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INFRARED TECHNIQUE FOR MEASURING A PARAMETER EG THICKNESS OF A THIN FILM
INFRARED TECHNIQUE FOR MEASURING A PARAMETER EG THICKNESS OF A THIN FILM
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机译:红外技术用于测量薄膜的参数EG厚度
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1348978 Photoelectric reflection and tranmission measurements BRUN SENSOR SYSTEMS Inc 5 Nov 1970 [5 Nov 1969] 51147/70 Heading G1A [Also in Division G3] In a dual beam reflection or transmission measurement apparatus for measuring a parameter, e.g. the thickness d, of an infrared transparent film C and in which the film is irradiated alternately by a beam which is strongly absorbed by the film and an unabsorbed reference beam the beams are both divergent so that the interference pattern caused by radiation being reflected at two different sufaces, B 1 and C 1 is substantially the same for each wavelength. To achieve this, the maximum allowable difference ## between the wavelengths is given by where # is the average wavelength. The alternating beams are derived from a single source having a collimating lens system and a rotating filter wheel. The circuitry of the detector 11, which may be a photo-voltaic cell or photoresistor, is synchronized with the motion of the filter wheel to provide on a meter 17 the ratio of the two detected beam intensities. The two alternating beams need not be strictly monochromatic. If each beam consists of a band of wavelengths centred on # and #2 respectively, then to avoid interference errors the minimum wavelength spread of each band is governed by the relationship In this embodiment, the film may be irradiated at a single angle of incidence or over a range of such angles, as previously described. Interference errors in transmission measurements may also be minimised using the method of the invention Fig. 2 (not shown). The output from the analyser circuit 12 may be supplied to a process control unit for controlling the thickness of a film applied to a moving substrate B.
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机译:1348978光电反射和透射测量BRUN SENSOR SYSTEMS Inc. 1970年11月5日[1969年11月5日] 51147/70标题G1A [也在G3分区中]在双光束反射或透射测量设备中,用于测量参数,例如:厚度为d的红外透明膜C,其中该膜被被该膜强烈吸收的光束和未吸收的参考光束交替照射,这两个光束均发散,因此由辐射引起的干涉图在两个位置反射不同的表面,对于每个波长,B 1和C 1基本上相同。为了实现这一点,波长之间的最大允许差值##由下式给出:其中#是平均波长。交变光束来自具有准直透镜系统和旋转滤镜轮的单一光源。可以是光伏电池或光敏电阻的检测器11的电路与滤光轮的运动同步,以在仪表17上提供两个检测到的光束强度之比。两个交替光束不必严格地是单色的。如果每个光束由分别以#和#2为中心的一个波长带组成,则为避免干扰错误,每个带的最小波长扩展由以下关系控制:在此实施例中,可以以单个入射角或如前所述,在这样的角度范围内。使用图2的本发明方法(未示出)也可以使传输测量中的干扰误差最小。可以将分析器电路12的输出提供给处理控制单元,以控制施加到移动基板B上的膜的厚度。
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