• Korean Journal of Optics and Photonics
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• v.5 no.2
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• pp.238-244
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• 1994

We numerically studied on the dark solitons propagation for initial amplitude and phase shapes in the normalized nonlinear Schr dinger equation(NLSE) which describes the propagations of optical solitons. As the propagation distance increases, odd dark solitons evolve into a black soliton and pairs of gray solitons which have a different sign of blackness, and even dark solitons evolve into pairs of gray solitons without black solitons. When there exists a black soliton and a gray soliton, even though the initial amplitude shape is same, the sign of blackness of a gray solitons determines whether they would collide or not. We could see that the energy of dark solitons evolve into a couple of solitons of different blackness since there exists a continuous range of dark solitons with arbitrary blackness parameter, and this phenomenon was more clearly seen from the change of phase shapes from that of amplitude shapes. hapes.

• Proceedings of the Korean Vacuum Society Conference
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• 2013.02a
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• pp.529-529
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• 2013

플라즈마를 진단하는 데에는 장비적으로나 현실적으로 많은 제약이 따른다. 따라서 측정 할 수 있는 parameter가 적다. 그리고 진단 장비의 성능에 따라서 측정된 data의 신뢰도가 결정된다. 그래서 플라즈마에 레이저를 쏘아서 생성되는 솔리톤의 RADIATION을 이용하여 플라즈마의 특성을 파악하려고 한다. 본 시뮬레이션은 Particle-In-Cell (PIC) 시뮬레이션을 이용하여 Underdense 플라즈마에 Terahertz 레이저를 쏘았을 경우 발생되는 솔리톤의 특성을 파악하였다. 2D 시뮬레이션으로 수행하였으며 플라즈마는 Underdense 플라즈마를 이용하였다. 레이저 Focusing 점의 위치와 솔리톤의 주파수, 플라즈마의 밀도 gradient 에 따른 솔리톤의 이동 및 특징, 플라즈마 밀도에 따른 솔리톤의 특징을 살펴보았다.

• Korean Journal of Optics and Photonics
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• v.10 no.6
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• pp.487-493
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• 1999

In this paper, we studied the characteristics of a soliton coupler using a bent nonlinear waveguide. The bent soliton coupler has very ,harp switching characteristic like the conventional soliton coupler due to the threshold effect of soliton emi,sion from the nonlinear waveguide. By using the bent structure, we can reduce the threshold power for the soliton emission. We consider the saturation effect of nonlinearity and the loss in the medium for more accurate and practical numerical analysis in wave propagation through the bent soliton coupler. The simulation results show that the consideration of the saturation effect and the ]os~ may be very important in the analyses and design of the nonlinear waveguide devices. The bent structure is useful for the emission of the spatial soliton with the low threshold power, when we consider the saturation and the loss effect. ffect.

• Korean Journal of Optics and Photonics
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• v.6 no.4
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• pp.345-351
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• 1995

We have studied experimentally the propagation characteristics of fundamental dark spatial solitons on finite-width backgrounds and conpared with the result of numerical simulations. It was verified experimentally that the width of dark solitons decreased but that of background increased as the beam intensity increased. The refractive index change obtained from soliton constant, which is for infinite-width background, was smaller than that from Z-scan method. Numerical simulations of fundamental dark solitons on a finite-width backgrounds showed that the peak intensity of background, the width of dark soliton and the soliton constant varied with the propagation length. If the change of soliton constant on finite-width backgrounds was considered, the refractive index change was in good agreement with that from Z-scan method. ethod.

