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    • 4. 发明申请
    • Polarization mode dispersion measuring device, method, recording medium
    • 极化模式色散测量装置,方法,记录介质
    • US20050052638A1
    • 2005-03-10
    • US10491787
    • 2002-10-09
    • Takeshi OzekiTomoyu YamashitaMotoki Imamura
    • Takeshi OzekiTomoyu YamashitaMotoki Imamura
    • G01M11/02G01M11/00G01J4/00
    • G01M11/333G01M11/336
    • A polarization mode dispersion measuring device reduced in time required to measure polarization mode dispersion τPMD. A polarization controller (12) allows a first (second) incident light to apply a synthetic incident light to an object to be measured (30) in line with a p-polarization axis (s-polarization axis) in a polarization separator (16). Accordingly, the phase shift equivalent value (optical angle frequency differentiation) and amplitude equivalent value (square value) of a first incident light component (second incident light component) in an output from the polarization separator (16) measured by a first measuring unit (20a) (second measuring unit (20b)) are respectively the phase shift equivalent value and amplitude equivalent value of a first column T11, T21 (second column T12, T22) when the transfer function matrix of the object to be measured (30) is a 2×2 matrix to thereby allow a control unit (2) to determine the polarization mode dispersion r PMD of the object to be measured (30). Since there is no need of switching the orientation setting of light output from the polarization controller (12) with the setting left fixed, time required to measure polarization mode dispersion τPMD can be shortened.
    • 偏振模色散测量装置减少测量偏振模色散τPMD所需的时间。 偏振控制器(12)允许第一(第二)入射光根据偏振分离器(16)中的p偏振轴(s偏振轴)将合成入射光施加到待测量对象(30) 。 因此,由第一测量单元测量的偏振分离器(16)的输出中的第一入射光分量(第二入射光分量)的相移等效值(光学角度频率微分)和振幅等效值(平方值) 20a)(第二测量单元(20b))分别是当被测量对象(30)的传递函数矩阵为(30)时的第一列T11,T21(第二列T12,T22)的相移等效值和振幅当量值 2×2矩阵,从而允许控制单元(2)确定被测量物体的偏振模色散r PMD(30)。 由于不需要将固定的偏振控制器(12)的光的输出的取向设置切换,所以可以缩短测量偏振模色散τPMD所需的时间。
    • 5. 发明授权
    • Optical characteristic measuring apparatus, the method thereof and recording medium
    • 光学特性测量装置,其方法和记录介质
    • US06519028B2
    • 2003-02-11
    • US09900968
    • 2001-07-10
    • Eiji KimuraMotoki Imamura
    • Eiji KimuraMotoki Imamura
    • G01N2100
    • G01M11/335G01M11/333G01M11/338
    • An apparatus for measuring optical characteristics includes a variable-wavelength light source for generating a variable-wavelength light, having an identification waveform when the wavelength changes, the identification waveform being distinguishable from a normal waveform before and after the wavelength changes, an optical modulator for modulating the variable-wavelength light at a predetermined frequency and inputting it to an optical fiber; and an identification waveform detector for detecting the identification waveform of light transmitted through the optical fiber, wherein since the identification waveform detector detects when the waveform starts to change, it is possible to obtain synchronization between an incidence side and an exit side of the optical fiber. Accordingly, it is possible to obtain synchronization between an incidence side and an exit side of a device-under-test even if the wavelength of light source is continuously swept, whereby characteristics such as chromatic dispersion and the like can be measured.
