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    • 1. 发明授权
    • Two-dimensional electrode constructions for ion processing
    • 用于离子处理的二维电极结构
    • US07501623B2
    • 2009-03-10
    • US11342485
    • 2006-01-30
    • Roger TongMingda WangGregory J. Wells
    • Roger TongMingda WangGregory J. Wells
    • H01J49/42
    • H01J49/423H01J49/4225
    • An electrode for use in a device such as an ion trap has an axial length extending generally in the direction of a central axis from a first axial end to a second axial end, and an inside surface. The inside surface includes a surface profile that is uniform from the first axial end to the second axial end, or at least is uniform for a uniform section length along the axial direction. The electrode may include an elongated surface feature such as a groove that extends for at least the uniform section length. An aperture may communicate with the groove. The electrode may be axially segmented into regions. Gaps between the regions may be oriented at an angle relative to a plane orthogonal to the central axis. The electrode may be one of several electrodes arranged as an electrode structure coaxially disposed about an elongated interior space.
    • 用于诸如离子阱的装置的电极具有从第一轴向端部到第二轴向端部以及内表面大致沿中心轴线的方向延伸的轴向长度。 内表面包括从第一轴向端到第二轴向端均匀的表面轮廓,或者至少沿着轴向方向具有均匀的截面长度是均匀的。 电极可以包括细长的表面特征,例如延伸至少均匀的截面长度的凹槽。 孔可以与凹槽连通。 电极可以轴向分段成区域。 区域之间的间隙可以相对于与中心轴线正交的平面成一定角度。 电极可以是布置成围绕细长内部空间同轴设置的电极结构的多个电极之一。
    • 2. 发明申请
    • Two-dimensional electrode constructions for ion processing
    • 用于离子处理的二维电极结构
    • US20070176095A1
    • 2007-08-02
    • US11342485
    • 2006-01-30
    • Roger TongMingda WangGregory Wells
    • Roger TongMingda WangGregory Wells
    • H01J49/42
    • H01J49/423H01J49/4225
    • An electrode for use in a device such as an ion trap has an axial length extending generally in the direction of a central axis from a first axial end to a second axial end, and an inside surface. The inside surface includes a surface profile that is uniform from the first axial end to the second axial end, or at least is uniform for a uniform section length along the axial direction. The electrode may include an elongated surface feature such as a groove that extends for at least the uniform section length. An aperture may communicate with the groove. The electrode may be axially segmented into regions. Gaps between the regions may be oriented at an angle relative to a plane orthogonal to the central axis. The electrode may be one of several electrodes arranged as an electrode structure coaxially disposed about an elongated interior space.
    • 用于诸如离子阱的装置的电极具有从第一轴向端部到第二轴向端部以及内表面大致沿中心轴线的方向延伸的轴向长度。 内表面包括从第一轴向端到第二轴向端均匀的表面轮廓,或者至少沿着轴向方向具有均匀的截面长度是均匀的。 电极可以包括细长的表面特征,例如延伸至少均匀的截面长度的凹槽。 孔可以与凹槽连通。 电极可以轴向分段成区域。 区域之间的间隙可以相对于与中心轴线正交的平面成一定角度。 电极可以是布置成围绕细长内部空间同轴设置的电极结构的多个电极之一。
    • 4. 发明授权
    • Mass scanning method using an ion trap mass spectrometer
    • 使用离子阱质谱仪的质谱扫描方法
    • US5714755A
    • 1998-02-03
    • US609364
    • 1996-03-01
    • Gregory J. WellsMingda WangEdward G. Marquette
    • Gregory J. WellsMingda WangEdward G. Marquette
    • G01N27/62H01J49/04H01J49/42B01D59/44H01J49/00
    • H01J49/424H01J49/429
    • An improved method of using an ion trap mass spectrometer is disclosed. According to the method an asymmetrical trapping field is applied to the trap. Preferably, the asymmetrical trapping field comprises a quadrupole field and a dipole field having the same frequency. In addition, higher order trapping field components, such as hexapole or octopole fields, may also be included, and the electrodes of the ion trap can be shaped to introduce such higher order field components. The effect of the asymmetrical trapping field of the present invention is to cause the center of the trapping field to be displaced from the mechanical center of the ion trap. A supplemental quadrupole field is then applied to the ion trap, the center of the supplemental quadrupole field being located at the mechanical center of the trap, i.e., it is displaced from the center of the trapping field. The supplement quadrupole field and the trapping field may be viewed as forming one combined field which acts upon the ions in the trap. The combined field is then scanned to cause ions of differing masses to be resonantly ejected from the ion trap in sequential mass order. Preferably, the combined field is scanned by scanning the voltage of the trapping field. Preferably, the supplemental field is set to have a frequency which is two-thirds of the trapping field frequency and is phase locked with the trapping field frequency.
    • 公开了使用离子阱质谱仪的改进方法。 根据该方法,将不对称捕获场应用于陷阱。 优选地,不对称捕获场包括具有相同频率的四极场和偶极场。 此外,还可以包括诸如六极或八极场的较高阶捕获场分量,并且离子阱的电极可被成形为引入这种较高阶场分量。 本发明的不对称捕获场的作用是使捕集场的中心从离子阱的机械中心位移。 然后将补充的四极场施加到离子阱,补充四极场的中心位于阱的机械中心,即其从俘获场的中心位移。 补充四极场和俘获场可以被视为形成一个组合场,其作用在阱中的离子上。 然后扫描组合场,使不同质量的离子以顺序的质量顺序从离子阱共振地喷出。 优选地,通过扫描捕获场的电压来扫描组合场。 优选地,补充场被设置为具有捕获场频率的三分之二的频率并且与捕获场频率锁相。
    • 7. 发明申请
    • Chemical structure-insensitive method and apparatus for dissociating ions
    • 用于离子离子化学结构不敏感的方法和装置
    • US20080217527A1
    • 2008-09-11
    • US11715199
    • 2007-03-07
    • Mingda Wang
    • Mingda Wang
    • B01D59/44
    • H01J49/426H01J49/005
    • In a method for exciting a precursor ion in an ion trap, the ion is trapped in a nonlinear trapping field that includes a quadrupolar field and a multipole field. The quadrupolar field is generated by applying a radio-frequency (RF) trapping voltage to the ion trap at a trapping amplitude and trapping frequency. A supplemental alternating-current (AC) voltage is applied to the ion trap at a supplemental amplitude and supplemental frequency. The supplemental amplitude is low enough to prevent ejection of the ion from the ion trap, and the supplemental frequency differs from the secular frequency of the ion by an offset amount. One or more operating parameters of the ion trap are adjusted, such that the ion absorbs energy from the supplemental field sufficient to undergo collision-induced dissociation (CID) without being in resonance with the supplemental field.
    • 在用于在离子阱中激发前体离子的方法中,离子被捕获在包括四极场和多极场的非线性捕获场中。 通过以捕获幅度和捕获频率向离子阱施加射频(RF)捕获电压来产生四极场。 补充的交流(AC)电压以补充的幅度和补充频率施加到离子阱。 辅助振幅足够低以防止离子从离子阱中喷射,并且补充频率与离子的长期频率不同,具有偏移量。 调整离子阱的一个或多个操作参数,使得离子从补充场吸收足以进行碰撞诱导解离(CID)的能量,而不与补充场共振。