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    • 4. 发明授权
    • Touch sensor with non-uniform resistive band
    • 具有不均匀电阻带的触摸传感器
    • US07265686B2
    • 2007-09-04
    • US10619915
    • 2003-07-15
    • G. Samuel HurstR. H. RitchieRobert J. WarmackDonald W. BouldinJoel C. Kent
    • G. Samuel HurstR. H. RitchieRobert J. WarmackDonald W. BouldinJoel C. Kent
    • H03K17/94
    • G06F3/045G06F3/0488
    • A touch sensors with improved topological equivalence between an equipotential space and a Cartesian space to which the equipotential space will be mapped. The touch sensor comprises a substrate with a touch region, and a set of electrodes that are electrically coupled to the touch region. The touch sensor further comprises a plurality of resistive band segments that frames the touch region. The electrodes are located between the resistive band segments. Each resistive band segment has a resistivity that is intermediate between the resistivity of the electrodes and the resistivity of the touch region, thereby providing a transition between the low resistivity electrodes and the high resistivity touch region, and improving the topological equivalence within the corners of the touch region. At least one of the band segments has a non-uniform linear resistance to provide further improvement to the topological equivalence.
    • 触摸传感器具有等位置空间与等位空间映射到的笛卡尔空间之间的拓扑等效性。 触摸传感器包括具有触摸区域的基板和电耦合到触摸区域的一组电极。 触摸传感器还包括多个阻挡接触区域的电阻带段。 电极位于电阻带段之间。 每个电阻带段具有在电极的电阻率和触摸区域的电阻率之间的电阻率,从而提供低电阻率电极和高电阻率接触区域之间的转变,并且改善电极的拐角内的拓扑等效性 触摸区域。 至少一个带段具有不均匀的线性电阻以提供对拓扑等效性的进一步改进。
    • 5. 发明授权
    • Neutron dosimeter
    • 中子剂量计
    • US4699751A
    • 1987-10-13
    • US544531
    • 1983-10-24
    • G. Samuel HurstHarold W. SchmittNorbert ThonnardTom J. Whitaker
    • G. Samuel HurstHarold W. SchmittNorbert ThonnardTom J. Whitaker
    • G01T3/00G21C17/00
    • G21C17/00G01T3/00
    • A dosimeter which incorporates new methods for determining neutron dose. Less than one millirad of dose due to neutrons of all energies down to approximately 10.sup.3 eV can be measured, and the response can be adjusted by design of the dosimeter. The dosimeter utilizes the sputtering of material from a target due to the action of the neutrons and measuring of the amount of sputtered material to determine the dose. The sputtered material may be, for example, a noble gas or an inert solid. Various radiator materials can be included to interact with the neutrons so that the resulting charged particles control the sputtering process and hereby increase the sensitivity of the dosimeter. The target material can be, for example, noble-gas-impregnated polycrystalline or amorphous metals. The sputtered material is analyzed using resonance ionization spectroscopy, sputter-initiated resonance ionization spectroscopy or other methods to determine its quantity and hence the neutron dose. Applications include, but are not limited to, personnel neutron dosimetry and stationary neutron monitors.
    • 一种剂量计,其包含用于确定中子剂量的新方法。 可以测量由于所有能量的中子降至约103eV的剂量小于1毫升,并且响应可以通过剂量计的设计来调节。 剂量计利用来自靶的材料的溅射,由于中子的作用并且测量溅射的材料的量以确定剂量。 溅射的材料可以是例如惰性气体或惰性固体。 可以包括各种散热器材料以与中子相互作用,使得所得的带电粒子控制溅射工艺,从而增加剂量计的灵敏度。 目标材料可以是例如贵金属气体浸渍的多晶或非晶金属。 使用共振电离光谱法,溅射引发的共振电离光谱法或其他方法分析溅射的材料以确定其量并因此确定中子剂量。 应用包括但不限于人员中子剂量测定法和固定中子监测仪。
    • 6. 发明授权
    • Instrument simulator system
    • 仪器模拟器系统
    • US5423683A
    • 1995-06-13
    • US152017
    • 1993-11-15
    • G. Samuel HurstHarvel A. WrightJohn D. Morris
    • G. Samuel HurstHarvel A. WrightJohn D. Morris
    • G01T1/16G01T7/00G09B9/00G09B23/20A61B6/00
    • G01T1/16G01T7/00G09B23/20G09B9/00
    • A health physics instrument simulator system permitting an operator to simulate measurement of radiation levels of a plurality of radiation types includes a memory for storing first data corresponding to an n-dimensional training space representing a predetermined physical location, second data defining a radiation source including source strength, source type and source location with respect to the training space and radiation intensity data based on the second data, where each of the radiation intensity data corresponds to one respective location in the training space, a selecting device for selecting a predetermined simulated radiation sensing instrument, a pointing device for identifying a location within the training space defining a current location of the simulated radiation sensing instrument and a display for displaying both an instrument display corresponding to the simulated radiation sensing instrument and radiation intensity data corresponding to the current location in the training space. Methods for operating a health physics instrument simulator system including a computer and a display are also disclosed.
