Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes

Autores
Cadranel, Alejandro; Oviedo, Paola Soledad; Pieslinger, German Eduardo; Yamazaki, Shiori; Kleiman, Valeria D.; Baraldo Victorica, Luis Mario; Guldi, Dirk M.
Año de publicación
2017
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
The picosecond excited state dynamics of [Ru(tpm)(bpy)(NCS)]+ (RubNCS+) and [Ru(tpm)(bpy)(CN)]+ (RubCN+) (tpm = tris(1-pyrazolyl)methane, bpy = 2,2′-bipyridine) have been analyzed by means of transient absorption measurements and spectroelectrochemistry. Emissive 3MLCTs with (GS)HOMO(h+)-(GS)LUMO(e-) configurations are the lowest triplet excited states regardless of whether 387 or 505 nm photoexcitation is used. 387 nm photoexcitation yields, after a few picoseconds, the emissive 3MLCTs. In contrast, 505 nm photoexcitation populates an intermediate excited state that we assign as a 3MLCT state, in which the hole sits in a metal-centered orbital of different symmetry, prior to its conversion to the emissive 3MLCTs. The disparities in terms of electronic configuration between the intermediate and the emissive 3MLCTs have two important consequences. On one hand, both states feature very different fingerprint absorptions in transient absorption measurements. On the other hand, the reconfiguration is impeded by a kinetic barrier. As such, the conversion is followed spectroscopically and kinetically on the 300 ps timescale.
Fil: Cadranel, Alejandro. Universitat Erlangen-Nuremberg; Alemania
Fil: Oviedo, Paola Soledad. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; Argentina
Fil: Pieslinger, German Eduardo. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; Argentina
Fil: Yamazaki, Shiori. University of Florida. Departament of Chemistry; Estados Unidos
Fil: Kleiman, Valeria D.. University of Florida. Departament of Chemistry; Estados Unidos
Fil: Baraldo Victorica, Luis Mario. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; Argentina
Fil: Guldi, Dirk M.. Universitat Erlangen-Nuremberg; Alemania
Materia
Ruthenium Polypyridines
MLCT Excited State
Nivel de accesibilidad
acceso abierto
Condiciones de uso
https://creativecommons.org/licenses/by/2.5/ar/
Repositorio
CONICET Digital (CONICET)
Institución
Consejo Nacional de Investigaciones Científicas y Técnicas
OAI Identificador
oai:ri.conicet.gov.ar:11336/65758

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network_name_str CONICET Digital (CONICET)
spelling Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexesCadranel, AlejandroOviedo, Paola SoledadPieslinger, German EduardoYamazaki, ShioriKleiman, Valeria D.Baraldo Victorica, Luis MarioGuldi, Dirk M.Ruthenium PolypyridinesMLCT Excited Statehttps://purl.org/becyt/ford/1.4https://purl.org/becyt/ford/1The picosecond excited state dynamics of [Ru(tpm)(bpy)(NCS)]+ (RubNCS+) and [Ru(tpm)(bpy)(CN)]+ (RubCN+) (tpm = tris(1-pyrazolyl)methane, bpy = 2,2′-bipyridine) have been analyzed by means of transient absorption measurements and spectroelectrochemistry. Emissive 3MLCTs with (GS)HOMO(h+)-(GS)LUMO(e-) configurations are the lowest triplet excited states regardless of whether 387 or 505 nm photoexcitation is used. 387 nm photoexcitation yields, after a few picoseconds, the emissive 3MLCTs. In contrast, 505 nm photoexcitation populates an intermediate excited state that we assign as a 3MLCT state, in which the hole sits in a metal-centered orbital of different symmetry, prior to its conversion to the emissive 3MLCTs. The disparities in terms of electronic configuration between the intermediate and the emissive 3MLCTs have two important consequences. On one hand, both states feature very different fingerprint absorptions in transient absorption measurements. On the other hand, the reconfiguration is impeded by a kinetic barrier. As such, the conversion is followed spectroscopically and kinetically on the 300 ps timescale.Fil: Cadranel, Alejandro. Universitat Erlangen-Nuremberg; AlemaniaFil: Oviedo, Paola Soledad. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; ArgentinaFil: Pieslinger, German Eduardo. