2022
DOI: 10.1021/acs.jpcc.2c00827
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Highly Charged Excitons and Biexcitons in Type-II Core/Crown Colloidal Nanoplatelets

Abstract: The optoelectronic properties of type-II CdSe/ CdTe colloidal nanoplatelets (NPLs) charged with neutral excitons (X 0 ) have been intensively investigated in the last years. Motivated by the recent experimental progress, here we use effective mass simulations to study the effect of charging core/ crown NPLs with a few extra electrons or holes. Emission spectra are calculated for charged excitons (X n , with n = 2 to n = −3) and biexcitons (XX). The strong Coulomb interactions within the platelet lead to a numb… Show more

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Cited by 9 publications
(14 citation statements)
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References 50 publications
(95 reference statements)
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“…415 Theoretical models predict that biexciton binding energies can be tuned by varying the relative sizes of CdSe/CdTe core/crowns. 416 Utilizing single-particle spectroscopy, relative biexciton quantum yields were measured. The ratio of antibunched features (from single exciton recombination) to the bunched (biexciton) feature at low excitation fluence is interpreted in these experiments as a measure of the relative QY of biexciton.…”
Section: Nonlinear Absorption and Second Harmonic Generation Numerous...mentioning
confidence: 99%
See 1 more Smart Citation
“…415 Theoretical models predict that biexciton binding energies can be tuned by varying the relative sizes of CdSe/CdTe core/crowns. 416 Utilizing single-particle spectroscopy, relative biexciton quantum yields were measured. The ratio of antibunched features (from single exciton recombination) to the bunched (biexciton) feature at low excitation fluence is interpreted in these experiments as a measure of the relative QY of biexciton.…”
Section: Nonlinear Absorption and Second Harmonic Generation Numerous...mentioning
confidence: 99%
“…In Type II, CdSe/CdTe core/crown systems, repulsive biexcitons with blueshifted emission and binding energies as high as 200 meV are observed . Theoretical models predict that biexciton binding energies can be tuned by varying the relative sizes of CdSe/CdTe core/crowns . Utilizing single-particle spectroscopy, relative biexciton quantum yields were measured.…”
Section: Synthesis and Structure Of Nplsmentioning
confidence: 99%
“…These methods were extended to make NCs of different shapes, resulting in colloidal CdTe nanorods, nanowires, nanotubes and tetrapods. , However, the colloidal synthesis of CdTe NPLs and the studies conducted on them have lagged behind. Compared to their Cd chalcogenide counterparts, CdTe NPLs showcase widely separated and distinct light-hole (LH) and heavy-hole (HH) features, a narrow, tunable emission line width, and fast PL decay lifetimes among other interesting characteristics and can have a considerable impact in optoelectronics and photon management technologies. Coupling these with a large absorption coefficient and high atomic numbers (48 and 52 for Cd and Te, respectively), they present themselves as materials with enormous prospects in radiation detection.…”
mentioning
confidence: 99%
“…However, CdTe NPLs are shown to suffer from low PL quantum yields (PLQYs) resulting from lattice defects which have pulled them down in the priority of research compared to CdSe NPLs. As a result, work on CdSe and CdS NPLs , has been replicated only partially with CdTe, , limiting its use in combination with other Cd chalcogenides such as CdSe and CdS in the form of core–shell, core–crown , and core–barrier–crown heterostructures . To date, two - dimensional CdTe nanostructures have been reported in the form of zincblende structured NPLs, wurtzite structured nanoribbons and CdTe nanosheets. , In 2013, Pedetti et al optimized the synthesis protocol for the colloidal synthesis of CdTe NPLs with zincblende structure, yielding NPL populations of different thicknesses defined with atomic precision.…”
mentioning
confidence: 99%
“…[189] These exchange interactions, in NPLs, such as CO and CC, may be particularly relevant and may also become increased due to the strong quantum and dielectric confinement, in the out-of-plane direction, combined with the weak lateral confinement , over the in-plane directions, seen in these types of nanostructures. In a typical CdSe-based CO NPL with large lateral dimensions: first, the energy spacing between ground and first excited states is about 10 meV [92,112,190] and secondly, when applying magnetic fields perpendicularly to the NPL plane, considerable diamagnetic shifts are enabled through the radial part of the first term in equations (1.34) and (1.35). The mean squared radius, x 2 + y 2 in both equation 1.34 and 1.35, increases with the lateral dimensions of the NPL, leading to significant diamagnetic shifts.…”
Section: Magnetic Propertiesmentioning
confidence: 99%