• 제어로봇시스템학회:학술대회논문집
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• 2001.10a
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• pp.40.3-40
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• 2001

The pulsed Nd:YAG laser is the most commonly used type of solid-state laser in many fields. In material processing and medical treatment, the power density control of a laser beam Considered to be significant, which depends on the flashlamp current pulse width and pulse repetition rate. For general laser power supply to control the laser power density, the secondary of the power transformer is connected to the rectifier and filter capacitor. The output of a rectifier is applied to a switching element in the secondary of the transformer. So power supply is complicated and the loss of switching is considerably. In addition, according to increasing pulse repetition rate, charged energy of energy-storage capacitor bank is not transferred sufficiently to flashlamp, and laser output efficiency decreases. In this study, we have ...

• Proceedings of the Optical Society of Korea Conference
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• 2001.08a
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• pp.150-151
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• 2001

• Korean Journal of Optics and Photonics
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• v.4 no.4
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• pp.442-446
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• 1993

A flashlamp pumped Ti: sapphire laser was designed and fabricated in the laboratory. In order to find out the optimum pumping condition, three kinds of discharge circuits of which the pulse width are 10${\mu}s$, 45${\mu}s$, 65${\mu}s$ were designed. The fluorescent energy converter LD-490 of which the fluorescence spectra is coincident to the absorption band of Ti: sapphire was used to improve the laser efficiency. The laser output characteristics for three different concentrations of LD-490 and for three different pumping pulse widths were measured. As a result, the shorter the flashlamp pulse width, the higher the overall efficiency was achieved. When pumping light pulsewidth was 10${\mu}s$, the best efficiency was obtained at the concentration 1.0${\times}10^{-3}$mol/l of LD-490 dye. At lower concentrations the efficiencies were decreased.

• Korean Journal of Optics and Photonics
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• v.4 no.2
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• pp.195-199
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• 1993

The output energy of Rh-6G dye laser was enhanced by the energy transfer in the mixture of Rh-6G and C-545. The laser was pumped by coaxial flashlamp filled argon gas. The optimum concentration of Rh-6G was $10_-4mol/l$ without mixing. The output energy was enhanced about 70 % at 0.4 % C-545 mixture with respect to the concentration of Rh-6G. The peak output power and the output energy were 27 kW and 50 mJ at the pumping energy of 346 J.

• Current Optics and Photonics
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• v.7 no.3
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• pp.297-303
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• 2023

In this paper, we demonstrated a high-energy (285 mJ) mid-infrared flashlamp-pumped electro-optically 𝚀-switched Er:YAG master oscillator power amplifier (MOPA) system and comprehensively investigated its temporal, spectral, and spatial characteristics. To increase the output energy, we optimized the delay between the timings at which the flashlamps of the master oscillator and power amplifier were triggered. In addition, the output energy was improved while minimizing thermal effects by cooling the MOPA system to a temperature slightly above the dew point. Consequently, the MOPA structure boosted the output energy without damaging the lithium niobate Pockels cell, which is a crucial element in 𝚀-switching. This design realized pulses with energies up to 0.285 J and pulse durations of approximately 140 ns at a wavelength of 2,936.7 nm. This high-energy mid-IR Er:YAG MOPA system can be used for various scientific, engineering, and military underwater applications.

• Proceedings of the KIEE Conference
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• 1995.07c
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• pp.1271-1274
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• 1995

In this paper, design feature and operation characteristics of compact Ruby laser for plasma diagonostics are described. A linear Xe flashlamp and a single elliptical cavity are adopted as optical pumping system. With charging energy of 484J, the maximum output energy of 170mJ, laser pulse width $110{\mu}s$, and slope efficiency 0.09% were obtained. If Q-switch system is added to this laser, we suppose this laser will be quite enough for diagonizing plasma.

• Proceedings of the Optical Society of Korea Conference
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• 1988.06a
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• pp.26-28
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• 1988

펌핑과의 스펙트럼을 전환시켜 색소레이저의 에너지를 증가시키기 위하여 에너지 전환색소 BBQ를 레이저색소 LD490에 첨가하여 실험하였다. rise time이 비교적 짧은 Ar flashlamp로서 펌핑하였고, 주입에너지는 160J이다. LD490의 레이저발진의 최적농도의 4$\times$10-10M/1에서 BBQ의 첨가농도를 바꾸면서 실험한 결과 4.5$\times$10-10M/1일 때 최대의 증가율을 보이고 이때 레이저 증가율은 180%까지 도달하였다. 레이저출력 증가율은 92%이다.

• Proceedings of the IEEK Conference
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• 2001.06e
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• pp.211-214
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• 2001

For general laser power supply, the secondary of the power transformer is connected to the rectifier and filter capacitor. The output of a rectifier is connected to a switching element in the secondary of the transformer. So the Dower supply is complicated and the loss of switching is considerably. In addition, according to increasing pulse repetition, charged energy of energy-storage capacitor is not transferred sufficiently to flashlamp, and laser output efficiency decreases. In this raper, to improve laser efficiency, we designed and fabricated the power supply in which the SCR was turned on in zero point by the methods of ZCC(zero crossing control), PFN(pulse forming network) in result, laser output efficiency increased by hte 4% other than conventional supply, when a repetition rate was increased by the 10[pps], In 20(pps), efficiency was increased by about 8%

• Korean Journal of Optics and Photonics
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• v.1 no.2
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• pp.204-209
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• 1990

The temperature variation at a laser rod center induced by high repetetion rate pumping was measured by counting the number of inteference frigne shift and found to be consistent with the theoretical value obtained from heat diffusion equation. The spatial homogeneity and energy transfer rate of flashlamp pumping by the single elliptical reflector plated with gold were evaluated by measuring interference fringes oever the cross section of a Nd:YAG laser rod.

• Proceedings of the Optical Society of Korea Conference
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• 1989.02a
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• pp.20-25
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• 1989

The nonlinear, time dependent photon transport equations of Frantz and Nodvik, which describe the amplification of an optical pulse in an active medium, are modified to a simpler equation which describes only the amplification of energy. with this equation, the output energy of the high power YLF(Nd3+)-Phosphate Glass(Nd3+) Laser System is calculated. When the stored energy density Est is 0.10J/㎤, 0.16J/㎤, 0.228J/㎤, and 0.50J/㎤, and with the assumption of uniform population inversion density, the final output energy of this laser system is 5.38J, 176J, 317J, and 283J, respectively. The gain saturation causes distortion of the output beam. This phenomenon is described in detail at the first three rod amplifier systems in the case of E=0.228J/㎤. The peak current and decay time constant of the flashlamps, which are used to obtain population inversion in the active medium, are investigated. The flashlamp driving circuit which has optimum operational performance should have {{{{ SQRT { LC} }} time about 100$\mu$sec.