Department of Chemistry and Biochemistry, Brigham Young University, Provo, Utah 84602-1030, United States.
J Am Soc Mass Spectrom. 2022 Jan 5;33(1):131-140. doi: 10.1021/jasms.1c00297. Epub 2021 Dec 20.
Determination of collision cross sections (CCS) using the cross-sectional areas by the Fourier transform ion cyclotron resonance (CRAFTI) technique is limited by the requirement that accurate pressures in the trapping cell of the mass spectrometer must be known. Experiments must also be performed in the energetic hard-sphere regime such that ions decohere after single collisions with neutrals; this limits application to ions that are not much more massive than the neutrals. To mitigate these problems, we have resonantly excited two (or more) ions of different / to the same center-of-mass kinetic energy in a single experiment, subjecting them to identical neutral pressures. We term this approach "multi-CRAFTI". This facilitates measurement of relative CCS without requiring knowledge of the pressure and enables determination of absolute CCS using internal standards. Experiments with tetraalkylammonium ions yield CCS in reasonable agreement with the one-ion-at-a-time CRAFTI approach and with ion mobility spectrometry (IMS) when differences in collision energetics are taken into account (multi-CRAFTI generally yields smaller CCS than does IMS due to the higher collision energies employed in multi-CRAFTI). Comparison of multi-CRAFTI and IMS results with CCS calculated from structures computed at the M06-2X/6-31+G* level of theory using projection approximation or trajectory method values, respectively, indicates that the computed structures have CCS increasingly smaller than the experimental CCS as / increases, implying the computational model overestimates interactions between the alkyl arms. For ions that undergo similar collisional decoherence processes, relative CCS reach constant values at lower collision energies than do absolute CCS values, suggesting a means of increasing the accessible upper / limit by employing multi-CRAFTI.
使用傅里叶变换离子回旋共振(CRAFTI)技术的截面面积来确定碰撞截面(CCS)受到质谱仪捕集池内准确压力必须已知的要求限制。实验还必须在硬球能区进行,使得离子在与中性碰撞后解相干;这限制了应用于比中性物质质量大不了多少的离子。为了解决这些问题,我们在单次实验中使不同/相同质心动能的两个(或更多)离子共振激发,使它们处于相同的中性压力下。我们将这种方法称为“多 CRAFTI”。这有助于在不要求压力知识的情况下测量相对 CCS,并使用内标法确定绝对 CCS。用四烷基铵离子进行的实验得出的 CCS 与一次一个离子的 CRAFTI 方法以及与离子迁移谱(IMS)一致,当考虑到碰撞能量的差异时(由于在多 CRAFTI 中采用了更高的碰撞能量,多 CRAFTI 通常会产生比 IMS 更小的 CCS)。多 CRAFTI 和 IMS 结果与从使用投影逼近或轨迹方法值分别在 M06-2X/6-31+G*理论水平上计算的结构计算得出的 CCS 的比较表明,计算出的结构的 CCS 随着/的增加而逐渐小于实验 CCS,这意味着计算模型高估了烷基臂之间的相互作用。对于经历相似碰撞解相干过程的离子,相对 CCS 在比绝对 CCS 值更低的碰撞能下达到恒定值,这表明采用多 CRAFTI 可以增加可访问的上限/限制。