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    • 3. 发明授权
    • Constraining arcuate divergence in an ion mirror mass analyser
    • 在离子镜质量分析仪中限制弓形散度
    • US09564307B2
    • 2017-02-07
    • US14945305
    • 2015-11-18
    • Thermo Fisher Scientific (Bremen) GmbH
    • Alexander A. Makarov
    • H01J49/40H01J49/42
    • H01J49/405H01J49/4245H01J49/425H01J49/427
    • A charged particle analyzer apparatus comprising two opposing ion mirrors each mirror comprising inner and outer field-defining electrode systems elongated along an axis z, the outer system surrounding the inner, whereby when the electrode systems are electrically biased the mirrors create an electrical field comprising opposing electrical fields along z; and at least one arcuate focusing lens for constraining the arcuate divergence of a beam of charged particles within the analyzer while the beam orbits around the axis z, the analyzer further comprising a disc having two faces at least partly spanning the space between the inner and outer field defining electrode systems and lying in a plane perpendicular to the axis z, the disc having resistive coating upon both faces. A mass spectrometer system comprising a plurality of the charged particle analyzers arranged as a parallel array.
    • 一种带电粒子分析仪装置,包括两个相对的离子镜,每个反射镜包括沿着轴线z延伸的内部和外部场限定电极系统,外部系统围绕内部,由此当电极系统被电偏置时,反射镜产生电场,包括相对 z电场; 以及至少一个弧形聚焦透镜,用于约束分束器内的带电粒子束的弓形发散,同时光束围绕轴线z运动,分析器还包括具有至少部分跨越内外两者之间的空间的两个面的圆盘 场定义电极系统并且位于垂直于轴线z的平面中,该盘在两个面上具有电阻涂层。 一种质谱仪系统,包括多个被布置成平行阵列的带电粒子分析器。
    • 6. 发明授权
    • Constraining arcuate divergence in an ion mirror mass analyser
    • US09196469B2
    • 2015-11-24
    • US13989697
    • 2011-11-24
    • Alexander A. Makarov
    • Alexander A. Makarov
    • H01J49/34H01J49/40H01J49/42
    • H01J49/405H01J49/4245H01J49/425H01J49/427
    • A method of selecting ions of interest from a beam of ions using an analyzer, the method comprising: (i) providing an analyzer comprising two opposing ion mirrors each mirror comprising inner and outer field-defining electrode systems elongated along an analyzer axis z, each system comprising one or more electrodes, the outer system surrounding the inner; (ii) causing the beam of ions to fly through the analyzer along a main flight path in the presence of an analyzer field so as to undergo within the analyzer at least one full oscillation in the direction of the analyzer axis while orbiting about or oscillating between one or more electrodes of the inner field defining electrode system; (iii) providing one or more sets of electrodes adjacent the main flight path; (iv) constraining the arcuate divergence from the main flight path of ions of interest by applying one set of voltages to one or more of the sets of electrodes adjacent the main flight path when the ions of interest are in the vicinity of at least one of said one or more sets of electrodes adjacent the main flight path and applying one or more different sets of voltages to the said one or more sets of electrodes adjacent the main flight path when the ions of interest are not in the vicinity of at least one of said one or more sets of electrodes adjacent the main flight path; and: (v) ejecting the ions of interest from the analyzer. Also provided is a charged particle analyzer comprising the two opposing ion mirrors comprising inner and outer field-defining electrode systems elongated along an analyzer axis z; and at least one arcuate focusing lens for constraining the arcuate divergence of a beam of charged particles within the analyzer while the beam orbits around the axis z, the analyzer further comprising a disc having two faces at least partly spanning the space between the inner and outer field defining electrode systems and lying in a plane perpendicular to the axis z, the disc having resistive coating upon both faces.
    • 8. 发明申请
    • TIME-OF-FLIGHT MASS SPECTROMETER
    • 飞行时间质谱仪
    • US20150270115A1
    • 2015-09-24
    • US14434596
    • 2013-09-18
    • Shimadzu Corporation
    • Osamu Furuhashi
    • H01J49/40
    • H01J49/405
    • In an ion reflector (4) configured from a plurality of electrodes, electrodes 42 disposed in a second stage region (S2) for reflecting ions after deceleration are formed thinner than electrodes (41) disposed in a first stage region (S1) for decelerating the ions.The thin electrodes suppress unevenness of potential, in particular, in a path away from the center axis of the reflector, which results in improvement of isochronism of an ion packet passing on the path. The thick electrodes (41, 43) disposed in the first stage region (S1) prevents stretching of the grid electrodes (G1, G2) from being affected, and unevenness of potential in the first stage region (S1) hardly affects isochronism of the ions. By appropriately adjusting thicknesses and a pitch of the electrodes (41, 42, 43, 44) adjacent to one another so as to align intervals between the electrodes (41, 42, 43, 44), it is possible to use spacers having the same size in common. Since the number of electrodes in the first stage region (S1) can be reduced, an increase in costs is suppressed. Consequently, it is possible to bring an electric field of an ion reflection region closer to an ideal state and improve mass-resolving power while suppressing costs.
    • 在由多个电极构成的离子反射体(4)中,比设置在第一阶段区域(S1)中的电极(41)更薄地设置在第二阶段区域(S2)中用于反射减速后的离子的电极42, 离子。 薄电极抑制电位的不均匀性,特别是在远离反射器的中心轴的路径中,这导致通过路径的离子包的等时性的改善。 设置在第一级区域(S1)中的厚电极(41,43)防止栅电极(G1,G2)的拉伸受到影响,第一级区域(S1)的电位不均匀性几乎不影响离子的等时性 。 通过适当地调整彼此相邻的电极(41,42,43,44)的厚度和间距以便对准电极(41,42,43,44)之间的间隔,可以使用具有相同的间隔物 大小相同 由于可以减少第一级区域(S1)中的电极的数量,因此抑制了成本的增加。 因此,可以使离子反射区域的电场更接近理想状态,并且能够在抑制成本的同时提高质量分辨能力。