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    • 41. 发明授权
    • Gridless ion mirrors with smooth fields
    • US11367608B2
    • 2022-06-21
    • US17049175
    • 2019-04-23
    • Micromass UK Limited
    • Anatoly Verenchikov
    • H01J49/40
    • An ion mirror 41 constructed of thin electrodes that are interconnected by resistive dividers 45 with potentials U1-U5 applied to knot electrodes to form segments 41-43 of linear potential distribution between the “knot” electrodes, yet without separating those field regions by meshes. Weak and controlled penetration of electric fields provide for a fine control over the field non linearity and over the equipotential line curvature, thus allowing to reach unprecedented level of ion optical quality: more than twice larger energy acceptance compared to thick electrode mirrors, up to sixth order time per energy focusing, ion spatial focusing and wide spatial acceptance. Novel mirrors can be formed very slim to arrange them into stacks for ion transverse displacement between ion reflections or for multiplexed mirror stacks. Printed circuit boards (PCB) are best suited for making novel ion mirrors, while novel ion mirrors are designed to suit PCB requirements.
    • 50. 发明授权
    • Mass spectrometer
    • US11239069B2
    • 2022-02-01
    • US17053128
    • 2018-05-31
    • SHIMADZU CORPORATION
    • Kazuma MaedaDaisuke Okumura
    • H01J49/42H01J49/02H01J49/06H01J49/40
    • When a Q-TOF type mass spectrometer is operated in an MS1 mode, a controller (40), at the time of measurement, controls voltage generators (31 to 33) such that only a V voltage (radio-frequency voltage for mass separation) and a direct-current bias voltage are applied to main rod electrodes of a quadrupole mass filter (12) without application of a U voltage (direct-current voltage for mass separation). During a measurement preparation period between a plurality of measurements to obtain one mass spectrum, the controller (40) controls a U voltage generator (31) so as to apply the U voltage to the main rod electrodes of the quadrupole mass filter (12). Accordingly, a direct-current electric field is formed between adjacent main rod electrodes around an ion optical axis (C) due to a potential difference, and electric charges accumulated in rod holders (122) holding the main rod electrodes are rapidly removed by an effect of this electric field. As a result, it is possible to eliminate a charge-up that has not been eliminated by a conventional method in which a polarity of a direct-current bias voltage applied to the rod electrodes is merely reversed.