Impurity induced confinement effects in size-separated Mn-doped CsPbCl3 nanocrystals

被引:1
|
作者
Forde, Aaron A. [1 ,2 ,3 ]
Thomas, Salim A. [1 ]
Petersen, Reed J. [4 ]
Kilin, Dmitri S. [5 ]
Hobbie, Erik K. [1 ,4 ,6 ]
机构
[1] North Dakota State Univ, Mat & Nanotechnol Program, Fargo, ND 58108 USA
[2] Los Alamos Natl Lab LANL, Theoret Div, Los Alamos, NM 87545 USA
[3] Los Alamos Natl Lab LANL, Ctr Nonlinear Studies, Los Alamos, NM 87545 USA
[4] North Dakota State Univ, Dept Phys, Fargo, ND 58108 USA
[5] North Dakota State Univ, Dept Chem & Biochem, Fargo, ND 58108 USA
[6] North Dakota State Univ, Dept Coatings & Polymer Mat, Fargo, ND 58108 USA
来源
PHYSICAL REVIEW MATERIALS | 2024年 / 8卷 / 06期
基金
美国国家科学基金会;
关键词
HALIDE PEROVSKITE NANOCRYSTALS; DOPANT ENERGY-TRANSFER; ANION-EXCHANGE; CSPBX3; X; DYNAMICS; BR; PHOTOLUMINESCENCE; EMISSION; EXCITON; CL;
D O I
10.1103/PhysRevMaterials.8.066001
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
Beyond quantum confinement, impurity doping of semiconductor nanocrystals (NCs) offers a degree of control over their optical and electronic properties, which are of interest for potential applications. Manganese (Mn)-doped CsPbCl3 NCs, for example, show synergistic effects in the visible, with large enhancements in both blue (exciton) and red (dopant) emission over a narrow range of dopant concentration. Although Mn concentration is the primary parameter, NC size offers an additional degree of control over the number of dopants per NC. Size-resolved CsPbCl3 NCs prepared in the limit of strong Mn doping highlight the emergence of defective NCs with deviations from anticipated confinement trends. The transition correlates with a redshift and increase in the amplitude of dopant emission, and we discuss these observations in the context of atomistic simulations of Ruddlesden-Popper defects in CsPbCl3.
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页数:8
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