• Journal of IKEEE
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• v.9 no.2 s.17
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• pp.115-122
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• 2005

We report 400 femto-second highly stable, nearly transform-limited, pulse generation at 10 GHz in $1540{\sim}1550$ nm wavelength region by adiabatic soliton pulse compression of an actively mode-locked fiber ring laser output. Without using any supermode selection device, supermode beating noise has been suppressed below -123 dB/Hz, resulting less than 100 femto-second timing jitters at the noise band of $1\;kHz{\sim}100\;MHz$.

• Proceedings of the Optical Society of Korea Conference
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• 2007.02a
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• pp.275-276
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• 2007

본 보고서에서는 삼진 연속 영 제한 부호를 광 디스크에 채용되게 하기 위해 여러 광 신호처리 기법의 변화을 소개한다. 삼진 광 정보의 기록 재생을 위해 광 기록 재생 시스템은 파형 등화법과 멀티 펄스 기록 보정법은 물론 적합한 오류 정정법을 필요로 하고 있다.

• Safe Food
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• v.6 no.3
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• pp.11-16
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• 2011

• Korean Journal of Optics and Photonics
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• v.16 no.5
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• pp.417-422
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• 2005

When an optical pulse propagates through the atmospheric channel, it is attenuated and spreaded by the atmospheric turbulence. This pulse broadening produces the intersymbol interference(ISI) between adjacent pulses. Therefore, adjacent pulses are overlapped, and the bit rates and the repeaterless transmission length are limited by the ISI. In this paper, the ISI as a function of the refractive index structure constant that presents the strength of atmospheric turbulence is found using the temporal momentum function, and is numerically analyzed fer the basic SONET transmission rates. The numerical results show that ISI is gradually increasing at the lower transmission rate than the OC-192(9.953 Gb/s) system and is slowly converging after rapid increasing at the higher transmission rate than the OC-768(39.813 Gb/s) system as the turbulence is stronger. Also, we know that accurate information transmission is possible to 10[km] at the OC-48(2.488 Gb/s) system under any atmospheric turbulence, but is impossible under the stronger turbulence than $10^{-14}[m^{-2/3}]$ at the 100 Gb/s system, $10^{-13}[m^{-2/3}]$ at the OC-768 system, and $10^{-12}[m^{-2/3}]$ at the OC-192 system, because the ISI is seriously induced.

• Proceedings of the KIEE Conference
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• 2000.07c
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• pp.2119-2122
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• 2000

포항 방사광 가속기의 선형 가속기에서는 80-MW 클라이스트론 부하를 구동하기 위하여 최대 펄스 정격출력 200 MW(400kv 500A, 평탄도 4.4 $\mu s$)인 대출력 펄스 트랜스포머가 요구된다. 펄스 트랜스포머는 펄스 전원공급 장치(Modulator)로부터 대출력 부하(Klystron)로 펄스 에너지를 전달하며 임피던스 정합을 시키는 기능을 한다. 모듈레이터의 고전압 출력 펄스에서 RF 에너지를 발생시키는데 사용되는 유효 출력 에너지는 출력 펄스의 평탄부의 에너지에 해당된다. 그러므로, 펄스 트랜스포머는 빠른 상승시간을 가지는 것이 요구된다. 빠른 상승시간을 얻기 위하여 누설자속, 분포용량이 작게 되도록 설계하여야 한다.

• Korean Journal of Optics and Photonics
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• v.15 no.5
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• pp.449-454
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• 2004

The optical limiter is an optical component which reduces laser beam intensity for the protection of eyes and light sensors. Carbon nanotube is now known as a highly efficient optical limiting material. Optical limiting effect of the multi-walled carbon nanotube suspensions, in several kinds of solvents such as distilled water, chloroform, ethanol and ethylene glycol, were measured in the range from room temperature to near to the boiling points of the solvents. The pulsed Nd:YAG laser whose wavelength is 1064 nm and pulse duration is 6 ns was used as a light source. The experimental result shows that the limiting efficiency was reduced as the temperature increased, and the suspension which has lower boiling point, viscosity and surface tension has highest efficiency.

• The Journal of Korean Institute of Communications and Information Sciences
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• v.24 no.6B
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• pp.1134-1141
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• 1999

In this paper, we implement an optical code division multiple access(OCDMA) system and analyze the performance of the implemented system. In the implemented system, a transmitter encodes input data into optical pulses by using laser diode, and spreads the encoded pulses in an encoder which consists of 4 stage delay lines. The decoder which is the same structure as that of encoder delays and combines the spreaded pulses, and thus recovers the original data. At first, we discuss the auto- and cross-correlations of OCDMA signals under both environments of single user and multi-users, and then verify the simulation results with experimental results. We also evaluate the effect of a number of stages of delay line and code length on the system performance through computer simulations. As experimental results we can see that if the decoder have the same configuration as that of encoder, the peak auto-correlation characteristics can be achieved, and thus we can recover the original data from received data. As simulation results we can see that although bit error rate decreases as code length decreases or the number of stage of delay line increases, it is difficult to implement the system because the pulse width becomes narrow. From the results, we can apply CDMA technologies to optical communication networks.

• Proceedings of the Optical Society of Korea Conference
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• 1999.08a
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• pp.96-97
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• 1999

• Korean Journal of Optics and Photonics
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• v.6 no.2
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• pp.142-147
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• 1995

Soliton pulse outputs are generated with figure '8' type erbium-doped fiber laser mode-locked by using a fiber loop mirror. The fiber loop mirror consists of an erbium-doped fiber amplifier at the one end of the loop, and 504 m-long dispersion-shifted fiber as a nonlinear medium. By pumping with a $1.48{\mu}m$ wavelength laser diode and adjusting the polarization controllers inside the loop, soliton pulses are generated with 1574 nm center wavelength and 1.2 nm linewidth. The soliton pulses are found randomly spaced within the fundamental period corresponding to cavity round trip time. The autocorrelation trace shows that the pulse width is 2.4 ps, which is in good agreement with the theoretical prediction. The pulsewidth- bandwidth product is found to be 0.348 which means that the pulses are nearly transform-limited.imited.

• Korean Journal of Optics and Photonics
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• v.4 no.4
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• pp.447-451
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• 1993

Long pulse XeCl excimer laser with 150 ns (FWHM) pulse duration is developed using a simple capacitor-charge transfer circuit. We measured the laser pulse width varying the gas mixture ratio and capacitance ratio, which dominantly affect the pulse width. In this way we can easily stretch the pulse width from short pulse to long pulse. The pulse width was stretched by 120 ns as the partial pressure of HC1 and Xe gas was reduced under constant gas mixture ratio ([Xe]/[HCl]= 15), and by varying the capacitance ratio (Cm/Cp) under fixed pressure, the pulse width was stretched by 60 ns.