    • 一种用于测量光学特性的装置包括:用于产生可变波长光的可变波长光源,当波长变化时具有识别波形,识别波形与波长变化前后的正常波形区分开;光学调制器, 以预定频率调制可变波长光并将其输入到光纤; 以及识别波形检测器,用于检测通过光纤传输的光的识别波形,其中由于识别波形检测器检测波形何时开始变化,可以获得光纤的入射侧和出射侧之间的同步 。 因此,即使光源的波长连续地扫过,也可以获得被测器件的入射侧和出射侧之间的同步,从而可以测量诸如色散等的特性。
    • 7. 发明授权
    • Electromagnetic wave measuring apparatus
    • 电磁波测量仪
    • US08053733B2
    • 2011-11-08
    • US12616992
    • 2009-11-12
    • Shigeki NishinaMotoki Imamura
    • Shigeki NishinaMotoki Imamura
    • G01J5/02
    • G01N21/3581
    • A desired spatial resolution upon a measurement can be attained by making an electromagnetic wave including a terahertz wave (frequency thereof is equal to or more than 0.01 [THz], and equal to or less than 100 [THz]) incident to a device under test. An electromagnetic wave measurement device includes an incident lens which makes an electromagnetic wave to be measured having a frequency equal to or more than 0.01 [THz] and equal to or less than 100 [THz] incident to a device under a test while decreasing a beam diameter of the electromagnetic wave to be measured, a scanning stage which rotates, about a line orthogonal to an optical axis of the incident lens as a rotational axis, the device under the test or the optical axis, and an electromagnetic wave detector which detects the electromagnetic wave to be measured which has transmitted through the device under the test, where a coordinate on the optical axis of a position which gives the minimum value d of the beam diameter is different from a coordinate on the optical axis of the rotational axis.
    • 测量时的期望空间分辨率可以通过使包含入射到被测器件的太赫兹波(其频率等于或大于0.01 [THz],等于或小于100 [THz])的电磁波来实现 。 电磁波测量装置包括入射透镜,该入射透镜使得测量的电磁波具有等于或大于在测试时入射到设备的0.01 [THz]且等于或小于100 [THz]的频率,同时减小光束 要测量的电磁波的直径,围绕与入射透镜的光轴正交的线作为旋转轴旋转的扫描台,被测装置或光轴的电磁波检测器,以及检测 通过测试中的装置传输的要测量的电磁波,其中给出光束直径的最小值d的位置的光轴上的坐标不同于旋转轴的光轴上的坐标。
    • 8. 发明申请
    • CARRIER AND ADHESION AMOUNT MEASURING APPARATUS, AND MEASURING METHOD, PROGRAM, AND RECORDING MEDIUM OF THE SAME
    • 载体和粘合量测量装置及其测量方法,程序和记录介质
    • US20110097649A1
    • 2011-04-28
    • US12608208
    • 2009-10-29
    • Motoki IMAMURAShigeki NISHINA
    • Motoki IMAMURAShigeki NISHINA
    • H01M4/64H01M4/88G06F19/00
    • G01N21/17G01N21/3504G01N21/3581
    • The present invention measures a quantity of attachment (such as density) of a material (such as catalyst and promoter) attached to a carrier. A carrier 1 includes attachment holes 12 to which a catalyst 24 attaches, and non-attachment holes 14 to which the catalyst 24 does not attach, where extension directions of the attachment holes 12 and the non-attachment holes 14 are parallel with each other (perpendicular to a first end surface 1a), and are opened on the first end surface 1a and a second end surface 1b. An attachment quantity measurement device includes an electromagnetic wave output device 2 that outputs a terahertz wave at a frequency equal to or more than 0.01 [THz] and equal to or less than 100 [THz] toward the carrier 1, an electromagnetic wave detector 4 that detects the terahertz wave which has transmitted through the carrier 1, a reference value deriving unit 7 that derives, based on a result detected by the electromagnetic wave detector 4, any one of an absorption rate, a group delay, and a dispersion of the terahertz wave in the non-attachment holes 14, and an attachment quantity deriving unit 8 that derives, based on the result detected by the electromagnetic wave detector 4 and the result derived by the reference value deriving unit 7, a weight or a density of the catalyst 24 present in the attachment holes 12.
