• 제목/요약/키워드: Laser optics

검색결과 1,034건 처리시간 0.028초

Adaptive Optics in Institute of Optics and Electronics, China

  • Jiang, Wenhan;Ling, Ning
    • 한국광학회:학술대회논문집
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    • 한국광학회 2000년도 하계학술발표회
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    • pp.3-3
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    • 2000
  • Adaptive Optical (AO) technology can compensate for wave-front errors in real-time to improve image and beam quality. The research and development on AO in China began in 1979. In 1980, the first laboratory on AO in China was established in Institute of Optics and Electronics (IOE), Chinese Academy of Sciences (CAS). Since then several AO systems have been built in this Laboratory. The 19-element system is the first AO system in the world ever used in inertial confinement fusion (ICF) facility in our knowledge. It corrects the static error of this large laser engineering. The 21-element system was firstly tested at the 1.2m telescope of Kunming Observatory in 1990 and then up-dated as an IR AO system installed at the 2.16m telescope of Beijing Observatory. The 37-element system was used with a turbulence cell in Laboratory on Atmospheric Optics in Hefei to conduct elementary research on Atmospheric Optics. The 61-element system for astronomical observation is newly developed. It has been successfully installed at the 1.2m telescope of Kunming Observatory and a laser guide star system will be integrated with the system. A compact AO system using our newly developed miniature DM for high resolution ophthalmic imaging of retina is also being built. The key elements of these AO systems, deformable mirrors and fast-steering mirrors, are all developed in this Laboratory. In this talk, the main configurations of these AO systems, some test results as well as the specifications of these active mirrors will be presented.

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적응적 에러 보정과 다이나믹 안정기를 이용한 레이저 유도 초음파 검사 시스템 개발 (Development of a Laser-Generated Ultrasonic Inspection System by Using Adaptive Error Correction and Dynamic Stabilizer)

  • 박승규;백성훈;박문철;임창환;나성웅
    • 비파괴검사학회지
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    • 제25권5호
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    • pp.391-399
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    • 2005
  • 레이저 유도 초음파 시스템은 놀은 공간분해능으로 스캐닝 하면서 광대역 범위에서 검사를 할 수 있는 비접촉식 검사 장치이다. 유도되는 초음파 신호의 크기는 펄스레이저의 출력에 의해서도 변화하지만, 연속발진 레이저빔이 위치하는 표면 상태에 따라서도 측정되는 초음파 세기는 크게 변화한다. 본 논문에서는 안정된 레이저 유도 초음파 시스템을 구성하기 위하여 펄스 레이저빔의 출력을 측정하여 초음파 발생 오차를 보정하였으며, 대상체 표면의 상태에 따라 크게 변화하는 측정용 레이저 간섭계의 측정 이득 변화를 매순간 측정하여 측정 오차를 보정하였다. 본 논문에서는 대상체 표면을 스캐닝 할 수 있도록 다이나믹 안정기가 부착된 레이저 유도 초음파 시스템을 개발하였다. 개발한 레이저 초음파 시스템은 스캐닝 과정에서 간섭계의 이득이 최대가 되는 순간을 적응적으로 포착하여 초음파를 발생시키고, 유도된 초음파 신호를 고속으로 샘플링 한 후에 실시간으로 신호처리를 한다. 본 논문에서는 안정적인 레이저 유도 초음파 시스템을 구성하기 위한 전체 시스템의 하드웨어 구성 방법과 제어 알고리듬에 대하여 기술한다. 또한 본 논문에서 제안한 발생오차 보정방법과 측정오차 보정 방법이 시스템의 성능 향상에 유효함을 실험을 통하여 확인하였다.

Infrared Dual-field-of-view Optical System Design with Electro-Optic/Laser Common-aperture Optics

  • Jeong, Dohwan;Lee, Jun Ho;Jeong, Ho;Ok, Chang Min;Park, Hyun-Woo
    • Current Optics and Photonics
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    • 제2권3호
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    • pp.241-249
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    • 2018
  • We report a midinfrared dual-field-of-view (FOV) optical system design for an airborne electro-optical targeting system. To achieve miniaturization and weight reduction of the system, it has a common aperture and fore-optics for three different spectral wavelength bands: an electro-optic (EO) band ($0.6{\sim}0.9{\mu}m$), a midinfrared (IR) band ($3.6{\sim}4.9{\mu}m$), and a designation laser wavelength ($1.064{\mu}m$). It is free to steer the line of sight by rotating the pitch and roll axes. Our design co-aligns the roll axis, and the line of sight therefore has a fixed entrance pupil position for all optical paths, unlike previously reported dual-FOV designs, which dispenses with image coregistration that is otherwise required. The fore-optics is essentially an achromatized, collimated beam reducer for all bands. Following the fore-optics, the bands are split into the dual-FOV IR path and the EO/laser path by a beam splitter. The subsequent dual-FOV IR path design consists of a zoom lens group and a relay lens group. The IR path with the fore-optics provides two stepwise FOVs ($1.50^{\circ}{\times}1.20^{\circ}$ to $5.40^{\circ}{\times}4.32^{\circ}$), due to the insertion of two Si lenses into the zoom lens group. The IR optical system is designed in such a way that the location and f-number (f/5.3) of the cold stop internally provided by the IR detector are maintained when changing the zoom. The design also satisfies several important performance requirements, including an on-axis modulation transfer function (MTF) that exceeds 10% at the Nyquist frequency of the IR detector pitch, with distortion of less than 2%.

