Cargando…

Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation

Strain-free GaAs cone–shell quantum structures (CSQS) with widely tunable wave functions (WF) are fabricated using local droplet etching (LDE) during molecular beam epitaxy (MBE). During MBE, Al droplets are deposited on an AlGaAs surface, which then drill low-density (about 1 × 10 [Formula: see tex...

Descripción completa

Detalles Bibliográficos
Autores principales: Heyn, Christian, Ranasinghe, Leonardo, Deneke, Kristian, Alshaikh, Ahmed, Duque, Carlos A., Hansen, Wolfgang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: MDPI 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10004794/
https://www.ncbi.nlm.nih.gov/pubmed/36903737
http://dx.doi.org/10.3390/nano13050857
_version_ 1784904923573387264
author Heyn, Christian
Ranasinghe, Leonardo
Deneke, Kristian
Alshaikh, Ahmed
Duque, Carlos A.
Hansen, Wolfgang
author_facet Heyn, Christian
Ranasinghe, Leonardo
Deneke, Kristian
Alshaikh, Ahmed
Duque, Carlos A.
Hansen, Wolfgang
author_sort Heyn, Christian
collection PubMed
description Strain-free GaAs cone–shell quantum structures (CSQS) with widely tunable wave functions (WF) are fabricated using local droplet etching (LDE) during molecular beam epitaxy (MBE). During MBE, Al droplets are deposited on an AlGaAs surface, which then drill low-density (about 1 × 10 [Formula: see text] cm(−2)) nanoholes with adjustable shape and size. Subsequently, the holes are filled with GaAs to form CSQS, where the size can be adjusted by the amount of GaAs deposited for hole filling. An electric field is applied in growth direction to tune the WF in a CSQS. The resulting highly asymmetric exciton Stark shift is measured using micro-photoluminescence. Here, the unique shape of the CSQS allows a large charge–carrier separation and, thus, a strong Stark shift of up to more than 16 meV at a moderate field of 65 kV/cm. This corresponds to a very large polarizability of 8.6 × 10 [Formula: see text] eVkV [Formula: see text] cm(2). In combination with simulations of the exciton energy, the Stark shift data allow the determination of the CSQS size and shape. Simulations of the exciton–recombination lifetime predict an elongation up to factor of 69 for the present CSQSs, tunable by the electric field. In addition, the simulations indicate the field-induced transformation of the hole WF from a disk into a quantum ring with a tunable radius from about 10 nm up to 22.5 nm.
format Online
Article
Text
id pubmed-10004794
institution National Center for Biotechnology Information
language English
publishDate 2023
publisher MDPI
record_format MEDLINE/PubMed
spelling pubmed-100047942023-03-11 Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation Heyn, Christian Ranasinghe, Leonardo Deneke, Kristian Alshaikh, Ahmed Duque, Carlos A. Hansen, Wolfgang Nanomaterials (Basel) Article Strain-free GaAs cone–shell quantum structures (CSQS) with widely tunable wave functions (WF) are fabricated using local droplet etching (LDE) during molecular beam epitaxy (MBE). During MBE, Al droplets are deposited on an AlGaAs surface, which then drill low-density (about 1 × 10 [Formula: see text] cm(−2)) nanoholes with adjustable shape and size. Subsequently, the holes are filled with GaAs to form CSQS, where the size can be adjusted by the amount of GaAs deposited for hole filling. An electric field is applied in growth direction to tune the WF in a CSQS. The resulting highly asymmetric exciton Stark shift is measured using micro-photoluminescence. Here, the unique shape of the CSQS allows a large charge–carrier separation and, thus, a strong Stark shift of up to more than 16 meV at a moderate field of 65 kV/cm. This corresponds to a very large polarizability of 8.6 × 10 [Formula: see text] eVkV [Formula: see text] cm(2). In combination with simulations of the exciton energy, the Stark shift data allow the determination of the CSQS size and shape. Simulations of the exciton–recombination lifetime predict an elongation up to factor of 69 for the present CSQSs, tunable by the electric field. In addition, the simulations indicate the field-induced transformation of the hole WF from a disk into a quantum ring with a tunable radius from about 10 nm up to 22.5 nm. MDPI 2023-02-25 /pmc/articles/PMC10004794/ /pubmed/36903737 http://dx.doi.org/10.3390/nano13050857 Text en © 2023 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/).
spellingShingle Article
Heyn, Christian
Ranasinghe, Leonardo
Deneke, Kristian
Alshaikh, Ahmed
Duque, Carlos A.
Hansen, Wolfgang
Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation
title Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation
title_full Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation
title_fullStr Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation
title_full_unstemmed Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation
title_short Strong Electric Polarizability of Cone–Shell Quantum Structures for a Large Stark Shift, Tunable Long Exciton Lifetimes, and a Dot-to-Ring Transformation
title_sort strong electric polarizability of cone–shell quantum structures for a large stark shift, tunable long exciton lifetimes, and a dot-to-ring transformation
topic Article
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10004794/
https://www.ncbi.nlm.nih.gov/pubmed/36903737
http://dx.doi.org/10.3390/nano13050857
work_keys_str_mv AT heynchristian strongelectricpolarizabilityofconeshellquantumstructuresforalargestarkshifttunablelongexcitonlifetimesandadottoringtransformation
AT ranasingheleonardo strongelectricpolarizabilityofconeshellquantumstructuresforalargestarkshifttunablelongexcitonlifetimesandadottoringtransformation
AT denekekristian strongelectricpolarizabilityofconeshellquantumstructuresforalargestarkshifttunablelongexcitonlifetimesandadottoringtransformation
AT alshaikhahmed strongelectricpolarizabilityofconeshellquantumstructuresforalargestarkshifttunablelongexcitonlifetimesandadottoringtransformation
AT duquecarlosa strongelectricpolarizabilityofconeshellquantumstructuresforalargestarkshifttunablelongexcitonlifetimesandadottoringtransformation
AT hansenwolfgang strongelectricpolarizabilityofconeshellquantumstructuresforalargestarkshifttunablelongexcitonlifetimesandadottoringtransformation