Department of Physics, Graduate School of Science, Osaka University, Osaka, 560-0043, Japan.
Hamamatsu Photonics K.K., Iwata, 438-0193, Japan.
J Mass Spectrom. 2021 Mar;56(3):e4706. doi: 10.1002/jms.4706.
Use of a two-stage microchannel plate (MCP) detector is common in time-of-flight (TOF) mass spectrometry because it shows excellent time resolution with sufficient gains. However, the gain drops significantly when the detector detects intense ion fluxes, such as matrix ions, by matrix-assisted laser desorption/ionization mass spectrometry. As a result, significant ion signals corresponding to analytes, such as proteins, are hidden, thereby hampering the mass spectral interpretation. However, details of this phenomenon have not previously been investigated using ions because of the lack of suitable measurement methods and apparatus. Thus, we herein report a novel method for controlling the TOF of two selected ions, as a function of time differences between each other using a multi-turn TOF mass spectrometer. This method involves the use of an isotope cluster of ions that fly in a figure-of-eight orbit and the extraction of an ion at a given lap number. A series of time differences (∆t) between two ions in a TOF spectrum can be generated using this method. We evaluated the time constants of gain recovery after high ion-flux detection for two sets of two-stage MCP detectors to obtain values of 1,600 and 180 μs for channel plate resistances of 500 and 71 MΩ, respectively. The obtained time constants from the gains determined at various values of ∆t were 0.48 and 0.38 fold (for 500 and 71 MΩ, respectively) of the values suggested from the channel plate resistance and capacitance.
使用两级微通道板(MCP)检测器在飞行时间(TOF)质谱中很常见,因为它具有出色的时间分辨率和足够的增益。然而,当检测器检测到高强度的离子通量(如基质离子)时,增益会显著下降,例如基质辅助激光解吸/电离质谱。结果,与分析物(如蛋白质)对应的显著离子信号被隐藏,从而阻碍了质谱解释。然而,由于缺乏合适的测量方法和仪器,以前没有使用离子研究过这种现象的细节。因此,我们在此报告了一种使用多圈 TOF 质谱仪根据彼此之间的时间差控制两个选定离子的 TOF 的新方法。该方法涉及使用在八字形轨道中飞行的离子同位素簇,并在给定圈数处提取离子。可以使用这种方法在 TOF 光谱中生成两个离子之间的一系列时间差(∆t)。我们评估了两种两级 MCP 检测器在高离子通量检测后的增益恢复时间常数,以获得通道板电阻分别为 500 和 71 MΩ时的 1600 和 180 μs 值。从在不同 ∆t 值下确定的增益获得的时间常数分别为通道板电阻和电容建议值的 0.48 和 0.38 倍(分别为 500 和 71 MΩ)。