2020
DOI: 10.21608/ajbas.2020.39888.1030
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Modulation of the Nonlinear Ion Acoustic Waves in a Weakly Relativistic Warm Plasma with Nonextensively Distributed Electrons

Abstract: A reductive perturbation technique (multiple scales) is applied to a weakly relativistic warm unmagnetized adiabatic plasma system consisting of inertial ions fluid and nonextensively distributed electrons. A nonlinear Schrödinger-type (NST) equation for finite wavenumber at the second order is derived. Using the reductive perturbation technique we derived the corresponding Korteweg-de Vries (K-dV) equation. For small wavenumber limit the K-dV equation is transformed into NST equation. It is found that the coe… Show more

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“…Equation (4) is a generalized cubic‐quintic NLS equation with cubic derivative terms. It is known to govern the propagation of ultrashort pulses in a single‐mode optical fiber, [ 47 ] the modulations of weakly nonlinear ions in acoustic plasma waves, [ 48 ] ferromagnetic chain, [ 49 ] evolutions of Stokes waves, [ 50 ] soliton propagation in optical fibers, and metamaterials, [ 51,52 ] etc. Equation (4) can also be applied to the description of high‐intensity pulse propagation, [ 53 ] controllable self‐steepening, [ 54 ] and generation of Cherenkov radiation [ 55 ] in quadratic crystals.…”
Section: Model Description and Basic Equationsmentioning
confidence: 99%
“…Equation (4) is a generalized cubic‐quintic NLS equation with cubic derivative terms. It is known to govern the propagation of ultrashort pulses in a single‐mode optical fiber, [ 47 ] the modulations of weakly nonlinear ions in acoustic plasma waves, [ 48 ] ferromagnetic chain, [ 49 ] evolutions of Stokes waves, [ 50 ] soliton propagation in optical fibers, and metamaterials, [ 51,52 ] etc. Equation (4) can also be applied to the description of high‐intensity pulse propagation, [ 53 ] controllable self‐steepening, [ 54 ] and generation of Cherenkov radiation [ 55 ] in quadratic crystals.…”
Section: Model Description and Basic Equationsmentioning
confidence: 99%