    • 允许操作者模拟多个辐射类型的辐射水平的测量的健康物理仪器模拟器系统包括用于存储对应于表示预定物理位置的n维训练空间的第一数据的存储器,定义包括源的辐射源的第二数据 相对于训练空间的强度,源类型和源位置以及基于第二数据的辐射强度数据,其中每个辐射强度数据对应于训练空间中的一个相应位置,选择装置,用于选择预定的模拟辐射感测 仪器,用于识别训练空间中定义模拟辐射感测仪器的当前位置的位置的指示设备和用于显示对应于模拟辐射感测仪器的仪器显示器和对应于当前位置的辐射强度数据的显示器 e培训空间。 还公开了用于操作包括计算机和显示器的健康物理仪器模拟器系统的方法。
    • 7. 发明授权
    • Instrument simulator system
    • 仪器模拟器系统
    • US5304065A
    • 1994-04-19
    • US974754
    • 1992-11-13
    • G. Samuel HurstHarvel A. WrightJohn D. Morris
    • G. Samuel HurstHarvel A. WrightJohn D. Morris
    • G01T1/16G01T7/00G09B9/00G09B23/20A61B6/00
    • G01T1/16G01T7/00G09B23/20G09B9/00
    • A health physics instrument simulator system permitting an operator to simulate measurement of radiation levels of a plurality of radiation types includes a memory for storing first data corresponding to an n-dimensional training space representing a predetermined physical location, second data defining a radiation source including source strength, source type and source location with respect to the training space and radiation intensity data based on the second data, where each of the radiation intensity data corresponds to one respective location in the training space, a selecting device for selecting a predetermined simulated radiation sensing instrument, a pointing device for identifying a location within the training space defining a current location of the simulated radiation sensing instrument and a display for displaying both an instrument display corresponding to the simulated radiation sensing instrument and radiation intensity data corresponding to the current location in the training space. Methods for operating a health physics instrument simulator system including a computer and a display are also disclosed.
    • 允许操作者模拟多个辐射类型的辐射水平的测量的健康物理仪器模拟器系统包括用于存储对应于表示预定物理位置的n维训练空间的第一数据的存储器,定义包括源的辐射源的第二数据 相对于训练空间的强度,源类型和源位置以及基于第二数据的辐射强度数据,其中每个辐射强度数据对应于训练空间中的一个相应位置,选择装置,用于选择预定的模拟辐射感测 仪器,用于识别训练空间中定义模拟辐射感测仪器的当前位置的位置的指示设备和用于显示对应于模拟辐射感测仪器的仪器显示器和对应于当前位置的辐射强度数据的显示器 e培训空间。 还公开了用于操作包括计算机和显示器的健康物理仪器模拟器系统的方法。
    • 8. 发明授权
    • Sputter initiated resonance ionization spectrometry
    • 溅射引发共振电离光谱法
    • US4442354A
    • 1984-04-10
    • US341895
    • 1982-01-22
    • G. Samuel HurstJames E. ParksHarold W. Schmitt
    • G. Samuel HurstJames E. ParksHarold W. Schmitt
    • G01N21/63G01N23/225G01Q30/20H01J49/14H01J49/16B01D59/44
    • H01J49/164G01N21/63G01N23/225H01J49/142
    • Apparatus and method are described for the quantitative analysis of a specific specie within a sample. The analysis has sufficient sensitivity for the detection of as little as one atom of the desired species. The method is accomplished by bombarding a sample with a highly focused charged particle beam; for example, a beam of positive argon ions having an energy from five to thirty kilovolts and a current of one milliampere or greater. This beam impinging upon the sample creates a cloud including secondary ions and neutral particles of the constituents of the sample. The cloud is irradiated with a laser beam having selected wavelengths therein for the unique ionization of the desired specie by means of resonance ionization spectroscopy (RIS). In most applications some energy and/or mass discrimination is required. The energy discrimination can be accomplished by passing the RIS ions through an energy filter, with the ions emanating therefrom having a narrow range of energy. Then, if desired, a mass discrimination may be accomplished in an appropriate mass analyzer such as a time of flight spectrometer, an r.f. quadrupole mass spectrometer or a magnetic sector mass spectrometer.
