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基态电子中光致电子自旋极化的金属离子控制

Metal Ion Control of Photoinduced Electron Spin Polarization in Electronic Ground States.

作者信息

Kirk Martin L, Shultz David A, Chen Ju, Hewitt Patrick, Daley David, Paudel Sangita, van der Est Art

机构信息

Department of Chemistry and Chemical Biology, The University of New Mexico, Albuquerque, New Mexico 87131-0001, United States.

The Center for High Technology Materials, The University of New Mexico, Albuquerque, New Mexico 87106, United States.

出版信息

J Am Chem Soc. 2021 Jul 21;143(28):10519-10523. doi: 10.1021/jacs.1c04149. Epub 2021 Jul 12.

Abstract

Both the sign and intensity of photoinduced electron spin polarization (ESP) in the electronic ground state doublet (S/D) 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 -phenylene bridge, (bpy)M(CAT--Ph-NN) () (bpy = 4,4'-di--butyl-2,2'-bipyridine, M = Pd () or Pt (), CAT = 3--butylcatecholate, -Ph = -phenylene). In both complexes, photoexcitation with visible light produces an initial exchange-coupled, three-spin (bpy, CAT = semiquinone (SQ), and NN), charge-separated doublet S (S = chromophore excited spin singlet configuration) excited state that rapidly decays to the ground state via a T (T = chromophore excited spin triplet configuration) state. This process is not expected to be spin selective, and only very weak ESP is found for . In contrast, strong ESP is generated in . It is postulated that zero-field-splitting-induced transitions between the chromophoric T and T states ( and ) and spin-orbit-induced transitions between T and NN-based quartet states () account for the differences in polarization.

摘要

通过改变金属离子的性质,可以控制发色团 - 自由基配合物电子基态双重态(S/D)中光诱导电子自旋极化(ESP)的符号和强度。这些配合物由一个有机自由基(硝酰基氮氧化物,NN)通过亚苯基桥共价连接到一个供体 - 受体发色团组成,(bpy)M(CAT--Ph-NN) ()(bpy = 4,4'-二 - 丁基 - 2,2'-联吡啶,M = Pd ()或Pt (),CAT = 3 - 丁基儿茶酚,-Ph = 亚苯基)。在这两种配合物中,用可见光进行光激发会产生一个初始的交换耦合三自旋(bpy、CAT = 半醌(SQ)和NN)电荷分离双重态S(S = 发色团激发自旋单重态构型)激发态,该激发态通过T态(T = 发色团激发自旋三重态构型)迅速衰减到基态。预计这个过程不是自旋选择性的,并且对于 仅发现非常弱的ESP。相比之下,在 中产生了强ESP。据推测发色团T和T态之间的零场分裂诱导跃迁( 和 )以及T和基于NN的四重态之间的自旋轨道诱导跃迁()解释了极化的差异。

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