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    • 8. 发明授权
    • Method for operating a time-of-flight mass spectrometer with orthogonal ion pulsing
    • 用正交离子脉冲操作飞行时间质谱仪的方法
    • US08927928B2
    • 2015-01-06
    • US13465669
    • 2012-05-07
    • Petra DeckerOliver Räther
    • Petra DeckerOliver Räther
    • H01J49/40H01J49/00
    • H01J49/0031H01J49/401
    • Methods are provided for acquiring sum spectra in a time-of-flight mass spectrometer with orthogonal pulsed acceleration, where each of the sum spectra is obtained from a plurality of summed individual spectra. The mass spectrometer has an ion storage device that collects the ions temporarily before they are transferred to an ion pulser, which pulses out the ions orthogonally. Acquisition conditions such as, for example, delay times between opening the ion storage device and the pulsed ejection in the ion pulser are varied for the individual spectra, which are added together to form the sum spectrum of ions with light masses and high masses.
    • 提供了用于在具有正交脉冲加速度的飞行时间质谱仪中获取总和光谱的方法,其中每个和光谱从多个相加的单个光谱获得。 质谱仪具有离子存储装置,其在离子脉冲发生器转移到离子脉冲发生器之前临时收集离子,从而正交地离子出离子。 对于各个光谱而言,采集条件例如打开离子存储装置之间的延迟时间和在离子脉冲发生器中的脉冲喷射之间是变化的,这些光谱被加在一起以形成具有光质量和高质量的离子的和光谱。
    • 9. 发明授权
    • Acquisition technique for MALDI time-of-flight mass spectra
    • MALDI飞行时间质谱的采集技术
    • US08912485B2
    • 2014-12-16
    • US13103672
    • 2011-05-09
    • Thomas MaierJochen Franzen
    • Thomas MaierJochen Franzen
    • H01J49/00H01J49/16H01J49/40
    • H01J49/0027H01J49/164H01J49/40
    • The invention relates to acquisition techniques for time-of-flight mass spectra with ionization of the analyte substances by matrix assisted laser desorption. Generally speaking, these acquisition techniques involve adding together a large number of individual time-of-flight spectra, each with restricted dynamic measuring range, to form a sum spectrum. The invention provides a method that improves, in particular, the reproducibility, the concentration accuracy and therefore the ability to quantify the mass spectra. Particular embodiments also increase the dynamic range of measurement. For this purpose, multiple series of mass spectra are acquired, whereby the energy density in the laser spot is increased in discrete steps. As a result, many ion signals saturate the detector and can therefore no longer be evaluated. However, it is possible to employ a technique in which the ion beam is increasingly defocused, or, secondly, to replace parts of the spectrum that are subject to saturation by intensity extrapolations from mass spectra acquired with lower energy density. In the first case, hundreds or thousands of individual mass spectra must be added together in order to increase the dynamic measuring range. In the second case, the finally acquired mass spectrum, with its replacements, forms a mass spectrum with a high dynamic measuring range, improved reproducibility and better concentration accuracy. The gradient of the increasing intensities of the ion signals, as a function of the energy density, supplies additional information about the proton affinity of the analyte ions. The concentration accuracy is enhanced because the increase in the number of proton donors in the ionization plasma leads to an increase in the ionization of those analyte substances that have a lower proton affinity.
    • 本发明涉及通过基质辅助激光解吸附物质分析物质离子化的飞行时间质谱采集技术。 一般来说,这些采集技术包括将大量具有限制动态测量范围的单个飞行时间频谱相加在一起以形成和频谱。 本发明提供了一种特别提高重现性,浓度精度以及因此量化质谱的能力的方法。 具体实施例还增加了测量的动态范围。 为此,获得了多个质谱系列,从而在离散步骤中激光斑点的能量密度增加。 因此,许多离子信号使检测器饱和,因此不再能被评估。 然而,可以采用这样一种技术,其中离子束越来越散焦,或者其次,通过由具有较低能量密度获得的质谱的强度外推替代经受饱和的部分光谱。 在第一种情况下,为了增加动态测量范围,必须将数百或数千个单个质谱加在一起。 在第二种情况下,最终获得的质谱与其替代物形成具有高动态测量范围,改进的再现性和更好的浓度精度的质谱。 作为能量密度的函数的离子信号的增加强度的梯度提供关于分析物离子的质子亲和力的附加信息。 由于离子化等离子体中的质子供体的数量的增加导致具有较低质子亲和力的分析物质的电离增加,所以浓度精度得到提高。
    • 10. 发明授权
    • Introduction of ions into electrostatic ion traps
    • 将离子引入静电离子阱
    • US08907271B2
    • 2014-12-09
    • US13559006
    • 2012-07-26
    • Claus Köster
    • Claus Köster
    • H01J49/26H01J49/42
    • H01J49/4245G01P3/48G05B9/03H01J49/26H01J49/42
    • Ions are introduced into a Kingdon ion trap in which the ions can oscillate harmonically in a potential well in the longitudinal direction, essentially decoupled from their transverse motion by a Kingdon ion guide, which can consist of a drill-hole through the wall of the ion trap housing electrodes and a central wire. An injection potential is first applied to the wire, but once the heaviest ions of interest have been injected into the trap, the potential of the wire is switched to the potential of the housing electrodes, to trap the ions in the trap. The ions introduced into the Kingdon ion trap may come from a small ion cloud, located in a Paul trap.
    • 离子被引入到Kingdon离子阱中,其中离子可以在纵向方向上在势阱中谐波地振荡,基本上通过Kingdon离子导向器与它们的横向运动分离,Kingdon离子引导件可以由穿过离子壁的钻孔组成 陷阱壳电极和中心线。 首先将注入电位施加到导线上,但是一旦将最重的感兴趣的离子注入陷阱中,则将电线的电位切换到壳体电极的电位,以将离子捕获到陷阱中。 引入金登离子阱的离子可能来自位于保护陷阱中的小离子云。