Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship

We have interpreted the two-photon absorption spectrum of water-soluble copper indium sulfide (CIS) QDs with stoichiometry 0.18 (Cu), 0.42 (In), and 2 (S) and an average diameter of approximately 2.6 nm. For that, we employed the wavelength-tunable femtosecond Z-scan technique and the parabolic effe...

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Autores:
Dos Reis, George B
Rodriguez, Ruben D.F
Dos Santos, Calink I.L
Gontijo Aparecida Pinto, Leiriana
Schiavon, Marco Antonio
De Boni, Leonardo
Mendonça, Cleber Renato
Vivas, Marcelo G.
Tipo de recurso:
Article of journal
Fecha de publicación:
2018
Institución:
Corporación Universidad de la Costa
Repositorio:
REDICUC - Repositorio CUC
Idioma:
eng
OAI Identifier:
oai:repositorio.cuc.edu.co:11323/928
Acceso en línea:
https://hdl.handle.net/11323/928
https://doi.org/10.1016/j.optmat.2018.10.023
https://repositorio.cuc.edu.co/
Palabra clave:
CuInS2 Quantum Dots
Femtosecond Laser
Nanomaterials
Parabolic Effective-Mass Approximation Model
Two-Photon Absorption
Wavelength-Tunable Femtosecond Z-Scan Technique
Rights
openAccess
License
Atribución – No comercial – Compartir igual
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oai_identifier_str oai:repositorio.cuc.edu.co:11323/928
network_acronym_str RCUC2
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repository_id_str
dc.title.eng.fl_str_mv Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
title Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
spellingShingle Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
CuInS2 Quantum Dots
Femtosecond Laser
Nanomaterials
Parabolic Effective-Mass Approximation Model
Two-Photon Absorption
Wavelength-Tunable Femtosecond Z-Scan Technique
title_short Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
title_full Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
title_fullStr Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
title_full_unstemmed Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
title_sort Femtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties Relationship
dc.creator.fl_str_mv Dos Reis, George B
Rodriguez, Ruben D.F
Dos Santos, Calink I.L
Gontijo Aparecida Pinto, Leiriana
Schiavon, Marco Antonio
De Boni, Leonardo
Mendonça, Cleber Renato
Vivas, Marcelo G.
dc.contributor.author.spa.fl_str_mv Dos Reis, George B
Rodriguez, Ruben D.F
Dos Santos, Calink I.L
Gontijo Aparecida Pinto, Leiriana
Schiavon, Marco Antonio
De Boni, Leonardo
Mendonça, Cleber Renato
Vivas, Marcelo G.
dc.subject.eng.fl_str_mv CuInS2 Quantum Dots
Femtosecond Laser
Nanomaterials
Parabolic Effective-Mass Approximation Model
Two-Photon Absorption
Wavelength-Tunable Femtosecond Z-Scan Technique
topic CuInS2 Quantum Dots
Femtosecond Laser
Nanomaterials
Parabolic Effective-Mass Approximation Model
Two-Photon Absorption
Wavelength-Tunable Femtosecond Z-Scan Technique
description We have interpreted the two-photon absorption spectrum of water-soluble copper indium sulfide (CIS) QDs with stoichiometry 0.18 (Cu), 0.42 (In), and 2 (S) and an average diameter of approximately 2.6 nm. For that, we employed the wavelength-tunable femtosecond Z-scan technique and the parabolic effective-mass approximation model, in which the excitonic transition energies were phenomenologically corrected due to the stoichiometry of the nanocrystal. This model considers a conduction band and three valence sub-bands allowing excitonic transitions via centrosymmetric (Δl = ±1, where l is the angular momentum of the absorbing state) and non-centrosymmetric (Δl = 0) channels. In such case, this became relevant because the CIS QDs with chalcopyrite crystalline structure is a non-centrosymmetric semiconductor. Thus, our experimental results pointed out two 2 PA allowed bands located at 715 nm (2hv = 3.47 eV) and 625 nm (2hv = 3.97 eV) with cross sections of (6.3 ± 1.0) x 102 GM and (4.5 ± 0.7) x 102 GM, respectively. According to the theoretical model, these 2 PA bands can be ascribed to the 1P1/2(h3) → 1S3/2(e) (lower energy band) and 1P1/2(hheavy) → 1S3/2(e) (90%)/(10%)1P1/2(hsplit-off) → 1P3/2(e) (higher energy band) excitonic transitions. A good agreement (magnitude and spectral position) between the experimental and theoretical data were obtained. However, our experimental data suggest that the higher-energy 2 PA band may have other contributions due to the mixing between the heavy- and the light-hole bands, which the effective mass model does not take into consideration.
