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    • 1. 发明授权
    • Thin film temperature measurement using optical absorption edge wavelength
    • 使用光吸收边缘波长的薄膜温度测量
    • US08786841B2
    • 2014-07-22
    • US13378788
    • 2010-06-21
    • Darryl BarlettCharles A. Taylor, IIBarry D. Wissman
    • Darryl BarlettCharles A. Taylor, IIBarry D. Wissman
    • G01N21/00G01N21/47
    • H01L21/67248H01L22/12
    • A technique for determining the temperature of a sample including a semiconductor film 20 having a measurable optical absorption edge deposited on a transparent substrate 22 of material having no measurable optical absorption edge, such as a GaN film 20 deposited on an Al2O3 substrate 22 for blue and white LEDs. The temperature is determined in realtime as the film 20 grows and increases in thickness. A spectra based on the diffusely scattered light from the film 20 is produced at each incremental thickness. A reference division is performed on each spectra to correct for equipment artifacts. The thickness of the film 20 and an optical absorption edge wavelength value are determined from the spectra. The temperature of the film 20 is determined as a function of the optical absorption edge wavelength and the thickness of the film 20 using the spectra, a thickness calibration table, and a temperature calibration table.
    • 一种用于确定样品的温度的技术,其包括具有沉积在不具有可测量的光吸收边缘的材料的透明基板22上的可测量的光吸收边缘的半导体膜20,例如沉积在用于蓝色的Al 2 O 3衬底22上的GaN膜20,以及 白色LED。 当膜20生长并且厚度增加时,温度是实时测定的。 在每个增量厚度下产生基于来自膜20的漫散射光的光谱。 在每个光谱上执行参考分区以校正设备伪像。 从光谱确定膜20的厚度和光吸收边缘波长值。 使用光谱,厚度校准表和温度校准表,确定膜20的温度作为光吸收边缘波长和膜20的厚度的函数。
    • 2. 发明申请
    • THIN FILM TEMPERATURE MEASUREMENT USING OPTICAL ABSORPTION EDGE WAVELENGTH
    • 使用光学吸收边缘波长的薄膜温度测量
    • US20120133934A1
    • 2012-05-31
    • US13378788
    • 2010-06-21
    • Darryl BarlettCharles A. Taylor, IIBarry D. Wissman
    • Darryl BarlettCharles A. Taylor, IIBarry D. Wissman
    • G01J3/28G01J5/00
    • H01L21/67248H01L22/12
    • A technique for determining the temperature of a sample including a semiconductor film 20 having a measurable optical absorption edge deposited on a transparent substrate 22 of material having no measurable optical absorption edge, such as a GaN film 20 deposited on an Al2O3 substrate 20 for blue and white LEDs. The temperature is determined in real-time as the film 20 grows and increases in thickness. A spectra based on the diffusely scattered light from the film 20 is produced at each incremental thickness. A reference division is performed on each spectra to correct for equipment artifacts. The thickness of the film 20 and an optical absorption edge wavelength value are determined from the spectra. The temperature of the film 20 is determined as a function of the optical absorption edge wavelength and the thickness of the film 20 using the spectra, a thickness calibration table, and a temperature calibration table.
    • 一种用于确定样品的温度的技术,包括沉积在不具有可测量的光吸收边缘的材料的透明基板22上的可测量的光吸收边缘的半导体膜20,例如沉积在用于蓝色的Al 2 O 3衬底20上的GaN膜20,以及 白色LED。 随着膜20的生长和厚度的增加,实时测定温度。 在每个增量厚度下产生基于来自膜20的漫散射光的光谱。 在每个光谱上执行参考分区以校正设备伪像。 从光谱确定膜20的厚度和光吸收边缘波长值。 使用光谱,厚度校准表和温度校准表,确定膜20的温度作为光吸收边缘波长和膜20的厚度的函数。
    • 3. 发明授权
    • Curvature/tilt metrology tool with closed loop feedback control
    • 具有闭环反馈控制的曲率/倾斜计量工具
    • US07391523B1
    • 2008-06-24
    • US10858358
    • 2004-06-01
    • Charles A. Taylor, IIDarryl BarlettDouglas PerryRoy Clarke
    • Charles A. Taylor, IIDarryl BarlettDouglas PerryRoy Clarke
    • G01B11/24
    • G01B11/2522
    • Apparatus for quantitatively measuring the curvature and/or relative tilt of large surfaces wherein a small array of parallel laser beams, each separated by a known distance, reflect from the surface of a sample and fall upon a feedback controlled front-surface steering mirror to a detector that measures both the change in separation of the reflected beams and the spatial translation of the entire array on the detector. The sample surface is translated beneath or in front of the fixed laser array by means of a computer controlled stage or other apparatus to create a 1-dimensional line scan or 2-dimensional map of both bow and relative tilt of the sample surface. A computer-driven, feedback-controlled steering mirror compensates for varying sample tilt by precisely realigning the reflected laser array onto the detector as the sample is translated. The apparatus also utilizes a laser with intensity feedback control to continuously optimize the reflected laser power for varying surface reflectivity as the sample is translated. This combination provides a means to quantitatively measure curvature and relative tilt of sample areas much larger than the actual laser beam array size.
    • 用于定量测量大表面的曲率和/或相对倾斜度的装置,其中每一个分开一段已知距离的平行激光束阵列从样品的表面反射并落在反馈控制的前表面导向镜上, 检测器测量反射光束的分离变化和检测器上整个阵列的空间平移。 样品表面借助于计算机控制级或其它装置在固定激光器阵列下方或前方平移,以产生样品表面的弓形和相对倾斜的一维线扫描或二维图。 计算机驱动的反馈控制的转向镜通过在反射样本被翻译时将反射的激光器阵列精确地重新配置到检测器上来补偿不同的样品倾斜。 该设备还利用具有强度反馈控制的激光器来连续优化反射激光功率,以在样品平移时改变表面反射率。 该组合提供了一种用于定量测量样品区域的曲率和相对倾斜度的方法,该样品区域远大于实际的激光束阵列尺寸。