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    • 51. 发明授权
    • Mass spectrometer
    • 质谱仪
    • US08164052B2
    • 2012-04-24
    • US12593006
    • 2008-03-26
    • Martin R. GreenJason Lee WildgooseJeffery Mark Brown
    • Martin R. GreenJason Lee WildgooseJeffery Mark Brown
    • H01J49/26H01J49/40
    • H01J49/0481H01J49/0072H01J49/065H01J49/40Y10T436/24
    • A mass spectrometer is disclosed comprising an Electron Transfer Dissociation cell (1). Positive analyte ions are fragmented into fragment ions upon colliding with singly charged negative reagent ions with the cell (1). The cell comprises a plurality of ring electrodes (1) which form a spherical trapping volume. Ions experience negligible RF heating over the majority, of the trapping volume which enables the kinetic energy of the analyte and reagent ions to be reduced to just above thermal temperatures. An Electron Transfer Dissociation cell (1) having an enhanced sensitivity is thereby provided. Fragment ions created within the cell (1) may be cooled and may be transmitted onwardly to an orthogonal acceleration Time of Flight mass analyser enabling a significant improvement in the resolution of the mass analyser to be obtained.
    • 公开了包含电子转移离解电池(1)的质谱仪。 当与单体电荷的负试剂离子碰撞时,阳性分析物离子被碎裂成碎片离子(1)。 电池包括形成球形捕获体积的多个环形电极(1)。 离子经验可忽略大部分的RF加热,捕集体积使分析物和试剂离子的动能降低到高于热温度。 由此提供了具有增强的灵敏度的电子转移解离单元(1)。 在细胞(1)内产生的片段离子可以被冷却并且可以向内传播到正交加速时间飞行质量分析仪,能够显着提高质量分析仪的分辨率。
    • 55. 发明申请
    • Mass Spectrometer
    • 质谱仪
    • US20100038530A1
    • 2010-02-18
    • US11813221
    • 2006-01-17
    • Kevin GilesMartin GreenJason Lee Wildgoose
    • Kevin GilesMartin GreenJason Lee Wildgoose
    • H01J49/04H01J49/42
    • H01J49/4235H01J49/4275
    • An ion guide or ion trap (1) is disclosed comprising a segmented linear ion guide or ion trap. Ions are confined radially within the ion guide or ion trap (1) by the application of an AC or RF voltage to the electrodes. A static potential well is maintained along at least a portion of the axial length of the ion guide or ion trap (1). A time varying homogeneous electric field is applied along at least a portion of the axial length of the ion guide or ion trap (1). The combination of the static axial potential well and the time varying axial homogeneous electric field causes ions to be ejected from the ion guide or ion trap (1) in a substantially non-resonant manner.
    • 公开了一种离子导向器或离子阱(1),其包括分段线性离子导向器或离子阱。 通过向电极施加AC或RF电压,离子在径向上被限制在离子导向器或离子阱(1)内。 沿离子导向器或离子阱(1)的轴向长度的至少一部分保持静电势阱。 沿离子导向器或离子阱(1)的轴向长度的至少一部分施加时变均匀电场。 静态轴向势阱和随时间变化的轴向均匀电场的组合导致离子以基本上非共振的方式从离子导向器或离子阱(1)喷出。
    • 57. 发明申请
    • Mass spectrometer
    • 质谱仪
    • US20090114808A1
    • 2009-05-07
    • US11916430
    • 2006-06-01
    • Robert Harold BatemanJeffery Mark BrownMartin Raymond GreenJason Lee Wildgoose
    • Robert Harold BatemanJeffery Mark BrownMartin Raymond GreenJason Lee Wildgoose
    • B01D59/44H01J49/00
    • H01J49/0036
    • A method of mass spectrometry is disclosed wherein voltage signals from an ion detector are analysed. A second differential of each voltage signal is obtained and the start and end times of observed voltage peaks are determined. The intensity and average time of each voltage peak is then determined and the intensity and time values are stored. An intermediate composite mass spectrum is then formed by combining the intensity and time values which relate to each voltage peak observed from multiple experimental runs. The various pairs of time and intensity data are then integrated to produce a smooth continuum mass spectrum. The continuum mass spectrum may then be further processed by determining the second differential of the continuum mass spectrum. The start and end times of mass peaks observed in the continuum mass spectrum may be determined. The intensity and mass to charge ratio of each mass peak observed in the continuum mass spectrum may then determined. A final discrete mass spectrum comprising just of an intensity value and mass to charge ratio per species of ion may then be displayed or output.
    • 公开了一种质谱法,其中分析了来自离子检测器的电压信号。 获得每个电压信号的第二差分,并且确定观察到的电压峰值的开始和结束时间。 然后确定每个电压峰值的强度和平均时间,并存储强度和时间值。 然后通过组合与多个实验运行中观察到的每个电压峰值相关的强度和时间值来形成中间复合质谱。 然后将各种时间和强度数据对被整合以产生平滑的连续质谱。 然后可以通过确定连续质谱的第二差分来进一步处理连续质谱。 可以确定在连续质谱中观察到的质量峰的开始和结束时间。 然后可以确定在连续质谱中观察到的每个质量峰的强度和质荷比。 然后可以显示或输出包括仅每个离子种类的强度值和质荷比的最终离散质谱。