publishDate 2018
dc.date.accessioned.none.fl_str_mv 2018-11-13T23:33:56Z
dc.date.available.none.fl_str_mv 2018-11-13T23:33:56Z
dc.date.issued.none.fl_str_mv 2018-10-13
dc.type.spa.fl_str_mv Artículo de revista
dc.type.coar.fl_str_mv http://purl.org/coar/resource_type/c_2df8fbb1
dc.type.coar.spa.fl_str_mv http://purl.org/coar/resource_type/c_6501
dc.type.content.spa.fl_str_mv Text
dc.type.driver.spa.fl_str_mv info:eu-repo/semantics/article
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dc.identifier.issn.spa.fl_str_mv 09253467
dc.identifier.uri.spa.fl_str_mv https://hdl.handle.net/11323/928
dc.identifier.doi.spa.fl_str_mv https://doi.org/10.1016/j.optmat.2018.10.023
dc.identifier.instname.spa.fl_str_mv Corporación Universidad de la Costa
dc.identifier.reponame.spa.fl_str_mv REDICUC - Repositorio CUC
dc.identifier.repourl.spa.fl_str_mv https://repositorio.cuc.edu.co/
identifier_str_mv 09253467
Corporación Universidad de la Costa
REDICUC - Repositorio CUC
url https://hdl.handle.net/11323/928
https://doi.org/10.1016/j.optmat.2018.10.023
https://repositorio.cuc.edu.co/
dc.language.iso.none.fl_str_mv eng
language eng
dc.rights.spa.fl_str_mv Atribución – No comercial – Compartir igual
dc.rights.accessrights.spa.fl_str_mv info:eu-repo/semantics/openAccess
dc.rights.coar.spa.fl_str_mv http://purl.org/coar/access_right/c_abf2
rights_invalid_str_mv Atribución – No comercial – Compartir igual
http://purl.org/coar/access_right/c_abf2
eu_rights_str_mv openAccess
dc.publisher.spa.fl_str_mv Optical Materials
institution Corporación Universidad de la Costa
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spelling Dos Reis, George BRodriguez, Ruben D.FDos Santos, Calink I.LGontijo Aparecida Pinto, LeirianaSchiavon, Marco AntonioDe Boni, LeonardoMendonça, Cleber RenatoVivas, Marcelo G.2018-11-13T23:33:56Z2018-11-13T23:33:56Z2018-10-1309253467https://hdl.handle.net/11323/928https://doi.org/10.1016/j.optmat.2018.10.023Corporación Universidad de la CostaREDICUC - Repositorio CUChttps://repositorio.cuc.edu.co/We have interpreted the two-photon absorption spectrum of water-soluble copper indium sulfide (CIS) QDs with stoichiometry 0.18 (Cu), 0.42 (In), and 2 (S) and an average diameter of approximately 2.6 nm. For that, we employed the wavelength-tunable femtosecond Z-scan technique and the parabolic effective-mass approximation model, in which the excitonic transition energies were phenomenologically corrected due to the stoichiometry of the nanocrystal. This model considers a conduction band and three valence sub-bands allowing excitonic transitions via centrosymmetric (Δl = ±1, where l is the angular momentum of the absorbing state) and non-centrosymmetric (Δl = 0) channels. In such case, this became relevant because the CIS QDs with chalcopyrite crystalline structure is a non-centrosymmetric semiconductor. Thus, our experimental results pointed out two 2 PA allowed bands located