• 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.

• 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.

• Korean Journal of Optics and Photonics
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• v.4 no.2
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• pp.200-205
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• 1993

We generated the second harmonic of Ti:sapphire laser in LiI$O_3$ and BBO crystals. Two LiI$O_3$, crystals and a BBO crystal were used, and the lengths of LiI$O_3$ crystals were 5, 10 mm and that of BBO was 7 mm. We measured the conversion efficiencies of LiI$O_3$ and BBO in the wavelength range of 780-810 nm, and compared with the caculation of theory. The measured second harmonic conversion coefficients were (1.06${\pm}0.05){\times}10^4\;W^1$(10mm), (5.28${\pm}0.33){\times}10^5\;W^1$(5mm), and (2.96${\pm}0.05){\times}10^5\;W^1$(BBO, 7 mm) at the fundamental wavelength of 794 nm.

• Korean Journal of Optics and Photonics
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• v.19 no.6
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• pp.408-415
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• 2008

The characteristics of a ferroelectric-domain inverted grating fabricated by applying a high-voltage pulse at room temperature in Ti-diffused channel waveguides in z-cut $LiNbO_3$ (Ti:PPLN) were examined for channel waveguide quasi phase-matched secondharmonic generation devices. The fabrication conditions of uniform periodic domain-inversion were examined. Ti:PPLN with period ${\Lambda}=16.6{\mu}m$ for SHG were fabricated and the performances were measured. A normalized SHG efficiency as high as 473 (%/W) was obtained with 49 mm interaction length.

• Proceedings of the Optical Society of Korea Conference
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• 1996.09a
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• pp.43-43
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• 1996

• Korean Journal of Optics and Photonics
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• v.16 no.5
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• pp.456-461
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• 2005

We numerically investigate the characteristic of single Nd:YAG rod laser with the convex-plane resonator configuration in order to get the best condition for high efficient intra-cavity second harmonic generation(SHG). The beam quality is analyzed with ABCD matrixes including the thermal lensing characteristic of Nd:YAG rod. The analysis is focused on stability, M2, beam waist and mode-volume of laser beam inside the resonator. The best conditions for SHG is obtained when a laser rod is set near the curved laser mirror.

• Proceedings of the Optical Society of Korea Conference
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• 2002.11a
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• pp.70-71
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• 2002

• Journal of Korean Ophthalmic Optics Society
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• v.4 no.2
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• pp.45-49
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• 1999

The second harmonic, wavelength is 397nm, of the continuous wave diode laser, whose maximum power is 35mW, was generated in $LiIO_3$ crystals in a ring enhancement cavity. 5mm- and 10mm-long crystals cut $43.21^{\circ}$ for optic axis were used in this experiment. Both surfaces of those were anti-reflection coated for 794nm. In case the crystal was inserted into the cavity, the condition of separation between two concave mirrors for the optimum mode matching was found. The conversion efficiency of second harmonic generation was increased by the resonant enhancement of pumping power in the ring enhancement cavity, and the frequency of diode laser was locked to that of the counter-propagation mode generated from the surface of crystal. When the pumping power was 28 mW, the infrared buildup factor was about 45 without the crystal, and 14 with the crystal due to the transmission loss of crystal. The maximum second harmonic powers of $1.5{\mu}W$ and $6.6{\mu}W$ were obtained, and corresponding conversion efficiencies were $(6.584{\pm}0.56){\times}10^{-3}$%, $2.6{\pm}0.21){\times}10%{-2}$% in 5mm- and 10mm-long $LiIO_3$, respectively.

• Proceedings of the Optical Society of Korea Conference
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• 1991.06a
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• pp.50-55
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• 1991

Mg 원자선속의 냉각에 쓰일 diode laser의 특성과 이용가능성을 연구하였다. Mg 원자의 3P2-3D3 천이의 공명선 383.8nm를 얻기 위하여 Mitsubishi사의 ML형 laser diode를 택하여 주입전류와 온도를 변화시키고, 회절격자를 써서 767.6nm의 laser 광을 얻은 후 LiIO3 결정에 의해 383.8nm인 제2조화파를 생성하였다. Ring cavity 내에서 기본파가 공명할 때 증강계수는 15이었다.

• Proceedings of the Optical Society of Korea Conference
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• 2009.02a
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• pp.137-138
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• 2009