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Ultrafast photoinduced charge transport in Pt(n) donor-acceptor assembly bearing naphthalimide electron acceptor and phenothiazine electron donor

机译:含萘二甲酰亚胺电子受体和吩噻嗪电子供体的Pt(n)供体-受体组件中的超快光诱导电荷传输

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摘要

Visible light-induced charge transfer dynamics were investigated in a novel transition metal triad acceptor-chromophore-donor, (NDI-phen)Pt(n)(-C=C-Ph-CH2-PTZ)2 (1), designed for photo-induced charge separation using a combination of time-resolved infrared (TRIR) and femtosecond electronic transient absorption (TA) spectroscopy, in 1, the electron acceptor is 1,4,5,8-naphthalene diimide (ND1), and the electron donor is phenothiazine (PTZ), and [(phen)Pt(-C=C-Ph-)] where phen is 1,10-phenanthroline, represents the chromophoric core. The first excited state observed in 1 is a ~3MLCT7 LL'CT, with {Pt(II)-acetylide}-to-phen character. Following that, charge transfer from the phen-anion onto the NDI subunit to form NDr-phen-[Pt-(C = C)2]~+-PTZ2 occurs with a time constant of 2.3 ps. This transition is characterised by appearance of the prominent NDI-anion features in both TRIR and TA spectra. The final step of the charge separation in 1 proceeds with a time constant of ~15 ps during which the hole migrates from the [Pt-(C=C)2] subunit to one of the PTZ groups. Charge recombination in 1 then occurs with two distinct time constants of 36 ns and 107 ns, corresponding to the back electron transfer to each of the two donor groups; a rather rare occurrence which manifests that the hole in the final charge-separated state is localised on one of the two donor PTZ groups. The assignment of the nature of the excited states and dynamics in 1 was assisted by TRIR investigations of the analogous previously reported ((COOEt)2bpy)Pt(C=C-Ph-CH2-PTZ)2 (2), (J. E. McGarrah and R. Eisenberg, Inorg. Chem., 2003, 42, 4355; J. E. McGarrah, J. T. Hupp and S. N. Smirnov, J. Phys. Chem. A 2009, 113, 6430) as well as (bpy)Pt(C C-Ph-C7H_(15))2, which represent the acceptor-free dyad, and the chromophoric core, respectively. Thus, the step-wise formation of the full charge-separated state on the picosecond time scale and charge recombination via tunnelling have been established; and the presence of two distinct charge recombination pathways has been observed.
机译:在新型的过渡金属三重态受体-发色团-供体(NDI-phen)Pt(n)(-C = C-Ph-CH2-PTZ)2(1)中研究了可见光诱导的电荷转移动力学时间分辨红外(TRIR)和飞秒电子瞬态吸收(TA)光谱结合使用-诱导的电荷分离,在1中,电子受体为1,4,5,8-萘二酰亚胺(ND1),电子给体是吩噻嗪(PTZ),且[(phen)Pt(-C = C-Ph-)](其中phen是1,10-菲咯啉)表示发色核。在1中观察到的第一个激发态是〜3MLCT7 LL'CT,具有{Pt(II)-acetylide} -phen的特征。随后,电荷从苯阴离子转移到NDI亚基上,形成NDr-phen- [Pt-(C = C)2]〜-PTZ2,其时间常数为2.3 ps。这种转变的特征是在TRIR和TA光谱中均显示出突出的NDI阴离子特征。 1中电荷分离的最后步骤以〜15 ps的时间常数进行,在此期间空穴从[Pt-(C = C)2]亚基迁移到PTZ组之一。然后在1中发生电荷重组,具有两个分别为36 ns和107 ns的不同时间常数,对应于向两个供体基团各自转移的反向电子。很少发生的现象表明,处于最终电荷分离状态的空穴位于两个施主PTZ组之一上。通过对先前报道的((COOEt)2bpy)Pt(C = C-Ph-CH2-PTZ)2(2),(JE McGarrah和R.Eisenberg,Inorg。Chem。,2003,42,4355; JE McGarrah,JT Hupp和SN Smirnov,J.Phys.Chem.A 2009,113,6430)以及(bpy)Pt(C C-Ph- C7H_(15))2,分别代表无受体的二元组和发色核。因此,已经建立了在皮秒时间尺度上逐步形成完全电荷分离状态和通过隧穿进行电荷复合的方法;并且已经观察到存在两种不同的电荷重组途径。

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