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第6族金属羰基中心向配体丢失和配体螯合的激发态演化。

Excited state evolution towards ligand loss and ligand chelation at group 6 metal carbonyl centres.

作者信息

Manton Jennifer C, Amirjalayer Saeed, Coleman Anthony C, McMahon Suzanne, Harvey Emma C, Greetham Gregory M, Clark Ian P, Buma Wybren Jan, Woutersen Sander, Pryce Mary T, Long Conor

机构信息

School of Chemical Sciences, Dublin City University, Dublin 9, Ireland.

出版信息

Dalton Trans. 2014 Dec 21;43(47):17797-805. doi: 10.1039/c4dt01544d.

Abstract

The photochemistry and photophysics of three model "half-sandwich" complexes (η(6)-benzophenone)Cr(CO)3, (η(6)-styrene)Cr(CO)3, and (η(6)-allylbenzene)Cr(CO)3 were investigated using pico-second time-resolved infrared spectroscopy and time-dependent density functional theory methods. The (η(6)-benzophenone)Cr(CO)3 complex was studied using two excitation wavelengths (470 and 320 nm) while the remaining complexes were irradiated using 400 nm light. Two independent excited states were detected spectroscopically for each complex, one an unreactive excited state of metal-to-arene charge-transfer character and the other with metal-to-carbonyl charge transfer character. This second excited state leads to an arrested release of CO on the pico-second time-scale. Low-energy excitation (470 nm) of (η(6)-benzophenone)Cr(CO)3 populated only the unreactive excited state which simply relaxes to the parent complex. Higher energy irradiation (320 nm) induced CO-loss. Irradiation of (η(6)-styrene)Cr(CO)3, or (η(6)-allylbenzene)Cr(CO)3 at 400 nm provided evidence for the simultaneous population of both the reactive and unreactive excited states. The efficiency at which the unreactive excited state is populated depends on the degree of conjugation of the substituent with the arene π-system and this affects the efficiency of the CO-loss process. The quantum yield of CO-loss is 0.50 for (η(6)-allylbenzene)Cr(CO)3 and 0.43 for (η(6)-styrene)Cr(CO)3. These studies provide evidence for the existence of two photophysical routes to CO loss, a minor ultrafast route and an arrested mechanism involving the intermediate population of a reactive excited state. This reactive excited state either relaxes to reform the parent species or eject CO. Thus the quantum yield of the CO-loss is strongly dependent on the excitation wavelength. Time-dependent density functional theory calculations confirm that the state responsible for ultrafast CO-loss has significant metal-centred character while the reactive state responsible for the arrested CO-loss has significant metal-to-carbonyl charge-transfer character. The CO-loss product (η(6)-allylbenzene)Cr(CO)2 formed following irradiation of (η(6)-allylbenzene)Cr(CO)3 reacts further with the pendent alkenyl group to form the chelate product (η(6),η(2)-allylbenzene)Cr(CO)2.

摘要

利用皮秒时间分辨红外光谱和含时密度泛函理论方法,研究了三种模型“半夹心”配合物(η(6)-二苯甲酮)Cr(CO)3、(η(6)-苯乙烯)Cr(CO)3和(η(6)-烯丙基苯)Cr(CO)3的光化学和光物理性质。对(η(6)-二苯甲酮)Cr(CO)3配合物使用两个激发波长(470和320 nm)进行研究,而其余配合物则用400 nm光照射。通过光谱检测到每种配合物有两个独立的激发态,一个是具有金属到芳烃电荷转移特征的非反应性激发态,另一个具有金属到羰基电荷转移特征。第二个激发态导致在皮秒时间尺度上CO的释放受阻。(η(6)-二苯甲酮)Cr(CO)3的低能量激发(470 nm)仅产生非反应性激发态,该激发态简单地弛豫回母体配合物。较高能量的照射(320 nm)诱导CO损失。在400 nm照射(η(6)-苯乙烯)Cr(CO)3或(η(6)-烯丙基苯)Cr(CO)3,为同时产生反应性和非反应性激发态提供了证据。非反应性激发态的产生效率取决于取代基与芳烃π体系的共轭程度,这影响了CO损失过程的效率。(η(6)-烯丙基苯)Cr(CO)3的CO损失量子产率为0.50,(η(6)-苯乙烯)Cr(CO)3的为0.43。这些研究为CO损失存在两条光物理途径提供了证据,一条是次要的超快途径,另一条是涉及反应性激发态中间态的受阻机制。这个反应性激发态要么弛豫以重新形成母体物种,要么排出CO。因此,CO损失的量子产率强烈依赖于激发波长。含时密度泛函理论计算证实,负责超快CO损失的态具有显著的以金属为中心的特征,而负责受阻CO损失的反应态具有显著的金属到羰基电荷转移特征。(η(6)-烯丙基苯)Cr(CO)3照射后形成的CO损失产物(η(6)-烯丙基苯)Cr(CO)2与侧链烯基进一步反应,形成螯合产物(η(6),η(2)-烯丙基苯)Cr(CO)2。

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