Driver Joshua A, Nagornov Konstantin O, Kozhinov Anton N, Tsybin Yury O, Kharchenko Andriy, Amster I Jonathan
Department of Chemistry, University of Georgia, Athens, GA, 30602, USA.
Spectroswiss Sàrl, EPFL Innovation Park, 1015, Lausanne, Switzerland.
J Am Soc Mass Spectrom. 2018 Jan;29(1):51-62. doi: 10.1007/s13361-017-1817-6. Epub 2017 Oct 16.
The current paradigm in FT-ICR cell design is to approximate the ideal three-dimensional quadratic trapping potential as closely as possible to maintain ion cloud spatial coherence and achieve long transients, either with hyperbolically shaped electrodes, shimming electrodes, or by dynamic harmonization. In sharp contrast, the FT-ICR analyzer cell with four narrow aperture detection electrodes (NADEL) introduces significant anharmonic terms to the trapping potential. This analyzer cell is capable of quadrupolar detection by which one can measure a signal that is close to the unperturbed cyclotron frequency. This is far less sensitive to trapping potential and space charge shifts than the reduced cyclotron frequency measured in conventional ICR cells. The quadrupolar mode of ion detection in NADEL cells has been examined previously by SIMION simulations of ion clouds with up to 500 ions per simulation. Here, the behavior of the NADEL analyzer cell is examined through particle-in-cell (PIC) simulations, which allows us to examine the behavior of large populations (tens of thousands) of ions with space charge considerations, and to calculate the induced charge on the NADEL detection electrodes, and thus the transient signal. PIC simulations confirm a unique spatial distribution of the ions, with a coherent motion that results in long transient signals. Dependence of the ion cloud and image current signal on cell design, ion energy, and magnetron radius are examined. Coalescence effects are compared with those found in a dynamically harmonized cell. The insensitivity of the measured cyclotron frequency to space-charge is demonstrated both with simulations and experimentally. Graphical Abstract ᅟ.
傅里叶变换离子回旋共振(FT-ICR)池设计的当前范式是尽可能接近理想的三维二次俘获势,以保持离子云的空间相干性并实现长瞬态,这可以通过双曲线形电极、匀场电极或动态谐调来实现。与之形成鲜明对比的是,具有四个窄孔径检测电极(NADEL)的FT-ICR分析仪池会在俘获势中引入显著的非谐项。这种分析仪池能够进行四极检测,通过该检测可以测量接近未受干扰的回旋频率的信号。与传统ICR池中测量的降低的回旋频率相比,这对俘获势和空间电荷偏移的敏感度要低得多。此前已通过SIMION对每次模拟最多包含500个离子的离子云进行模拟,研究了NADEL池中离子检测的四极模式。在此,通过粒子模拟(PIC)研究了NADEL分析仪池的行为,这使我们能够在考虑空间电荷的情况下研究大量(数万)离子的行为,并计算NADEL检测电极上的感应电荷,进而计算瞬态信号。PIC模拟证实了离子独特的空间分布,其相干运动会产生长瞬态信号。研究了离子云与镜像电流信号对池设计、离子能量和磁控管半径的依赖性。将合并效应与在动态谐调池中发现的效应进行了比较。通过模拟和实验都证明了测量的回旋频率对空间电荷不敏感。图形摘要ᅟ。