Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress
ABSTRACT: The effects of hydrostatic stress on the binding energy and the density of shallow-donor and shallow-acceptor impurity states in a GaAs–(Ga, Al)As quantum well are calculated using a variational procedure within the effective-mass approximation. Results are for different well widths and hy...
- Autores:
-
López Ríos, Sonia Yaneth
Porras Montenegro, Nelson
Duque Echeverri, Carlos Alberto
- Tipo de recurso:
- Article of investigation
- Fecha de publicación:
- 2003
- Institución:
- Universidad de Antioquia
- Repositorio:
- Repositorio UdeA
- Idioma:
- eng
- OAI Identifier:
- oai:bibliotecadigital.udea.edu.co:10495/4866
- Acceso en línea:
- http://hdl.handle.net/10495/4866
- Palabra clave:
- Hidrostática
Hydrostatics
Pozos cuánticos
Quantum wells
Energía de enlace
Binding energy
Aguas poco profundas
Estres hidrostático
Densidad de estados
Masa efectiva
Impurezas en GaAs
- Rights
- openAccess
- License
- https://creativecommons.org/licenses/by-nc-nd/4.0/
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Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| title |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| spellingShingle |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress Hidrostática Hydrostatics Pozos cuánticos Quantum wells Energía de enlace Binding energy Aguas poco profundas Estres hidrostático Densidad de estados Masa efectiva Impurezas en GaAs |
| title_short |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| title_full |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| title_fullStr |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| title_full_unstemmed |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| title_sort |
Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stress |
| dc.creator.fl_str_mv |
López Ríos, Sonia Yaneth Porras Montenegro, Nelson Duque Echeverri, Carlos Alberto |
| dc.contributor.author.none.fl_str_mv |
López Ríos, Sonia Yaneth Porras Montenegro, Nelson Duque Echeverri, Carlos Alberto |
| dc.contributor.researchgroup.spa.fl_str_mv |
Grupo de Educación en Ciencias Experimentales y Matemáticas (GECEM) |
| dc.subject.decs.none.fl_str_mv |
Hidrostática Hydrostatics |
| topic |
Hidrostática Hydrostatics Pozos cuánticos Quantum wells Energía de enlace Binding energy Aguas poco profundas Estres hidrostático Densidad de estados Masa efectiva Impurezas en GaAs |
| dc.subject.lemb.none.fl_str_mv |
Pozos cuánticos Quantum wells Energía de enlace Binding energy |
| dc.subject.proposal.spa.fl_str_mv |
Aguas poco profundas Estres hidrostático Densidad de estados Masa efectiva |
| dc.subject.proposal.none.fl_str_mv |
Impurezas en GaAs |
| description |
ABSTRACT: The effects of hydrostatic stress on the binding energy and the density of shallow-donor and shallow-acceptor impurity states in a GaAs–(Ga, Al)As quantum well are calculated using a variational procedure within the effective-mass approximation. Results are for different well widths and hydrostatic stresses, as a function of the impurity position along the growth direction of the structure. We have found that in the low-pressure regime the binding energy changes linearly for both donor and acceptor impurities, independently of the sizes of the well. However, for high pressures (greater than 13.5 kbar) this is valid for acceptors but not for donors due to the -X crossover. We have shown that there are two special structures in the density of impurity states, one associated with on-centre and the other with on-edge impurities. Also, we have observed that the density of impurity states depends strongly on the applied hydrostatic stress. |
| publishDate |
2003 |
| dc.date.issued.none.fl_str_mv |
2003 |
| dc.date.accessioned.none.fl_str_mv |
2016-10-07T23:12:32Z |
| dc.date.available.none.fl_str_mv |
2016-10-07T23:12:32Z |
| dc.type.spa.fl_str_mv |
Artículo de investigación |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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https://purl.org/redcol/resource_type/ART |
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http://purl.org/coar/version/c_970fb48d4fbd8a85 |
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info:eu-repo/semantics/article |
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info:eu-repo/semantics/publishedVersion |
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http://purl.org/coar/resource_type/c_2df8fbb1 |
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publishedVersion |
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López Ríos, S. Y., Porras-Montenegro, N., & Duque, C. A. (2003). Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells: effects of an applied hydrostatic stress. Semiconductor Science and Technology, 18(7), 718-722. |
| dc.identifier.issn.none.fl_str_mv |
0268-1242 |
| dc.identifier.uri.none.fl_str_mv |
http://hdl.handle.net/10495/4866 |
| dc.identifier.eissn.none.fl_str_mv |
1361-6641 |
| identifier_str_mv |
