Kaiser Nathan K, Weisbrod Chad R, Webb Brian N, Bruce James E
Department of Chemistry, Washington State University, Pullman, WA 99164-4630, USA.
J Am Soc Mass Spectrom. 2008 Apr;19(4):467-78. doi: 10.1016/j.jasms.2007.12.009. Epub 2008 Jan 6.
With Fourier transform ion cyclotron resonance (FTICR) mass spectrometry one determines the mass-to-charge ratio of an ion by measuring its cyclotron frequency. However, the need to confine ions to the trapping region of the ion cyclotron resonance (ICR) cell with electric fields induces deviations from the unperturbed cyclotron frequency. Additional perturbations to the observed cyclotron frequency are often attributed to changes in space charge conditions. This study presents a detailed investigation of the observed ion cyclotron frequency as a function of ion z-axis kinetic energy. In a perfect three-dimensional quadrupolar field, cyclotron frequency is independent of position within the trap. However, in most ICR cell designs, this ideality is approximated only near the trap center and deviations arise from this ideal quadrupolar field as the ion moves both radially and axially from the center of the trap. To allow differentiation between deviations in observed cyclotron frequency caused from changes in space charge conditions or differences in oscillation amplitude, ions with identical molecular weights but different axial kinetic energy, and thus amplitude of z-axis motion, were simultaneously trapped within the ICR cell. This allows one to attribute deviations in observed cyclotron frequency to differences in the average force from the radial electric field experienced by ions of different axial amplitude. Experimentally derived magnetron frequency is compared with the magnetron frequency calculated using SIMION 7.0 for ions of different axial amplitude. Electron promoted ion coherence, or EPIC, is used to reduce the differences in radial electric fields at different axial positions. Thus with the application of EPIC, the differences in observed cyclotron frequencies are minimized for ions of different axial oscillation amplitudes.
利用傅里叶变换离子回旋共振(FTICR)质谱仪,通过测量离子的回旋频率来确定其质荷比。然而,需要利用电场将离子限制在离子回旋共振(ICR)池的捕获区域内,这会导致与未受扰动的回旋频率产生偏差。观察到的回旋频率的额外扰动通常归因于空间电荷条件的变化。本研究详细考察了观察到的离子回旋频率作为离子z轴动能的函数。在完美的三维四极场中,回旋频率与阱内位置无关。然而,在大多数ICR池设计中,只有在阱中心附近才能近似达到这种理想状态,随着离子从阱中心径向和轴向移动,会偏离这种理想的四极场。为了区分由空间电荷条件变化或振荡幅度差异引起的观察到的回旋频率偏差,将具有相同分子量但轴向动能不同,从而z轴运动幅度不同的离子同时捕获在ICR池内。这使得人们能够将观察到的回旋频率偏差归因于不同轴向幅度的离子所经历的径向电场平均力的差异。将实验得出的磁控管频率与使用SIMION 7.0计算的不同轴向幅度离子的磁控管频率进行比较。电子促进离子相干(EPIC)用于减少不同轴向位置处的径向电场差异。因此,通过应用EPIC,不同轴向振荡幅度的离子观察到的回旋频率差异被最小化。