Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy
The exciton-phonon coupling in high-quality cubic phase zinc telluride (ZnTe) nanorods (NRs) is investigated by resonant micro-Raman spectroscopy near the direct bandgap of ZnTe. The scattering cross section of longitudinal optical (LO) phonon is enhanced significantly in the resonant process, where...
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sg-ntu-dr.10356-953942023-02-28T19:35:52Z Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy Zhang, Q. Zhang, J. Utama, M. I. B. Peng, B. Mata, Maria de la Arbiol, Jordi Xiong, Qihua School of Physical and Mathematical Sciences DRNTU::Science::Physics The exciton-phonon coupling in high-quality cubic phase zinc telluride (ZnTe) nanorods (NRs) is investigated by resonant micro-Raman spectroscopy near the direct bandgap of ZnTe. The scattering cross section of longitudinal optical (LO) phonon is enhanced significantly in the resonant process, where the enhancement factor of LO modes is much higher than that of the transverse optical (TO) modes, indicating a dominant Fröhlich electron-phonon interaction mechanism. Up to fifth-order LO phonons are observed by resonant Raman scattering at room temperature. The Huang-Rhys factor of individual NRs—and thus the exciton-LO coupling strengths—is evaluated, showing increasing with the NR diameter. Surface optical (SO) phonon and its high-order overtones are observed between nLO and (n − 1)LO + TO for the first time, whose positions are consistent with a dielectric continuum model. Strong acoustic phonon-exciton coupling induces a high-frequency shoulder above each nLO peaks with two maxima located around 14 cm−1 and 32 cm−1, which are assigned to transverse acoustic and longitudinal acoustic phonons, respectively. The resonant multiphonon scattering process involving acoustic and LO phonons is discussed based on an exciton-intermediated cascade model, where a scattering sequence of acoustic phonon followed by LO phonons is favorable. These results advance the understanding of electron-phonon coupling and exciton scattering in quasi-one-dimensional systems, especially in the scarcely documented ZnTe compound, facilitating the development and optimization of NR-based optoelectronic devices. Published version 2013-02-26T03:37:24Z 2019-12-06T19:14:00Z 2013-02-26T03:37:24Z 2019-12-06T19:14:00Z 2012 2012 Journal Article Zhang, Q., Zhang, J., Utama, M. I. B., Peng, B., Mata, M. d. l., Arbiol, J., et al. (2012). Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy. Physical Review B, 85(8), 085418-. https://hdl.handle.net/10356/95394 http://hdl.handle.net/10220/9251 10.1103/PhysRevB.85.085418 en Physical review B © 2012 American Physical Society. This paper was published in Physical Review B and is made available as an electronic reprint (preprint) with permission of American Physical Society. The paper can be found at the following official DOI: [http://dx.doi.org/10.1103/PhysRevB.85.085418]. One print or electronic copy may be made for personal use only. Systematic or multiple reproduction, distribution to multiple locations via electronic or other means, duplication of any material in this paper for a fee or for commercial purposes, or modification of the content of the paper is prohibited and is subject to penalties under law. application/pdf |
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DRNTU::Science::Physics Zhang, Q. Zhang, J. Utama, M. I. B. Peng, B. Mata, Maria de la Arbiol, Jordi Xiong, Qihua Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy |
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The exciton-phonon coupling in high-quality cubic phase zinc telluride (ZnTe) nanorods (NRs) is investigated by resonant micro-Raman spectroscopy near the direct bandgap of ZnTe. The scattering cross section of longitudinal optical (LO) phonon is enhanced significantly in the resonant process, where the enhancement factor of LO modes is much higher than that of the transverse optical (TO) modes, indicating a dominant Fröhlich electron-phonon interaction mechanism. Up to fifth-order LO phonons are observed by resonant Raman scattering at room temperature. The Huang-Rhys factor of individual NRs—and thus the exciton-LO coupling strengths—is evaluated, showing increasing with the NR diameter. Surface optical (SO) phonon and its high-order overtones are observed between nLO and (n − 1)LO + TO for the first time, whose positions are consistent with a dielectric continuum model. Strong acoustic phonon-exciton coupling induces a high-frequency shoulder above each nLO peaks with two maxima located around 14 cm−1 and 32 cm−1, which are assigned to transverse acoustic and longitudinal acoustic phonons, respectively. The resonant multiphonon scattering process involving acoustic and LO phonons is discussed based on an exciton-intermediated cascade model, where a scattering sequence of acoustic phonon followed by LO phonons is favorable. These results advance the understanding of electron-phonon coupling and exciton scattering in quasi-one-dimensional systems, especially in the scarcely documented ZnTe compound, facilitating the development and optimization of NR-based optoelectronic devices. |
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School of Physical and Mathematical Sciences |
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School of Physical and Mathematical Sciences Zhang, Q. Zhang, J. Utama, M. I. B. Peng, B. Mata, Maria de la Arbiol, Jordi Xiong, Qihua |
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Article |
author |
Zhang, Q. Zhang, J. Utama, M. I. B. Peng, B. Mata, Maria de la Arbiol, Jordi Xiong, Qihua |
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Zhang, Q. |
title |
Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy |
title_short |
Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy |
title_full |
Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy |
title_fullStr |
Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy |
title_full_unstemmed |
Exciton-phonon coupling in individual ZnTe nanorods studied by resonant Raman spectroscopy |
title_sort |
exciton-phonon coupling in individual znte nanorods studied by resonant raman spectroscopy |
publishDate |
2013 |
url |
https://hdl.handle.net/10356/95394 http://hdl.handle.net/10220/9251 |
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1759854701117964288 |