    • 描述了用于样品中特定物种的定量分析的装置和方法。 该分析具有足够的灵敏度,用于检测少至一个所需物种的原子。 该方法通过用高度聚焦的带电粒子束轰击样品来实现; 例如,具有五至三十千伏的能量和一毫安或更大的电流的正氩离子束。 撞击样品的这种光束会产生包含样品成分的二次离子和中性粒子的云。 用其中选择的波长的激光束照射云,以通过共振电离光谱法(RIS)进行所需物种的独特电离。 在大多数应用中,需要一些能量和/或质量的区别。 能量鉴别可以通过将RIS离子通过能量过滤器来实现,其中从其发出的离子具有窄的能量范围。 然后,如果需要,可以在合适的质量分析仪中进行质量鉴别,例如飞行时间谱仪,r.f. 四极杆质谱仪或磁性部门质谱仪。
    • 9. 发明授权
    • Method and apparatus for noble gas atom detection with isotopic
selectivity
    • 同位素选择性惰性气体原子检测方法与装置
    • US4426576A
    • 1984-01-17
    • US300019
    • 1981-09-08
    • G. Samuel HurstMarvin G. PayneChung-Hsuan ChenJames E. Parks
    • G. Samuel HurstMarvin G. PayneChung-Hsuan ChenJames E. Parks
    • H01J49/02H01J49/04H01J49/16H01J49/42B01D59/44
    • H01J49/162H01J49/0422
    • Apparatus and methods of operation are described for determining, with isotopic selectivity, the number of noble gas atoms in a sample. The analysis is conducted within an evacuated chamber which can be isolated by a valve from a vacuum pumping system capable of producing a pressure of 10.sup.-8 Torr. Provision is made to pass pulses of laser beams through the chamber, these pulses having wavelengths appropriate for the resonance ionization of atoms of the noble gas under analysis. A mass filter within the chamber selects ions of a specific isotope of the noble gas, and means are provided to accelerate these selected ions sufficiently for implantation into a target. Specific types of targets are discussed. An electron measuring device produces a signal relatable to the number of ions implanted into the target and thus to the number of atoms of the selected isotope of the noble gas removed from the gas sample. The measurement can be continued until a substantial fraction, or all, of the atoms in the sample have been counted.Furthermore, additional embodiments of the apparatus are described for bunching the atoms of a noble gas for more rapid analysis, and for changing the target for repetitive cycling of the gas in the chamber. The number of repetitions of the cyclic steps depend upon the concentration of the isotope of interest, the separative efficiency of the mass filter, etc. The cycles are continued until a desired selectivity is achieved. Also described are components and a method of operation for a pre-enrichment operation for use when an introduction of a total sample would elevate the pressure within the chamber to levels in excess of those for operation of the mass filter, specifically a quadrupole mass filter.Specific examples of three noble gas isotope analyses are described.
    • 描述了操作的装置和方法,以同位素选择性来确定样品中惰性气体原子的数量。 该分析在真空室内进行,其可以通过阀从能够产生10-8托的压力的真空泵系统隔离。 提供了将激光束的脉冲通过腔室,这些脉冲具有适于分析的惰性气体的原子的共振电离的波长。 室内的质量过滤器选择惰性气体的特定同位素的离子,并且提供了用于将这些选定的离子充分加速以植入靶中的装置。 讨论具体类型的目标。 电子测量装置产生与植入靶中的离子数相关的信号,从而产生从气体样品中除去的惰性气体的选定同位素原子数。 可以继续测量,直到已经计数了样品中的大部分原子或全部原子。 此外,描述了该设备的附加实施例,用于聚合惰性气体的原子以进行更快速的分析,并且用于改变靶室以使腔室中的气体重复循环。 循环步骤的重复次数取决于所关心的同位素的浓度,质量过滤器的分离效率等。循环持续到达到期望的选择性。 还描述了当全部样品的引入将室内的压力升高到超过用于质量过滤器,特别是四极质量过滤器的操作的水平时,用于预浓缩操作的组件和操作方法。 描述了三种惰性气体同位素分析的具体实例。