/nanomaterials-13-01833-g012.jpg
https://cdn.ncbi.nlm.nih.gov/pmc/blobs/5086/10301285/f1fa9aeadba2/nanomaterials-13-01833-g013.jpg

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2
Non-Markovian diffusion of excitons in layered perovskites and transition metal dichalcogenides.激子在层状钙钛矿和过渡金属二硫属化物中的非马尔可夫扩散
Phys Chem Chem Phys. 2022 Jun 8;24(22):13941-13950. doi: 10.1039/d2cp00557c.
3
Polaron Masses in CH_{3}NH_{3}PbX_{3} Perovskites Determined by Landau Level Spectroscopy in Low Magnetic Fields.
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Phys Rev Lett. 2021 Jun 11;126(23):237401. doi: 10.1103/PhysRevLett.126.237401.
4
Enhancing the Hot-Phonon Bottleneck Effect in a Metal Halide Perovskite by Terahertz Phonon Excitation.通过太赫兹声子激发增强金属卤化物钙钛矿中的热声子瓶颈效应
Phys Rev Lett. 2021 Feb 19;126(7):077401. doi: 10.1103/PhysRevLett.126.077401.
5
Optically Cooling Cesium Lead Tribromide Nanocrystals.光学冷却溴化铯铅纳米晶体。
Nano Lett. 2020 Dec 9;20(12):8874-8879. doi: 10.1021/acs.nanolett.0c03910. Epub 2020 Nov 16.
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