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溶液中双核金属配合物的振动弛豫和系间窜越。

Vibrational relaxation and intersystem crossing of binuclear metal complexes in solution.

机构信息

Ecole Polytechnique Fédérale de Lausanne, Laboratory of Ultrafast Spectroscopy, ISIC, 1015 Lausanne, Switzerland.

出版信息

J Am Chem Soc. 2011 Jan 19;133(2):305-15. doi: 10.1021/ja106769w. Epub 2010 Dec 16.

Abstract

The ultrafast vibrational-electronic relaxation upon excitation into the singlet (1)A(2u) (dσ*→pσ) excited state of the d(8)-d(8) binuclear complex Pt(2)(P(2)O(5)H(2))(4) has been investigated in different solvents by femtosecond polychromatic fluorescence up-conversion and femtosecond broadband transient absorption (TA) spectroscopy. Both sets of data exhibit clear signatures of vibrational relaxation and wave packet oscillations of the Pt-Pt stretch vibration in the (1)A(2u) state with a period of 224 fs, that decay on a 1-2 ps time scale, and of intersystem crossing (ISC) into the (3)A(2u) state. The vibrational relaxation and ISC times exhibit a pronounced solvent dependence. We also extract from the TA measurements the spectral distribution of the wave packet at a given delay time, which reflects the distribution of Pt-Pt bond distances as a function of time, i.e., the structural dynamics of the system. We clearly establish the vibrational relaxation and coherence decay processes, and we demonstrate that PtPOP represents a clear example of a harmonic oscillator that does not comply with the optical Bloch description due to very efficient coherence transfer between vibronic levels. We conclude that a direct Pt-solvent energy dissipation channel accounts for the vibrational cooling in the singlet state. ISC from the (1)A(2u) to the (3)A(2u) state is induced by spin-vibronic coupling with a higher-lying triplet state and/or (transient) symmetry breaking in the (1)A(2u) excited state. The particular structure, energetics, and symmetry of the molecule play a decisive role in determining the relatively slow rate of ISC, despite the large spin-orbit coupling strength of the Pt atoms.

摘要

激发到 d(8)-d(8)双核配合物Pt(2)(P(2)O(5)H(2))(4)的单重态(1)A(2u)(dσ*→pσ)激发态后,超快振动电子弛豫已在不同溶剂中通过飞秒多色荧光上转换和飞秒宽带瞬态吸收(TA)光谱进行了研究。两组数据均显示出(1)A(2u)态中 Pt-Pt 伸缩振动的振动弛豫和波包振荡的清晰特征,其周期为 224 fs,在 1-2 ps 时间尺度上衰减,并发生系间穿越(ISC)到(3)A(2u)态。振动弛豫和 ISC 时间表现出明显的溶剂依赖性。我们还从 TA 测量中提取出给定延迟时间处波包的光谱分布,该分布反映了 Pt-Pt 键距随时间的分布,即系统的结构动力学。我们清楚地确定了振动弛豫和相干衰减过程,并证明 PtPOP 代表了一个明显的非谐振荡器的例子,由于振动态之间的相干转移非常有效,它不符合光学 Bloch 描述。我们得出结论,一个直接的 Pt-溶剂能量耗散通道解释了单重态中的振动冷却。从(1)A(2u)到(3)A(2u)态的 ISC 是由自旋-振动态耦合引起的,其中涉及更高的三重态和/或(瞬态)在(1)A(2u)激发态中对称破缺。尽管 Pt 原子的自旋轨道耦合强度很大,但分子的特殊结构、能量和对称性在决定相对较慢的 ISC 速率方面起着决定性的作用。

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