• 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.11 no.2
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• pp.91-96
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• 2000

We propose a novel in-line fiber optic circular polarizing mirror utilizing cholesteric lIquid crystal (CLC) polymer [11m for the fiber laser applications. Ions matrix representation of this device has been derived and venfied experimentally. In a Fabry-Perot cavity configuration, a CLC fiber optic rmrror has been used to achieve longitudinal mode suppression as well as to obtain passively mode~locked laser operations with 630 fs laser pulses via nonlinear polarization evoluhon.oluhon.

• Proceedings of the Korean Society of Precision Engineering Conference
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• 2008.11a
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• pp.749-750
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• 2008

• Proceedings of the Optical Society of Korea Conference
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• 2005.07a
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• pp.310-311
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• 2005

• Proceedings of the Korean Society of Laser Processing Conference
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• 2005.06a
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• pp.85-90
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• 2005

• Proceedings of the Korean Society of Laser Processing Conference
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• 2005.11a
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• pp.137-140
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• 2005

• Proceedings of the Korean Society of Laser Processing Conference
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• 2005.11a
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• pp.109-113
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• 2005

• Journal of the Korean Ceramic Society
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• v.31 no.8
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• pp.861-868
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• 1994

CaO-Al2O3 glass is a good candidate as optical fiber amplifier and laser. In this study, optical properties for 4I13/2longrightarrow4I15/2 transition of Er3+ ions doped in CaO-Al2O3 glasses were investigated. Optical absorptions, radiative transition probabilities and lifetimes for 4I13/2 level were evaluated by using Judd-Ofelt theory. Also, induced- emmision cross-sections of 4I13/2longrightarrow4I15/2 transition were calculated. Radiative transition probability and lifetime of 4I13/2 level were 144.6s-1, 690$mutextrm{s}$ respectively for 60CaO.40Al2O3 glass(FS0) and 152.6s-1, 660 $mutextrm{s}$ for 54 CaO.36Al2O3.10SiO2 glass (FS10). Each induced-emission cross sections for FS0 and FS10 was 0.749$\times$10-20 $\textrm{cm}^2$, 0.892$\times$10-20 $\textrm{cm}^2$. Obtained values were comparable with those of ZBLA glass studied as optical fiber amplifier and laser material.

• Proceedings of the Korean Institute of Information and Commucation Sciences Conference
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• 2017.10a
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• pp.711-713
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• 2017

Fiber Brag grating sensors were written in standard Ge-doped telecom optical fiber (Corning SMF-28) using an 800nm femtosecond laser and a phase mask. It were exposed to gamma-radiation up to a dose of 100 kGy to evaluate the radiation effect. The fs-FBG-2 sensor showed incomplete optical characteristics during irradiation, but the fs-FBG-1 sensor showed excellent radiation resistance with Bragg wavelength shift(BWS) of less than 10pm at a dose of 100 kGy.

• The Journal of the Convergence on Culture Technology
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• v.6 no.4
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• pp.721-726
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• 2020

Genetic algorithm was first introduced to study adaption phenomena occurring in nature based on Darwin's theory of survival of the fittest. It has been used when analytical approach is not possible because of a large number of variables. In this paper, we demonstrated that genetic algorithm could be used to obtain physically optimized experimental values. We programmed a genetic algorithm that uses a few Gaussian functions to find a given function value and the same algorithm was connected to the laser system to obtain laser pulses of 40fs of maximum pulse width and 1mJ of maximum output power. This study shows that genetic algorithm can be applied to laser systems to obtain the optimized laser pulses.