Munkerup Kristin, Romanov Dmitri, Bohinski Timothy, Stephansen Anne B, Levis Robert J, Sølling Theis I
KAUST Catalysis Center, Division of Physical Science & Engineering, 4700-King Abdullah University of Science and Technology , 23955 Thuwal, Kingdom of Saudi Arabia.
Department of Chemistry, University of Copenhagen , Universitetsparken 5, 2100 Copenhagen Ø, Denmark.
J Phys Chem A. 2017 Nov 16;121(45):8642-8651. doi: 10.1021/acs.jpca.7b09185. Epub 2017 Nov 7.
Light harvesting via energy storage in azobenzene has been a key topic for decades and the process of energy distribution over the molecular degrees of freedom following photoexcitation remains to be understood. Dynamics of a photoexcited system can exhibit high degrees of nonergodicity when it is driven by just a few degrees of freedom. Typically, an internal conversion leads to the loss of such localization of dynamics as the intramolecular energy becomes statistically redistributed over all molecular degrees of freedom. Here, we present a unique case where the excitation energy remains localized even subsequent to internal conversion. Strong-field ionization is used to prepare cis- and trans-azobenzene radical cations on the D surface with little excess energy at the equilibrium neutral geometry. These D ions are preferably formed because in this case D and D switch place in the presence of the strong laser field. The postionization dynamics are dictated by the potential energy landscape. The D surface is steep downhill along the cis/trans isomerization coordinate and toward a common minimum shared by the two isomers in the region of D/D conical intersection. Coherent cis/trans torsional motion along this coordinate is manifested in the ion transients by a cosine modulation. In this scenario, D becomes populated with molecules that are energized mainly along the cis-trans isomerization coordinate, with the kinetic energy above the cis-trans interconversion barrier. These activated azobenzene molecules easily cycle back and forth along the D surface and give rise to several periods of modulated signal before coherence is lost. This persistent localization of the internal energy during internal conversion is provided by the steep downhill potential energy surface, small initial internal energy content, and a strong hole-lone pair interaction that drives the molecule along the cis-trans isomerization coordinate to facilitate the transition between the involved electronic states.
几十年来,通过偶氮苯中的能量存储进行光捕获一直是一个关键课题,而光激发后能量在分子自由度上的分布过程仍有待了解。当光激发系统仅由几个自由度驱动时,其动力学可以表现出高度的非遍历性。通常,随着分子内能量在所有分子自由度上进行统计重新分布,内转换会导致这种动力学局域化的丧失。在此,我们展示了一种独特的情况,即即使在发生内转换之后,激发能仍保持局域化。利用强场电离在平衡中性几何结构下以几乎没有多余能量的方式在D表面制备顺式和反式偶氮苯自由基阳离子。这些D离子之所以优先形成,是因为在这种情况下,D和D在强激光场存在时会发生位置互换。电离后的动力学由势能面决定。D表面沿着顺/反异构化坐标陡峭地下坡,并朝着D/D锥形交叉区域中两种异构体共有的一个共同最小值倾斜。沿着这个坐标的相干顺/反转角运动在离子瞬态中表现为余弦调制。在这种情况下,D态被主要沿着顺-反异构化坐标获得能量且动能高于顺-反互变势垒的分子所占据。这些被激活的偶氮苯分子很容易沿着D表面来回循环,并在失去相干性之前产生几个周期的调制信号。内转换过程中内能的这种持续局域化是由陡峭的下坡势能面、较小的初始内能含量以及一种强空穴-孤对相互作用提供的,这种相互作用驱使分子沿着顺-反异构化坐标运动,以促进相关电子态之间的跃迁。