López Ríos, S. Y., Porras-Montenegro, N., & Duque, C. A. (2003). Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells: effects of an applied hydrostatic stress. Semiconductor Science and Technology, 18(7), 718-722. 0268-1242 1361-6641 |
| url |
http://hdl.handle.net/10495/4866 |
| dc.language.iso.spa.fl_str_mv |
eng |
| language |
eng |
| dc.relation.ispartofjournalabbrev.spa.fl_str_mv |
Semicond. Sci. Technol. |
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722 |
| dc.relation.citationissue.spa.fl_str_mv |
7 |
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718 |
| dc.relation.citationvolume.spa.fl_str_mv |
18 |
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Semiconductor Science and Technology |
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https://creativecommons.org/licenses/by-nc-nd/4.0/ |
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Atribución-NoComercial-SinDerivadas 2.5 Colombia |
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López Ríos, Sonia YanethPorras Montenegro, NelsonDuque Echeverri, Carlos AlbertoGrupo de Educación en Ciencias Experimentales y Matemáticas (GECEM)2016-10-07T23:12:32Z2016-10-07T23:12:32Z2003López Ríos, S. Y., Porras-Montenegro, N., & Duque, C. A. (2003). Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells: effects of an applied hydrostatic stress. Semiconductor Science and Technology, 18(7), 718-722.0268-1242http://hdl.handle.net/10495/48661361-6641ABSTRACT: The effects of hydrostatic stress on the binding energy and the density of shallow-donor and shallow-acceptor impurity states in a GaAs–(Ga, Al)As quantum well are calculated using a variational procedure within the effective-mass approximation. Results are for different well widths and hydrostatic stresses, as a function of the impurity position along the growth direction of the structure. We have found that in the low-pressure regime the binding energy changes linearly for both donor and acceptor impurities, independently of the sizes of the well. However, for high pressures (greater than 13.5 kbar) this is valid for acceptors but not for donors due to the -X crossover. We have shown that there are two special structures in the density of impurity states, one associated with on-centre and the other with on-edge impurities. Also, we have observed that the density of impurity states depends strongly on the applied hydrostatic stress.application/pdfengInstitute of Physics Publishing Ltd.https://creativecommons.org/licenses/by-nc-nd/4.0/http://creativecommons.org/licenses/by-nc-nd/2.5/co/Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Binding energy and density of shallow impurity states in GaAs–(Ga, Al)As quantum wells : effects of an applied hydrostatic stressArtículo de investigaciónhttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARThttp://purl.org/coar/version/c_970fb48d4fbd8a85info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionHidrostáticaHydrostaticsPozos cuánticosQuantum wellsEnergía de enlaceBinding energyAguas poco profundasEstres hidrostáticoDensidad de estadosMasa efectivaImpurezas en GaAsSemicond. Sci. Technol.722771818Semiconductor Science and TechnologyPublicationCC-LICENSElicense_urllicense_urlArtículo de investigacióntext/plain; charset=utf-849https://bibliotecadigital.udea.edu.co/bitstreams/ceccf327-c250-42c0-aeec-4716862cd0ee/download4afdbb8c545fd630ea7db775da747b2fMD52falseAnonymousREADlicense_textlicense_texttext/html; charset=utf-80https://bibliotecadigital.udea.edu.co/bitstreams/d9eec9e3-83c5-42e6-a682-1179206bab44/downloadd41d8cd98f00b204e9800998ecf8427eMD53falseAnonymousREADlicense_rdflicense_rdfLicenciaapplication/rdf+xml; charset=utf-80https://bibliotecadigital.udea.edu.co/bitstreams/e815af65-0d36-426b-9e66-fd0d5518c8ba/downloadd41d8cd98f00b204e9800998ecf8427eMD54falseAnonymousREADLICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://bibliotecadigital.udea.edu.co/bitstreams/c644e16d-fb41-4068-838f-1bdd977b301a/download8a4605be74aa9ea9d79846c1fba20a33MD55falseAnonymousREADORIGINALLopezSonia_2003_BindingEnergy.pdfLopezSonia_2003_BindingEnergy.pdfArtículo de investigaciónapplication/pdf212137https://bibliotecadigital.udea.edu.co/bitstreams/a1fc9a4f-97de-491a-a344-4e061fb399af/download39a81fc44c69794164cc1d82769d136cMD51trueAnonymousREADTEXTLopezSonia_2003_BindingEnergy.pdf.txtLopezSonia_2003_BindingEnergy.pdf.txtExtracted texttext/plain17539https://bibliotecadigital.udea.edu.co/bitstreams/06510d2c-31c7-4d64-8cd7-16147ffa2f87/download6e17b642361aedf8fb6d7aff8e773fe0MD510falseAnonymousREADTHUMBNAILLopezSonia_2003_BindingEnergy.pdf.jpgLopezSonia_2003_BindingEnergy.pdf.jpgGenerated Thumbnailimage/jpeg6728https://bibliotecadigital.udea.edu.co/bitstreams/66c03f85-5151-4872-b6a8-4a2fc5110a71/download14fe28a72854411b7f06075724516db8MD511falseAnonymousREAD10495/4866oai:bibliotecadigital.udea.edu.co:10495/48662025-03-26 17:07:43.766https://creativecommons.org/licenses/by-nc-nd/4.0/open.accesshttps://bibliotecadigital.udea.edu.coRepositorio Institucional de la Universidad de Antioquiaaplicacionbibliotecadigitalbiblioteca@udea.edu.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 |
