Department of Physics and Astronomy, Aarhus University , Ny Munkegade 120, DK-8000 Aarhus C, Denmark.
Acc Chem Res. 2014 Apr 15;47(4):1417-25. doi: 10.1021/ar500025h. Epub 2014 Mar 27.
In a charge-transfer (CT) transition, electron density moves from one end of the molecule (donor) to the other end (acceptor). This type of transition is of paramount importance in nature, for example, in photosynthesis, and it governs the excitation of several protein biochromophores and luminophores such as the oxyluciferin anion that accounts for light emission from fireflies. Both transition energy and oscillator strength are linked to the coupling between the donor and acceptor groups: The weaker the coupling, the smaller the excitation energy. But a weak coupling necessarily also causes a low oscillator strength possibly preventing direct excitation (basically zero probability in the noncoupling case). The coupling is determined by the actual spacer between the two groups, and whether the spacer acts as an insulator or a conductor. However, it can be difficult or even impossible to distinguish the effect of the spacer from that of local solvent molecules that often cause large solvent shifts due to different ground-state and excited-state stabilization. This calls for gas-phase spectroscopy experiments where absorption by the isolated molecule is identified to unequivocally establish the intrinsic molecular properties with no perturbations from a microenvironment. From such insight, the effect of a protein microenvironment on the CT excited state can be deduced. In this Account, we review our results over the last 5 years from mass spectroscopy experiments using specially designed apparatus on several charged donor-acceptor ions that are based on the nitrophenolate moiety and π-extended derivatives, which are textbook examples of donor-acceptor chromophores. The phenolate oxygen is the donor, and the nitro group is the acceptor. The choice of this system is also based on the fact that phenolate is a common structural motif of biochromophores and luminophores, for example, it is a constituent of the oxyluciferin anion. A presentation of the setups used for gas-phase ion spectroscopy in Aarhus is given, and we address issues of whether double bonds or triple bonds best convey electronic coupling between the phenolate oxygen and the nitro group, the significance of separating the donor and acceptor spatially, the influence of cross-conjugation versus linear conjugation, and along this line ortho versus meta versus para configuration, and not least the effect of a single solvent molecule (water, methanol, or acetonitrile). From systematic studies, a clear picture has emerged that has been supported by high-level calculations of electronically excited states. Our work shows that CC2 coupled-cluster calculations of vertical excitation energies are within 0.2 eV of experimental band maxima, and importantly, that the theoretical method is excellent in predicting the relative order of excitation energies of a series of nitrophenolates. Finally, we discuss future challenges such as following the change in absorption as a function of the number of solvent molecules and when gradually approaching the bulk limit.
在电荷转移 (CT) 跃迁中,电子密度从分子的一端(供体)转移到另一端(受体)。这种类型的跃迁在自然界中至关重要,例如在光合作用中,它控制着几种蛋白质生色团和发光团的激发,例如氧荧光素阴离子,它负责萤火虫的发光。跃迁能量和振子强度都与供体和受体基团之间的耦合有关:耦合越弱,激发能越小。但是,弱耦合必然也会导致低振子强度,可能阻止直接激发(在非耦合情况下基本上为零概率)。耦合由两组之间的实际间隔决定,以及间隔物是作为绝缘体还是导体。然而,区分间隔物的影响与局部溶剂分子的影响可能会很困难,甚至不可能,因为溶剂的稳定化会导致不同的基态和激发态,从而导致大的溶剂位移。这需要进行气相光谱实验,在该实验中,通过孤立分子的吸收来确定固有分子性质,而不会受到微环境的干扰。由此可知,可以推断蛋白质微环境对 CT 激发态的影响。在本综述中,我们回顾了过去 5 年来在奥胡斯使用专门设计的装置进行质谱实验的结果,这些实验基于硝基酚盐部分和π 扩展衍生物的带电供体-受体离子,这些是供体-受体生色团的典型示例。酚盐氧是供体,硝基是受体。选择该系统的另一个原因是,酚盐是生物生色团和发光团的常见结构基序,例如,它是氧荧光素阴离子的组成部分。介绍了在奥胡斯使用的气相离子光谱学的设置,并讨论了双键或三键是否最好地传递了酚盐氧和硝基之间的电子耦合、空间分离供体和受体的重要性、交叉共轭与线性共轭的影响、沿此线邻位、间位和对位构型的影响,以及溶剂分子(水、甲醇或乙腈)的影响。通过系统研究,出现了一个清晰的画面,该画面得到了电子激发态的高级计算的支持。我们的工作表明,CC2 耦合簇计算的垂直激发能量与实验带最大值相差 0.2 eV,重要的是,该理论方法在预测一系列硝基酚盐的激发能的相对顺序方面非常出色。最后,我们讨论了未来的挑战,例如随着溶剂分子数量的变化以及逐渐接近体相极限时,吸收的变化。