Hierarchy of instabilities for two counter-streaming magnetized pair beams: influence of field obliquity

Abstract

The hierarchy of unstable modes when two counter-streaming pair plasmas interact over a flow-aligned magnetic field has been recently investigated [PoP \textbf{23}, 062122 (2016)]. The analysis is here extended to the case of an arbitrarily tilted magnetic field. The two plasma shells are initially cold and identical. For any angle $θ\in [0,π/2]$ between the field and the initial flow, the hierarchy of unstable modes is numerically determined in terms of the initial Lorentz factor of the shells $γ_0$, and the field strength as measured by a parameter denoted $σ$. For $θ=0$, four different kinds of mode are likely to lead the linear phase. The hierarchy simplifies for larger $θ$'s, partly because the Weibel instability can no longer be cancelled in this regime. For $θ>0.78$ (44$^\circ$) and in the relativistic regime, the Weibel instability always govern the interaction. In the non-relativistic regime, the hierarchy becomes $θ$-independent because the interaction turns to be field-independent. As a result, the two-stream instability becomes the dominant one, regardless of the field obliquity.