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    • 8. 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)。
    • 10. 发明授权
    • Correction of spectra for stray radiation
    • 杂散辐射光谱校正
    • US5428558A
    • 1995-06-27
    • US168800
    • 1993-12-17
    • Jerry E. CahillAlan M. GanzPaul SavianoDavid TracyYongdong Wang
    • Jerry E. CahillAlan M. GanzPaul SavianoDavid TracyYongdong Wang
    • G01J3/02G01J3/28G01N21/27G01D18/00
    • G01J3/28G01J2003/2866
    • A method and apparatus are provided for correction of spectra for stray radiation in a spectrometric instrument, involving a sequence of steps as follows. Spectral patterns are obtained with the instrument initially for monochromatic radiation at a plurality of selected calibration wavelengths. By computer program, the peak profile at the calibration wavelength in each pattern is replaced with a substitute based on the remaining pattern. The resulting data are interpolated to effect values denoted "stray proportions" for the ordered wavelengths of the instrument. Spectral data at each ordered wavelength are obtained with the instrument for a sample, and multiplied in the computer program by stray proportions for corresponding wavelengths to effect further sets of values denoted "stray portions" that are identified to the ordered wavelengths. Each set is identified to one of the wavelength increments of the instrument across the spectral range. In each set, the stray portions for the ordered wavelengths are summed. The total for each wavelength increment is subtracted from the original sample data for the increment to effect spectral data corrected for stray.
    • 提供了一种用于校正光谱仪器中杂散辐射的光谱的方法和装置,涉及如下的一系列步骤。 在多个选定的校准波长下,仪器最初用于单色辐射获得光谱图案。 通过计算机程序,每个模式中校准波长处的峰值曲线被替换为基于剩余模式的替代。 内插所得数据以对仪器的有序波长表示为“杂散比”的值。 用样品的仪器获得每个有序波长的光谱数据,并在计算机程序中乘以相应波长的杂散比例,以实现被标识为有序波长的标记为“杂散部分”的另外一组值。 每个组被识别为跨越光谱范围的仪器的波长增量之一。 在每组中,将有序波长的杂散部分相加。 从原始采样数据中减去每个波长增量的总和,以增加修正为杂散的光谱数据。