• Proceedings of the Optical Society of Korea Conference
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• 2003.07a
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• pp.12-13
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• 2003

광 솔리톤은 고속, 장거리 광통신시스템에서 분산과 self-phase modulation(SPM)에 의한 문제를 해결하기 위한 효과적인 기술 중의 하나이다. 현재, 솔리톤 전송은 장거리 해저 광전송시스템 뿐만 아니라 중거리 및 근거리 고속 전송시스템에서도 적용하기 위한 연구가 집중되고 있다. 특히, 솔리톤 전송은 광전중계기 없이 장거리 전송이 가능한 장점으로 인하여 기존의 중, 단거리링크를 초고속링크로 업그레이드하기 위하여 많은 연구가 진행되고 있다. (중략)

• Korean Journal of Optics and Photonics
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• v.12 no.6
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• pp.507-510
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• 2001

A numerical analysis based on the nonlinear Schroedinger equation is presented to analyze the propagation stability of the average soliton in a simple nonlinear amplifying loop mirror. The ratio of amplification period to soliton period and the length fraction of the erbium-doped fiber in the loop are varied to investigate their effects on the soliton stability. It is observed that stable soliton propagation is obtained even when the amplification period is only slightly shorter than the soliton period when the length fraction of the erbium-doped fiber in the loop is small, which is different from the previously published condition for stable average soliton propagation.

• The Journal of Korean Institute of Communications and Information Sciences
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• v.19 no.7
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• pp.1191-1202
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• 1994

We numerically investigate a stable propagation regime of soliton pulse trains in fibers with periodically copensated loss by lumped optical amplifiers. When amplification solition pulses is 1.2~1.5 and the minimum soliton separation normalized by the soliton width becomes about 6. In cases of L=50[km], the allowable range of A is 1.5~1.7 under =6. The maximum allowable variation of the loss compensation in each lumped amplifier becomes +-2% of the fiber loss when L=50[km], A=1.6, and =6. Generally, the allowable rages of the soliton amplitude A and amplifier gain are inversely proportional to the amplification period L.

• Korean Journal of Optics and Photonics
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• v.8 no.4
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• pp.308-314
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• 1997

We have studied the generation of an array of dark spatial solitons in a self-deforcusing medium. Unlike a single fundamental dark spatial soliton, we show numerically that the generation of an array of dark spatial solitons from a spatially sinusoidal input beam needs an adiabatic amplification of nonlinear refractive index with the beam propagation distance. In experiment, we establish a Mach-Zehnder interferometer for making the sinusoidal input beam and use a cylindrical lens for the adiabatic amplification. We observe that the dark soliton's dip-width becomes narrower and the background intensity distribution becomes flatter with increasing the nonlinearity.

• Korean Journal of Optics and Photonics
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• v.12 no.1
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• pp.48-54
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• 2001

We investigate the generation of the dark spatial soliton and its role of wave guiding in Fe doped$LiNbO_3$ A cw Ar+ laser of 488 nm is used for the generation of the dark spatial soliton. The generation of the dark spatial soliton is observed even at the laser intensity as low as 10 mW/cm2. The self-defocusing effect is observed when the direction of the intensity variation is parallel to the optic axis, while it can't be seen when perpendicular to the axis. So, it is verified that the refractive index change is generated parallel to the optic axis. When 633 nm He-Ne laser beam is injected into the dark spatial soliton, the beam propagates just as in the diffraction free medium. So, it is verified that the dark spatial soliton can act as a waveguide.eguide.

• Proceedings of the Optical Society of Korea Conference
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• 2000.02a
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• pp.312-313
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• 2000

공간솔리톤(spatial soliton)은 빔이 매질을 진행할 때 자기집속 효과(self-focusing effect) 와 자기확산 효과(self-defocusing effect)에 의해서 회절이 보상되어 형성된다. Kerr 매질에서는 굴절률의 변화가 빔의 세기에 비례하하므로 솔리톤을 발생시키기 위해서는 수 MW/$ extrm{cm}^2$ 이상인 빔의 세기가 요구된다. 광굴절 매질은 광굴절효과에 의해서 굴절률의 변화로 공간솔리톤을 발생시킨다. 비균일한 빔이 매질에 입사되면 전도대로 여기된 free carrier가 분포 차이에 의해서 확산이 일어나게 된다. 그리고 외부에서 걸어준 전기장 및 광기전력 효과로 인한 drift가 일어나게 되고 이것에 의해 생긴 공간 전하장(space charge field)에 의하여 굴절률의 변화가 생긴다. (중략)