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Excitons in Core-Shell Nanowires with Polygonal Cross Sections.
Sitek, Anna; Urbaneja Torres, Miguel; Torfason, Kristinn; Gudmundsson, Vidar; Bertoni, Andrea; Manolescu, Andrei.
Afiliação
  • Sitek A; School of Science and Engineering , Reykjavik University , Menntavegur 1 , IS-101 Reykjavik , Iceland.
  • Urbaneja Torres M; Department of Theoretical Physics, Faculty of Fundamental Problems of Technology , Wroclaw University of Science and Technology , Wybrzeze Wyspianskiego 27 , 50-370 Wroclaw , Poland.
  • Torfason K; School of Science and Engineering , Reykjavik University , Menntavegur 1 , IS-101 Reykjavik , Iceland.
  • Gudmundsson V; School of Science and Engineering , Reykjavik University , Menntavegur 1 , IS-101 Reykjavik , Iceland.
  • Bertoni A; Science Institute , University of Iceland , Dunhaga 3 , IS-107 Reykjavik , Iceland.
  • Manolescu A; Istituto Nanoscienze-CNR , Via Campi 213a , I-41125 Modena , Italy.
Nano Lett ; 18(4): 2581-2589, 2018 04 11.
Article em En | MEDLINE | ID: mdl-29578727
ABSTRACT
The distinctive prismatic geometry of semiconductor core-shell nanowires leads to complex localization patterns of carriers. Here, we describe the formation of optically active in-gap excitonic states induced by the interplay between localization of carriers in the corners and their mutual Coulomb interaction. To compute the energy spectra and configurations of excitons created in the conductive shell, we use a multielectron numerical approach based on the exact solution of the multiparticle Hamiltonian for electrons in the valence and conduction bands, which includes the Coulomb interaction in a nonperturbative manner. We expose the formation of well-separated quasidegenerate levels, and focus on the implications of the electron localization in the corners or on the sides of triangular, square, and hexagonal cross sections. We obtain excitonic in-gap states associated with symmetrically distributed electrons in the spin singlet configuration. They acquire large contributions due to Coulomb interaction, and thus are shifted to much higher energies than other states corresponding to the conduction electron and the vacancy localized in the same corner. We compare the results of the multielectron method with those of an electron-hole model, and we show that the latter does not reproduce the singlet excitonic states. We also obtain the exciton lifetime and explain selection rules which govern the recombination process.
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Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2018 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2018 Tipo de documento: Article