Abstract:
PURPOSE: A phase sensitivity determining method and an apparatus thereof are provided to determine the phase delay of an accelerometer by analyzing an interferential signal acquired through a single optical detector. CONSTITUTION: A beam splitter(400) partitions a laser generated in a laser generator(300). A fixed mirror(500) radiates a reflected first split laser to the beam splitter. An accelerometer(100) radiates a reflected second split laser to the beam splitter. An optical detector measures an interference signal between the first split laser and the second split laser. A phase and magnitude calibrator(1020) measures the phase sensitivity and size sensitivity of the interferential signal transformed to the frequency domain.
Abstract:
A method for measuring the thickness and profile of a thin film by dispersive white-light interferometry based on reflectrometry is provided to effectively separate thickness and profile complicatedly mixed in interference patterns for measuring the thickness and profile of an ultra thin film of 100 nm or less. A method for measuring the thickness and profile of a thin film by dispersive white-light interferometry based on reflectrometry includes the steps of obtaining light intensity distribution according to the wavelength of the thin film by obtaining interference patterns of interference light, obtaining an absolute reflection rate by the light intensity distribution, obtaining the thickness(d) of the thin film by the absolute reflection rate, extracting a first phase change value according to the thickness and profile from the interference patterns of synthesized light, extracting a second phase change value according to the thickness included in the first phase change value, obtaining a third phase change value according to the profile by compensating the second phase change value from the first phase change value, and obtaining a profile value(h) from the third phase change value.
Abstract:
본 발명은 백색광주사간섭계를 이용한 미세한 삼차원 형상을 측정하는 장치의 설계에 있어서, 기존의 마이켈슨형의 백색광주사간섭계의 구성에 널리 사용되고 있는 현미경 대물렌즈를 매크로렌즈로 대치하여, 한 번에 측정할 수 있는 측정대상물의 횡방향 면적 영역을 획기적으로 확장할 수 있는 새로운 원리 및 이의 세부적 구현 방법에 관한 것이다. 매크로렌즈를 도입한 백색광주사간섭계는 백색광 조명광학계, 상기 백색광을 측정면과 기준면에 조사하기 위해 측정광과 기준광으로 분리하는 광분할기, 상기 측정면과 기준면에서 반사된 측정광과 기준광을 동시에 결상하기 위한 매크로렌즈, 그리고 상기 매크로렌즈로부터 얻어진 백색광 간섭무늬를 획득하는 영상획득부로 구성된다. 상기와 같이 구성되는 본 발명은 일반 카메라의 접사촬영에 널리 사용되는 매크로렌즈를 활용하여 한 번에 측정할 수 있는 미세한 삼차원 형상의 횡방향 면적 영역을 무제한적으로 확장하여, 대면적의 대상물을 고속으로 측정할 수 있는 장점을 제공한다. 백색광주사간섭, 매크로렌즈, 대영역 삼차원 형상측정.
Abstract:
본 발명은 다중채널 위상천이 모아레 기법을 이용한 임의 표면의 3차원 형상 측정에 관한 것으로, 특히 위상이 천이된 다수의 모아레 무늬를 얻기 위해, 종래에는 격자를 이송수단에 의해 이동시키면서 모아레 무늬를 획득하던 것을 홀로그램을 사용하여 별도의 이송수단을 사용하지 않고도 위상이 천이된 다수의 모아레 무늬를 얻고 상기 모아레 무늬를 해석함으로써 임의 표면의 3차원 형상 측정하는 것을 특징으로 한다. 본 발명에서 제시하는 다중채널 위상천이 모아레 기법을 이용한 삼차원 형상측정기는 크게 영사시스템, 결상시스템, 중앙처리부 및 측정결과 표시장치로 구성된다. 상기 영사시스템은 격자형상을 측정대상물체에 투영하는 부분으로 격자를 렌즈를 통하여 투영하는 형태 혹은 레이저를 이용하여 쉽게 얻을 수 있는 격자형태의 간섭무늬를 투영하는 형태가 주로 사용되며, 결상시스템은 렌즈, 홀로그램, 격자, 모아레무늬 획득부 등으로 구성되고, 상기 광학요소들은 시스템의 특성에 따라 제외되거나, 다른 광학요소로 대치될 수 있다. 상기 영사시스템으로 측정대상물체에 투영된 격자형상은 결상시스템의 렌즈를 통해 결상시스템 내의 홀로그램에 결상되어 모아레 무늬를 형성한다. 홀로그램은 렌즈를 통해서 들어온 광을 여러 개의 같은 광들로 분할하여 동시에 여러 개의 모아레 무늬를 형성할 수 있도록 하기 위해, 필요에 따라 일차원 혹은 이차원 회절격자 형태의 홀로그램이 사용된다. 모아레 무늬 획득부는 상기 격자에서 생성된 모아레 무늬를 렌즈 등을 통하여 영상획득 수단을 통해 획득하고 중앙처리부 및 측정결과 표시장치로 전송한다.
