TY - JOUR
T1 - Internal shocks and the blazar sequence - Low and intermediate power BL Lac objects
T2 - Low and intermediate power BL Lac objects
AU - Guetta, D
AU - Ghisellini, G
AU - Lazzati, D
AU - Celotti, A
PY - 2004/7
Y1 - 2004/7
N2 - We consider internal shocks as the main dissipation mechanism responsible for the emission in blazars and show that it can satisfactorily account for the properties of all blazars. In particular, we extend previous work (Spada et al. 2001) on powerful objects, to intermediate (BL Lac) and low power sources (Mkn 421), in order to reproduce the whole of the blazar sequence. The model self-consistently treats the dynamics, spectral emission and its variability. The key parameters driving the phenomenological sequence are the jet power and the properties of the broad line region, which regulate the cooling efficiency of the emitting particles and thus the shape of the spectral energy distribution. By assuming that the remaining parameters are similar for all objects it has been possible to reproduce the full range of the observed spectral "states". A more detailed comparison of the variability properties shows (for Mkn 421) a good agreement in the X-ray band, while in the optical the simulated flux appears to be too variable. For BL Lac lags (∼10 days) are predicted between the y-rays and the infrared emission.
AB - We consider internal shocks as the main dissipation mechanism responsible for the emission in blazars and show that it can satisfactorily account for the properties of all blazars. In particular, we extend previous work (Spada et al. 2001) on powerful objects, to intermediate (BL Lac) and low power sources (Mkn 421), in order to reproduce the whole of the blazar sequence. The model self-consistently treats the dynamics, spectral emission and its variability. The key parameters driving the phenomenological sequence are the jet power and the properties of the broad line region, which regulate the cooling efficiency of the emitting particles and thus the shape of the spectral energy distribution. By assuming that the remaining parameters are similar for all objects it has been possible to reproduce the full range of the observed spectral "states". A more detailed comparison of the variability properties shows (for Mkn 421) a good agreement in the X-ray band, while in the optical the simulated flux appears to be too variable. For BL Lac lags (∼10 days) are predicted between the y-rays and the infrared emission.
KW - galaxies : jets
KW - galaxies : nuclei
KW - radio continuum : galaxies
KW - galaxies : individual : Mkn 421, BL Lac
UR - http://www.scopus.com/inward/record.url?scp=3142684758&partnerID=8YFLogxK
U2 - 10.1051/0004-6361:20040235
DO - 10.1051/0004-6361:20040235
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
SN - 0004-6361
VL - 421
SP - 877
EP - 886
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
IS - 3
ER -