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Metal Ion Control of Photoinduced Electron Spin Polarization in Electronic Ground States.
Kirk, Martin L; Shultz, David A; Chen, Ju; Hewitt, Patrick; Daley, David; Paudel, Sangita; van der Est, Art.
Afiliação
  • Kirk ML; Department of Chemistry and Chemical Biology, The University of New Mexico, Albuquerque, New Mexico 87131-0001, United States.
  • Shultz DA; The Center for High Technology Materials, The University of New Mexico, Albuquerque, New Mexico 87106, United States.
  • Chen J; Department of Chemistry, North Carolina State University, Raleigh, North Carolina 27695-8204, United States.
  • Hewitt P; Department of Chemistry and Chemical Biology, The University of New Mexico, Albuquerque, New Mexico 87131-0001, United States.
  • Daley D; Department of Chemistry, North Carolina State University, Raleigh, North Carolina 27695-8204, United States.
  • Paudel S; Department of Chemistry, North Carolina State University, Raleigh, North Carolina 27695-8204, United States.
  • van der Est A; Department of Chemistry and Chemical Biology, The University of New Mexico, Albuquerque, New Mexico 87131-0001, United States.
J Am Chem Soc ; 143(28): 10519-10523, 2021 Jul 21.
Article em En | MEDLINE | ID: mdl-34251803
Both the sign and intensity of photoinduced electron spin polarization (ESP) in the electronic ground state doublet (2S0/D0) of chromophore-radical complexes can be controlled by changing the nature of the metal ion. The complexes consist of an organic radical (nitronyl nitroxide, NN) covalently attached to a donor-acceptor chromophore via a m-phenylene bridge, (bpy)M(CAT-m-Ph-NN) (1) (bpy = 4,4'-di-tert-butyl-2,2'-bipyridine, M = PdII (1-Pd) or PtII (1-Pt), CAT = 3-tert-butylcatecholate, m-Ph = meta-phenylene). In both complexes, photoexcitation with visible light produces an initial exchange-coupled, three-spin (bpy•-, CAT•+ = semiquinone (SQ), and NN•), charge-separated doublet 2S1 (S = chromophore excited spin singlet configuration) excited state that rapidly decays to the ground state via a 2T1 (T = chromophore excited spin triplet configuration) state. This process is not expected to be spin selective, and only very weak emissive ESP is found for 1-Pd. In contrast, strong absorptive ESP is generated in 1-Pt. It is postulated that zero-field-splitting-induced transitions between the chromophoric 2T1 and 4T1 states (1-Pd and 1-Pt) and spin-orbit-induced transitions between 2T1 and NN-based quartet states (1-Pt) account for the differences in polarization.

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article

Texto completo: 1 Base de dados: MEDLINE Idioma: En Ano de publicação: 2021 Tipo de documento: Article