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    • 1. 发明授权
    • Imaging polarimetry
    • 成像偏光仪
    • US07336360B2
    • 2008-02-26
    • US11352458
    • 2006-02-13
    • Kazuhiko OkaTomohiro MizunoAtsushi TaniguchiHiroshi Okabe
    • Kazuhiko OkaTomohiro MizunoAtsushi TaniguchiHiroshi Okabe
    • G01J4/00
    • G02B27/281G01J4/04
    • To effectively reduce a measurement error in a parameter indicating two-dimensional spatial distribution of a state of polarization generated by variations in retardation of a birefringent prism pair due to a temperature change or other factors, while holding a variety of properties of an imaging polarimetry using the birefringent prism pair. By noting that reference phase functions φ1(x, y) and φ2(x, y) are obtained by solving an equation from each vibration component contained in an intensity distribution I(x, y), the reference phase functions φ1(x, y) and φ2(x, y) are calibrated concurrently with measurement of two-dimensional spatial distribution S0(x, y), S1(x, y), S2(x, y), and S3(x, y) of Stokes parameters.
    • 为了有效地降低由于温度变化或其他因素导致的双折射棱镜对的延迟变化产生的偏振态的二维空间分布的参数的测量误差,同时保持成像偏振法的各种性质,使用 双折射棱镜对。 通过注意到通过求解包含在强度分布中的每个振动分量的方程来获得参考相位函数phi1(x,y)和φi2(x,y) I(x,y),参考相位函数phi <1>(x,y)和phi <2>(x,y)与二维空间 (x,y),S&lt; 1&gt;(x,y),S 2(x,y)以及S 3 (x,y)。
    • 2. 发明申请
    • Imaging polarimetry
    • 成像偏光仪
    • US20070030551A1
    • 2007-02-08
    • US11352458
    • 2006-02-13
    • Kazuhiko OkaTomohiro MizunoAtsushi TaniguchiHiroshi Okabe
    • Kazuhiko OkaTomohiro MizunoAtsushi TaniguchiHiroshi Okabe
    • G02B26/00G02F1/01
    • G02B27/281G01J4/04
    • To effectively reduce a measurement error in a parameter indicating two-dimensional spatial distribution of a state of polarization generated by variations in retardation of a birefringent prism pair due to a temperature change or other factors, while holding a variety of properties of an imaging polarimetry using the birefringent prism pair. By noting that reference phase functions φ1(x, y) and φ2(x, y) are obtained by solving an equation from each vibration component contained in an intensity distribution I(x, y), the reference phase functions φ1(x, y) and φ2(x, y) are calibrated concurrently with measurement of two-dimensional spatial distribution S0(x, y), S1(x, y), S2(x, y), and S3(x, y) of Stokes parameters.
    • 为了有效地降低由于温度变化或其他因素导致的双折射棱镜对的延迟变化产生的偏振态的二维空间分布的参数的测量误差,同时保持成像偏振法的各种性质,使用 双折射棱镜对。 通过注意到通过求解包含在强度分布中的每个振动分量的方程来获得参考相位函数phi1(x,y)和φi2(x,y) I(x,y),参考相位函数phi <1>(x,y)和phi <2>(x,y)与二维空间 (x,y),S&lt; 1&gt;(x,y),S 2(x,y)和S 3 (x,y)。
    • 3. 发明授权
    • Spectroscopic polarimetry
    • 光谱极化法
    • US07623236B2
    • 2009-11-24
    • US11329389
    • 2006-01-11
    • Kazuhiko OkaAtsushi TaniguchiHiroshi Okabe
    • Kazuhiko OkaAtsushi TaniguchiHiroshi Okabe
    • G01J4/00
    • G01J4/04
    • To effectively reduce a measurement error in a parameter indicating a state of spectroscopic polarization generated by variations in retardation of a retarder due to a temperature change or other factors, while holding a variety of properties of a channeled spectroscopic polarimeter. By noting that reference phase functions φ1(σ) and φ2(σ) are obtained by solving an equation from each vibration component contained in a channeled spectrum P(σ), the reference phase functions φ1(σ) and φ2(σ) are calibrated concurrently with measurement of spectrometric Stokes parameters S0(σ), S1(σ), S2(σ), and S3(σ).
