• Title/Summary/Keyword: Second harmonic generation

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Quasi-phase matched optical parametric oscillators using periodically poled $KNbO_3$ crystals (주기적으로 분극 반전된 $KNbO_3$를 이용한 준위상 정합 광 매개 진동자)

  • Lee Gwang Jo;Kim Jung Hyeon;Im Min Ho;O Hyeon Ho;Lee Don Hui;Yun Chun Seop
    • Proceedings of the Optical Society of Korea Conference
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    • 2003.02a
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    • pp.230-231
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    • 2003
  • $KNbO_3$is one of the best materials for efficient nonlinear frequency conversion, due to its large nonlinear optical coefficient ($d_{33}$ = 20.6 pm/V), wide transparency range (0.4 ~ 5 $\mu$m) and freedom from photorefractive effects. Quasi-phase-matched second harmonic generation using periodically poled $KNbO_3$ (PPKN) crystals has been reported. Here we report on fabrication of PPKN and demonstration of a pulsed optical param etric oscillator (QPM OPO) pumped by an Nd:YAG laser. (omitted)

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Synthesis and Characterization of Nonlinear Optical Polymers Having Quinoline-based Chromophores

  • Kim, Min-Ho;Jin, Jung-Il;Lee, Chul-Joo;Kim, Nak-Joong;Park, Ki-Hong
    • Bulletin of the Korean Chemical Society
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    • v.23 no.7
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    • pp.964-970
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    • 2002
  • We synthesized three kinds of chromophores incorporating aromatic quinoline unit as a $\pi-conjugated$ bridge in order to prepare more thermally stable nonlinear optical (NLO) chromophores than general stilbene unit. The NLO poly(methylmethacrylate) copolymer, polyimides, and polyester were successfully synthesized by these corresponding quinoline-based monomers. Their physical and optical properties were investigated by thermogravimetry, gel permeation chromatography, ultraviolet-visible spectroscopy, second harmonic generation (SHG) and electro-optic (EO) measurement. All the polymers exhibited better thermal stability,however their NLO activity was a little lower than that of general stilbene-based NLO polymers. Among three kinds of polymers, the PMMA copolymer with quinoline chromophores had the largest SHG coefficient d33 value of 27 pm/V (at 1.064 $\mu\textrm{m})$ and EO coefficient r33 value of 6.8 pm/V (at 1.3 $\mu\textrm{m}$).

Second Harmonic Generation of Femtosecond Pulse With MgO: Periodically Poled LiNbO$_3$ (주기적으로 분극 반전된 MgO: LiMbO$_3$를 이용한 펨토초 펄스의 2차 조화파 발생)

  • ;;;Sunao Kurimura;Trhunori Taira
    • Proceedings of the Optical Society of Korea Conference
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    • 2001.02a
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    • pp.236-237
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    • 2001
  • 최근 빠른 정보산업의 발달로 대용량의 정보를 초고속으로 전달해야 할 필요성으로 인해 광전송 시스템의 개발이 활발히 진행되고 있다. 특히 광통신 시스템이나 주변의 계측장비들과의 결합이 쉽다는 잇점 때문에 모드록킹된 광섬유 레이저는 이 분야의 광원으로서 매우 중요하게 쓰이고 있으며, 연구가 많이 진행되고 있다. 본 실험에 사용된 광섬유 레이저는 파장 1.55 $mu extrm{m}$대역에서 이득을 얻을 수 있는 어븀(Er$^{3+}$ )이 첨가된 광섬유를 사용하여 4.5 MHz의 빠른 반복률로 모드록킹 되도록 제작된 (Newgrid, (FFL-1550-PML-0) 것이며 펄스 폭은 320 fs, 중심파장은 1.566 $\mu\textrm{m}$, 펄스의 첨두 출력은 6.3 kW이다. (중략)

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Pulse Compression and Second Harmonic Generation of sub-30fs Ti:sapphire Laser (Sub 30fs Ti:sapphire s레이저의 펄스폭 압축 및 2차 조화파 발생)

  • 김점술;정재룡;박용섭
    • Proceedings of the Optical Society of Korea Conference
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    • 2001.02a
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    • pp.238-239
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    • 2001
  • sub-30fs 펄스폭의 상용 Ti:sapphire 레이저시스템에 대한 펄스압축기 및 2차 조화파 발생기를 제작하여 특성을 평가하였다. 그림la에서 82MHz의 주파수로 모드록되는 상용 Ti:sapphire 레이저 (Spectra-Physics Millennia/Tsunami laser)의 출력이 반사경 Ml, M2를 거쳐 펄스압축기에 입사되고 압축되어 나온 펄스가 다시 M6, M7를 거쳐 2차 조화파발생기로 입사되는 2단구조로 설계되었다. 압축기에 입사되기전 평균파워는 파장 800nm에서 520mW로 측정되었으며, 측정된 스펙트럼 반치폭 47nm에 (그림 2a)에 대해 chirp-free sech$^2$t 펄스로 가정할 경우 본 레이저시스템의 변환한계 펄스폭은 14.5fs로 계산된다. (중략)

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A study on the Second-Harmonic Generation(SBG) Conversion Characteristics of Nd:YAG Laser adopted Differential Superposition Mesh (중첩회로를 적용한 펄스형 Nd:YAG 레이저의 2차 SHG 변환효율에 관한 특성연구)

  • 김휘영;박두열
    • Proceedings of the IEEK Conference
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    • 2001.06e
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    • pp.215-218
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    • 2001
  • A pulsed Nd:YAG laser is used widely for materials processing and medical instrument. It's very important to control the laser energy density in those fields using a pulsed Nd:YAG laser. A pulse repetition rate and a pulse width are regarded as the most dominant factors to control the energy density of laser beam. In this paper, the alternating charge and discharge system was designed to adjust a pulse repetition rate. This system is controlled by microprocessor and allows to frequence an expensive condenser for high frequency to cheap one for low frequency. In addtion, The microcontroller monitors the flow of cooling water, short circuit, and miss firing and so on. We designed Nd:YAG laser firmware with smart microcontroller, and want to explain general matters about the firmware from now.

