2019
DOI: 10.1021/acs.nanolett.9b00122
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Manipulating the Transition Dipole Moment of CsPbBr3 Perovskite Nanocrystals for Superior Optical Properties

Abstract: Colloidal cesium lead halide perovskite nanocrystals exhibit unique photophysical properties including high quantum yields, tunable emission colors, and narrow photoluminescence spectra that have marked them as promising light emitters for applications in diverse photonic devices. Randomly oriented transition dipole moments have limited the light outcoupling efficiency of all isotropic light sources, including perovskites. In this report we design and synthesize deep blue emitting, quantum confined, perovskite… Show more

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Cited by 73 publications
(80 citation statements)
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“…The strong polarization is consistent with a strong IP orientation of the transition dipole of the excitons. [39][40][41] To gain qualitative insight in the exciton transport along the IP and OP directions of the crystal, we look at the photoluminescence emission profile following near-diffraction-limited excitation (λex = 405 nm, FWHM = 250 nm). While the excitation profile is fully symmetric, we observe a distinctly asymmetric emission profile on the ac crystal plane that is elongated along the IP direction (see Figure 1D).…”
Section: Introductionmentioning
confidence: 99%
“…The strong polarization is consistent with a strong IP orientation of the transition dipole of the excitons. [39][40][41] To gain qualitative insight in the exciton transport along the IP and OP directions of the crystal, we look at the photoluminescence emission profile following near-diffraction-limited excitation (λex = 405 nm, FWHM = 250 nm). While the excitation profile is fully symmetric, we observe a distinctly asymmetric emission profile on the ac crystal plane that is elongated along the IP direction (see Figure 1D).…”
Section: Introductionmentioning
confidence: 99%
“…B right excitons in quantum-confined two-dimensional (2D) materials have their transition dipole moment (TDM) oriented in parallel to the surface plane [1][2][3][4] , which is essential to enable high-efficiency quantum optics 5,6 and electroluminescent devices 7,8 . It is desirable to fabricate the decoupled multi-quantumwell (MQW) superlattices 3 by inserting atomically thin quantum barriers (QBs) between individual 2D material layers 9 .…”
mentioning
confidence: 99%
“…Since the quantum emission characteristics are mediated by the TDMs that orthogonally interact with the electromagnetic fields of the emitted photons, the dipole orientation of bright excitons in 2D materials is predominantly in-plane (IP) [1][2][3][4] , analogous to those in the planar molecules 7 . When interlayer coupling comes into play, the symmetry is broken and the outof-plane (OP) components are induced 23,25 .…”
mentioning
confidence: 99%
“…It is clear from the band structure diagrams in figure 3 that band gap is increased when we replace the I atoms by Br atoms due to decrease in atomic size. This is due to fact that as the I has the more number of nucleons than Br atom, so the I, due to its large size have the less electrostatic force of attraction between nucleus and the outermost electrons (shielding [21]. b [22].…”
Section: Electronic Propertiesmentioning
confidence: 99%