    • 为了有效地降低由于温度变化引起的延迟器的延迟的变化而产生的光谱极化的状态的参数的测量误差,或其他因素,同时保持通道的分光偏振计的各种特性。 通过从通道谱P(sigma)中包含的每个振动分量求解方程得到参考相函数phi1(sigma)和phi2(sigma),参考相函数phi1(sigma)和phi2(sigma)被校准 同时测量光谱学斯托克斯参数S0(sigma),S1(sigma),S2(sigma)和S3(sigma)。
    • 4. 发明申请
    • Spectroscopic polarimetry
    • 光谱极化法
    • US20060170921A1
    • 2006-08-03
    • US11329389
    • 2006-01-11
    • Kazuhiko OkaAtsushi TaniguchiHiroshi Okabe
    • Kazuhiko OkaAtsushi TaniguchiHiroshi Okabe
    • G01J4/00
    • G01J4/04
    • To effectively reduce a measurement error in a parameter indicating a state of spectroscopic polarization generated by variations in retardation of a retarder due to a temperature change or other factors, while holding a variety of properties of a channeled spectroscopic polarimeter. By noting that reference phase functions φ1(σ) and φ2(σ) are obtained by solving an equation from each vibration component contained in a channeled spectrum P(σ), the reference phase functions φ1(σ) and φ2(σ) are calibrated concurrently with measurement of spectrometric Stokes parameters S0(σ), S1(σ), S2(σ), and S3(σ).
    • 为了有效地降低由于温度变化引起的延迟器的延迟的变化而产生的光谱极化的状态的参数的测量误差,或其他因素,同时保持通道的分光偏振计的各种特性。 通过注意到通过从通道谱P(sigma)中包含的每个振动分量求解方程来获得参考相位函数phi1(sigma)和φi2(sigma) ,参考相位函数phi1(sigma)和phi2(sigma)与光谱测量斯托克斯参数S 0(sigma)的测量同时校准 ),S 1(sigma),S 2(sigma)和S 3(sigma)。
    • 5. 发明授权
    • Measuring apparatus, measuring method, and characteristic measurement unit
    • 测量装置,测量方法和特征测量单元
    • US07796257B2
    • 2010-09-14
    • US12087663
    • 2006-12-27
    • Yukitoshi OtaniKazuhiko OkaToshitaka WakayamaAtsushi Taniguchi
    • Yukitoshi OtaniKazuhiko OkaToshitaka WakayamaAtsushi Taniguchi
    • G01J4/00
    • G01N21/21G01J4/04
    • A measuring apparatus includes a light intensity information acquisition section 40 that acquires light intensity information relating to a measurement light containing a given band component, the measurement light having been modulated by optical elements included in an optical system 10 and a measurement target (or a sample 100), and a calculation section 50 that calculates at least one matrix element of a Mueller matrix that indicates the optical characteristics of the measurement target based on the light intensity information relating to the measurement light and a theoretical expression for the light intensity of the measurement light. The light intensity information acquisition section 40 acquires the light intensity information relating to a plurality of the measurement lights obtained from the optical system 10 by changing setting of a principal axis direction of at least one of the optical elements. The calculation section 50 performs a carrier amplitude coefficient calculation process, and a matrix element calculation process that calculates the at least one matrix element based on a carrier amplitude coefficient and the theoretical expression for the carrier amplitude coefficient including the at least one matrix element.
