Calculation of two-photon absorption by nanocrystals of CsPbBr3
We present calculations of the two-photon absorption cross section σ(2)(ω) for nanocrystals (NCs) of the inorganic perovskite CsPbBr3 for photon energies ω ranging from the absorption threshold at 2ω≈2.3eV up to 2ω=3.1eV. The calculations employ a 4×4k⋅p envelope-function model, with final-state exc...
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sg-ntu-dr.10356-1510902021-07-03T20:11:33Z Calculation of two-photon absorption by nanocrystals of CsPbBr3 Blundell, S. A. Nguyen, T. P. T. Guet, Claude School of Materials Science and Engineering Energy Research Institute @ NTU (ERI@N) Science::Physics Electronic Structure Excitons We present calculations of the two-photon absorption cross section σ(2)(ω) for nanocrystals (NCs) of the inorganic perovskite CsPbBr3 for photon energies ω ranging from the absorption threshold at 2ω≈2.3eV up to 2ω=3.1eV. The calculations employ a 4×4k⋅p envelope-function model, with final-state excitons described in a self-consistent Hartree-Fock approximation. The k⋅p corrections to σ(2)(ω) are found to be rather large, giving a reduction of about 30% in the cross section at the largest energies considered. The cross section is shown to be independent of polarization in the effective-mass approximation (EMA), but including k⋅p corrections leads to a small difference in σ(2)(ω) between circular and linear polarization, which rises to about 16% at 2ω=3.1eV. The theoretical cross section follows closely a power-law dependence on NC size, σ(2)(ω)∝Lα, with theoretical exponents α=3.4 (EMA) or α=3.2 (4×4k⋅p model), in excellent agreement with experiment. The dominant contribution to the exponent α is shown to be the number of final-state excitons per unit energy. Measured values of the absolute (normalized) cross section σ(2)(ω) show a large spread of values, differing by as much as a factor of 25 for some NC sizes. Our calculations strongly favor a group of measurements at the lower end of the reported range of σ(2)(ω). National Research Foundation (NRF) Published version The authors would like to thank Sum T. C. for helpful discussions. They acknowledge the France-Singapore Merlion Project 2.05.16 for supporting mutual visits. T.P.T.N. and S.A.B. are grateful to F. Schuster of the CEA's PTMA program for financial support. C.G. gratefully acknowledges financial support from the National Research Foundation through the Competitive Research Program, Grant No. NRF-CRP14-2014-03. 2021-06-28T09:44:06Z 2021-06-28T09:44:06Z 2021 Journal Article Blundell, S. A., Nguyen, T. P. T. & Guet, C. (2021). Calculation of two-photon absorption by nanocrystals of CsPbBr3. Physical Review B, 103(4), 045415-. https://dx.doi.org/10.1103/PhysRevB.103.045415 2469-9950 https://hdl.handle.net/10356/151090 10.1103/PhysRevB.103.045415 2-s2.0-85100488618 4 103 045415 en NRF-CRP14-2014-03 Physical Review B © 2021 American Physical Society (APS). All rights reserved. This paper was published in Physical Review B and is made available with permission of American Physical Society (APS). application/pdf |
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Science::Physics Electronic Structure Excitons Blundell, S. A. Nguyen, T. P. T. Guet, Claude Calculation of two-photon absorption by nanocrystals of CsPbBr3 |
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We present calculations of the two-photon absorption cross section σ(2)(ω) for nanocrystals (NCs) of the inorganic perovskite CsPbBr3 for photon energies ω ranging from the absorption threshold at 2ω≈2.3eV up to 2ω=3.1eV. The calculations employ a 4×4k⋅p envelope-function model, with final-state excitons described in a self-consistent Hartree-Fock approximation. The k⋅p corrections to σ(2)(ω) are found to be rather large, giving a reduction of about 30% in the cross section at the largest energies considered. The cross section is shown to be independent of polarization in the effective-mass approximation (EMA), but including k⋅p corrections leads to a small difference in σ(2)(ω) between circular and linear polarization, which rises to about 16% at 2ω=3.1eV. The theoretical cross section follows closely a power-law dependence on NC size, σ(2)(ω)∝Lα, with theoretical exponents α=3.4 (EMA) or α=3.2 (4×4k⋅p model), in excellent agreement with experiment. The dominant contribution to the exponent α is shown to be the number of final-state excitons per unit energy. Measured values of the absolute (normalized) cross section σ(2)(ω) show a large spread of values, differing by as much as a factor of 25 for some NC sizes. Our calculations strongly favor a group of measurements at the lower end of the reported range of σ(2)(ω). |
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School of Materials Science and Engineering |
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School of Materials Science and Engineering Blundell, S. A. Nguyen, T. P. T. Guet, Claude |
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Article |
author |
Blundell, S. A. Nguyen, T. P. T. Guet, Claude |
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Blundell, S. A. |
title |
Calculation of two-photon absorption by nanocrystals of CsPbBr3 |
title_short |
Calculation of two-photon absorption by nanocrystals of CsPbBr3 |
title_full |
Calculation of two-photon absorption by nanocrystals of CsPbBr3 |
title_fullStr |
Calculation of two-photon absorption by nanocrystals of CsPbBr3 |
title_full_unstemmed |
Calculation of two-photon absorption by nanocrystals of CsPbBr3 |
title_sort |
calculation of two-photon absorption by nanocrystals of cspbbr3 |
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2021 |
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https://hdl.handle.net/10356/151090 |
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1705151319396843520 |