Generation of Thermoelastic Waves by Irradiating a Metal Slab with a Line-Focused Laser Pulse

  • Yoo, Jae-Gwon;Baik, S.H.
    • 비파괴검사학회지
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    • 제26권3호
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    • pp.181-189
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    • 2006
  • A 2D finite-element numerical simulation has been developed to investigate the generation of ultrasonic waves in a homogeneous isotropic elastic slab under a line-focused laser irradiation. Discussing the physical processes involved in the thermoelastic phenomena, we describe a model for the pulsed laser generation of ultrasound in a metal slab. Addressing an analytic method, on the basis of an integral transform technique, for obtaining the solutions of the elastodynamic equation, we outline a finite element method for a numerical simulation of an ultrasonic wave propagation. We present the numerical results for the displacements and the stresses generated by a line-focused laser pulse on the surface of a stainless steel slab.

파장변조 광흡수 분광법을 이용한 농도 계측 기법 (Species Concentration Measurement Technique Using Wavelength Modulation Absorption Spectroscopy)

  • 안재현;김용모
    • 한국분무공학회지
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    • 제9권4호
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    • pp.67-76
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    • 2004
  • Diode laser absorption sensors are advantageous because they may provide fast, sensitive, absolute, and selective measurements of species concentration. These systems are very attractive for practical applications owing to its compactness, reasonable cost, robustness, and ease of use. In addition, diode lasers we fiber-optic compatible and thus enable simultaneous measurements of multiple species along a line-of-sight. Recent advances of room-temperature, near-IR and visible diode laser sources for telecommunication, optical data storage applications make it possible to be applied for combustion diagnostics based on diode laser absorption spectroscopy. Therefore, combined with fiber-optics and high sensitive detection strategies, compact and portable sensor systems are now appearing for variety of applications. The objectives of this research are to develop new gas sensing system and to verify feasibility of this system. Wavelength modulation spectroscopy has been demonstrated in these experiments and has a bright prospect to this diode laser system.

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줌렌즈 광속확대기를 적용한 레이저 레이더용 송수광 내접형 광학계 설계 (Inscribed Transceiver Optical System Design for Laser Radar with Zoom-type Expander)

  • 고해석;옥창민;홍진석;이창재;박찬근;김현규
    • 한국광학회지
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    • 제24권1호
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    • pp.23-28
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    • 2013
  • 송광광학계의 광원으로 사용되는 광섬유 레이저의 개구수, NA가 0.13~0.22의 범위에 있으면, 이 NA에 관계없이 1 km 전방에서 빔직경이 4.8 m 또는 6.8 m이 되도록 줌렌즈형 광속확대기를 적용한 송광광학계를 설계하였으며, 표적에서의 foot prints를 통하여 빔직경을 확인하였다. $16{\times}16$($100{\mu}m{\times}100{\mu}m$) 픽셀 검출기를 사용하는 수광광학계를 설계하였으며, 검출면의 픽셀 위치에 따른 spot diameter는 모두 $55{\mu}m$ 이하가 됨을 확인하였다. 스캔을 고려하여 송광광학계를 수광부 대물렌즈에 내접하도록 구성하였으며, 이때 송광부에 의하여 가려진 부분은 11%가 되었다.

고효율 태양광 모듈 제작을 위한 스트링 공정 최적화 (Shingled String for the High Performance Photovoltaic Module)

  • 지홍섭;문대한;송진호;정채환
    • Current Photovoltaic Research
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    • 제6권4호
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    • pp.119-123
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    • 2018
  • The High Performance Module With The Shingled String Has Several Advantages Such As The Larger Active Area, Higher Open-Circuit Voltage And Smaller Cell To Module (Ctm) Loss. To Obtain Increase Of Power In Pv Shingled Module, The Detailed Condition Of Various Parameters Related To Cutting And Bonding Process Were Investigated In This Study. We Searched The Optimized Cutting Conditions Of Laser Scan Speed, The Number Of Laser-Scribing And Also Bonding Conditions Of Electrically Conductive Adhesives (Eca) By Varying Amount Of Eca, Curing Time And Curing Temperature. The Shingled Pv Module Showed 25.4W of Maxmimum Power At 60 Rpm Of Dipensing Motor Speed, 30 Seconds Of Curing Time And $140^{\circ}C$ Of Curing Temperature, Respectively.