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    • 12. 发明授权
    • Electrostatic trap
    • 静电诱捕器
    • US08198581B2
    • 2012-06-12
    • US12749334
    • 2010-03-29
    • Alexander MakarovEduard V. DenisovGerhard JungWilko BalschunStevan Roy Horning
    • Alexander MakarovEduard V. DenisovGerhard JungWilko BalschunStevan Roy Horning
    • H01J49/28
    • H01J49/4245H01J49/0027H01J49/02H01J49/282H01J49/406H01J49/425
    • An electrostatic trap such as an orbitrap is disclosed, with an electrode structure. An electrostatic trapping field of the form U′(r, φ, z) is generated to trap ions within the trap so that they undergo isochronous oscillations. The trapping field U′(r, φ, z) is the result of a perturbation W to an ideal field U(r, φ, z) which, for example, is hyperlogarithmic in the case of an orbitrap. The perturbation W may be introduced in various ways, such as by distorting the geometry of the trap so that it no longer follows an equipotential of the ideal field U(r, φ, z), or by adding a distortion field (either electric or magnetic). The magnitude of the perturbation is such that at least some of the trapped ions have an absolute phase spread of more than zero but less than 2 Π radians over an ion detection period Tm.
    • 公开了诸如轨道捕获器的静电捕获器,具有电极结构。 产生形式为U'(r,&phgr; z)的静电捕获场,以捕获陷阱内的离子,使得它们经历同步振荡。 捕获场U'(r,&phgr; z)是对于理想场U(r,&phgr; z)的扰动W的结果,其在例如轨道捕获的情况下例如是超对数的。 扰动W可以以各种方式引入,例如通过使陷波器的几何形状变形,使得其不再遵循理想场U(r,&phgr; z)的等电位,或者通过添加失真场(电 或磁性)。 扰动的幅度使得至少一些捕获的离子的绝对相位差大于零但小于2&Pgr; 弧度超过离子检测周期Tm。
    • 13. 发明授权
    • Electrostatic trap
    • 静电诱捕器
    • US08716654B2
    • 2014-05-06
    • US13737771
    • 2013-01-09
    • Alexander A. MakarovEduard V. DenisovGerhard JungWilko BalschunStevan R. Horning
    • Alexander A. MakarovEduard V. DenisovGerhard JungWilko BalschunStevan R. Horning
    • H01J49/26
    • H01J49/4245H01J49/0027H01J49/02H01J49/282H01J49/406H01J49/425
    • An electrostatic trap such as an orbitrap is disclosed, with an electrode structure. An electrostatic trapping field of the form U′ (r, Φ, z) is generated to trap ions within the trap so that they undergo isochronous oscillations. The trapping field U′(r, Φ, z) is the result of a perturbation W to an ideal field U(r, Φ, z) which, for example, is hypologarithmic in the case of an orbitrap. The perturbation W may be introduced in various ways, such as by distorting the geometry of the trap so that it no longer follows an equipotential of the ideal field U(r, Φ, z), or by adding a distortion field (either electric or magnetic). The magnitude of the perturbation is such that at least some of the trapped ions have an absolute phase spread of more than zero but less than 2 π radians over an ion detection period Tm.
    • 公开了诸如轨道捕获器的静电捕获器,具有电极结构。 产生U'(r,Φ,z)形式的静电捕获场,以捕获陷阱内的离子,使它们经历同步振荡。 捕获场U'(r,Φ,z)是对于理想场U(r,Φ,z)的扰动W的结果,其在轨道捕获的情况下例如是对数的。 扰动W可以以各种方式引入,例如通过使陷波器的几何形状变形,使得其不再遵循理想场U(r,Φ,z)的等电位,或者通过添加失真场(电或 磁性)。 扰动的幅度使得至少一些捕获的离子具有大于零但小于2的绝对相位扩展; 弧度超过离子检测周期Tm。
    • 14. 发明授权
    • Electrostatic trap
    • 静电诱捕器
    • US07714283B2
    • 2010-05-11
    • US10587478
    • 2006-06-05
    • Alexander MakarovEduard V. DenisovGerhard JungWilko BalschunStevan Roy Horning
    • Alexander MakarovEduard V. DenisovGerhard JungWilko BalschunStevan Roy Horning
    • H01J49/28
    • H01J49/4245H01J49/0027H01J49/02H01J49/282H01J49/406H01J49/425
    • An electrostatic trap such as an orbitrap is disclosed, with an electrode structure. An electrostatic trapping field of the form U′(r,φ,z) is generated to trap ions within the trap so that they undergo isochronous oscillations. The trapping field U′(r, φ,z) is the result of a perturbation W to an ideal field U(r, φ,z) which, for example, is hyperlogarithmic in the case of an orbitrap. The perturbation W may be introduced in various ways, such as by distorting the geometry of the trap so that it no longer follows an equipotential of the ideal field U(r, φ,z), or by adding a distortion field (either electric or magnetic). The magnitude of the perturbation is such that at least some of the trapped ions have an absolute phase spread of more than zero but less than about 2π radians over an ion detection period Tm.
