• Proceedings of the Korean Society of Precision Engineering Conference
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• 2011.06a
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• pp.151-152
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• 2011

• Proceedings of the Korean Society of Precision Engineering Conference
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• 2010.11a
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• pp.65-66
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• 2010

• Proceedings of the Optical Society of Korea Conference
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• 2001.02a
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• pp.242-243
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• 2001

고출력 펨토초 레이저 기술은 커렌즈 모드록킹 기술, Ti：sapphire 이득매질의 개발, chirped pulse amplification (CPA) 등의 도움으로 1980년대 후반부터 급속히 발전해 왔다. 생성된 펨토초 펄스의 시간적 특성을 정확히 알아내기 위한 방법들도 많이 연구되어 주파수 분해 괌게이팅(FROG)이나 주파수위상 간섭계(SPIDER) 등의 방법들이 기존의 자체상관계를 대체하게 되었다. 극초단 레이저 펄스는 넓은 스펙트럼을 갖고 첨두출력이 높기 때문에 매질이나 광학계를 지나면서 군지연분산, 자체위상변조 등의 효과에 의한 시간적 위상변화가 쉽게 생긴다. (중략)

• Proceedings of the Optical Society of Korea Conference
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• 2002.07a
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• pp.112-113
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• 2002

최근에 극초단 고출력 레이저가 개발됨에 따라 이에 의한 강한 비선형 현상중의 하나인 고차 조화파(high-order harmonics)의 발생이 가능하게 되었다. 조사 레이저와 원자 간의 결맞는 과정에 의해서 생성된 고차 조화파는 레이저와 같은 좋은 결맞음과 펨토초 이하의 아주 짧은 펄스폭을 가질 수 있기 때문에 플라즈마 진단, 극자외선 광원을 이용한 비선형 광학, 아토초 영역의 물리적 현상을 관측하는데 아주 유용한 광원이 될 것으로 여겨져 오고 있다. (중략)

• Korean Journal of Optics and Photonics
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• v.4 no.1
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• pp.66-72
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• 1993

Additive-pulse mode-locking (APM) was performed in a $1.053{\mu}m$ cw Nd:YLF laser by coupling a nonlinear external external cavity to the main cavity. The APM pulsewidth was 4.5 ps and the average output power was 1.5 W. This APM pulse was compressed by an optical fiber and a grating pair to be as short as 210 fs with a peak power of 17 kW.

• Korean Journal of Optics and Photonics
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• v.5 no.4
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• pp.466-472
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• 1994

An Argon laser pumped Ti:Sapphire laser has been constructed and self-mode locked. Mode-locking was initiated by a moving mirror mounted on the ball slider and maintained by the self-focusing in the laser crystal and an aperture inside the resonator. A prism pair was used to reduce group velocity dispersion. The bandwidth and the pulse width of the mode-locked pulse were 11 nm, $1000\pm20fs$, respectively. ively.

• Korean Journal of Optics and Photonics
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• v.1 no.1
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• pp.87-97
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• 1990

With the recent advent of various ultrashort pulse lasers, time-resolved laser spectroscopic techniques have been widely recognized as versatile tools to study ultrafast phenomena in many research areas. These techniques are currently being employed not only to study atomic and molecular physics but to characterize the excited state or the carrier dynamics on surfaces of semiconductors, metals and thin layer materials. Also the sweetching speed measurement of ultrafast electro-optic devices using ultrashort laser pulses becomes important in high-speed electronics. Here, some principles of spectroscopic techniques with ps or fs lasers and their applications are summarized briefly.

• 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.

• 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 Korean Institute of Information and Commucation Sciences Conference
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• 1999.11a
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• pp.177-183
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• 1999

In this paper, we analyze transmission characteristics of ultrashort laser pulses using the property of Raised-cosine pulse which are systematically obtained following Class-2 PRS model. The high-order pulses are easily derived front a modified PRS system model as Class-1 PRS model. This may be based on the fact that the spectra and bandwidths of the high-order pulses are beautifully related to their orders. And we make clear they are very useful to cover wider area and more accurate transmission characteristics of ultrashort pulses than Gaussian or Sech pulse approximations used conventionally. First modifying the generalized PRS system model, we propose a new model for deriving any type of high-order pulse. And we offer a novel analysis method of ultrashort pulse transmission which has any shape and FWHM, using the proposed model. In addition, by fixing the pulse range $\tau$=1(ps) and varying the order of the pulse from n=1 to n=100, we obtain spectra of ultrashort pulses with 1(ps)-100(fs) FWHM's, and width of FWHM in the Class-2 PRS model 50~100(fs) smaller than Class-1 PRS model. As a one-step further, we derive PSD's of their pulse trains when they are applied to Unipolar signaling scheme. These PSD's are derided in the range of possible pulse intervals. All of these results are not only coincided with some conventional experimental works but also will to applied to any pioneering ultrashort pulse in the future.