next previous
Up: Optical photometric monitoring

1. Introduction

The Compton Gamma Ray Observatory (CGRO) satellite has recently discovered that highly variable and radio-loud quasars are also strong tex2html_wrap_inline1954-ray emitters (Fichtel et al. 1994; von Montigny et al. 1995; Thompson et al. 1995). The power released by such objects above tex2html_wrap_inline1956 can overcome that in the other bands by even two orders of magnitude (see e.g. Dondi & Ghisellini 1995).

Many theoretical models have been proposed in order to explain this phenomenon and observational constraints are the only tool that can operate a choice among them. According to a group of models, the tex2html_wrap_inline1958-ray emission can be due to inverse Compton scattering of optical photons on relativistic electrons inside a jet. In turn, the seed photons may either be produced by the same relativistic electrons through synchrotron process (Maraschi et al. 1992) or come from some external region [e.g. from the accretion disk, as in the model by Dermer & Schlickeiser (1993), or from the broad line region illuminated by the accretion disk, as in the model by Sikora et al. (1994)].

Through the optical observation of strong tex2html_wrap_inline1960-ray emitting blazars it is thus possible to obtain information about the mechanisms that rule the production of the seed photons for the tex2html_wrap_inline1962 radiation. In particular, optical monitoring simultaneous with tex2html_wrap_inline1964 observations can confirm the expected temporal correlation between the two emissions and constitutes a crucial test for the theoretical predictions. Indeed, in the case of seed photons produced by the same relativistic electrons which are responsible for the tex2html_wrap_inline1966 radiation, besides a simultaneous variability in the two bands, larger amplitude variations in the tex2html_wrap_inline1968 one are expected, since any increase in the relativistic electron number contributes twice to the tex2html_wrap_inline1970 emission. If, on the contrary, the seed photons were produced outside, the tex2html_wrap_inline1972-ray emission intensity would vary more or less linearly with the optical one. A non-simultaneous variability would be a problem for both the models.

For the above reasons, an optical monitoring campaign has been started at the Torino Observatory since November 1994 with the aim of following the optical behaviour of a list of tex2html_wrap_inline1974-ray loud blazars. The observations were intensified, when possible, during CGRO pointings. Collaborations with other institutes were started on some sources: as for OJ 287, 3C 66A, and AO 0235+164 we joined the OJ-94 Project (e.g. Sillanpää et al. 1996; Takalo et al. 1996a,b; Villata et al. 1996), while for OF 038, S5 0716+714, PKS 0735+178, S4 0954+658, and ON 231 a national collaboration with the Roma and Perugia groups was set up (Massaro et al. 1996; Ghisellini et al. 1996; Latini et al. 1996; Fiorucci et al. 1996; Tosti et al. 1996). In this paper we present the results of the optical monitoring of the remaining twenty blazars in the Torino program list. In Sect. 2 a description of the instrumental equipment and data reduction procedure is given and the list of the observed sources is presented. Sect. 3 contains, for each source, a brief summary of previously published data in the optical (and tex2html_wrap_inline1976) band and the presentation and description of the light curves we obtained within the period from November 15, 1994 to November 7, 1995. For the BL Lac object PKS 2254+074 we show the results of UBVRI photopolarimetry too. Photometric sequence calibrations are also given for ten sources. Finally, the main conclusions of this work are drawn in Sect. 4.


next previous
Up: Optical photometric monitoring

Copyright EDP Sciences
web@edpsciences.com