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Scatterometer basing on a STAR GEM idea for optical measurements of microlenses

机译:基于STAR GEM理念的散射仪,用于微透镜的光学测量

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It is important to measure both reflectance (R ) and transmittance (T ) with the same accuracy. But many commercial accessories are exchanged by themselves or a sample is replaced on the other position in one accessory, when the reflection measurement is changed from the transmission measurement, so that it is impossible to measure reflectance and transmittance with the same accuracy. Accordingly the absorptance (A=1-R-T ) of the sample is not a sufficient index to evaluate the optical properties. A new scatterometer, which overcomes the defect, has been developed in AIST. It consists mainly of two ellipsoidal mirrors and a new detection system, which is composed of a hemispherical lens, a fiber optic taper and a CCD camera. These mirrors are a belt-shape and a quarter ellipsoidal mirrors with two focal points and are combined such that each focal point is a common focal point, on which the sample is placed. A rotating mirror is set on a remaining focal point of the belt-shape mirror. Each arrangement, where the rotating mirror looks at the upper or lower arm of the belt-shape mirror, is for the transmission or reflection measurement, respectively. The center of the hemispherical lens in the detection system is set on a remaining focal point of the quarter mirror, the incident plane of the fiber optic taper coincides with the image plane of the hemispherical lens and the outgoing plane of the fiber optic taper is in contact with the CCD camera. A clear image can be obtained using this detection system. The absolute values of the reflectance and transmittance and the light distributions of the reflection and transmission of the micro-ball-lenses, whose radii were 0.75, 1, 2.5 and 4.8mm, were measured. The systematic errors of our scatterometer are briefly discussed.© (2012) COPYRIGHT Society of Photo-Optical Instrumentation Engineers (SPIE). Downloading of the abstract is permitted for personal use only.
机译:重要的是要以相同的精度测量反射率(R)和透射率(T)。但是,当反射测量值与透射率测量值发生变化时,许多商业附件会自行更换,或者在一个附件中的另一个位置上更换样品,因此不可能以相同的精度测量反射率和透射率。因此,样品的吸收率(A = 1-R-T)不足以评价光学性能。 AIST已开发出一种克服了这一缺陷的新型散射仪。它主要由两个椭球面镜和一个新的检测系统组成,该系统由半球透镜,光纤锥和CCD摄像机组成。这些反射镜是带状的且具有两个焦点的四分之一椭圆形反射镜,并且组合在一起使得每个焦点都是放置样品的公共焦点。在带状镜的其余焦点上设置有旋转镜。旋转镜对准带状镜的上臂或下臂的每种布置分别用于透射或反射测量。检测系统中半球透镜的中心位于四分之一镜的剩余焦点上,光纤锥的入射平面与半球透镜的像平面重合,光纤锥的出射平面位于与CCD相机接触。使用该检测系统可以获得清晰的图像。测量半径为0.75、1、2.5和4.8mm的微球透镜的反射率和透射率的绝对值以及反射和透射的光分布。简要讨论了我们的散射仪的系统误差。©(2012)COPYRIGHT光电仪器工程师协会(SPIE)。摘要的下载仅允许个人使用。

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