On the self‐induced transparency effect of the three‐wave resonance process

1978 ◽  
Vol 19 (1) ◽  
pp. 168-176 ◽  
Author(s):  
S. C. Chiu
Keyword(s):  
The Self ◽  
Wave Resonance ◽  
Induced Transparency ◽  
Resonance Process

The Influence of Level Degeneracy on the Self-Induced Transparency Effect

1968 ◽  
Vol 21 (16) ◽  
pp. 1151-1155 ◽  
Author(s):  
C. K. Rhodes ◽  
A. Szöke ◽  
A. Javan
Keyword(s):  
The Self ◽  
Level Degeneracy ◽  
Induced Transparency

The effect of retarded interaction on the self-induced transparency phenomenon

1979 ◽  
Vol 92 (2) ◽  
pp. 467-472
Author(s):  
V. R. Nagibarov ◽  
O. Kh. Khasanov
Keyword(s):  
The Self ◽  
Induced Transparency

Coupled-mode analysis of the self-induced-transparency soliton switch

1992 ◽  
Vol 46 (3) ◽  
pp. 1594-1605 ◽  
Author(s):  
A. Guzman ◽  
F. S. Locati ◽  
M. Romagnoli ◽  
S. Wabnitz
Keyword(s):  
The Self ◽  
Mode Analysis ◽  
Coupled Mode ◽  
Induced Transparency

Exact Solutions of the Self-Induced Transparency Equations

1971 ◽  
Vol 27 (6) ◽  
pp. 330-333 ◽  
Author(s):  
R. K. Bullough ◽  
F. Ahmad
Keyword(s):  
Exact Solutions ◽  
The Self ◽  
Induced Transparency

Formation of a Cesium Plasma by Continuous-Wave Resonance Excitation

2000 ◽  
Vol 54 (8) ◽  
pp. 1245-1249 ◽  
Author(s):  
Dimitri Pappas ◽  
Benjamin W. Smith ◽  
Nicolo Omenettó ◽  
James D. Winefordner
Keyword(s):  
Radiative Decay ◽  
Continuous Wave ◽  
Nonlinear Behavior ◽  
Optical Emission ◽  
Resonance Excitation ◽  
Number Density ◽  
Charge Coupled Device ◽  
Wave Resonance ◽  
Cesium Plasma ◽  
Resonance Process

The generation of a plasma in cesium vapor via a resonance process is described. The maximum irradiance used was 1.5 W/cm2, which is several orders of magnitude lower than the irradiances conventionally used to form plasmas. Plasma emission consisted of radiative decay from excited-state Cs atoms. Optical emission from the plasma was observed from laser powers of 200 μW with a nonintensified charge-coupled device (CCD). The ionization efficiency of the plasma was approximately 0.001, with the majority of the atoms in the plasma ionized. The plasma was found to behave linearly with respect to laser power; however nonlinear behavior was observed as the number density was altered. A collisional mechanism is proposed for the formation of the plasma.

THE QUADRATIC STARK EFFECT AND ONE-PHOTON SELF-INDUCED TRANSPARENCY

1988 ◽  
Vol 02 (07) ◽  
pp. 849-852
Author(s):  
A.A. ZABOLOTSKII
Keyword(s):  
Frequency Shift ◽  
Soliton Solution ◽  
Stark Effect ◽  
The Self ◽  
Nonlinear Frequency ◽  
Self Consistent ◽  
Quadratic Stark Effect ◽  
Induced Transparency ◽  
Nonlinear Frequency Shift

The self-consistent Maxwell-Bloch Eqs. containing linear detuning and nonlinear frequency shift are considered. The soliton solution is found and discussed. The new regimes of self-induced transparency are predicted.

Multi-Soliton Solutions for an Inhomogeneous Nonlinear Schrödinger– Maxwell–Bloch System in the Erbium-Doped Fiber

2011 ◽  
Vol 66 (12) ◽  
pp. 712-720 ◽  
Author(s):  
Ming Wang ◽  
Wen-Rui Shan ◽  
Xing Lü ◽  
Bo Qin ◽  
Li-Cai Liu
Keyword(s):  
Phase Shift ◽  
Symbolic Computation ◽  
Soliton Solutions ◽  
Nonlinear Effects ◽  
The Self ◽  
Optical Pulses ◽  
Nonlinear Schrödinger ◽  
Erbium Doped ◽  
Variable Dispersion ◽  
Induced Transparency

Under investigation in this paper is an inhomogeneous nonlinear Schrödinger-Maxwell-Bloch system with variable dispersion and nonlinear effects, which describes the propagation of optical pulses in an inhomogeneous erbium-doped fiber. Under certain coefficient constraints, multi-soliton solutions are obtained by the Hirota method and symbolic computation. Evolution and interaction of the solitons are plotted, and the self-induced transparency effect caused by the doped erbium atoms is found to lead to the change of the soliton velocity and phase. Overall phase shift can be observed when the parameter accounting for the interaction between the silica and doped erbium atoms is taken as a constant.

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