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; ArgentinaFil: Yamazaki, Shiori. University of Florida. Departament of Chemistry; Estados UnidosFil: Kleiman, Valeria D.. University of Florida. Departament of Chemistry; Estados UnidosFil: Baraldo Victorica, Luis Mario. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; ArgentinaFil: Guldi, Dirk M.. Universitat Erlangen-Nuremberg; AlemaniaRoyal Society of Chemistry2017-08info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionhttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfapplication/pdfapplication/pdfapplication/pdfapplication/pdfhttp://hdl.handle.net/11336/65758Cadranel, Alejandro; Oviedo, Paola Soledad; Pieslinger, German Eduardo; Yamazaki, Shiori; Kleiman, Valeria D.; et al.; Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes; Royal Society of Chemistry; Chemical Science; 8; 11; 8-2017; 7434-74422041-65202041-6539CONICET DigitalCONICETenginfo:eu-repo/semantics/altIdentifier/url/http://xlink.rsc.org/?DOI=C7SC02670Finfo:eu-repo/semantics/altIdentifier/doi/10.1039/C7SC02670Finfo:eu-repo/semantics/openAccesshttps://creativecommons.org/licenses/by/2.5/ar/reponame:CONICET Digital (CONICET)instname:Consejo Nacional de Investigaciones Científicas y Técnicas2025-11-05T09:44:10Zoai:ri.conicet.gov.ar:11336/65758instacron:CONICETInstitucionalhttp://ri.conicet.gov.ar/Organismo científico-tecnológicoNo correspondehttp://ri.conicet.gov.ar/oai/requestdasensio@conicet.gov.ar; lcarlino@conicet.gov.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:34982025-11-05 09:44:10.993CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicasfalse
dc.title.none.fl_str_mv Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
title Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
spellingShingle Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
Cadranel, Alejandro
Ruthenium Polypyridines
MLCT Excited State
title_short Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
title_full Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
title_fullStr Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
title_full_unstemmed Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
title_sort Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes
dc.creator.none.fl_str_mv Cadranel, Alejandro
Oviedo, Paola Soledad
Pieslinger, German Eduardo
Yamazaki, Shiori
Kleiman, Valeria D.
Baraldo Victorica, Luis Mario
Guldi, Dirk M.
author Cadranel, Alejandro
author_facet Cadranel, Alejandro
Oviedo, Paola Soledad
Pieslinger, German Eduardo
Yamazaki, Shiori
Kleiman, Valeria D.
Baraldo Victorica, Luis Mario
Guldi, Dirk M.
author_role author
author2 Oviedo, Paola Soledad
Pieslinger, German Eduardo
Yamazaki, Shiori
Kleiman, Valeria D.
Baraldo Victorica, Luis Mario
Guldi, Dirk M.
author2_role author
author
author
author
author
author
dc.subject.none.fl_str_mv Ruthenium Polypyridines
MLCT Excited State
topic Ruthenium Polypyridines
MLCT Excited State
purl_subject.fl_str_mv https://purl.org/becyt/ford/1.4
https://purl.org/becyt/ford/1
dc.description.none.fl_txt_mv The picosecond excited state dynamics of [Ru(tpm)(bpy)(NCS)]+ (RubNCS+) and [Ru(tpm)(bpy)(CN)]+ (RubCN+) (tpm = tris(1-pyrazolyl)methane, bpy = 2,2′-bipyridine) have been analyzed by means of transient absorption measurements and spectroelectrochemistry. Emissive 3MLCTs with (GS)HOMO(h+)-(GS)LUMO(e-) configurations are the lowest triplet excited states regardless of whether 387 or 505 nm photoexcitation is used. 387 nm photoexcitation yields, after a few picoseconds, the emissive 3MLCTs. In contrast, 505 nm photoexcitation populates an intermediate excited state that we assign as a 3MLCT state, in which the hole sits in a metal-centered orbital of different symmetry, prior to its conversion to the emissive 3MLCTs. The disparities in terms of electronic configuration between the intermediate and the emissive 3MLCTs have two important consequences. On one hand, both states feature very different fingerprint absorptions in transient absorption measurements. On the other hand, the reconfiguration is impeded by a kinetic barrier. As such, the conversion is followed spectroscopically and kinetically on the 300 ps timescale.
