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Rotation of the polarization ellipse for broad-band and narrow-band optical pulses. Analytical solutions
In present days the evolution of broad-band laser pulses, propagating in various types of waveguides, has been of a great interest among the scientists. Currently, it is easy for phase-modulated femtosecond pulses the condition Δω≈ω 0 to be obtained. It is known that nowadays it is possible also to...
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Published in: | Journal of physics. Conference series 2023-05, Vol.2487 (1), p.12031 |
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creator | Kasapeteva, Z Dakova, A Slavchev, V Dakova, D Kovachev, L |
description | In present days the evolution of broad-band laser pulses, propagating in various types of waveguides, has been of a great interest among the scientists. Currently, it is easy for phase-modulated femtosecond pulses the condition
Δω≈ω
0
to be obtained. It is known that nowadays it is possible also to reach the attosecond region where the spectral bandwidth of the pulse happens to be of order of the carrier frequency also. Light pulses who fulfil this initial condition are called broad-band. On the other hand, the non-fulfilling pulses are the narrow-band ones.
In the present paper it is investigated the parametric interaction of two components of one optical pulse by using the Generalized System of Nonlinear Amplitude Equations (GSNAE). GSNAE was analytically solved. A difference in the period of oscillations of the energy exchange between the two components is found. |
doi_str_mv | 10.1088/1742-6596/2487/1/012031 |
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Δω≈ω
0
to be obtained. It is known that nowadays it is possible also to reach the attosecond region where the spectral bandwidth of the pulse happens to be of order of the carrier frequency also. Light pulses who fulfil this initial condition are called broad-band. On the other hand, the non-fulfilling pulses are the narrow-band ones.
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Δω≈ω
0
to be obtained. It is known that nowadays it is possible also to reach the attosecond region where the spectral bandwidth of the pulse happens to be of order of the carrier frequency also. Light pulses who fulfil this initial condition are called broad-band. On the other hand, the non-fulfilling pulses are the narrow-band ones.
In the present paper it is investigated the parametric interaction of two components of one optical pulse by using the Generalized System of Nonlinear Amplitude Equations (GSNAE). GSNAE was analytically solved. 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Δω≈ω
0
to be obtained. It is known that nowadays it is possible also to reach the attosecond region where the spectral bandwidth of the pulse happens to be of order of the carrier frequency also. Light pulses who fulfil this initial condition are called broad-band. On the other hand, the non-fulfilling pulses are the narrow-band ones.
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source | Publicly Available Content Database; Free Full-Text Journals in Chemistry |
subjects | Carrier frequencies Exact solutions Femtosecond pulses Optical pulses Physics Pulse propagation Wave propagation Waveguides |
title | Rotation of the polarization ellipse for broad-band and narrow-band optical pulses. Analytical solutions |
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