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231226s2023 xx |||||o 00| ||eng c |
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|a 10.1002/adma.202208354
|2 doi
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|a pubmed24n1168.xml
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|a (DE-627)NLM350495904
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|a (NLM)36537857
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|a DE-627
|b ger
|c DE-627
|e rakwb
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|a eng
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| 100 |
1 |
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|a Zhu, Chenglian
|e verfasserin
|4 aut
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|a Many-Body Correlations and Exciton Complexes in CsPbBr3 Quantum Dots
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|c 2023
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|a Text
|b txt
|2 rdacontent
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|a ƒaComputermedien
|b c
|2 rdamedia
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|a ƒa Online-Ressource
|b cr
|2 rdacarrier
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|a Date Completed 02.03.2023
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|a Date Revised 02.03.2023
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|a published: Print-Electronic
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|a Citation Status PubMed-not-MEDLINE
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|a © 2023 The Authors. Advanced Materials published by Wiley-VCH GmbH.
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|a All-inorganic lead-halide perovskite (LHP) (CsPbX3 , X = Cl, Br, I) quantum dots (QDs) have emerged as a competitive platform for classical light-emitting devices (in the weak light-matter interaction regime, e.g., LEDs and laser), as well as for devices exploiting strong light-matter interaction at room temperature. Many-body interactions and quantum correlations among photogenerated exciton complexes play an essential role, for example, by determining the laser threshold, the overall brightness of LEDs, and the single-photon purity in quantum light sources. Here, by combining cryogenic single-QD photoluminescence spectroscopy with configuration-interaction (CI) calculations, the size-dependent trion and biexciton binding energies are addressed. Trion binding energies increase from 7 to 17 meV for QD sizes decreasing from 30 to 9 nm, while the biexciton binding energies increase from 15 to 30 meV, respectively. CI calculations quantitatively corroborate the experimental results and suggest that the effective dielectric constant for biexcitons slightly deviates from the one of the single excitons, potentially as a result of coupling to the lattice in the multiexciton regime. The findings here provide a deep insight into the multiexciton properties in all-inorganic LHP QDs, essential for classical and quantum optoelectronic devices
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|a Journal Article
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|a CsPbBr3 quantum dots
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|a binding energies in exciton complexes
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|a configuration interaction methods
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|a effective mass calculations
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4 |
|a polarons
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4 |
|a quantum correlations
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| 650 |
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|a single quantum dot spectroscopy
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| 700 |
1 |
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|a Nguyen, Tan
|e verfasserin
|4 aut
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| 700 |
1 |
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|a Boehme, Simon C
|e verfasserin
|4 aut
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| 700 |
1 |
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|a Moskalenko, Anastasiia
|e verfasserin
|4 aut
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| 700 |
1 |
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|a Dirin, Dmitry N
|e verfasserin
|4 aut
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| 700 |
1 |
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|a Bodnarchuk, Maryna I
|e verfasserin
|4 aut
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| 700 |
1 |
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|a Katan, Claudine
|e verfasserin
|4 aut
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| 700 |
1 |
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|a Even, Jacky
|e verfasserin
|4 aut
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1 |
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|a Rainò, Gabriele
|e verfasserin
|4 aut
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1 |
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|a Kovalenko, Maksym V
|e verfasserin
|4 aut
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| 773 |
0 |
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|i Enthalten in
|t Advanced materials (Deerfield Beach, Fla.)
|d 1998
|g 35(2023), 9 vom: 09. März, Seite e2208354
|w (DE-627)NLM098206397
|x 1521-4095
|7 nnns
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| 773 |
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|g volume:35
|g year:2023
|g number:9
|g day:09
|g month:03
|g pages:e2208354
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|u http://dx.doi.org/10.1002/adma.202208354
|3 Volltext
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|d 35
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|e 9
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