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Magnetoluminescence from trion and biexciton in type-II quantum dot

We theoretically investigate optical Aharonov-Bohm (AB) effects on trion and biexciton in the type-II semiconductor quantum dots, in which holes are localized near the center of the dot, and electrons are confined in a ring structure formed around the dot. Many-particle states are calculated numeric...

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Detalles Bibliográficos
Autores principales: Okuyama, Rin, Eto, Mikio, Hyuga, Hiroyuki
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Springer 2011
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3211441/
https://www.ncbi.nlm.nih.gov/pubmed/21711894
http://dx.doi.org/10.1186/1556-276X-6-351
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author Okuyama, Rin
Eto, Mikio
Hyuga, Hiroyuki
author_facet Okuyama, Rin
Eto, Mikio
Hyuga, Hiroyuki
author_sort Okuyama, Rin
collection PubMed
description We theoretically investigate optical Aharonov-Bohm (AB) effects on trion and biexciton in the type-II semiconductor quantum dots, in which holes are localized near the center of the dot, and electrons are confined in a ring structure formed around the dot. Many-particle states are calculated numerically by the exact diagonalization method. Two electrons in trion and biexciton are strongly correlated to each other, forming a Wigner molecule. Since the relative motion of electrons are frozen, the Wigner molecule behaves as a composite particle whose mass and charges are twice those of an electron. As a result, the period of AB oscillation for trion and biexciton becomes h/2e as a function of magnetic flux penetrating the ring. We find that the magnetoluminescence spectra from trion and biexciton change discontinuously as the magnetic flux increases by h/2e. PACS: 71.35.Ji, 73.21.-b, 73.21.La, 78.67.Hc
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spelling pubmed-32114412011-11-09 Magnetoluminescence from trion and biexciton in type-II quantum dot Okuyama, Rin Eto, Mikio Hyuga, Hiroyuki Nanoscale Res Lett Nano Express We theoretically investigate optical Aharonov-Bohm (AB) effects on trion and biexciton in the type-II semiconductor quantum dots, in which holes are localized near the center of the dot, and electrons are confined in a ring structure formed around the dot. Many-particle states are calculated numerically by the exact diagonalization method. Two electrons in trion and biexciton are strongly correlated to each other, forming a Wigner molecule. Since the relative motion of electrons are frozen, the Wigner molecule behaves as a composite particle whose mass and charges are twice those of an electron. As a result, the period of AB oscillation for trion and biexciton becomes h/2e as a function of magnetic flux penetrating the ring. We find that the magnetoluminescence spectra from trion and biexciton change discontinuously as the magnetic flux increases by h/2e. PACS: 71.35.Ji, 73.21.-b, 73.21.La, 78.67.Hc Springer 2011-04-20 /pmc/articles/PMC3211441/ /pubmed/21711894 http://dx.doi.org/10.1186/1556-276X-6-351 Text en Copyright ©2011 Okuyama et al; licensee Springer. http://creativecommons.org/licenses/by/2.0 This is an Open Access article distributed under the terms of the Creative Commons Attribution License (http://creativecommons.org/licenses/by/2.0), which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.
spellingShingle Nano Express
Okuyama, Rin
Eto, Mikio
Hyuga, Hiroyuki
Magnetoluminescence from trion and biexciton in type-II quantum dot
title Magnetoluminescence from trion and biexciton in type-II quantum dot
title_full Magnetoluminescence from trion and biexciton in type-II quantum dot
title_fullStr Magnetoluminescence from trion and biexciton in type-II quantum dot
title_full_unstemmed Magnetoluminescence from trion and biexciton in type-II quantum dot
title_short Magnetoluminescence from trion and biexciton in type-II quantum dot
title_sort magnetoluminescence from trion and biexciton in type-ii quantum dot
topic Nano Express
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC3211441/
https://www.ncbi.nlm.nih.gov/pubmed/21711894
http://dx.doi.org/10.1186/1556-276X-6-351
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