Complete Mapping of Interacting Charging States in Single Coupled Colloidal Quantum Dot Molecules

被引:12
|
作者
Panfil, Yossef E. [1 ,2 ]
Cui, Jiabin [1 ,2 ,3 ,4 ]
Koley, Somnath [1 ,2 ]
Banin, Uri [1 ,2 ]
机构
[1] Hebrew Univ Jerusalem, Inst Chem, IL-91904 Jerusalem, Israel
[2] Hebrew Univ Jerusalem, Ctr Nanosci & Nanotechnol, IL-91904 Jerusalem, Israel
[3] Soochow Univ, Nucl Med, State Key Lab Radiat Med & Protect, Sch Radiol & Interdisciplinary Sci RADX, Suzhou 215123, Peoples R China
[4] Soochow Univ, Collaborat Innovat Ctr Radiol Med Jiangsu Higher, Suzhou 215123, Peoples R China
基金
欧洲研究理事会;
关键词
Colloidal QDs; Quantum dot molecule; Nanocrystals; Single particle spectroscopy; Time tagged time-resolved fluorescence; AUGER RECOMBINATION; HETEROSTRUCTURES; NANOCRYSTALS; COMPUTATION; EMISSION; GROWTH;
D O I
10.1021/acsnano.1c10329
中图分类号
O6 [化学];
学科分类号
0703 ;
摘要
Colloidal quantum dots (CQDs), major building blocks in modern optoelectronic devices, have so far been synthesized with only one emission center where the exciton resides. Recent development of coupled colloidal quantum dots molecules (CQDM), where two core-shell CQDs are fused to form two emission centers in close proximity, allows exploration of how charge carriers in one CQD affect the charge carriers in the other CQD. Cryogenic single particle spectroscopy reveals that while CQD monomers manifest a simple emission spectrum comprising a main emission peak with well-defined phonon sidebands, CQDMs exhibit a complex spectrum with multiple peaks that are not all spaced according to the known phonon frequencies. Based on complementary emission polarization and time-resolved analysis, this is assigned to fluorescence of the two coupled emission centers. Moreover, the complex peak structure shows correlated spectral diffusion indicative of the coupling between the two emission centers. Utilizing Schro??dinger-Poisson self-consistent calculations, we directly map the spectral behavior, alternating between neutral and charged states of the CQDM. Spectral shifts related to electrostatic interaction between a charged emission center and the second emission center are thus fully mapped. Furthermore, effects of moving surface charges are identified, whereby the emission center proximal to the charge shows larger shifts. Instances where the two emission centers are negatively charged simultaneously are also identified. Such detailed mapping of charging states is enabled by the coupling within the CQDM and its anisotropic structure. This understanding of the coupling interactions is progress toward quantum technology and sensing applications based on CQDMs.
引用
收藏
页码:5566 / 5576
页数:11
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