Abstract:
Disclosed is a point diffraction interferometer for analyzing the surface profile of an object in a predetermined shape. The present invention relates to a phase-shifting point diffraction interferometer using inclined-section optical fiber light source, which is capable of minimizing a system error by directly using spherical waves emitted from a point beam source as a reference wavefront to move an error caused by a reference surface.
Abstract:
PURPOSE: A hetero mode helium-neon laser and a heterodyne laser interferometer are provided to measure displacement of a moving object by using super heterodyne phase measurement. CONSTITUTION: A heterodyne laser interferometer includes a laser source section(70), an optical interferometer section(60), a frequency converting section(80), and a phase measuring device. The laser source section(70) includes a hetero mode helium-neon laser generator(71). Light generated from the laser source section(70) has two frequencies. A part(74) of light generated from the laser source section(70) is used as a reference signal and other light(75) generated from the laser source section(70) is used as a measuring signal. The reference signal is converted into an electric signal(76) through a photo detector(73).
Abstract:
PURPOSE: A method and a system for measuring a large-scaled image are provided to simultaneously determine various space coordination of an object to be measured by using a plurality of optical probe having two point-light sources. CONSTITUTION: A large-scaled image measuring system includes a light source section(500), a detecting section(530), and a central processing section(560). The light source section(500) has a plurality of optical probes having two point-light sources, a light source(501) for supplying light to two point-light sources, an optical switch(502) for adjusting an amount of light introduced into an optical distributor from the light source(501), and a plurality of phase shifting devices(506,507,508). The detecting section(530) includes a detecting device for detecting an interference pattern and a detecting device control section. The central processing section(560) has a calculating section(564), an image processing section(565), an optical switch control section(562), a phase shifting devices control section(561) and a central control section(563).
Abstract:
PURPOSE: A Fizeau interferometer using an oblique section fiber light source is provided to improve the reliability of measuring results by removing beam splitting elements from a measuring wavefront. CONSTITUTION: A Fizeau interferometer includes a single mode fiber(12), a laser generator(11) for outputting beams to the single mode fiber, a collimator for converting the light of the laser generator to the parallel light, a reference plate(17) for transmitting and reflecting the parallel light to a target(18) in order to generate a reference wavefront, and a CCD camera(14) for detecting an interference fringe of the reference wavefront. The Fizeau interferometer further includes an oblique section fiber light source which is coupled to the single mode fiber. A beam split coating layer is formed on an oblique section of the oblique section fiber light source.
Abstract:
PURPOSE: A method and system for determination of coordinates is provided to reduce measurement error by permitting two optical fibers in the probe to approach closely to a three-dimensional object, while simplifying configuration of the system. CONSTITUTION: A system for determination of coordinates, comprises two optical fibers(50,60) for radiation arranged in a probe(80) disposed in a three-dimensional space; a light source(10) for providing light to optical fibers; a single mode fiber(30) interconnected between optical fibers for radiation and the light source, and which transmits light; a piezo-electric element(70) for changing optical path; an image obtaining unit for obtaining interference patterns generated by the light radiated from optical fibers for radiation; and a control/analysis unit for obtaining curvature of the obtained interference pattern and determining central point of the curvature.
Abstract:
PURPOSE: A two-dimensional white light interference method and interferometry is provided to minimize error of measurement, while compensating for the error caused due to the change of phase, through a single measurement. CONSTITUTION: An interferometry is characterized in that the step height(h) of differential metal materials is measured by an equation which is defined by a step height value(H) measured by using a Fringe peak of a white light interferogram, a step height value(h1) measured at a frequency k1(wavelength lambda1) by using a monochromatic light interference method, and a step height value(h2) measured at a frequency k2(wavelength lambda2) by using a monochromatic light interference method. The equation is h (equals) H(minus)1/2(k0(h2(minus)h1))/(k2(minus)k1), wherein k0 is the central frequency of white light source, k1 is the frequency of white light source for measuring the step height value(h1), and k2 is the frequency of light source for measuring the step height value(h2).