    • 本发明测量附着于载体的材料(如催化剂和助催化剂)的附着量(如密度)。 载体1包括催化剂24附着的附接孔12和催化剂24未附着的未安装孔14,其中安装孔12和非安装孔14的延伸方向彼此平行( 垂直于第一端面1a),并且在第一端面1a和第二端面1b上开口。 安装量测量装置包括电磁波输出装置2,其以等于或大于0.01 [THz]且等于或小于100 [THz]的频率向载体1输出太赫兹波;电磁波检测器4,其 检测通过载波1发送的太赫兹波;基准值导出单元7,其基于由电磁波检测器4检测到的结果导出太赫兹的吸收率,群延迟和色散中的任何一个 基于由电磁波检测器4检测到的结果和由基准值导出单元7导出的结果导出催化剂的重量或密度的附着量导出单元8, 24存在于附接孔12中。
    • 9. 发明申请
    • ELECTROMAGNETIC WAVE MEASURING APPARATUS
    • 电磁波测量装置
    • US20110075127A1
    • 2011-03-31
    • US12616992
    • 2009-11-12
    • Shigeki NISHINAMotoki IMAMURA
    • Shigeki NISHINAMotoki IMAMURA
    • G01J3/00
    • G01N21/3581
    • A desired spatial resolution upon a measurement can be attained by making an electromagnetic wave including a terahertz wave (frequency thereof is equal to or more than 0.01 [THz], and equal to or less than 100 [THz]) incident to a device under test. An electromagnetic wave measurement device includes an incident lens which makes an electromagnetic wave to be measured having a frequency equal to or more than 0.01 [THz] and equal to or less than 100 [THz] incident to a device under a test while decreasing a beam diameter of the electromagnetic wave to be measured, a scanning stage which rotates, about a line orthogonal to an optical axis of the incident lens as a rotational axis, the device under the test or the optical axis, and an electromagnetic wave detector which detects the electromagnetic wave to be measured which has transmitted through the device under the test, where a coordinate on the optical axis of a position which gives the minimum value d of the beam diameter is different from a coordinate on the optical axis of the rotational axis.
    • 测量时的期望空间分辨率可以通过使包含入射到被测器件的太赫兹波(其频率等于或大于0.01 [THz],等于或小于100 [THz])的电磁波来实现 。 电磁波测量装置包括入射透镜,该入射透镜使得测量的电磁波具有等于或大于在测试时入射到设备的0.01 [THz]且等于或小于100 [THz]的频率,同时减小光束 要测量的电磁波的直径,围绕与入射透镜的光轴正交的线作为旋转轴旋转的扫描台,被测装置或光轴的电磁波检测器,以及检测 通过测试中的装置传输的要测量的电磁波,其中给出光束直径的最小值d的位置的光轴上的坐标不同于旋转轴的光轴上的坐标。
    • 10. 发明授权
    • Apparatus and method for measuring optical characteristics and recording medium
    • 用于测量光学特性和记录介质的装置和方法
    • US06433865B1
    • 2002-08-13
    • US09975557
    • 2001-10-12
    • Eiji KimuraMotoki ImamuraToshio KawazawaSatoru Nagumo
    • Eiji KimuraMotoki ImamuraToshio KawazawaSatoru Nagumo
    • G01N2100
    • G01M11/335G01M11/333G01M11/338
    • To provide an apparatus for measuring chromatic dispersion when modulating frequency of a variable wavelength light source is different from modulating frequency of a fixed wavelength light source for reference. This apparatus is provided with a variable wavelength light phase comparator 24 for obtaining a phase difference &phgr;x-&phgr;x′ between a variable wavelength light component and a signal having the first modulating frequency fmx, a fixed wavelength light phase comparator 25 for obtaining a phase difference between a phase difference &phgr;0-&phgr;0′ between a fixed wavelength light component and an electrical signal having the second modulating frequency fm0, a phase difference converter 26 for converting the phase difference &phgr;0-&phgr;0′ calculated by the fixed wavelength light phase comparator 25 into &phgr;ex, which corresponds to the first modulating frequency fmx, and a true phase difference calculator 27 for measuring a true phase difference &phgr; between the phase difference &phgr;x-&phgr;x′ calculated by the variable wavelength light phase comparator 24, and the converted result &phgr;ex of phase difference converter 26, and obtains the true phase difference &phgr; from which an affect of contraction/extension of a DUT 30 is removed when the first modulating frequency fmx and the second modulating frequency fm0 are different, thereby measuring wave dispersion.
    • 提供一种用于测量可变波长光源的调制频率时的色散的装置与用于参考的固定波长光源的调制频率不同。该装置设置有可变波长光相位比较器24,用于获得相位差phix- 可变波长光分量和具有第一调制频率fmx的信号之间的“phix”,固定波长光相位比较器25,用于获得固定波长光分量与具有第一调制频率fmx的电信号之间的相位差phi0-phi0'之间的相位差 第二调制频率fm0,用于将由固定波长光相位比较器25计算出的相位差phi0-phi0'转换成对应于第一调制频率fmx的phiex的相位差转换器26和用于测量 相位差phix-phix'ca之间的真相位差phi 由可变波长光相位比较器24计算的相位差转换器26的转换结果phix,并获得当第一调制频率fmx和 第二调制频率fm0不同,从而测量波分散。