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1999
The present chapter is devoted to presenting the theory of four-wave mixing in semiconductor optical amplifiers (SOAs). At first, a model describing the dynamics in terms of rate equations is developed. The rate equations are derived from density matrix equations, and after coupling with the propagation equation for the field envelope and its phase, a ...
K. Obermann, A. Mecozzi, J. Mørk
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The present chapter is devoted to presenting the theory of four-wave mixing in semiconductor optical amplifiers (SOAs). At first, a model describing the dynamics in terms of rate equations is developed. The rate equations are derived from density matrix equations, and after coupling with the propagation equation for the field envelope and its phase, a ...
K. Obermann, A. Mecozzi, J. Mørk
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1985
OPC in four-wave mixing (FWM) has been realized for various third-order optical nonlinearities. Irrespective of the type of third-order nonlinearity of a medium, a phenomenological study of the generation of a phase-conjugated wave in FWM is carried out in much the same way.
Boris Ya. Zel’dovich +2 more
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OPC in four-wave mixing (FWM) has been realized for various third-order optical nonlinearities. Irrespective of the type of third-order nonlinearity of a medium, a phenomenological study of the generation of a phase-conjugated wave in FWM is carried out in much the same way.
Boris Ya. Zel’dovich +2 more
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International Meeting on Instabilities and Dynamics of Lasers and Nonlinear Optical Systems, 1985
We have extended the work of Kai Druhl, Bob Wenzel and John Carlsten1 on solitons in stimulated Raman scattering to include four-wave mixing phenomena. We have studied coherent anti-Stokes Raman scattering (CARS) and second Stokes generation (SSG). We have found that CARS exhibits a soliton-like structure, whereas SSG exhibits a real soliton.
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We have extended the work of Kai Druhl, Bob Wenzel and John Carlsten1 on solitons in stimulated Raman scattering to include four-wave mixing phenomena. We have studied coherent anti-Stokes Raman scattering (CARS) and second Stokes generation (SSG). We have found that CARS exhibits a soliton-like structure, whereas SSG exhibits a real soliton.
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2004
Four-Wave-Mixing (FWM), or sometimes four-photon-mixing (FPM), describes a nonlinear optical effect at which four waves or photons interact with each other due to the third order nonlinearity of the material. As a result, new waves with sum and difference frequencies are generated during the propagation in the waveguide.
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Four-Wave-Mixing (FWM), or sometimes four-photon-mixing (FPM), describes a nonlinear optical effect at which four waves or photons interact with each other due to the third order nonlinearity of the material. As a result, new waves with sum and difference frequencies are generated during the propagation in the waveguide.
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1988
Nonlinear optics began with harmonic generation and frequency mixing. Dynamics hardly entered the analysis, which was aimed at obtaining steady-state conversion efficiences from known nonlinear susceptibilities or vice versa. From the perspective of nonlinear dynamics, which developed via laser physics [1] and optical bistability [2,3] the non ...
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Nonlinear optics began with harmonic generation and frequency mixing. Dynamics hardly entered the analysis, which was aimed at obtaining steady-state conversion efficiences from known nonlinear susceptibilities or vice versa. From the perspective of nonlinear dynamics, which developed via laser physics [1] and optical bistability [2,3] the non ...
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Laser Diagnostics and Minor Species Detection in Combustion Using Resonant Four-Wave Mixing
Progress in Energy and Combustion Science, 2011Paul Ewart, Johannes Kiefer
exaly