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    • 2. 发明授权
    • Container, container positioning method, and measuring method
    • 集装箱,集装箱定位方法和测量方法
    • US08330110B2
    • 2012-12-11
    • US12617129
    • 2009-11-12
    • Shigeki NishinaShigeaki Naitoh
    • Shigeki NishinaShigeaki Naitoh
    • G01J5/02
    • G01N21/3581G01N21/3563
    • A container according to the present invention contains at least a part of a device under test to be measured by a terahertz wave measurement device. The container includes a gap portion that internally disposes at least a part of the device under test, and an enclosure portion that includes a first flat surface portion and a second flat surface portion, and disposes the gap portion between the first flat surface portion and the second flat surface portion, thereby enclosing the gap portion. Moreover, a relationship n1−0.1≦n2≦n1+0.1 holds where n2 is a refractive index of the enclosure portion, and n1 is a refractive index of the device under test. Further, the first flat surface portion intersects with a travel direction of the terahertz wave at the right angle.
    • 根据本发明的容器包含被太赫兹波测量装置测量的被测器件的至少一部分。 容器包括内部配置被测设备的至少一部分的间隙部分和包括第一平坦表面部分和第二平坦表面部分的封闭部分,并且将间隙部分设置在第一平坦表面部分和第二平坦部分之间 第二平坦表面部分,从而包围间隙部分。 此外,关系n1-0.1≦̸ n2≦̸ n1 + 0.1成立,其中n2是封装部分的折射率,n1是被测器件的折射率。 此外,第一平面部与直角的太赫兹波的行进方向交叉。
    • 5. 发明申请
    • CONTAINER, CONTAINER POSITIONING METHOD, AND MEASURING METHOD
    • 集装箱,集装箱定位方法和测量方法
    • US20110057103A1
    • 2011-03-10
    • US12617129
    • 2009-11-12
    • Shigeki NISHINAShigeaki NAITOH
    • Shigeki NISHINAShigeaki NAITOH
    • G01J5/00G01R31/26
    • G01N21/3581G01N21/3563
    • A container according to the present invention contains at least a part of a device under test to be measured by a terahertz wave measurement device. The container includes a gap portion that internally disposes at least a part of the device under test, and an enclosure portion that includes a first flat surface portion and a second flat surface portion, and disposes the gap portion between the first flat surface portion and the second flat surface portion, thereby enclosing the gap portion. Moreover, a relationship n1→0.1≦n2≦n1+0.1 holds where n2 is a refractive index of the enclosure portion, and n1 is a refractive index of the device under test. Further, the first flat surface portion intersects with a travel direction of the terahertz wave at the right angle.
    • 根据本发明的容器包含被太赫兹波测量装置测量的被测器件的至少一部分。 容器包括内部配置被测设备的至少一部分的间隙部分和包括第一平坦表面部分和第二平坦表面部分的封闭部分,并且将间隙部分设置在第一平坦表面部分和第二平坦部分之间 第二平坦表面部分,从而包围间隙部分。 此外,n1→0.1≦̸ n2≦̸ n1 + 0.1的关系成立,其中n2是外壳部分的折射率,n1是被测器件的折射率。 此外,第一平面部与直角的太赫兹波的行进方向交叉。
    • 6. 发明授权
    • Monochromator and spectrometric method
    • 单色器和光谱法
    • US06411382B1
    • 2002-06-25
    • US09548581
    • 2000-04-13
    • Shigeki Nishina
    • Shigeki Nishina
    • G01J318
    • G01J3/1804
    • The monochromator and the spectrometric method are disclosed wherein the measured beam converted into a parallel beam by a first collimator is diffracted by a plane diffraction grating, then the diffracted beam is returned so that the diffracted beam after the return is separated from that before the return along rulings of the plane diffraction grating, the diffracted beam is diffracted again by the plane diffraction grating, then the beam condensed by a second collimator is allowed to pass through an exit slit.
    • 公开了单色仪和光谱测量方法,其中通过平面衍射光栅衍射由第一准直仪转换成平行光束的测量光束,然后衍射光束返回,使得返回之后的衍射光束与返回之前的衍射光束分离 沿着平面衍射光栅的排列,衍射光束再次被平面衍射光栅衍射,则允许由第二准直器聚焦的光束通过出射狭缝。
    • 8. 发明授权
    • Optical sampling apparatus
    • 光采样装置
    • US07760344B2
    • 2010-07-20
    • US12036303
    • 2008-02-25
    • Shigeki Nishina
    • Shigeki Nishina
    • G01J11/00
    • G01J11/00G02F1/3536
    • Provided is an optical sampling apparatus that samples light to be measured having a pulse waveform, including a sampling light output section that outputs a first sampling light and a second sampling light, both having pulse waveforms of a spectrum different from that of the light to be measured; a first sampling section that includes a first nonlinear optical medium, which causes a nonlinear optical effect by causing at least a portion of the light to be measured and the first sampling light to pass therethrough and outputs light generated by the nonlinear optical effect, and that outputs at least a portion of the light generated by the nonlinear optical effect as a first output light; and a second sampling section that includes a second nonlinear optical medium, which causes a nonlinear optical effect by causing at least a portion of the first output light and the second sampling light to pass therethrough with a temporal overlap in order to output light generated by the nonlinear optical effect, and that outputs at least a portion of the light generated by the nonlinear optical effect as a second output light.
