• 제목/요약/키워드: 2nd harmonic

검색결과 168건 처리시간 0.026초

Laser Patterning of Indium Tin Oxide for Flat Panel Display (평판디스플레이를 위한 Indium Tin Oxide의 레이저 페터닝)

  • Ahn, Min-young;Lee, Kyoung-cheol;Lee, Cheon
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 한국전기전자재료학회 2000년도 하계학술대회 논문집
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    • pp.340-343
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    • 2000
  • ITO(Indium Tin Oxide) films for transparent electrodes of FPD(Flat Panel Display) were patterned in atmosphere using laser. A pulse type(repetition rate of 10 Hz) Q-switched Nd:YAG laser which can generate the fundamental wavelength at 1064 nm or its harmonics(532, 266 nm) was used for Patterning of the ITO film. In case of using the second harmonic(532 nm) of Nd:YAG laser, the ITO film(thickness of 20 nm) was removed clearly with a laser fluence of 5.2 J/$\textrm{cm}^2$ and a beam scan speed of 200${\mu}{\textrm}{m}$/s. But the glass substrate was damaged when the laser fluence was over 5.2 J/$\textrm{cm}^2$. We discussed the etching mechanism of the ITO film using Nd:YAG laser with observation of the etching characteristics including a depths and widths of ITO films as a function of laser fluence using SEM(Scanning Electron Microscopy) and surface profiler($\alpha$-step 500).

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An Experimental Study on the Characteristics for Open-Tube and Closed-Tube Thermoacoustic Effects (2)- The 2nd, 3rd Harmonic (개방관과 밀폐관의 열음향 효과에 관한 하모닉 특성 연구(2) - 2차, 3차 하모닉)

  • 송규조;박종호;이성노
    • Progress in Superconductivity and Cryogenics
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    • 제4권1호
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    • pp.135-139
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    • 2002
  • In this study, the experimental open-tube and close-tube thermoacoustic apparatuses were built. In order to determine the optimum length of resonant tube and the optimum length of stack, the resonant characteristics of thermoacoustic apparatuses were investigated, The length of resonant tube varies from 400mm to 850mm. The experimental frequency varies from 100Hz to 1000Hz. In case of the second and third harmonics, the maximum temperature difference of open-tube thermoacoustic apparatus is 53$^{\circ}C$ (resonator length: 400mm) and the maximum temperature difference of closed-tube thermoacoustic apparatus is 51$^{\circ}C$ (resonator length: 500mm). In the open-tube thermoacoustic apparatus, the peak efficiency point is about 2%, 55%, 69% in the resonant tube and in the closed-tube thermoacoustic apparatus, the peak efficiency point is about 2%, 41%, 50% in the resonant tube.

Detection of Damage of Rd6G Film Using Surface Second-Harmonic Generation (표면 제2고조파 발생을 이용한 색소 Rd6G박막층의 손상 분석)

  • 유대혁;고춘수;임용식;이재형;장준성
    • Korean Journal of Optics and Photonics
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    • 제5권2호
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    • pp.272-277
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    • 1994
  • The damage of a thin film of Rd6G dye was probed by Surface Second-Harmonic Generation(SSHG) method. A portion of the Rd6G thin film on glass substrate was damaged by 532 nm laser beam, and the damage was probed by detecting intensity variation of SSHG. The result was confirmed through direct observation with optical microscope.oscope.

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A characteristics study on the Second-harmonic generation conversion efficiency of Pulsed Nd:YAG Laser adopted Superposition multiple Mesh Networks (중첩다단 메쉬회로를 적용한 펄스형 Nd:YAG 레이저의 2차 고조파 변환효율에 관한 특성연구)

  • 김휘영
    • Journal of the Korea Computer Industry Society
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    • 제2권4호
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    • pp.565-572
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    • 2001
  • At the most recent years, laser medical instruments, laser applications and laser nuclear fusion need strong visible light and ultraviolet rays. Nonlinear optical devices, such as harmonic generators and parametric oscillators, provide a means of extending the frequency range of available laser sources. Frequency conversion is a useful technique for extending the utility of high-power lasers. It utilizes the nonlinear optical response of an optical medium in intense radiation fields to generate new frequencies. These progresses have been used to generate high-power radiation in all spectral regions, from the ultraviolet to the far infrared. Optical parametric oscillators and amplifiers generate two waves of lower frequency They are capable of generating a range of wavelengths from a single frequency source, in some cases spanning the entire visible and near infrared regions. Consequently, in order to obtain the green light, the pulsed Nd:YAG laser using multiple-mesh PFN(Pulsed Forming Network) method with Nonlinear optical device was adopted. We compared the current pulseshapes with the laser output energy, and conversion efficiency.

