Mathematics – Logic
Scientific paper
May 1999
adsabs.harvard.edu/cgi-bin/nph-data_query?bibcode=1999aas...194.5032d&link_type=abstract
American Astronomical Society, 194th AAS Meeting, #50.32; Bulletin of the American Astronomical Society, Vol. 31, p.902
Mathematics
Logic
1
Scientific paper
We present the results of a polarization sensitive VLBA monitoring program of the AGN BL Lacertae spanning epochs 1995.4 - 1998.3. The images show the ejection of four highly polarized superluminal components (denoted S7, S8, S9, and S10 chronologically). The trajectories of the components are clearly non-radial. Extrapolation of the position of the components to their respective birth epochs indicates that some of the components are apparently created in pairs, with a fast component and a slow component; the birth epochs are t_0 = (1994.12 +/- 0.13, 1994.20 +/- 0.05) for (S7, S8) and t_0 = (1996.35 +/- 0.09, 1996.47 +/- 0.10) for (S9, S10). The apparent velocities (beta_ {app}) for the components are S7: (4.1+/-0.1)h(-1) , S8: (2.4+/-0.6)h(-1) , S9: (6.1+/-0.6)h(-1) , and S10:(3.1+/-0.2)h(-1) . There has been no obvious radio counterpart to the large optical-gamma ray outburst at epoch 1997.6 (from three subsequent epochs.) The core component polarization was low and found to satisfy a nu (2) frequency dependence expected from a turbulent foreground Faraday screen with characteristic spatial scale s_0 ~ 0.3 a.u. We have applied the helical model of Hardee (1987) to explain the components' non-radial trajectories. The best fit trajectories indicate that the angle of the helical axis to the line of sight is consistent with Theta =~ 9arcdeg and the jet half-opening angle is Psi =~ 2arcdeg . Using the polarized maps, we have applied a relativistic shock model (Hughes et al. 1985) to the components and have determined that the three slower components (S7, S8, and S10) are weak shocks (compression k ~ 0.7) and that the fastest component (S9) is a strong shock (k ~ 0.4).
Denn Grant Russell
Mutel Robert L.
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