• Title/Summary/Keyword: spatial soliton

Search Result 11, Processing Time 0.023 seconds

The generation of dark spatial soliton in photorefractive photovoltaic medium (광굴절 광기전력 물질에서의 어두운 공간솔리톤 발생)

  • 전진호;전남희;이원규;노영철;이재형;장준성
    • Korean Journal of Optics and Photonics
    • /
    • v.12 no.1
    • /
    • pp.48-54
    • /
    • 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.

  • PDF

Soliton coupler using a bent nonlinear waveguide (굽은 비선형 도파로를 이용한 솔리톤 결합기)

  • 정준영;강병한;정제명
    • Korean Journal of Optics and Photonics
    • /
    • v.10 no.6
    • /
    • pp.487-493
    • /
    • 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.

  • PDF

Propagation Characteristics of Fundamental Dark spatial Solitons on Finite-width Backgrounds (유한한 폭을 갖는 배경에서 기본 어두운 공간 솔리톤의 진행특성)

  • 김광훈;문희종;임용식;이재형;장준성
    • Korean Journal of Optics and Photonics
    • /
    • v.6 no.4
    • /
    • pp.345-351
    • /
    • 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.

  • PDF

Dark Spatial Soliton Generation in the Photorefractive Photovoltaic Material (광굴절 광기전력 매질에서 어두운 공간솔리톤 발생)

  • 전남희;전진호;이재형;장준성
    • Proceedings of the Optical Society of Korea Conference
    • /
    • 2000.02a
    • /
    • pp.312-313
    • /
    • 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)

  • PDF

An array of dark spatial solitons generated by an adiabatic amplification of nonlinear refractive index with the beam propagation distance (진행거리에 따른 비선형 굴절률의 점진적 증폭에 의하여 생성된 어두운 공간솔리톤 배열)

  • 전진호;김광훈;문희종;고광훈;이원규;노영철;이재형;장준성
    • Korean Journal of Optics and Photonics
    • /
    • v.8 no.4
    • /
    • pp.308-314
    • /
    • 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.

  • PDF

Three-dimensional odd ring dark spatial solitons

  • Kim, Guang-Hoon;Jeon, Jin-Ho;Noh, Young-Chul;Ko, Kwang-Hoon;Moon, Hee-Jong;Lee, Jai-Hyung;Chang, Joon-Sung
    • Journal of the Optical Society of Korea
    • /
    • v.1 no.2
    • /
    • pp.104-109
    • /
    • 1997
  • The propagation properties of three-dimensional dark spatial solitons having odd ring formation is analyzed numerically in the frame of the (1 + 2)-dimensional nonlinear Schrodinger equation and compared with a pair of odd dark solitons. We discuss the experimental excitation condition of an odd ring dark soliton, which is superimposed on a finite-width background beam, with phase masks.

Single Carrier Spectroscopy of Bisolitons on Si(001) Surfaces

  • Lyo, In-Whan
    • Proceedings of the Korean Vacuum Society Conference
    • /
    • 2010.02a
    • /
    • pp.13-13
    • /
    • 2010
  • Switching an elementary excitation by injecting a single carrier would offer the exciting opportunity for the ultra-high data storage technologies. However, there has been no methodology available to investigate the interaction of low energy discrete carriers with nano-structures. In order to map out the spatial dependency of such single carrier level interactions, we developed a pulse-and-probe algorithm, combining with low temperature scanning tunneling microscopy. The new tool, which we call single carrier spectroscopy, allows us to track the interaction with the target macrostructure with tunneling carriers on a single carrier basis. Using this tool, we demonstrate that it is possible not only to locally write and erase individual bi-solitons, reliably and reversibly, but also to track of creation yields of single and multiple bi-solitons. Bi-solitons are pairs of solitons that are elementary out-of-phase excitations on anti-ferromagnetically ordered pseudo-spin system of Si dimers on Si(001)-c(42) surfaces. We found that at low energy tunneling the single bisoliton creation mechanism is not correlated with the number of carriers tunneling, but with the production of a potential hole under the tip. An electric field at the surface determines the density of the local charge density under the tip, and band-bending. However a rapid, dynamic change of a field produces a potential hole that can be filled by energetic carriers, and the amount of energy released during filling process is responsible for the creation of bi-solitons. Our model based on the field-induced local hole gives excellent explanation for bi-soliton yield behaviors. Scanning tunneling spectroscopy data supports the existence of such a potential hole. The mechanism also explains the site-dependency of bi-soliton yields, which is highest at the trough, not on the dimer rows. Our study demonstrates that we can manipulate not just single atoms and molecules, but also single pseudo-spin excitations as well.

  • PDF

Anomalous Propagation Characteristics of an Airy Beam in Nonlocal Nonlinear Medium

  • Wu, Yun-Long;Ye, Qin;Shao, Li
    • Current Optics and Photonics
    • /
    • v.5 no.2
    • /
    • pp.191-197
    • /
    • 2021
  • The anomalous propagation characteristics of a single Airy beam in nonlocal nonlinear medium are investigated by utilizing the split-step Fourier-transform method. We show that besides the normal straight propagation trajectory, the breathing solitons formed by the interaction between Airy beam and nonlocal nonlinear medium can propagate along the sinusoidal trajectory, and the anomalous trajectory can be modulated arbitrarily by altering the initial amplitude and the nonlocal nonlinear coefficient. In addition, the initial amplitude and the nonlocal nonlinear coefficient can have inverse impacts on the formation and transformation of the equilibrium state of spatial solitons, when the two parameters are larger than certain values. Therefore, the reversible transformation of the evolution dynamics of two soliton states can be realized by adjusting those two parameters properly. Finally, it is shown that the propagation properties of the solitons formed by the interaction between Airy beam and nonlocal nonlinear medium can be controlled arbitrarily, by adjusting the distribution factor and nonlocal coefficient.

Propagation and interaction of two dimensional solitary waves in organic single crystal of polydiacetylene para-toluene sulfonate (유기단결정 Polydiacetylene Para-toluene Sulfonate에서 2차원 공간고립파의 진행과 상호 작용 전산모의)

  • 류재명;조재흥;황보창권;정진호
    • Korean Journal of Optics and Photonics
    • /
    • v.13 no.5
    • /
    • pp.400-407
    • /
    • 2002
  • Two dimensional solitary waves are stably propagated in a saturable medium which has a saturable nonlinear index as input intensity. However, in the case of low intensity. a negative fifth-order nonlinear medium has properties of a saturable medium. So a Gaussian beam travels stably. The propagation process into the fifth order nonlinear medium of the Gaussian beam with a weak intensity is investigated by using the computer simulation of the two-dimensional nonlinear Schrodinger equation. As a result, it is confirmed that the two-dimensional spatial solitary waves are stably propagated in this medium when the incident powers are self-trapping powers. In the condition of the phase difference and collisional angle between two input beams of 180 degree and 0.05 degree, respectively, we can confirm that all optical switching is as simple as controlling the incident power of one input beam.