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ITO Thin Film Ablation Using KrF Excimer Laser and its Characteristics

  • Lee, Kyoung-Chel;Lee, Cheon;Le, Yong-Feng
    • Transactions on Electrical and Electronic Materials
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    • 제1권4호
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    • pp.20-24
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    • 2000
  • This study aimed to develop ITO(Indium Tim Oxide) tin films ablation with a pulsed type KrF excimer laser required for the electrode patterning application in flat panel display into small geometry on a large substrate are. The threshold fluence for ablating ITO on glass substrate is about 0.1 J/㎠. And its value is much smaller than that using 3 .sup rd/ harmonic Nd:YAG laser. Through the optical microscope measurement the surface color of the ablated ITO is changed into dark brown due to increase of surface roughness and transformation of chemical composition by the laser light. The laser-irradiated regions were all found to be electrically isolating from the original surroundings. The XPS analysis showed that the relative surface concentration of Sn and In was essentially unchanged (In:Sn=5:1)after irradiating the KrF excimer laser. Using Al foil made by 2$\^$nd/ harmonic Na:YAG laser, the various ITO patterning is carried out.

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Crystallization in Li$_2$O-A1$_2$O$_3$-SiO$_2$ Glass induced by 355 nm Nd:YAG Laser Irradiation

  • Lee, Yong-Su;Kang, Won-Ho
    • Journal of the Microelectronics and Packaging Society
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    • 제7권2호
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    • pp.43-46
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    • 2000
  • Nd:YAG laser of 355 nm wavelength, which amounts to 3.5 eV, produced by a harmonic generator was used to create Ag metallic particles as seeds for nucleation in photosensitive glass containing $Ag^+$ and $Ce^{3+}$ . The pulse widths and frequency of the laser were 8ns and 10 Hz, respectively. For crystalline growth, heat-treatment following laser irradiation was carried out at $570^{\circ}C$ for 1h. Then, the $LiAlSi_3O^8$ crystal phase appeared in the laser irradiated lithium aluminum silicate glass. We present the effect of laser-induced nucleation compared with spontaneous nucleation by heat treatment fur crystallization in the glass.

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Frequency Miner Characteristics for Direct Conversion Receiver (직접변환수신기에 적합한 주파수 혼합기의 특성분석)

  • 박필재;유현규;조한진
    • Proceedings of the Korea Electromagnetic Engineering Society Conference
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    • 한국전자파학회 2000년도 종합학술발표회 논문집 Vol.10 No.1
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    • pp.154-157
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    • 2000
  • One of the problems using DCR(Direct Conversion Receiver) type architecture are DC offset, Poor channel selectivity. APDP(Anti Parallel Diode Pair) can be mood candidate for the DCR frequency mixer due to its inherent 2nd harmonic suppression. APDP shows good IP2 and DC suppression. This paper describes single APDP LO power characteristics, IP2, and receiver structure utilizing APDP frequency mixer.

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Spectrum Narrowing Characteristics of a Tunable Ti:sapphire Laser (파장가변 Ti:sapphire 레이저의 협대역 특성)

  • 이용우;이주희
    • Korean Journal of Optics and Photonics
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    • 제6권1호
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    • pp.16-20
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    • 1995
  • We have studied the spectral narrowing characteristics of the tunable Ti:sapphire laser pumped by the second harmonic generation of Nd:YAG laser. Ti:sapphire laser has uniform excitation distribution by both-side end pumping. We have controlled the angle of grating linearly and achieved the continuous selection of wavelength in the broad range from 705 to 835 nm. The output energy of $380{\mu}J$ at 790 nm. the spectral linewidth of $0.13cm_{-1}$ and the beam divergence of 1.2 mrad have been obtained. The wavelength range with power more than 50% of maximum output was 730-825 nm.825 nm.

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x$^{(3)}$ Measurement through Self-focusing with Non-gaussian Beam (비 Gaussian 빛에 의한 자체집광을 이용한 x$^{(3)}$측정)

  • 이범구
    • Korean Journal of Optics and Photonics
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    • 제4권4호
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    • pp.428-433
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    • 1993
  • The second harmonic of Q-switched Nd:YAG laser beam with gaussian mode is cut off by pinhole of a certain radius and its central portion passed through pinhole is focused by converging lens. It is confirmed that the shape of this beam in focal region is central symmetric but non-gaussian. Change of transmittance due to self-focusing is investigated by scanning (z-scan) $CS_2$ of 1 mm thickness in the focal region. It is found that the observed results can be consistently explained by Fresnel theory within 1.5% accuracy and efficiency of self-focusing depends on spatial shape of incident beam.

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