Relativistic Shock Wave eith Degenerate Electrons Trapped in Landau Quantized Magnetic Field: Effect of Non-Thermal Heavy Negative Ion

Authors

  • Apul. N. DEV, Manoj Kr. Deka

Abstract

The distribution of the relativistic supersonic shock wave in the quantum plasma is studied in the quantized magnet field of Landau with electrons and non-thermal strong negative ions. The existence of the shock wave in such a plasma is studied by using the traditional theoretical solution of the three-dimensional Plasma equation with degenerate electron-density trapped magnetically in a quantized magnet field, relativistic parameter and in the presence of strong negative ions that vary from thermal equilibrium.The electron's degenerate density and the parameter for magnetic measurement and the relative factor have an extraordinary effect on the kind of propagation in this plasma of supersonic shock waves. The non-thermal negative ion population with normalized negative ion density and history have a profound effect on the amplitude of the shock wave. For any particular degenerate electron density, the simultaneous increase of population of nonthermal negative ion and background normalized negative ion density results in the lowest possible shock wave amplitude whereas , the simultaneous increase of nonthermal population of negative ion, normalized negative ion density, relativistic factor and magnetic field results in the highest possible shock wave amplitude within the chosen set of plasma parameters. The relativistic factor leads the height of the shock wave and decreases with a relativistic effect that grows irrespective of any changes in other plasma parameters. A comprehensive comparative analysis is carried out on the function of each leading parameter in the amplitude of the shock wave.

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Published

2020-05-18

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Articles