Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds

Detalhes bibliográficos
Autor(a) principal: Buckup, Tiago
Data de Publicação: 2006
Outros Autores: Savolainen, Janne, Wohlleben, Wendel, Herek, Jennifer L., Hashimoto, Hideki, Correia, Ricardo Rego Bordalo, Motkus, Marcus
Tipo de documento: Artigo
Idioma: eng
Título da fonte: Repositório Institucional da UFRGS
Texto Completo: http://hdl.handle.net/10183/205002
Resumo: A series of all-trans-carotenoids with N=9, 13, and 15 conjugated bonds has been studied by pump-probe and pump-deplete-probe spectroscopies to obtain a systematic analysis of the energy flow between the different electronic states. The ultrafast dynamics in the carotenoids are initialized by excitation to the S2 state and subsequently manipulated by an additional depletion pulse in the near-IR spectral range. The changes in the dynamics after depletion of the excited state population allowed differentiation of the excited state absorption into two components, a major one corresponding to the well known S1 state and the small contribution on the red wing of the S0-S2 absorption band originating from the hot ground state. We found no evidence for an additional electronically excited state, usually called S∗. Instead, a deactivation mechanism that includes the hot ground state supports the observed results nicely in the framework of a simple three state model (S2, S1, and S0).
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spelling Buckup, TiagoSavolainen, JanneWohlleben, WendelHerek, Jennifer L.Hashimoto, HidekiCorreia, Ricardo Rego BordaloMotkus, Marcus2020-01-28T04:12:08Z20060021-9606http://hdl.handle.net/10183/205002000575808A series of all-trans-carotenoids with N=9, 13, and 15 conjugated bonds has been studied by pump-probe and pump-deplete-probe spectroscopies to obtain a systematic analysis of the energy flow between the different electronic states. The ultrafast dynamics in the carotenoids are initialized by excitation to the S2 state and subsequently manipulated by an additional depletion pulse in the near-IR spectral range. The changes in the dynamics after depletion of the excited state population allowed differentiation of the excited state absorption into two components, a major one corresponding to the well known S1 state and the small contribution on the red wing of the S0-S2 absorption band originating from the hot ground state. We found no evidence for an additional electronically excited state, usually called S∗. Instead, a deactivation mechanism that includes the hot ground state supports the observed results nicely in the framework of a simple three state model (S2, S1, and S0).application/pdfengThe journal of chemical physics. New York. Vol. 125, no. 19 (Nov. 2006), 194505, 7 p.CarotenóidesEspectroscopiaPump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bondsEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSTEXT000575808.pdf.txt000575808.pdf.txtExtracted Texttext/plain34938http://www.lume.ufrgs.br/bitstream/10183/205002/2/000575808.pdf.txt7d66f6f531dc6bf4ec75f4d8dc830454MD52ORIGINAL000575808.pdfTexto completo (inglês)application/pdf670137http://www.lume.ufrgs.br/bitstream/10183/205002/1/000575808.pdf3b742298e9b5ac393172a9675b4610c2MD5110183/2050022020-01-29 05:08:41.089372oai:www.lume.ufrgs.br:10183/205002Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2020-01-29T07:08:41Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false
dc.title.pt_BR.fl_str_mv Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
title Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
spellingShingle Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
Buckup, Tiago
Carotenóides
Espectroscopia
title_short Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
title_full Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
title_fullStr Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
title_full_unstemmed Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
title_sort Pump-probe and pump-deplete-probe spectroscopies on carotenoids with N=9–15 conjugated bonds
author Buckup, Tiago
author_facet Buckup, Tiago
Savolainen, Janne
Wohlleben, Wendel
Herek, Jennifer L.
Hashimoto, Hideki
Correia, Ricardo Rego Bordalo
Motkus, Marcus
author_role author
author2 Savolainen, Janne
Wohlleben, Wendel
Herek, Jennifer L.
Hashimoto, Hideki
Correia, Ricardo Rego Bordalo
Motkus, Marcus
author2_role author
author
author
author
author
author
dc.contributor.author.fl_str_mv Buckup, Tiago
Savolainen, Janne
Wohlleben, Wendel
Herek, Jennifer L.
Hashimoto, Hideki
Correia, Ricardo Rego Bordalo
Motkus, Marcus
dc.subject.por.fl_str_mv Carotenóides
Espectroscopia
topic Carotenóides
Espectroscopia
description A series of all-trans-carotenoids with N=9, 13, and 15 conjugated bonds has been studied by pump-probe and pump-deplete-probe spectroscopies to obtain a systematic analysis of the energy flow between the different electronic states. The ultrafast dynamics in the carotenoids are initialized by excitation to the S2 state and subsequently manipulated by an additional depletion pulse in the near-IR spectral range. The changes in the dynamics after depletion of the excited state population allowed differentiation of the excited state absorption into two components, a major one corresponding to the well known S1 state and the small contribution on the red wing of the S0-S2 absorption band originating from the hot ground state. We found no evidence for an additional electronically excited state, usually called S∗. Instead, a deactivation mechanism that includes the hot ground state supports the observed results nicely in the framework of a simple three state model (S2, S1, and S0).
publishDate 2006
dc.date.issued.fl_str_mv 2006
dc.date.accessioned.fl_str_mv 2020-01-28T04:12:08Z
dc.type.driver.fl_str_mv Estrangeiro
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dc.identifier.uri.fl_str_mv http://hdl.handle.net/10183/205002
dc.identifier.issn.pt_BR.fl_str_mv 0021-9606
dc.identifier.nrb.pt_BR.fl_str_mv 000575808
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url http://hdl.handle.net/10183/205002
dc.language.iso.fl_str_mv eng
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dc.relation.ispartof.pt_BR.fl_str_mv The journal of chemical physics. New York. Vol. 125, no. 19 (Nov. 2006), 194505, 7 p.
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