Seto C, Grossert J S, Waddell D S, Curtis J M, Boyd R K
Department of Chemistry, Dalhousie University, Halifax, Nova Scotia, Canada.
J Am Soc Mass Spectrom. 2001 May;12(5):571-9. doi: 10.1016/S1044-0305(01)00220-3.
Comparison of collisionally activated fragment spectra of long-chain quaternary ammonium ions, formed by liquid-assisted secondary ion mass spectrometry (LSIMS) and electrospray ionization (ESI), shows the latter are dominated by radical cations while the former yield mainly even-electron charge-site-remote (CSR) fragments, similar to the report for different precursors by Cheng et al., J. Am. Soc. Mass Spectrom. 1998, 9, 840. Here, mixed-site fragmentation products (formal loss of a radical directly bonded to the nitrogen plus a radical derived from the long chain) are of comparable importance for both ionization techniques. These observations are difficult to understand if the CSR ions are formed by a concerted rearrangement-elimination reaction, since precollision internal energies of the ESI ions are much lower than those of the ions from LSIMS. Alternatively, if one discards the concerted mechanism for high-energy CA, and assumes that the even-electron fragments are predominantly formed via homolytic bond cleavage, the colder radical cations from ESI survive to the detector while the more energized counterparts from LSIMS preferentially lose a hydrogen atom to yield the CSR ions, as proposed by Wysocki and Ross (Int. J. Mass Spectrom. Ion Processes 1991, 104, 179). The present work also attempts to reconcile discrepancies involving critical energies and known structures for neutral fragments.
通过液相辅助二次离子质谱法(LSIMS)和电喷雾电离(ESI)形成的长链季铵离子的碰撞激活碎片光谱比较表明,后者以自由基阳离子为主,而前者主要产生偶电子电荷位点远程(CSR)碎片,这与Cheng等人在《美国质谱学会杂志》1998年第9卷第840页中对不同前体的报道相似。在这里,混合位点裂解产物(直接与氮键合的自由基加上长链衍生的自由基的形式损失)对于这两种电离技术具有相当的重要性。如果CSR离子是通过协同重排-消除反应形成的,这些观察结果就很难理解,因为ESI离子的碰撞前内能远低于LSIMS离子的内能。或者,如果放弃高能碰撞激活的协同机制,并假设偶电子碎片主要通过均裂键断裂形成,那么ESI中较冷的自由基阳离子能够存活到检测器,而LSIMS中能量较高的对应物则优先失去一个氢原子以产生CSR离子,正如Wysocki和Ross所提出的(《国际质谱和离子过程杂志》1991年第104卷第179页)。本工作还试图协调涉及中性碎片的临界能量和已知结构的差异。