Department of Chemistry, Graduate School of Science, Osaka Prefecture University, 1-1, Gakuencho, Nakaku, Sakai, Osaka 599-8531, Japan.
J Chem Phys. 2012 Nov 14;137(18):184308. doi: 10.1063/1.4765103.
High-energy electron transfer dissociation (HE-ETD) on collisions with alkali metal targets (Cs, K, and Na) was investigated for CH(3)X(+) (X = Cl, Br, and I) ions by a charge inversion mass spectrometry. Relative peak intensities of the negative ions formed via HE-ETD strongly depend on the precursor ions and the target alkali metals. The dependency is explained by the exothermicities of the respective dissociation processes. Peak shapes of the negative ions, especially of the X(-) ions, which comprise a triangle and a trapezoid, also strongly depend on the precursor ions and the target alkali metals. The trapezoidal part of the I(-) peak observed with the Na target is more dominant and much broader than that with the Cs target. This dependence on the targets shows an inverse relation between the peak width and the available energy, which corresponds to the exothermicity assuming formation of fragment pair in their ground internal states. From a comparison of the kinetic energy release value calculated from the trapezoidal shape of I(-) with the available energy of the near-resonant level on the CH(3)I potential energy curve reported by ab initio calculations, the trapezoidal part is attributed to the dissociation to CH(3) + I((2)P(3/2)) via the repulsive (3)Q(1) state of CH(3)I, which is not dominant in the photo-dissociation of CH(3)I. The observation of trapezoid shape of the CH(2)I(-) peak with the Cs target indicates spontaneous dissociation via repulsive potential from the (3)R(2) Rydberg state, although the correlation between the (3)R(2) Rydberg state and relevant repulsive states has not been reported by any theoretical calculation.
通过电荷反转质谱法研究了与碱金属靶(Cs、K 和 Na)碰撞时 CH(3)X(+)(X = Cl、Br 和 I)离子的高能电子转移解离(HE-ETD)。通过 HE-ETD 形成的负离子的相对峰强度强烈依赖于前体离子和靶碱金属。这种依赖性可以通过各自的解离过程的放热性来解释。负离子的峰形,特别是 X(-)离子的峰形,包括一个三角形和一个梯形,也强烈依赖于前体离子和靶碱金属。用 Na 靶观察到的 I(-)峰的梯形部分比用 Cs 靶观察到的更占主导地位且更宽。这种对靶的依赖性表明峰宽与可用能量之间存在反比关系,这与假定在其基态内部态形成碎片对的放热性相对应。通过将从 I(-)的梯形形状计算出的动能释放值与从头算计算报告的 CH(3)I 势能曲线上的近共振能级的可用能量进行比较,梯形部分归因于通过 CH(3)I 的排斥(3)Q(1)态解离为 CH(3) + I((2)P(3/2)),这在 CH(3)I 的光解中不是主要的。用 Cs 靶观察到 CH(2)I(-)峰的梯形形状表明,尽管尚未通过任何理论计算报告(3)R(2) Rydberg 态与相关排斥态之间的相关性,但通过排斥势从(3)R(2) Rydberg 态自发解离。