1996A&A...313..759R


Query : 1996A&A...313..759R

1996A&A...313..759R - Astronomy and Astrophysics, volume 313759-767 (1996/9-3)

A model for the soft γ-ray variability in MeV blazars.

ROMERO G.E.

Abstract (from CDS):

Recent observations with the COMPTEL instrument on the Compton Gamma Ray Observatory (CGRO) have revealed that several blazar-type sources present a strong peak in the 0.75-8.0 MeV range of their emission. Moreover, at least four of these objects have displayed variability in the soft γ-ray flux over timescales of months. In this paper I present a model for such variability based on the interaction of a strong relativistic shock with density inhomogeneities in the inner pair beam of these sources. The shock increases the soft γ-emission by compression of the particle density and the consequent enhancement of the blue-shifted annihilation radiation. The shocked particles also emit synchrotron radiation producing simultaneous or quasi-simultaneous outbursts at lower frequencies. This model is applied to the well-studied quasar 3C 273, a source for which multifrequency temporal observations are available.

Abstract Copyright: ∼

Journal keyword(s): quasars: general - quasars: individual: 3C 273 - shock waves - gamma rays: theory

Simbad objects: 14

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Number of rows : 14
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 MCG+01-12-009 Bla 04 33 11.0956735296 +05 21 15.619461552   15.72 15.05 10.08   ~ 2099 2
2 QSO B0506-612 Bla 05 06 43.98874900 -61 09 40.9939787   17.16 16.85 16.9   ~ 186 2
3 GRO J0516-609 gam 05 16 -60.9           ~ 22 0
4 3C 273 BLL 12 29 06.6998257176 +02 03 08.597629980   13.05 14.830 14.11   ~ 6022 1
5 3C 273C4 Rad ~ ~           ~ 10 0
6 3C 273C5 Rad ~ ~           ~ 10 0
7 3C 273C6 Rad ~ ~           ~ 7 0
8 3C 273C8 Rad ~ ~           ~ 8 0
9 3C 273C7 Rad ~ ~           ~ 7 0
10 3C 273C9 Rad ~ ~           ~ 8 0
11 3C 273C10 Rad ~ ~           ~ 4 0
12 3C 273C3 Rad ~ ~           ~ 10 0
13 3C 273C2 Rad ~ ~           ~ 10 0
14 3C 273C1 Rad ~ ~           ~ 6 0

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