2023
DOI: 10.1021/acs.nanolett.3c04361
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Long-Lived and Bright Biexcitons in Quantum Dots with Parabolic Band Potentials

Benjamin T. Diroll,
Muchuan Hua,
Burak Guzelturk
et al.
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Cited by 6 publications
(3 citation statements)
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“…The core/shell quantum dot shows a much smaller LY, around 1000 ph MeV −1 , consistent with prior reports 9 . Our LY characterization method also showed a much smaller LY (6,700 ph MeV −1 ) when measuring a core/gradient-shell quantum dot structure 31 . This indicates that the QSs show a substantial improvement in scintillation efficiency.…”
Section: Resultsmentioning
confidence: 84%
“…The core/shell quantum dot shows a much smaller LY, around 1000 ph MeV −1 , consistent with prior reports 9 . Our LY characterization method also showed a much smaller LY (6,700 ph MeV −1 ) when measuring a core/gradient-shell quantum dot structure 31 . This indicates that the QSs show a substantial improvement in scintillation efficiency.…”
Section: Resultsmentioning
confidence: 84%
“…This geometric separation of charge carriers results in multiexciton formation that is advantageous for lasing and can affect the single-photon purity. 32,[35][36][37][38] The two main methods to grow large core/shell CdSe/CdS are successive ionic layer adsorption and reaction (SILAR) and high-temperature continuous injection (HTCI). 29,30,39 The differences between the two methods and the correlation between synthetic conditions and QD properties have been rigorously studied by Hollingsworth and coworkers.…”
Section: Introductionmentioning
confidence: 99%
“…The largest emissive QDs without silica shells reported in the literature to date are the traditional quasi-type II giant core/shell CdSe/CdS QDs, with 15–20 CdS monolayers (MLs) and total diameters ranging from 20 to 50 nm. The giant CdS shells not only increase the size of the emissive QDs but also reduce blinking through Auger recombination suppression and isolate the exciton from surface interactions. ,, In these quasi-type II core/shell systems, the electron wave function is delocalized into the CdS shell, while the hole wave function is effectively confined within the CdSe core. This geometric separation of charge carriers results in multiexciton formation that is advantageous for lasing and can affect the single-photon purity. , …”
Section: Introductionmentioning
confidence: 99%