  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 $\theta \in [0,\pi/2]$ 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 $\gamma_0$, and the field
strength as measured by a parameter denoted $\sigma$. For $\theta=0$, four
different kinds of mode are likely to lead the linear phase. The hierarchy
simplifies for larger $\theta$'s, partly because the Weibel instability can no
longer be cancelled in this regime. For $\theta>0.78$ (44$^\circ$) and in the
relativistic regime, the Weibel instability always govern the interaction. In
the non-relativistic regime, the hierarchy becomes $\theta$-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.
