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    • 1. 发明授权
    • System and method for adaptively adjusting clock skew in a variably loaded memory bus
    • 用于在可变加载的存储器总线中自适应地调整时钟偏移的系统和方法
    • US06915443B2
    • 2005-07-05
    • US09904814
    • 2001-07-13
    • Christopher D. McBridePaul V. BrownellTimothy R. McJunkin
    • Christopher D. McBridePaul V. BrownellTimothy R. McJunkin
    • G06F1/10G06F1/04G06F1/12G06F13/00G11C7/00
    • G06F1/10
    • The preferred embodiments of the present invention are directed to the selective phase lag and time delay of clock signals within a computer system to compensate for additional parasitic capacitance that may be added to that system because of its open architecture. More particularly, the preferred embodiments are directed to clock signal path circuits where each circuit has multiple signal paths of varying lengths. By allowing the clock signals to propagate along a particular path, phase lag or time delay is added to those clock signals. Selection of a particular path for the clock signal is made by activating electrically controlled switches which themselves are activated or deactivated by software programs that run during power-up of the computer system that determine required phase lag or time delay of those clock signals as a function of parasitic capacitance in the computer system.
    • 本发明的优选实施例涉及计算机系统内的时钟信号的选择性相位滞后和时间延迟,以补偿由于其开放架构而可能添加到该系统的附加寄生电容。 更具体地,优选实施例涉及时钟信号路径电路,其中每个电路具有不同长度的多个信号路径。 通过允许时钟信号沿特定路径传播,相位滞后或时间延迟被添加到那些时钟信号。 用于时钟信号的特定路径的选择是通过激活电控开关来实现的,该开关本身由计算机系统的上电期间运行的软件程序激活或去激活,所述软件程序确定那些时钟信号作为一个功能的所需相位滞后或时间延迟 的计算机系统中的寄生电容。
    • 3. 发明申请
    • APPARATUS, SYSTEM, AND METHOD FOR LASER-INDUCED BREAKDOWN SPECTROSCOPY
    • 用于激光诱发断裂光谱的装置,系统和方法
    • US20130016349A1
    • 2013-01-17
    • US13183228
    • 2011-07-14
    • Andrew J. Effenberger, JR.Jill R. ScottTimothy R. McJunkin
    • Andrew J. Effenberger, JR.Jill R. ScottTimothy R. McJunkin
    • G01J3/30
    • 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。
    • 7. 发明申请
    • METHOD AND APPARATUS FOR ION CYCLOTRON SPECTROMETRY
    • 用于离子色谱分析的方法和装置
    • US20090032696A1
    • 2009-02-05
    • 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 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 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。 光谱仪还可以包括用于在真空室内产生捕获电场的装置,该装置包括至少第一部分,该第一部分引起增加离子的回旋加速器频率的第一磁控管效应,以及引起第二磁控管效应的至少第二部分, 降低离子的回旋加速器频率。 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,使得穿过第一和第二部分的离子将不会在回旋加速器频率中经历净变化。
    • 9. 发明申请
    • APPARATUSES AND METHODS FOR FORMING ELECTROMAGNETIC FIELDS
    • 用于形成电磁场的装置和方法
    • US20110266436A1
    • 2011-11-03
    • US13096823
    • 2011-04-28
    • Jill R. ScottTimothy R. McJunkinPaul L. Tremblay
    • Jill R. ScottTimothy R. McJunkinPaul L. Tremblay
    • H01J49/26H05H7/00H05H13/02H01F7/06
    • H05H7/04H01J49/062H01J49/067
    • An electromagnetic field generator includes a semiconductive material shaped to form a complex electromagnetic field including a magnetic field and an electric field. An instrument includes a passage configured such that charged particle may travel therein, and a semiconductive material configured to form a complex electromagnetic field that is configured to control motion of the charged particles within the passage. Another instrument includes a housing defining a chamber, and an electromagnetic field generator within the chamber that comprises a material configured to form an electric field component of an electromagnetic field, and a material configured to form a magnetic field component of the electromagnetic field. A method of controlling motion of charged particles includes controlling motion of at least one charged particle by forming a complex electromagnetic field with a semiconductive material that is shaped to form the complex electromagnetic field.
    • 电磁场发生器包括形成为形成包括磁场和电场的复杂电磁场的半导体材料。 仪器包括构造为使得带电粒子可以在其中行进的通道,以及配置成形成复合电磁场的半导体材料,该复合电磁场被配置为控制通道内的带电粒子的运动。 另一个仪器包括限定腔室的壳体和室内的电磁场发生器,其包括被配置为形成电磁场的电场分量的材料以及被配置为形成电磁场的磁场分量的材料。 控制带电粒子的运动的方法包括通过形成复合电磁场来形成至少一个带电粒子的运动,所述复合电磁场被形成为形成复合电磁场的半导体材料。