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Synthesis, Optical and Electrical Studies of Nonlinear Optical Crystal: L-Arginine Semi-oxalate

  • Vasudevan, P.;Sankar, S.;Jayaraman, D.
    • Bulletin of the Korean Chemical Society
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    • v.34 no.1
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    • pp.128-132
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    • 2013
  • L-Arginine semi-oxalate (LASO) single crystal has been grown by solution growth technique at room temperature. The crystal structure and lattice parameters were determined for the grown crystal by single crystal X-ray diffraction studies. Photoluminescence studies confirm the violet fluorescence emission peak at 395 nm. Optical constants like band gap, refractive index, reflectance, extinction coefficient and electric susceptibility were determined from UV-VIS-NIR spectrum. The dielectric constant, dielectric loss and ac conductivity of the compound were calculated at different temperatures and frequencies to analyze the electrical properties. The solid state parameters such as plasma energy, Penn gap, Fermi energy and polarizability were calculated to analyze second harmonic generation (SHG). Nonlinear optical property was discussed to confirm the SHG efficiency of the grown crystal.

Measurement of the nonlinear optical susceptibilies of porous silicon (다공질 규소의 비선형 광학감수율 측정)

  • 조창호;서영석;김영유
    • Korean Journal of Optics and Photonics
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    • v.10 no.4
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    • pp.289-293
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    • 1999
  • The nonlinear susceptibilities of the porous silicon surface were determined from the second harmonic generation. The value of nonlinear susceptibility, ${\chi}^{(2)}_{zzz}$ was $1.04{\times}10_{-7}$ esu which had an intensity of two orders of magnitude greater than that of silicon crystal wafers. The orientation angle of absorbed molecules on the porous silicon surface was ${16.8}^{\circ}$.

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A Study on Rubbing-induced Molecular Alignment on an Orientation Layer of Polyimide for Liquid Crystal Display (LCD의 폴리이미드 배향막에서 Rubbing에 의한 분자배향에 관한 연구)

  • 최승우;정재원;김승빈;황상만;천희곤;조동율
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.11 no.4
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    • pp.306-313
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    • 1998
  • To elucidate the liquid crystal(LC) molecules alignment mechanism, it is important to determine the molecular orientation of the rubbed polymer surface molecules that directly contact with LC molecules. In this work, the molecular orientation on a rubbed surface of polyimide (SE-3310, Nissan) film has been studied by polarized FTIR absorption spectroscopy. It has been found that molecular chain on the rubbed surface of polymide film are oriented along the rubbing direction and are tilted up on an average by 5.0$^{\circ}$. In the SHG(Second Harmonic Generation) measurement, the pretilt angle of molecular chain on the poylmide fim was 4.6$^{\circ}$ fro, the surface plane. And the pedit angle of liquid crystal (ZLI-2293, Merck) molecules measured by crystal rotation method was 5.4$^{\circ}$in the same rubbing condition.

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Study of electric properties of pentacene field effect transistor using C- V and SHG measurements (C-V, SHG를 이용한 pentacene FFT의 전기적 특성 연구)

  • Lim, Eun-Ju;Takaaki, Manaka;Tamura, Ryosuke;Iwamoto, Mitsumasa
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2007.06a
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    • pp.70-71
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    • 2007
  • Analyzing pentacene field effect transistors (FETs) with Au source and drain electrodes as Maxwell-Wagner effect elements, electron and hole injection from the Au electrodes into the FET channel were examined using current-voltage (I-V), capacitance-voltage (C-V) and optical second harmonic generation (SHG) measurements. Based on these results, a mechanism of the hole and electron injection into pentacene from the Au electrodes and subsequently recombination mechanism with light-emitting in the pentacene layer are discussed, with taking into account the presence of trapped charges.

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Simple method for determining the crystalline axes of nonlinear uniaxial crystal using second-harmonic generation (2차 조화파 발생을 이용하여 비선형광학 단축결정의 결정축 찾는 방법)

  • 정창수;김도석;이범구
    • Proceedings of the Optical Society of Korea Conference
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    • 2000.08a
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    • pp.92-93
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    • 2000
  • 1961년에 비선형 광학이 시작된$^{(1)}$ 이후로 비선형 광학의 큰 응용 잠재성 때문에 많은 비선형 광학 결정이 개발되어 왔고, 현재도 많은 연구실에서 제조 및 연구되고 있다. 일단 결정이 만들어지면 결정축(X,Y,Z축)이 파악되어야 모든 연구나 응용이 가능하다. 이러한 결정축의 측정은 X선, 중성자, 또는 전자를 이용하는 회절 방법을 통하여 가능하며, 이 중 X선회절 장비가 가장 많이 쓰인다.$^{(2 4)}$ 그러나 이러한 장비들은 값이 워낙 비싸서, 결정축 측정외에 그다지 쓸모가 없는 비선형 광학 물질 제조 연구실이나 광학 연구실에서는 이 장비를 구입하기가 다소 어려운 것이 현실이다. 더구나 이 방법은 해석이 복잡하다는 단점이 있다. (중략)

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