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    • 2. 发明申请
    • Correction of Chemical Image Collected Using ATR Through Germanium Hemisphere
    • 使用ATR通过锗半球收集的化学图像的校正
    • US20120259599A1
    • 2012-10-11
    • US13084261
    • 2011-04-11
    • Francis J. DECKFederico IZZIAKoichi Nishikida
    • Francis J. DECKFederico IZZIAKoichi Nishikida
    • G06F7/60G06G7/48
    • G06T5/006G06F17/5009G06T2207/10056G06T2207/30136
    • A method and corresponding apparatus provide correction of chemical images collected with a germanium hemisphere ATR microscope. A modeled is developed for rays passing through a simulated germanium (Ge) hemisphere attenuated total reflection (ATR) microscope. The model determines a data set for rays reaching the detector plane. Movement of the hemisphere is simulated along a first axis between each data set determination. A calculated background spectrum is produced by multiplying the percentage of rays by a background spectrum to produce a calculated background spectrum. A real Ge hemisphere ATR microscope having parameters that substantially match those of the simulated Ge hemisphere microscope is then used to collect a chemical image of a sample that is in contact with the Ge hemisphere. The collected image is then corrected to produce a corrected chemical image.
    • 一种方法和相应的装置提供用锗半球ATR显微镜收集的化学图像的校正。 模拟的射线通过模拟锗(Ge)半球衰减全反射(ATR)显微镜。 该模型确定到达检测器平面的光线的数据集。 在每个数据集确定之间沿着第一轴模拟半球的运动。 通过将光线的百分比乘以背景谱产生计算的背景谱产生计算的背景谱。 然后使用具有与模拟的Ge半球显微镜基本匹配的参数的真实Ge半球ATR显微镜来收集与Ge半球接触的样品的化学图像。 然后校正收集的图像以产生校正的化学图像。
    • 4. 发明授权
    • Correction of chemical image collected using ATR through germanium hemisphere
    • 使用ATR通过锗半球收集的化学图像的校正
    • US08521491B2
    • 2013-08-27
    • US13084261
    • 2011-04-11
    • Francis J. DeckKoichi NishikidaFederico Izzia
    • Francis J. DeckKoichi NishikidaFederico Izzia
    • G06G7/48
    • G06T5/006G06F17/5009G06T2207/10056G06T2207/30136
    • A method and corresponding apparatus provide correction of chemical images collected with a germanium hemisphere ATR microscope. A model is developed for rays passing through a simulated germanium (Ge) hemisphere attenuated total reflection (ATR) microscope. The model determines a data set for rays reaching the detector plane. Movement of the hemisphere is simulated along a first axis between each data set determination. A calculated background spectrum is produced by multiplying the percentage of rays by a background spectrum to produce a calculated background spectrum. A real Ge hemisphere ATR microscope having parameters that substantially match those of the simulated Ge hemisphere microscope is then used to collect a chemical image of a sample that is in contact with the Ge hemisphere. The collected image is then corrected to produce a corrected chemical image.
    • 一种方法和相应的装置提供用锗半球ATR显微镜收集的化学图像的校正。 开发了通过模拟锗(Ge)半球衰减全反射(ATR)显微镜的射线的模型。 该模型确定到达检测器平面的光线的数据集。 在每个数据集确定之间沿着第一轴模拟半球的运动。 通过将光线的百分比乘以背景谱产生计算的背景谱产生计算的背景谱。 然后使用具有与模拟的Ge半球显微镜基本匹配的参数的真实Ge半球ATR显微镜来收集与Ge半球接触的样品的化学图像。 然后校正收集的图像以产生校正的化学图像。
    • 6. 发明申请
    • Optical Resonance Analysis System
    • 光学共振分析系统
    • US20060262313A1
    • 2006-11-23
    • US11460932
    • 2006-07-28
    • Dar BahattJerry CahillKoichi NishikidaEnrico PicozzaPaul SavianoDavid TracyYongdong Wang
    • Dar BahattJerry CahillKoichi NishikidaEnrico PicozzaPaul SavianoDavid TracyYongdong Wang
    • G01N21/55
    • G01N21/7703G01N21/553
    • An optical resonance analysis system comprising a sensor means (60) and an illumination means (400) for generating non-monochromatic illumination. The illumination means (400) further comprises a means for generating illumination at a plurality of angles, a lens system for projecting said illumination at said plurality of angles (390) and a dispersive device (380) for dispersing said illumination at each of said plurality of angles so that there is a correlation between said plurality of angles and the wavelengths of said illumination such that a resonance condition is generated on said sensor mean (60) for all wavelengths generated by said non-monochromatic source simultaneously. The analysis system also comprises a detection means (90) for detecting the reflected or transmitted illumination. Another embodiment comprises an anamorphic imaging means (120).
    • 一种光学共振分析系统,包括传感器装置(60)和用于产生非单色照明的照明装置(400)。 照明装置(400)还包括用于以多个角度产生照明的装置,用于以所述多个角度(390)投射所述照明的透镜系统和用于将所述照明分散在所述多个角度的分散装置(380) 的角度,使得在所述多个角度和所述照明的波长之间存在相关性,使得对于由所述非单色源同时产生的所有波长的所述传感器平均值(60)产生共振条件。 分析系统还包括用于检测反射或透射照明的检测装置(90)。 另一实施例包括变形成像装置(120)。
    • 8. 发明授权
    • Optical resonance analysis system
    • 光学共振分析系统
    • US06600563B1
    • 2003-07-29
    • US09486424
    • 2000-07-17
    • Dar BahattJerry E. CahillKoichi NishikidaEnrico G. PicozzaPaul G. SavianoDavid H. TracyYongdong Wang
    • Dar BahattJerry E. CahillKoichi NishikidaEnrico G. PicozzaPaul G. SavianoDavid H. TracyYongdong Wang
    • G01N2155
    • G01N21/7703G01N21/553
    • An optical resonance analysis system comprising a sensor means (60) and an illumination means (400) for generating non-monochromatic illumination. The illumination means (400) further comprises a means for generating illumination at a plurality of angles, a lens system for projecting said illumination at said plurality of angles (390) and a dispersive device (380) for dispersing said illumination at each of said plurality of angles so that there is a correlation between said plurality of angles and the wavelengths of said illumination such that a resonance condition is generated on said sensor mean (60) for all wavelengths generated by said non-monochromatic source simultaneously. The analysis system also comprises a detection means (90) for detecting the reflected or transmitted illumination. Another embodiment comprises an anamorphic imaging means (120).
    • 一种光学共振分析系统,包括传感器装置(60)和用于产生非单色照明的照明装置(400)。 照明装置(400)还包括用于以多个角度产生照明的装置,用于以所述多个角度(390)投射所述照明的透镜系统和用于将所述照明分散在所述多个角度的分散装置(380) 的角度,使得在所述多个角度和所述照明的波长之间存在相关性,使得对于由所述非单色源同时产生的所有波长的所述传感器平均值(60)产生共振条件。 分析系统还包括用于检测反射或透射照明的检测装置(90)。 另一实施例包括变形成像装置(120)。