    • 提供一种光采样装置,其对具有脉波波形的被测量光进行采样,该采样光输出部分输出具有不同于光的光谱的脉冲波形的第一采样光和第二采样光 测量; 第一采样部分,其包括第一非线性光学介质,其通过使待测量的光的至少一部分和第一采样光通过并且输出由非线性光学效应产生的光而引起非线性光学效应,并且 将由非线性光学效果产生的光的至少一部分输出为第一输出光; 以及第二采样部分,其包括第二非线性光学介质,其通过使第一输出光和第二采样光的至少一部分通过其中的时间重叠而引起非线性光学效应,以便输出由 非线性光学效应,并且将由非线性光学效应产生的光的至少一部分输出为第二输出光。
    • 9. 发明授权
    • Light-measuring device for accurate and continuous measurement of light
intensity
    • 光度测量装置,用于准确连续地测量光强度
    • US5969809A
    • 1999-10-19
    • US126781
    • 1998-07-31
    • Shigeki Nishina
    • Shigeki Nishina
    • G01J1/20G01J1/42G01J1/44G01J1/40
    • G01J1/20G01J1/42G01J1/44
    • A light-measuring device is disclosed for continuously and accurately measuring the intensity of light beams of from low intensity to high intensity. The intensity of a light beam to be measured is measured by a photodiode. A bias voltage is applied to the photodiode by a bias power source to improve the saturation characteristic. When the measured light beam is of high intensity, an analog switch and a photo MOS relay are switched on. When measuring a light beam with medium intensity, only the analog switch is turned off and a bias voltage is not applied to the photodiode. When measuring a light beam with low intensity, the bias voltage is not applied to the photodiode by switching off the photo MOS relay.
    • 公开了一种用于连续且精确地测量从低强度到高强度的光束的强度的光测量装置。 通过光电二极管测量待测光束的强度。 通过偏置电源将偏置电压施加到光电二极管以提高饱和特性。 当测量光束强度高时,模拟开关和光电MOS继电器接通。 当测量中等强度的光束时,只有模拟开关被关闭,偏置电压不会施加到光电二极管。 当测量低强度的光束时,通过关闭光电MOS继电器,偏置电压不会施加到光电二极管。
    • 10. 发明授权
    • Michelson interferometer including a non-polarizing beam splitter
    • 包括非偏振分束器的迈克尔逊干涉仪
    • US5867271A
    • 1999-02-02
    • US491907
    • 1995-07-14
    • Isao TokumotoShigeki Nishina
    • Isao TokumotoShigeki Nishina
    • G01J3/453G01B9/02
    • G01J3/4535
    • A light power spectrum is accurately measured, in spite of the polarized light-dependency of the non-polarizing beam splitter 12. Incident light 11 is separated by a polarizing/separating element 31 into orthogonal polarized light components 11a and 11b. The orthogonal polarized light components have their polarizing directions rotated by 45 degrees in opposite directions with respect to their P wave components and S wave components at the reflecting/transmitting face of the non-polarizing beam splitter. The reflected and transmitted from the non-polarizing beam splitter 12 are reflected by a stationary reflector 16 and a moving reflector 17 back to the non-polarizing beam splitter 12 and are recombined to interfere with each other at the reflecting/transmitting face of the non-polarizing beam splitter. The resulting interference lights are received by a common light-receiver.
    • PCT No.PCT / JP94 / 01905 Sec。 371 1995年7月14日第 102(e)日期1995年7月14日PCT 1994年11月11日提交PCT尽管非偏振分束器12具有偏振光依赖性,但是准确地测量了光功率谱。入射光11被偏振/ 将元件31分离为正交偏振光分量11a和11b。 正交偏振光分量的偏振方向相对于非偏振光束分离器的反射/透射面处的P波分量和S波分量在相反方向上旋转45度。 来自非偏振光束分离器12的反射和透射被固定反射器16和移动反射器17反射回非偏振光束分离器12,并被重新组合以在非偏振光束分离器12的反射/透射面处彼此干涉 极化分束器。 所产生的干扰光由普通的光接收器接收。