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Nagasawa and Nishida [20] studied the nonlinear reflection and refraction of the soliton from a metallic electrode in a double-plasma (DP) device.
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This paper studies the interaction between non-viscous damping and nonlinearities for nonlinear oscillators with reflection symmetry.
Due to nonlinear response of ionospheric reflection coefficient to these factors, finding an accurate relation between these parameters and reflection coefficient is an arduous task.
The sensitive behavior on the surface amplitude can be understood by reflection and nonlinear dissipation of Alfvén waves (SI06).
The reflection of nonlinear solitary waves is studied in a plasma under the effect of an external magnetic field and constant ionization along with finite ion temperature.
Since the ions carry finite temperature in the plasmas, the temperature should also be taken into consideration while studying these nonlinear waves and their reflection.
In addition to the effect of the wave reflection, the nonlinear dissipation of the Alfvén waves also plays a role in the sensitive dependence on the input wave energy (SI06).
In [1], the authors provide the range of values of the real parameter ω for which the Green's function has constant sign and apply these results to prove the existence of constant sign solutions for the nonlinear periodic problem with reflection of the argument u ′ ( t ) = h ( t, u ( t ), u ( − t ) ), t ∈ [ − T, T ], u ( − T ) = u ( T ).
We investigate the reflection of highly nonlinear solitary waves in one-dimensional granular crystals interacting with large plates.
The TMM approach can also be readily applied to a wide variety of cases, such as beam propagation through induced reflection gratings in nonlinear media.
Because the ionization is an inelastic collisional phenomenon, the collisions should be taken into consideration to make a deep understanding of this plasma with regard to the excitation of nonlinear solitary waves and their reflection.
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