at 715 nm (2hv = 3.47 eV) and 625 nm (2hv = 3.97 eV) with cross sections of (6.3 ± 1.0) x 102 GM and (4.5 ± 0.7) x 102 GM, respectively. According to the theoretical model, these 2 PA bands can be ascribed to the 1P1/2(h3) → 1S3/2(e) (lower energy band) and 1P1/2(hheavy) → 1S3/2(e) (90%)/(10%)1P1/2(hsplit-off) → 1P3/2(e) (higher energy band) excitonic transitions. A good agreement (magnitude and spectral position) between the experimental and theoretical data were obtained. However, our experimental data suggest that the higher-energy 2 PA band may have other contributions due to the mixing between the heavy- and the light-hole bands, which the effective mass model does not take into consideration.Dos Reis, George B-e77d314c-05e2-4e8b-8709-d62a691d2bbc-0Rodriguez, Ruben D.F-7229698d-b56e-4980-8e9f-7a6b5e8140bf-0Dos Santos, Calink I.L-182b4837-4c54-4b16-a864-780faebf43ee-0Gontijo Aparecida Pinto, Leiriana-019e0408-3486-402c-83a3-77da39830944-0Schiavon, Marco Antonio-c77383eb-7158-4569-ab43-911d4c06639e-0De Boni, Leonardo-1512485b-5ae7-41bb-ad93-884ec1267e98-0Mendonça, Cleber Renato-b8684928-3b62-415d-a198-656aa5bd3f4d-0Vivas, Marcelo G.-0ccec8cf-e645-445c-8ecc-6283c4a664e8-0engOptical MaterialsAtribución – No comercial – Compartir igualinfo:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2CuInS2 Quantum DotsFemtosecond LaserNanomaterialsParabolic Effective-Mass Approximation ModelTwo-Photon AbsorptionWavelength-Tunable Femtosecond Z-Scan TechniqueFemtosecond Two-Photon Absorption Spectroscopy Of Copper Indium Sulfide Quantum Dots: A Structure-Optical Properties RelationshipArtículo de revistahttp://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/acceptedVersionPublicationORIGINALFemtosecond Two-Photon Absorption Spectroscopy Of Copper.pdfFemtosecond Two-Photon Absorption Spectroscopy Of Copper.pdfapplication/pdf288181https://repositorio.cuc.edu.co/bitstreams/e9886698-1117-4521-a720-5e7b4ee1bd98/download207fb75abcaa4dfb57624b0f2f5eff99MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://repositorio.cuc.edu.co/bitstreams/3d019470-07b1-47a1-9e34-40f0a1c22924/download8a4605be74aa9ea9d79846c1fba20a33MD52THUMBNAILFemtosecond Two-Photon Absorption Spectroscopy Of Copper.pdf.jpgFemtosecond Two-Photon Absorption Spectroscopy Of Copper.pdf.jpgimage/jpeg53725https://repositorio.cuc.edu.co/bitstreams/e5e6c549-673c-4ef4-8470-9de53e2bd26d/downloadaf9fed06f63c5aa4ed1fdef1114524cfMD54TEXTFemtosecond Two-Photon Absorption Spectroscopy Of Copper.pdf.txtFemtosecond Two-Photon Absorption Spectroscopy Of Copper.pdf.txttext/plain2141https://repositorio.cuc.edu.co/bitstreams/bfb86a8a-c443-4e53-bf71-5537ca8b650c/downloada5cf9f32cae5e6a6716e83d794619ae0MD5511323/928oai:repositorio.cuc.edu.co:11323/9282024-09-17 10:48:28.234open.accesshttps://repositorio.cuc.edu.coRepositorio de la Universidad de la Costa CUCrepdigital@cuc.edu.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