• Title/Summary/Keyword: Twyman-green interferometer

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Simultaneous measurement of the parallelism and the relative surface figure of a nontransparent plate using visible light (가시광선을 이용한 불투과 평면창의 평행도 및 상대적 표면형상 동시측정)

  • 김연수;김현숙
    • Korean Journal of Optics and Photonics
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    • v.13 no.2
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    • pp.89-91
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    • 2002
  • A test method that can measure the parallelism and the surface figure of an nontransparent plate using visible light is proposed. The testing system consists of a Twyman-Green interferometer. In addition, test results for the IR filter of IR MTF measuring system are described.

A Study on Assembly and Evaluation of SIL optical Head for surface Recording of SIL based NFR (고체침지렌즈 기반 근접장 표면 기록을 위한 고체침지렌즈 광학 헤드의 조립 및 평가에 대한 연구)

  • Min, Cheol-Ki;Kim, Tae-Seob;Yoon, Yong-Joong;Park, No-Cheol;Park, Young-Pil
    • Transactions of the Society of Information Storage Systems
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    • v.4 no.1
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    • pp.19-22
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    • 2008
  • For the assembly and evaluation of solid immersion lens (SIL) optical head which is the key component of SIL based near field recording (NFR) technology, we modify the Twyman-Green interferometer. Super-hemisphere SIL optical head for the surface recording is assembled and evaluated by the modified Twyman-Green interferometer. In order to verify the optical performance of the assembled SIL optical head, we compare the measured results of the SIL optical head with the simulation ones. Finally, we show the feasibility of applying the assembled SIL optical head to near field recording system by the experiment of the dynamic gap control based on test bed.

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Surface profile measurement with FFT method and stabilized interferometer (안정화된 간섭계와 FFT를 이용한 표면 측정)

  • 류진;김현수;박종락;김진태
    • Proceedings of the Korean Society of Machine Tool Engineers Conference
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    • 2004.10a
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    • pp.269-273
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    • 2004
  • The moduled interferometer with waveplates, polarizing beam splitter, etc. for four phase shifted interference patterns was stabilized with the and Fast Fourier Transform (FFT) method was used to investigate the surface profile measurement from the interferenece pattern from Twyman-Green interferometer using a mathcad.

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Multiphase Homodyne Laser Interferometer with Four Bucket (Four-bucket 알고리즘을 이용한 레이저 간섭계)

  • Park, Yoon-Chang;Jeong, Kyung-Min
    • Journal of the Korean Society for Precision Engineering
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    • v.16 no.10
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    • pp.203-208
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    • 1999
  • By tilting the reference mirror of Twynman-Green interferometer having a reference mirror and a moving mirror, firinge pattern composed of bright and dark parallel lines can be obtained and the fringe pattern is shifted according to the displacement of the mowing mirror. Several studies are executed for displacement measurement by detecting the intensity of the fringe with photo-diodes having small detecting area. In this study, to improve the sensitivity and robustness, the intensity of fringe is detected by using a large-area quadratic photo-diode masked with a grating panel having four kinds of binary grating having phase-difference of 0, {\pi}$/4, {\pi}$/2, 3 {\pi}$/4. The phase of the fringe is calculated with a simple 4-buckets algorithm. A experimental result shows that standard deviation of 5.653 nm is obtained comparing with a capacitive type gap sensor having nearly 1 nm accuracy.

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Development of Interferometer for Performance Assessment of IR Optical System (적외선 광학계통 성능평가를 위한 간섭계 개발)

  • 홍경희;고재준;이성태;장세안;오명호
    • Korean Journal of Optics and Photonics
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    • v.2 no.4
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    • pp.179-185
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    • 1991
  • Twyman-Green interferometer is developed for assessment of IR optical system performance. Light source is $CO_2$ gas laser which has 10.6$\mu \textrm m$ wavelength. The light beam is expanded to 2.5 cm dia by Ge lens and splitted by ZnSe parallel plane plate. One of the beams is reflected by refernce mirror which is operated PZT. The fringe will be detected by a pyro-electric vidicon camera and displayed by a CRT monitor. Here, the IR firinge is recorded on the thermal paper. In visible region, the light source is He-Ne laser. The fringe is detected by a CCD camera and displayed by the CRT monitor. The intensity of the fringe is digitized by a image card and processed by a PC. The wavefront aberration function, PSF and OTF are calculated. The results are displayed in 3-D graphs on the monitor or printed out by a line printer.

