• Title/Summary/Keyword: Second harmonic generation

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The Surface Morphology of Polymer Langmuir Film (고분자 Langmuir 박막의 표면형상)

  • Jung, Chi-Sup
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.18 no.1
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    • pp.81-88
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    • 2005
  • The Langmuir monolayers of polyamic acid salts with three kinds of alkyl chains have been investigated by means of conventional $\pi$-A isotherms and second harmonic generation measurements proposed in this paper. The surface molecular density dependence of second harmonic intensity clearly shows the region of aggregation while corresponding $\pi$-A isotherm doesn't show any changes in the surface morphology at the same region. The surface morphology analysis based on the second harmonic measurement was consistent with the Brewster angle microscope measurement results.

Efficient Second Harmonic Generation of Pulsed Nd-YAG Laser Radiation with Noncritically Phase-Matchable $LiNbO_3$ in Room-Temperature

  • Jong-Soo Lee;Bong-Hoon Kang;Bum Ku Rhee;Chong-Don Kim;Gi-Tae Joo
    • The Korean Journal of Ceramics
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    • v.6 no.3
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    • pp.206-208
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    • 2000
  • 0.65 mol% MgO-doped LiNbO$_3$single crystals were grown by CZ method. The obtained single crystals were colorless and transparent. Noncritically phase-matched second harmonic generation (SHG) of 532-nm radiation from 1064-nm in MgO-doped LiNbO$_3$has been investigated by using pulsed Nd:YAG laser. The phase-matching temperature was room temperature. SHG conversion efficiencies were typically achieved higher than 50% at the phase-matching temperature with no photorefractive damage in the region of fundamental power density which was used in this experiment. The thermo-birefringence coefficient and the electro-birefringence coefficient of SHG were calculated from the temperature phase-matching profile with the electric field.

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Second harmonic generation of YCOB($YCa_4O(BO_3)_3$) (YCOB($YCa_4O(BO_3)_3$)의 제2조화파 발생)

  • 장원권
    • Korean Journal of Optics and Photonics
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    • v.10 no.4
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    • pp.301-305
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    • 1999
  • The phase matching conditions of the new optical crystal grown by Czochralski pulling method, YCOB($YCa_4O(BO_3)_3$) with wavelength were suggested, and the second harmonic generation efficiency for the fundamental of Nd:YAG laser of 1064 nm was investigated. The variation of nonlinearity with rare earth ion doping was also investigated by measuring the second harmonic generation efficiencies of $Yb^{3+}$ + $Nd^{3+}$and ion doped YCOBs.

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Second Harmonic Generation on the Surface of Porous Silicon Superlattice (초격자 다공질규소 표면에서 제 2고조파 발생)

  • Cho, Chang-Ho;Park, Jong-Dae
    • The Journal of Natural Sciences
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    • v.12 no.1
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    • pp.31-39
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    • 2002
  • Second harmonic generation was measured in porous silicon superlattices surface which were made by changing and anodization current density and the anodization time periodically in the process of obtaining porous silicon. The technique of second harmonic generation is used as a probe to the surface of porous silicon superlattice by using Nd:YAG laser. We have investigated the surface structure and nonlinear-optics properties of porous silicon superlattice.

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Second Harmonic Generation of Low Power Laser Diode Using a Ring Enhancement Cavity (고리형 Enhancement Cavity 를 이용한 저출력 반도체 레이저의 제2조화파 발생)

  • 오차환
    • Korean Journal of Optics and Photonics
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    • v.4 no.2
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    • pp.206-211
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    • 1993
  • We carried out the second harmonic generation of low power CW laser diode with maximum power of 30 mW in $LilO_3$ crystals. We used a ring enhancement cavity to increase the second harmonic conversion efficiency. The ring enhancement cavity was Composed of two flat mirrors and two concave mirrors. The focal length of concave mirrors was 25 mm, and 5 mm long and 10 mm long $LilO_3$ crystals were used. We measured the second harmonic power according to the pumping power and compared with theoretical value. We obtained 397 nm second harmonic power of about $6.6{\mu}W$ in 10 mm long $LilO_3$ crystal with the fundumental 794 nm pumping power of 28 mW.

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Second Harmonic Generation and Frequency Stabilization of a Diode Laser Using an External Ring Resonator

  • Kwon, Taeg-Yong;Yang, Sung-Hoon;Lee, Ho-Seong
    • Journal of the Optical Society of Korea
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    • v.2 no.1
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    • pp.1-4
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    • 1998
  • The second harmonic light of an 842 nm diode laser was generated from a KNbO3 crystal in an external ring resonator. The power of the second harmonic light was about 0.8 mV at an input fundamental power of 87 mW. The laser frequency was stabilized to the resonance frequency of the ring resonator, and the frequency fluctuation was measured as about 3 MHz.

DIRECT PROBING OF CARRIER MOTION IN ORGANIC FIELD EFFECT TRANSISTOR BY OPTICAL SECOND HARMONIC GENERATION

  • Iwamoto, Mitsumasa;Manaka, Takaaki;Lim, Eun-Ju
    • 한국정보디스플레이학회:학술대회논문집
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    • 2008.10a
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    • pp.1561-1563
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    • 2008
  • We report an optical second harmonic generation measurement that allows direct probing of dynamical carrier motion in organic field effect transistors. Carrier injection and transport process are discriminated. The mobility and contact resistance of pentacene FETs are determined from the visualized diffusion-like carrier motion.

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Characteristics of multi-stage dye laser amplification and Second Harmonic Generation (색소레이저의 다단 증폭 및 SHG 특성)

  • 이영우
    • Journal of the Korea Institute of Information and Communication Engineering
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    • v.8 no.4
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    • pp.946-949
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    • 2004
  • We obtained ultra-short single pulse with an energy of 80 uJ from Distributed feedback Dye laser. Using three stages of amplifiers constructed by two stages of dye amplifiers and one bethune cell amplifier, we obtained high power pulse and second harmonic generation with BBO in ultraviolet region.

Estimation of the Ratio of Nonlinear Optical Tensor Components by Measuring Second Harmonic Generation and Parametric Down Conversion Outputs in a Single Periodically Poled LiNbO3 Crystal

  • Kumar, CH. S.S. Pavan;Kim, Jiung;Kim, Byoung Joo;Cha, Myoungsik
    • Current Optics and Photonics
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    • v.2 no.6
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    • pp.606-611
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    • 2018
  • Measurement of the nonlinear optical coefficients is not an easy task since it requires complicated experimental setup and analysis. We suggest an easy way to estimate the relative nonlinear optical tensor components by direct measurement of the output powers of the second harmonic generation and spontaneous parametric down conversion experiments. The experiments were done in quasi-phase-matched type-0 as well as type-1 interactions at similar pump wavelengths in a 5% MgO-doped periodically poled $LiNbO_3$ crystal to obtain the ratio of the nonlinear optical tensor components $d_{33}/d_{31}$ in each experiment. The obtained ratios were then compared with the previously ascertained values [J. Opt. Soc. Am. B, 14, 2268-2294 (1997)].