ABSTRACT
We performed relativistic magnetohydrodynamic
simulations of the hydrodynamic boosting mechanism for relativistic
jets explored by Aloy & Rezzolla (2006) using the RAISHIN code.
Simulation results show that the presence of a magnetic field may change
the properties of the shock interface between the tenuous, overpressured
jet (V^z_j) flowing tangentially to a dense external medium.
Magnetic fields can lead to more efficient acceleration of the jet,
in comparison to the pure-hydrodynamic case. A "poloidal'' magnetic
field (B^z), tangent to the interface and parallel to the jet flow,
produces both a stronger outward moving shock and a stronger inward
moving rarefaction wave. This leads to a large velocity component normal
to the interface in addition to acceleration tangent to the interface,
and the jet is thus accelerated to larger Lorentz factors than those
obtained in the pure-hydrodynamic case. In contrast, a strong ``toroidal''
magnetic field (B^y), tangent to the interface but perpendicular
to the jet flow, also leads to stronger acceleration tangent to the
shock interface relative to the pure-hydrodynamic case, but to a lesser
extent than found for the "poloidal'' case due to the fact that the
velocity component normal to the shock interface is now much smaller.
Overall, the acceleration efficiency in the ``toroidal'' case is less
than that of the "poloidal''
case but both geometries still result in higher Lorentz factors than
the pure-hydrodynamic case. Thus, the presence and relative orientation
of a magnetic field in relativistic jets can significant modify the
hydrodynamic boost mechanism studied by Aloy \& Rezzolla (2006).