    • 公开了诸如轨道捕获器的静电捕获器,具有电极结构。 产生形式为U'(r,&phgr,z)的静电捕获场,以捕获陷阱内的离子,使它们经历同步振荡。 捕获场U'(r,&phgr,,z)是对于理想场U(r,&phgr;,z)的扰动W的结果,其在例如轨道捕获的情况下例如是超对数的。 扰动W可以以各种方式引入,例如通过使陷波器的几何形状变形,使得其不再遵循理想场U(r,&phgr,z)的等电位,或者通过添加失真场(电 或磁性)。 扰动的幅度使得至少一些捕获的离子具有大于零但小于约2的绝对相位扩展; 弧度超过离子检测周期Tm。
    • 16. 发明申请
    • CAST IRON OR ALUMINUM SECTIONAL BOILER
    • 铸铁或铝组件锅炉
    • US20110139093A1
    • 2011-06-16
    • US12921054
    • 2009-02-24
    • Rainer RauschGerhard Jung
    • Rainer RauschGerhard Jung
    • F24H1/30
    • F24H1/32
    • A cast iron or aluminum sectional boiler, in particular a condensing boiler, having generally annular sections, one front section, one cover-like rear section and at least one center section being provided which form a furnace chamber having generally surrounding heating gas passages, and their annular water compartments are connected to one another via hubs. The sections have one lower return connection and one upper feed connection as well as at least two anchor rods for holding the section block together. The cast iron or aluminum sectional boiler is optimized with respect to compactness and robustness. Annular gaps are in each case provided as heating gas passages between two adjacent sections, each of which, starting from the furnace chamber, runs approximately radially outwards and leads into an exhaust gas collection chamber on the outside of the sections.
    • 一种铸铁或铝分段锅炉,特别是冷凝锅炉,其具有大体环形部分,一个前部分,一个盖状后部部分和至少一个中心部分,其形成具有大致周围的加热气体通道的炉室,以及 它们的环形水隔间通过轮毂相互连接。 这些部分具有一个下部返回连接和一个上部进料连接以及用于将截面块保持在一起的至少两个锚杆。 铸铁或铝分段锅炉在紧凑性和坚固性方面进行了优化。 在每个情况下,环形间隙都设置在两个相邻部分之间的加热气体通道,每个区域从炉室开始大致径向向外延伸,并且进入排气收集室。
    • 18. 发明授权
    • Mass spectrometer having an ICP source
    • 质谱仪具有ICP源
    • US5552599A
    • 1996-09-03
    • US315569
    • 1994-09-30
    • Ulrich GiessmannGerhard JungCurt Brunnee
    • Ulrich GiessmannGerhard JungCurt Brunnee
    • H01J49/02H01J49/10H01J49/32
    • H01J49/32H01J49/105
    • A mass spectrometer includes an inductive coupled plasma source whose flame is near ground potential, an interface, a flight tube, and an analyzer that includes magnetic and electric sectors, and an ion detector, which detector is operated at high voltage for ion acceleration. The magnetic sector includes a magnet and pole pieces that are insulated electrically relative to the flight tube. The pressure within the interface preferably does not exceed 10.sup.-3 mbar. By varying the magnetic field and the acceleration potential, identification of a specified mass over defined time intervals is carried out. The disclosed mass spectrometer provides improved coupling between the plasma ion source and a double-focussing analyzer, while advantageously providing a low voltage regime for the plasma source.
    • 质谱仪包括其火焰接近地电位的感应耦合等离子体源,界面,飞行管和包括磁性和电气部分的分析仪,以及离子检测器,该检测器以高电压操作用于离子加速。 磁性部件包括相对于飞行管电绝缘的磁体和极片。 界面内的压力优选不超过10-3毫巴。 通过改变磁场和加速电位,执行在规定的时间间隔内确定指定的质量。 所公开的质谱仪提供等离子体离子源和双重聚焦分析仪之间的改进的耦合,同时有利地为等离子体源提供低电压状态。