Dead zone in the polar-cap accelerator of pulsars
arXiv:1206.6344 · doi:10.1088/0004-637X/762/2/76
Abstract
We study plasma flows above pulsar polar caps using time-dependent simulations of plasma particles in the self-consistent electric field. The flow behavior is controlled by the dimensionless parameter alpha=(j/c rho_GJ) where j is the electric current density and rho_GJ is the Goldreich-Julian charge density. The region of the polar cap where 0<alpha<1 is a "dead zone" --- in this zone particle acceleration is inefficient and pair creation is not expected even for young, rapidly rotating pulsars. Pulsars with polar caps near the rotation axis are predicted to have a hollow-cone structure of radio emission, as the dead zone occupies the central part of the polar cap. Our results apply to charge-separated flows of electrons (j<0) or ions (j>0). In the latter case, we consider the possibility of a mixed flow consisting of different ion species, and observe the development of two-stream instability. The dead zone at the polar cap is essential for the development of an outer gap near the null surface rho_GJ=0.
10 pages, 11 figures, accepted to ApJ
References in corpus (2)
Cited by in corpus (9)
- Electrodynamics of axisymmetric pulsar magnetosphere with electron-positron discharge: a numerical experiment
- Gamma-Ray Emission in Dissipative Pulsar Magnetospheres: From Theory to Fermi Observations
- Electrodynamics of pulsar magnetospheres
- Filling the Magnetospheres of Weak Pulsars
- Physics of Pair Producing Gaps in Black Hole Magnetospheres
- An incomplete model of RRATs and of nulls mode-changes and subpulses
- PSR B1133+16: radio emission height and plasma composition
- Electric Field Screening with Back-Flow at Pulsar Polar Cap
- A multi-component Langmuir-mode source for the observed pulsar coherent emission