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The ion acoustic wave is taken to propagate and evolve into solitary structure at an angle with the direction of an external magnetic field.
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Of course we see that at f ≈ 0 the solitary structure disappears and system do not supports solitons in the pure e p limit.
The IA solitary structure experiences a decrease (increase) in amplitude (width) with a decreasing f, as for low values of f the IA solitary structure may be disappears.
We found that the solitary structure becomes narrower and larger in the e i limit, while the solitary structure collapses in the e p limit. .
We found that the solitary structure becomes narrower and larger in the e i limit, while the solitary structure collapses in the e p limit.
Hence, the solitary structure can be understood as bunch of ions in the plasma.
This means that deviation of electrons/positrons from thermodynamics equilibrium makes the solitary structure more spiky.
In Figure 4, we have plotted the solitary structure with the positron-to-electron temperature ratio.
It is found that deviation from thermodynamics equilibrium increases the existence domain of solitary solution and also makes the IA solitary structure more spiky.
We call the structure corresponding to the fast wave as the fast compressive solitary structure and the structure corresponding to the slow wave as the slow compressive solitary structure.
Then, for values of f and l ξ greater than critical values, the solitary structure disappears (see also Fig. 1).
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