Fil: Cadranel, Alejandro. Universitat Erlangen-Nuremberg; Alemania
Fil: Oviedo, Paola Soledad. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; Argentina
Fil: Pieslinger, German Eduardo. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; Argentina
Fil: Yamazaki, Shiori. University of Florida. Departament of Chemistry; Estados Unidos
Fil: Kleiman, Valeria D.. University of Florida. Departament of Chemistry; Estados Unidos
Fil: Baraldo Victorica, Luis Mario. Consejo Nacional de Investigaciones Científicas y Técnicas. Oficina de Coordinación Administrativa Ciudad Universitaria. Instituto de Química, Física de los Materiales, Medioambiente y Energía. Universidad de Buenos Aires. Facultad de Ciencias Exactas y Naturales. Instituto de Química, Física de los Materiales, Medioambiente y Energía; Argentina
Fil: Guldi, Dirk M.. Universitat Erlangen-Nuremberg; Alemania
description The picosecond excited state dynamics of [Ru(tpm)(bpy)(NCS)]+ (RubNCS+) and [Ru(tpm)(bpy)(CN)]+ (RubCN+) (tpm = tris(1-pyrazolyl)methane, bpy = 2,2′-bipyridine) have been analyzed by means of transient absorption measurements and spectroelectrochemistry. Emissive 3MLCTs with (GS)HOMO(h+)-(GS)LUMO(e-) configurations are the lowest triplet excited states regardless of whether 387 or 505 nm photoexcitation is used. 387 nm photoexcitation yields, after a few picoseconds, the emissive 3MLCTs. In contrast, 505 nm photoexcitation populates an intermediate excited state that we assign as a 3MLCT state, in which the hole sits in a metal-centered orbital of different symmetry, prior to its conversion to the emissive 3MLCTs. The disparities in terms of electronic configuration between the intermediate and the emissive 3MLCTs have two important consequences. On one hand, both states feature very different fingerprint absorptions in transient absorption measurements. On the other hand, the reconfiguration is impeded by a kinetic barrier. As such, the conversion is followed spectroscopically and kinetically on the 300 ps timescale.
publishDate 2017
dc.date.none.fl_str_mv 2017-08
dc.type.none.fl_str_mv info:eu-repo/semantics/article
info:eu-repo/semantics/publishedVersion
http://purl.org/coar/resource_type/c_6501
info:ar-repo/semantics/articulo
format article
status_str publishedVersion
dc.identifier.none.fl_str_mv http://hdl.handle.net/11336/65758
Cadranel, Alejandro; Oviedo, Paola Soledad; Pieslinger, German Eduardo; Yamazaki, Shiori; Kleiman, Valeria D.; et al.; Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes; Royal Society of Chemistry; Chemical Science; 8; 11; 8-2017; 7434-7442
2041-6520
2041-6539
CONICET Digital
CONICET
url http://hdl.handle.net/11336/65758
identifier_str_mv Cadranel, Alejandro; Oviedo, Paola Soledad; Pieslinger, German Eduardo; Yamazaki, Shiori; Kleiman, Valeria D.; et al.; Trapping intermediate MLCT states in low-symmetry {Ru(bpy)} complexes; Royal Society of Chemistry; Chemical Science; 8; 11; 8-2017; 7434-7442
2041-6520
2041-6539
CONICET Digital
CONICET
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/url/http://xlink.rsc.org/?DOI=C7SC02670F
info:eu-repo/semantics/altIdentifier/doi/10.1039/C7SC02670F
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
https://creativecommons.org/licenses/by/2.5/ar/
eu_rights_str_mv openAccess
rights_invalid_str_mv https://creativecommons.org/licenses/by/2.5/ar/
dc.format.none.fl_str_mv application/pdf
application/pdf
application/pdf
application/pdf
application/pdf
dc.publisher.none.fl_str_mv Royal Society of Chemistry
publisher.none.fl_str_mv Royal Society of Chemistry
dc.source.none.fl_str_mv reponame:CONICET Digital (CONICET)
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reponame_str CONICET Digital (CONICET)
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repository.name.fl_str_mv CONICET Digital (CONICET) - Consejo Nacional de Investigaciones Científicas y Técnicas
repository.mail.fl_str_mv dasensio@conicet.gov.ar; lcarlino@conicet.gov.ar
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