    • 测量装置包括光强度信息获取部分40,其获取与包含给定频带分量的测量光有关的光强度信息,测量光已被包括在光学系统10中的光学元件和测量对象(或样品 100),以及计算部50,其基于与测量光有关的光强度信息和测量光强度的理论表达式,计算指示测量对象的光学特性的Mueller矩阵的至少一个矩阵元素 光。 光强度信息获取部40通过改变至少一个光学元件的主轴方向的设定来获取与从光学系统10获得的多个测量光有关的光强度信息。 计算部分50执行载波幅度系数计算处理和基于载波幅度系数和包括至少一个矩阵元素的载波幅度系数的理论表达式来计算至少一个矩阵元素的矩阵元素计算处理。
    • 7. 发明申请
    • Spectroscopic polarimetry
    • 光谱极化法
    • US20060238759A1
    • 2006-10-26
    • US11388205
    • 2006-03-24
    • Hiroshi OkabeKenichi MatobaKazuhiko Oka
    • Hiroshi OkabeKenichi MatobaKazuhiko Oka
    • G01J4/00
    • G01J4/04G01J3/447
    • In the channeled spectroscopic polarimetry, a measurement error of a parameter showing a spectropolarization characteristic of a sample is effectively removed, the error being generated by various variations in retardation of a retarder depending upon the state of the sample. With attention being focused on that the retardation of the retarder may be kept constant by stabilization of an incident direction of light that transmits through the retarder, the retarder was arranged on the light source side with respect to the sample so as to effectively remove an influence relative to a measurement error, such as variations in direction of a light ray due to the sample.
    • 在通道光谱极化法中,有效地消除了示出样品的分光偏振特性的参数的测量误差,该误差是由取决于样品状态的延迟器的延迟的各种变化产生的。 关注的是通过使通过延迟器透射的光的入射方向的稳定化可以使延迟器的延迟保持恒定,延迟器相对于样品被布置在光源侧,以便有效地消除影响 相对于测量误差,例如由于样品导致的光线的方向的变化。
    • 8. 发明申请
    • Measuring Apparatus, Measuring Method, and Characteristic Measurement Unit
    • 测量装置,测量方法和特性测量单元
    • US20090051916A1
    • 2009-02-26
    • US12087663
    • 2006-12-27
    • Yukitoshi OtaniKazuhiko OkaToshitaka WakayamaAtsushi Taniguchi
    • Yukitoshi OtaniKazuhiko OkaToshitaka WakayamaAtsushi Taniguchi
    • G01J4/00
    • G01N21/21G01J4/04
    • A measuring apparatus includes a light intensity information acquisition section 40 that acquires light intensity information relating to a measurement light containing a given band component, the measurement light having been modulated by optical elements included in an optical system 10 and a measurement target (or a sample 100), and a calculation section 50 that calculates at least one matrix element of a Mueller matrix that indicates the optical characteristics of the measurement target based on the light intensity information relating to the measurement light and a theoretical expression for the light intensity of the measurement light. The light intensity information acquisition section 40 acquires the light intensity information relating to a plurality of the measurement lights obtained from the optical system 10 by changing setting of a principal axis direction of at least one of the optical elements. The calculation section 50 performs a carrier amplitude coefficient calculation process, and a matrix element calculation process that calculates the at least one matrix element based on a carrier amplitude coefficient and the theoretical expression for the carrier amplitude coefficient including the at least one matrix element.
    • 测量装置包括光强度信息获取部分40,其获取与包含给定频带分量的测量光有关的光强度信息,测量光已被包括在光学系统10中的光学元件和测量对象(或样品 100),以及计算部50,其基于与测量光有关的光强度信息和测量光强度的理论表达式,计算指示测量对象的光学特性的Mueller矩阵的至少一个矩阵元素 光。 光强度信息获取部40通过改变至少一个光学元件的主轴方向的设定来获取与从光学系统10获得的多个测量光有关的光强度信息。 计算部分50执行载波幅度系数计算处理和基于载波幅度系数和包括至少一个矩阵元素的载波幅度系数的理论表达式来计算至少一个矩阵元素的矩阵元素计算处理。