Hot-Carrier Relaxation in CdSe/CdS Core/Shell Nanoplatelets

被引:10
|
作者
Pelton, Matthew [1 ,2 ]
Wang, Yana [3 ]
Fedin, Igor [4 ,5 ,6 ]
Talapin, Dmitri V. [4 ,5 ]
O'Leary, Stephen K. [3 ]
机构
[1] Univ Maryland Baltimore Cty, Dept Phys, Baltimore, MD 21250 USA
[2] Argonne Natl Lab, Ctr Nanoscale Mat, Argonne, IL 60439 USA
[3] Univ British Columbia, Sch Engn, Kelowna, BC V1V 1V7, Canada
[4] Univ Chicago, Dept Chem, Chicago, IL 60637 USA
[5] Univ Chicago, James Franck Inst, Chicago, IL 60637 USA
[6] Los Alamos Natl Lab, Los Alamos, NM 87545 USA
来源
JOURNAL OF PHYSICAL CHEMISTRY C | 2020年 / 124卷 / 01期
基金
加拿大自然科学与工程研究理事会; 美国国家科学基金会;
关键词
CESIUM LEAD HALIDE; ENERGY-LOSS RATES; PEROVSKITE NANOPLATELETS; ELECTRON RELAXATION; QUANTUM; DYNAMICS; RECOMBINATION; SPECTROSCOPY; THICKNESS;
D O I
10.1021/acs.jpcc.9b08006
中图分类号
O64 [物理化学(理论化学)、化学物理学];
学科分类号
070304 ; 081704 ;
摘要
We present time-resolved photoluminescence (PL) spectroscopy of a series of colloidal CdSe/CdS core/shell nanoplatelets with different core and shell thicknesses. Exciton numbers are determined from the integrated PI, intensities, and carrier temperatures are determined from the high-energy exponential tail of the PL spectra. For times between 10 and 1000 ps, the measured carrier relaxation dynamics are well described by a simple model of Auger reheating: biexcitonic Auger recombination continually increases the average energy of the carriers (while decreasing their number), and this reheating sets a bottleneck to cooling through electron-phonon coupling. For times between 1 and 10 ps, the relaxation dynamics are consistent with electron-phonon coupling, where the bottleneck is now the decay of the longitudinal optical phonon population. Comparison of relaxation dynamics to recombination dynamics reveals changes in the carrier-phonon coupling for shell thicknesses greater than 4 monolayers.
引用
收藏
页码:1020 / 1026
页数:7
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