| نویسندگان | Seyed mohammadd Khorashadizadeh |
| نشریه | Monthly Notices of the Royal Astronomical Society |
| شماره صفحات | 3059-3065 |
| شماره سریال | 489 |
| شماره مجلد | 489 |
| نوع مقاله | Full Paper |
| تاریخ انتشار | 2019 |
| رتبه نشریه | ISI |
| نوع نشریه | چاپی |
| کشور محل چاپ | ایران |
| نمایه نشریه | JCR،Scopus |
| کلید واژه ها | Magnetic field, waves |
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چکیده مقاله
The aim of this study is to highlight the temporal evolution of the longitudinal wave instability
due to the interaction between a rotating electron beam and the magnetoactive plasma region
in space plasma structures. The plasma structure which could be either in the solar atmosphere
or any active plasma region in space is considered weakly turbulent, where the quasi-linear
theory is implemented to enable analytic insight on the wave–particle interaction in the course
of the event. It is found that in a weakly turbulent plasma, quasi-linear saturation of the
longitudinal wave is accompanied by a significant alteration in the distribution function in the
resonant region. In case of a pure electrostatic wave, the wave amplitude experiences elevation
due to the energy transfer from the plasma particles. This causes flattening of the bump on
tail (BOT) in the electron distribution function. If the gradient of the distribution function is
positive, the chance that the beam would excite the wave is probable. In such a situation a
plateau on the distribution function (∂f/∂v ≈ 0) is formed that will stop the diffusion of beam
particles in the velocity space. Evolution of the electron distribution function experiences a
decreases of the instability of the longitudinal wave. It is deduced that the growth rate of the
wave instability is inversely proportional to the wave energy. Regarding the Sun, in addition
to creating micro-turbulence due to wave–particle interaction, as the wave elevates to higher
altitudes it enters a saturated energy state before releasing energy that may be a candidate for
the generation of radio bursts.