Department of Chemistry, University of California, Berkeley, California 94720, United States.
Chemical Sciences Division, Lawrence Berkeley National Laboratory, Berkeley, California 94720, United States.
J Am Chem Soc. 2023 Feb 15;145(6):3554-3560. doi: 10.1021/jacs.2c12334. Epub 2023 Feb 3.
Tabletop X-ray spectroscopy measurements at the carbon -edge complemented by calculations are used to investigate the influence of the bromine atom on the carbon core-valence transitions in the bromobenzene cation (BrBz). The electronic ground state of the cation is prepared by resonance-enhanced two-photon ionization of neutral bromobenzene (BrBz) and probed by X-rays produced by high-harmonic generation (HHG). Replacing one of the hydrogen atoms in benzene with a bromine atom shifts the transition from the 1s orbital of the carbon atom (C*) bonded to bromine by ∼1 eV to higher energy in the X-ray spectrum compared to the other carbon atoms (C). Moreover, in BrBz, the X-ray spectrum is dominated by two relatively intense transitions, 1s→π* and 1s→σ*(C*-Br), where the second transition is enhanced relative to the neutral BrBz. In addition, a doublet peak shape for these two transitions is observed in the experiment. The 1s→π* doublet peak shape arises due to the spin coupling of the unpaired electron in the partially vacant π orbital (from ionization) with the two other unpaired electrons resulting from the transition from the 1s core orbital to the fully vacant π* orbitals. The 1s→σ* doublet peak shape results from several transitions involving σ* and vibrational C*-Br mode activations following the UV ionization, which demonstrates the impact of the C*-Br bond length on the core-valence transition as well as on the relaxation geometry of BrBz.
采用桌面 X 射线能谱测量,并结合计算,研究了溴原子对溴苯阳离子(BrBz)中碳芯价跃迁的影响。阳离子的电子基态通过中性溴苯(BrBz)的共振增强双光子电离来制备,并通过高次谐波产生(HHG)产生的 X 射线来探测。与其他碳原子(C)相比,在苯中用一个溴原子取代一个氢原子,会将与溴键合的碳原子(C*)的 1s 轨道的跃迁从 X 射线光谱中移动到更高的能量,约为 1 eV。此外,在 BrBz 中,X 射线光谱主要由两个相对较强的跃迁主导,即 1s→π和 1s→σ(C*-Br),其中第二个跃迁相对于中性 BrBz 增强。此外,在实验中观察到这两个跃迁的双峰峰形。1s→π双峰峰形是由于未配对电子在部分空的π轨道(来自电离)与来自 1s 芯轨道到完全空的π轨道的跃迁的另外两个未配对电子之间的自旋耦合引起的。1s→σ双峰峰形是由于 UV 电离后涉及σ和振动 C*-Br 模式激活的几个跃迁引起的,这表明了 C*-Br 键长对芯价跃迁以及 BrBz 的弛豫几何的影响。