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3-D Profilometry by Phase Shifting Profilometry (위상이동법을 이용한 3차원 형상측정법의 연구)

  • 오동석;남기봉
    • Korean Journal of Optics and Photonics
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    • v.5 no.2
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    • pp.191-197
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    • 1994
  • We investigated the properties of various methods of 3 dimensional profilometry to choose the phase shifting technique for the reconstruction of the shape of a given specimen. The pattern was generated by a Twyman-Green interferometer and a PZT was used to shift the fringes on the target surface. The shape was calculated with Hariharan algorithm within the uncertainty of a scaling factor. The optical noise inherent in the laser source was observed to influence the final outcome to a great extent and the need for an exact calibration was noted. noted.

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Profiling of fine displacement of spherical surface using Fourier transform method (푸리에 변환 간섭 해석법을 이용한 구면의 미세 변위 측정)

  • 손영준;주신호;권진혁;최옥식
    • Korean Journal of Optics and Photonics
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    • v.8 no.3
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    • pp.199-203
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    • 1997
  • Fine displacement of spherical suface was detected and analyzed by Twyman-Green interferometer and the interferogram analysis using Fourier transform method. The surface profile was obtained from single interferogram by introducing the carrier freguency to the interferogram. The interferogram was processed in the spatial frequency domain by fast Fourier transform, and the phase distribution was obtained by inverse Fourier transform. The 3-dimensional distribution for the surface displacement was obtained. It was compared with the calculated surface displacement and the error was less than λ/10.

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Fourier transform method of surface topography and interferometry (푸리에 변환을 이용한 파면위상의 복구)

  • 남기봉
    • Korean Journal of Optics and Photonics
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    • v.3 no.1
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    • pp.20-26
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    • 1992
  • The fourier transform method of retrieving the phase of the test wavefront from a Twyman-Green interferometer was reviewed by numerical simulations and experiments. Of the two methods reviewed, Takeda's approach proved more reliable in reconstructing the deformation of the test surface. The application of this approach to a plane mirror showed the existence of the surface curvature, whose maximum deviation was about $\lambda$/6. The accuracy in the measurement was evaluated to be around $\lambda$/40.

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Parabolic mirror test using Computer Generated Hologram (Computer Generated Hologram을 이용한 포물명경 형상측정)

  • 김성하;곽종훈;최옥신;송재봉;이윤우;이인원
    • Korean Journal of Optics and Photonics
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    • v.11 no.2
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    • pp.80-84
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    • 2000
  • Parabolic almninium mlITOr of m.5('||'&'||'cent; 50 nun) was fabncated by a diamond tummg machine. Computer generated hologram (CGH) for the test of parabolic mirror was encoded by binary phase hologram Approximation of curved fringe to line was made by staircase encoding. After fringe data 1ransformed mto a Post Scnpt file. magnified master CGH was printed by a laser printer, and then it reduced to the photographIc film. Parabolic mirror was tested by Twyman-Green interferometer with CGH at VIewing arm. Its experimental result was compared with those of surface profile and auto-collimatIon test, and then the errors were analyzed.

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Near field scanning optical interferometer using facet reflection of a tapered optical fiber (광섬유 탐침의 반사를 이용한 파면 분석 근접장 주사 광간섭계)

  • 유장훈;임상엽;이현호;박승한
    • Korean Journal of Optics and Photonics
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    • v.15 no.3
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    • pp.248-253
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    • 2004
  • We propose a near- field scanning optical interferometer (NSOI) based on the facet reflection of a nano-sized moveable tapered optical fiber. The interferometer can measure the position and the wave-front of a focused spot simultaneously. The interfering fringes are generated by the reflected beams from the sample surface and from the fiber facet. The wave-front analysis at the focusing position is obtained by using a phase shifting technique with a four-step algorithm. It is found that the resolution for controlling the focal position of our proposed NSOI is less than λ/3 and the measured wave-front aberration at the focal position is in good agreement with the ones obtained by a Twyman-Green interferometer.