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    • 11. 发明授权
    • Method and apparatus for ion cyclotron spectrometry
    • 离子回旋光谱法的方法和装置
    • US07777182B2
    • 2010-08-17
    • US11833079
    • 2007-08-02
    • David A. DahlJill R. ScottTimothy R. McJunkin
    • David A. DahlJill R. ScottTimothy R. McJunkin
    • B01D59/44
    • H01J49/38B01D59/44
    • An ion cyclotron spectrometer may include a vacuum chamber that extends at least along a z-axis and means for producing a magnetic field within the vacuum chamber so that a magnetic field vector is generally parallel to the z-axis. The ion cyclotron spectrometer may also include means for producing a trapping electric field within the vacuum chamber that includes at least a first section that induces a first magnetron effect that increases a cyclotron frequency of an ion and at least a second section that induces a second magnetron effect that decreases the cyclotron frequency of an ion. The cyclotron frequency changes induced by the first and second magnetron effects substantially cancel one another so that an ion traversing the at least first and second sections will experience no net change in cyclotron frequency.
    • 离子回旋加速器光谱仪可以包括至少沿z轴延伸的真空室,以及用于在真空室内产生磁场的装置,使得磁场矢量大致平行于z轴。 离子回旋加速器光谱仪还可以包括用于在真空室内产生捕获电场的装置,其包括至少第一部分,其引起第一磁控管效应,其增加离子的回旋加速器频率,以及至少第二部分诱导第二磁控管 降低离子的回旋加速度的效果。 由第一和第二磁控管效应引起的回旋加速器频率变化基本相互抵消,使得穿过至少第一和第二部分的离子将不会经历回旋加速器频率的净变化。
    • 14. 发明授权
    • Apparatus, system, and method for laser-induced breakdown spectroscopy
    • 用于激光诱发击穿光谱的装置,系统和方法
    • US08891073B2
    • 2014-11-18
    • US13183228
    • 2011-07-14
    • Andrew J. Effenberger, Jr.Jill R. ScottTimothy R. McJunkin
    • Andrew J. Effenberger, Jr.Jill R. ScottTimothy R. McJunkin
    • G01N21/00G01J3/30G01B9/02G01J3/443G01J3/26G01N21/71G01J3/18
    • G01J3/18G01J3/26G01J3/443G01N21/718
    • In laser-induced breakdown spectroscopy (LIBS), an apparatus includes a pulsed laser configured to generate a pulsed laser signal toward a sample, a constructive interference object and an optical element, each located in a path of light from the sample. The constructive interference object is configured to generate constructive interference patterns of the light. The optical element is configured to disperse the light. A LIBS system includes a first and a second optical element, and a data acquisition module. The data acquisition module is configured to determine an isotope measurement based, at least in part, on light received by an image sensor from the first and second optical elements. A method for performing LIBS includes generating a pulsed laser on a sample to generate light from a plasma, generating constructive interference patterns of the light, and dispersing the light into a plurality of wavelengths.
    • 在激光诱发击穿光谱(LIBS)中,一种装置包括脉冲激光器,其经配置以产​​生朝向样品的脉冲激光信号,构造干涉物体和光学元件,每个位于来自样品的光的路径中。 构造性干扰对象被配置为产生光的建设性干涉图案。 光学元件构造成分散光。 LIBS系统包括第一和第二光学元件,以及数据采集模块。 数据采集​​模块被配置为至少部分地基于图像传感器从第一和第二光学元件接收的光来确定同位素测量。 用于执行LIBS的方法包括在样本上产生脉冲激光以产生来自等离子体的光,产生光的建设性干涉图案,以及将光分散成多个波长。
    • 16. 发明授权
    • Method and apparatuses for ion cyclotron spectrometry
    • 离子回旋光谱法的方法和装置
    • US08129678B2
    • 2012-03-06
    • US12818051
    • 2010-06-17
    • David A. DahlJill R. ScottTimothy R. McJunkin
    • David A. DahlJill R. ScottTimothy R. McJunkin
    • B01D59/44
    • H01J49/38B01D59/44
    • An ion cyclotron spectrometer may include a vacuum chamber that extends at least along a z-axis and means for producing a magnetic field within the vacuum chamber so that a magnetic field vector is generally parallel to the z-axis. The ion cyclotron spectrometer may also include means for producing a trapping electric field within the vacuum chamber. The trapping electric field may comprise a field potential that, when taken in cross-section along the z-axis, includes at least one section that is concave down and at least one section that is concave up so that ions traversing the field potential experience a net magnetron effect on a cyclotron frequency of the ions that is substantially equal to zero. Other apparatuses and a method for performing ion cyclotron spectrometry are also disclosed herein.
    • 离子回旋加速器光谱仪可以包括至少沿z轴延伸的真空室,以及用于在真空室内产生磁场的装置,使得磁场矢量大致平行于z轴。 离子回旋加速器光谱仪还可以包括在真空室内产生捕获电场的装置。 捕获电场可以包括场电位,当沿着z轴截取横截面时,其包括至少一个凹陷的部分和至少一个向上凹进的部分,使得穿过场电位的离子经历一个 净磁控管对基本上等于零的离子的回旋加速器的影响。 本文还公开了其他装置和执行离子回旋光谱法的方法。
    • 17. 发明申请
    • METHOD AND APPARATUSES FOR ION CYCLOTRON SPECTROMETRY
    • 离子色谱法的方法和装置
    • US20100320378A1
    • 2010-12-23
    • US12818051
    • 2010-06-17
    • David A. DahlJill R. ScottTimothy R. McJunkin
    • David A. DahlJill R. ScottTimothy R. McJunkin
    • H01J49/34B01D59/44H01J49/02H01J1/02
    • H01J49/38B01D59/44
    • An ion cyclotron spectrometer may include a vacuum chamber that extends at least along a z-axis and means for producing a magnetic field within the vacuum chamber so that a magnetic field vector is generally parallel to the z-axis. The ion cyclotron spectrometer may also include means for producing a trapping electric field within the vacuum chamber. The trapping electric field may comprise a field potential that, when taken in cross-section along the z-axis, includes at least one section that is concave down and at least one section that is concave up so that ions traversing the field potential experience a net magnetron effect on a cyclotron frequency of the ions that is substantially equal to zero. Other apparatuses and a method for performing ion cyclotron spectrometry are also disclosed herein.
    • 离子回旋加速器光谱仪可以包括至少沿z轴延伸的真空室,以及用于在真空室内产生磁场的装置,使得磁场矢量大致平行于z轴。 离子回旋加速器光谱仪还可以包括在真空室内产生捕获电场的装置。 捕获电场可以包括场电位,当沿着z轴截取横截面时,其包括至少一个凹陷的部分和至少一个向上凹进的部分,使得穿过场电位的离子经历一个 净磁控管对基本上等于零的离子的回旋加速器的影响。 本文还公开了其他装置和执行离子回旋光谱法的方法。