• Title/Summary/Keyword: 음향-광변조기

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High resolution heterodyne interferometric technique with AOM for measuring the thermal expansion (음향광변조기를 이용한 고분해능의 헤테로다인 간섭식 열팽창 측정기술)

  • 최병일;이상현;김종철;임동건
    • Korean Journal of Optics and Photonics
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    • v.13 no.6
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    • pp.530-536
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    • 2002
  • The accurate measurements of thermal expansion coefficients is one of the most important techniques required not only in material science but also in industries. A high precision interferometric dilatometer, using acoustic optical modulator, has been constructed and its performance has been tested. The system consists of a double-path optical heterodyne interferometer and a radiant heating furnace. This provides highly accurate length measurement, and allows rapid heating and cooling method for the specimen. A three longitudinal mode frequency stabilized He-Ne laser, using the secondary beat frequency, is constructed. Its stability is found to be $5{\times}10^{-9}$. The uncertainty in the length measurement is estimated to be of nanometer order in the range between room temperature to 1100 K.

정사각형 평판의 진동 진폭 측정을 위한 스트로보스코픽 ESPI 기법 적용

  • 정현철;김경석;강기수;이유황;지창준
    • Proceedings of the Korean Society of Precision Engineering Conference
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    • 2004.05a
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    • pp.174-174
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    • 2004
  • 본 논문에서는 4변이 고정된 정사각형 알루미늄 평판의 진동 진폭을 측정하기 위하여, 기존의 위상 이동 ESP떼 스트로보스코프식 조사를 적용한 스트로보스코픽 ESPI 기법을 이용하였다. 일반적으로 시간평균 ESPI를 이용하면 진동하고 있는 대상체의 정성적인 진동 패턴을 측정할 수 있다. 그러나 시간평균 ESPI로는 진동하고 있는 대상체의 두께방향으로의 진폭량을 측정하기는 어렵다. 또한 일반적인 위상이동법을 적용시킬 경우, 대상체가 진동을 하게 됨으로써 정확한 진동 진폭을 측정하기 어렵다.(중략)

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Acousto-Optical Third Order Correlator Using 2-D Ultrasonic Diffractor Cell (2차원 초음파 회절격자를 이용한 음향-광3차 상관기의 구성)

  • Jang, Gyeong-Yeong;Sato, Takuso
    • Transactions of the Korean Society of Mechanical Engineers A
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    • v.20 no.1
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    • pp.206-213
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    • 1996
  • Third order correlation funciton is to be advantageous to detect unique features embedded in various random signals that are undetectable with second order correlation or power spectrum. In this paper, we will introduce optical modulator which consists of a laser light source, 2-dimensional ultrasonic diffractor cell with signal controlling circuitry, and a CCD camera connected to personal computer for image processing. With this modulator, the third order correlaiton pattern of signal can be immediately obtained at the camera due to parallel nature of optical computing.

The CGH in the Electro-holographic system using the Bragg type AOSLM (Bragg type 음향광변조기를 채택한 Electro-holographic system에서의 computer generated Fresnel hologram의 구현)

  • ;;;;Tru Thi Van Anh
    • Proceedings of the Optical Society of Korea Conference
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    • 2002.07a
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    • pp.142-143
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    • 2002
  • KIST에서는 Pulsed Laser를 사용하여 3차원 image를 재생할 수 있는 Electro-Holographic System을 만들어 CGH이미지를 구현하였다. CGH 이미지를 구현하기 위한 SLM (Spatial Light Modulator)으로 TeO$_2$ 결정의 Shear Mode 에서 동작하는 Bragg type의 다채널 AOSLM(Acousto-optic Spatial Light Modulator)이 사용되었다. 이 Bragg type 다채널 AOSLM에서는 광원이 특정 Bragg 각도로 입사하였을 때 다른 고위 차수는 억압되고 +나 -의 첫번째 차수의 회절 빔만이 형성된다. (중략)

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Laser Damage Threshold Increase of A/R Coating Films for 200MHz AOM (A/R 코팅 변화에 따른 200MHz AOM의 laser damage threshold 증가)

  • Kim, Yong-Hun;Lee, Hang-Hun;Lee, Jin-Ho;Park, Yeong-Jun;Park, Jeong-Ho
    • Korean Journal of Materials Research
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    • v.7 no.3
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    • pp.213-217
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    • 1997
  • AOhf(Hcousto-r)l)tic niodulator) with :!OOlIiz freclucncl- and Sfi(;(Seconrl harmonic generation) green lasel-Lvith 53% nm wavelength were used for Il\'IIII~Dii.it,ii v~ilco disk recorder) FOI rhe appli~aptin of high densit]. optical recording, a high po\ver I ~ c r is r c ~ ~ l i ~ i l - u l ic I !tic. s\-sti,m a n d optic.,~I io;iting l,t)c>rs of each optical device must have a high laser damage threshoid hie rn;itie ant] retlwtive coatings on a $TeO_{2}$ singlc crystal. which is used as an acoustooptic material, by E-beam evaporation method. Laser damage threshold \vas nicdsureci hy Ar laser with the input power oi 0.55LV 1,aser damage threiholti 01 $ZrO_{2}$ and $SiO_{2}$. filn-is were higher than $AI_{2}O_{3}$ f i l m U'e also investigated a long--tern1 stability of the output po\ver of St{(; green laser

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