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WEBT multiwavelength monitoring and XMM-Newton observations of 
BL Lacertae in 2007–2008

C. M. RaiteriINAF, Osservatorio Astronomico di Torino, Italy e-mail: [raiteri;villata]@oato.inaf.itM. VillataINAF, Osservatorio Astronomico di Torino, Italy e-mail: [raiteri;villata]@oato.inaf.itA. CapettiINAF, Osservatorio Astronomico di Torino, Italy e-mail: [raiteri;villata]@oato.inaf.itM. F. AllerDepartment of Astronomy, University of Michigan, MI, USAU. BachMax-Planck-Institut für Radioastronomie, Bonn, GermanyP. CalcideseOsservatorio Astronomico della Regione Autonoma Valle d'Aosta, ItalyMark GurwellHarvard-Smithsonian Center for Astroph., Cambridge, MA, USAV. M. LarionovAstron. Inst., St.-Petersburg State Univ., RussiaJ. OhlertK. NilssonTuorla Observatory, Dept. of Physics and Astronomy, Univ. of Turku, Piikkiö, FinlandA. StrigachevInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaI. AgudoInstituto de Astrofísica de Andalucía (CSIC), Granada, SpainH. D. AllerDepartment of Astronomy, University of Michigan, MI, USAR. BachevInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaE. BenítezInstituto de Astronomía, Universidad Nacional Autónoma de México, MexicoA. BerdyuginTuorla Observatory, Dept. of Physics and Astronomy, Univ. of Turku, Piikkiö, FinlandM. BöttcherDepartment of Physics and Astronomy, Ohio Univ., OH, USAC. S. BuemiINAF, Osservatorio Astrofisico di Catania, ItalyS. ButtiglioneSISSA-ISAS, Trieste, ItalyD. CarosatiArmenzano Astronomical Observatory, ItalyP. CharlotCNRS, Laboratoire d'Astrophysique de Bordeaux – UMR 5804, Floirac, FranceW. P. ChenInstitute of Astronomy, National Central University, TaiwanD. DultzinInstituto de Astronomía, Universidad Nacional Autónoma de México, MexicoE. FornéL. FuhrmannMax-Planck-Institut für Radioastronomie, Bonn, GermanyJosé L. GómezInstituto de Astrofísica de Andalucía (CSIC), Granada, SpainA. C. GuptaARIES, Manora Peak, Nainital, IndiaJ. HeidtD. HiriartInstituto de Astronomía, Universidad Nacional Autónoma de México, MexicoW.‐S. HsiaoInstitute of Astronomy, National Central University, TaiwanM. JelínekInst. de Astrofísica de Andalucía, CSIC, SpainS. G. JorstadInst. for Astrophysical Research, Boston University, MA, USAG. N. KimeridzeAbastumani Astrophysical Observatory, GeorgiaT. S. KonstantinovaAstron. Inst., St.-Petersburg State Univ., RussiaE. N. KopatskayaAstron. Inst., St.-Petersburg State Univ., RussiaA. KostovInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaO. M. KurtanidzeAbastumani Astrophysical Observatory, GeorgiaA. LähteenmäkiMetsähovi Radio Obs., Helsinki Univ. of Technology, FinlandL. LanteriINAF, Osservatorio Astronomico di Torino, Italy e-mail: [raiteri;villata]@oato.inaf.itL. V. LarionovaAstron. Inst., St.-Petersburg State Univ., RussiaP. LetoINAF, Istituto di Radioastronomia, Sezione di Noto, ItalyG. LatevSofia University, BulgariaJ.-F. Le CampionCNRS, Laboratoire d'Astrophysique de Bordeaux – UMR 5804, Floirac, FranceChung‐Uk LeeKorea Astronomy and Space Science Institute, South KoreaR. LigustriE. LindforsTuorla Observatory, Dept. of Physics and Astronomy, Univ. of Turku, Piikkiö, FinlandA P MarscherInstitute for Astrophysical Research, Boston University, MA, USAB. MihovInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaM. G. NikolashviliAbastumani Astrophysical Observatory, GeorgiaY. NikolovInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaE. OvcharovSofia University, BulgariaDavid A. PrincipeDepartment of Physics and Astronomy, Ohio Univ., OH, USAT. PursimoNordic Optical Telescope, Santa Cruz de La Palma, SpainB. RagozzineDepartment of Physics and Astronomy, Ohio Univ., OH, USAR. M. RobbDept. of Physics and Astronomy, Univ. of Victoria, Victoria, CanadaJ. AgramuntA. C. SadunDept. of Phys., Univ. of Colorado Denver, Denver, CO USAR. SagarARIES, Manora Peak, Nainital, IndiaE. SemkovInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaL. A. SiguaAbastumani Astrophysical Observatory, GeorgiaR. L. SmartINAF, Osservatorio Astronomico di Torino, Italy e-mail: [raiteri;villata]@oato.inaf.itM. SorciaInstituto de Astronomía, Universidad Nacional Autónoma de México, MexicoL. O. TakaloTuorla Observatory, Dept. of Physics and Astronomy, Univ. of Turku, Piikkiö, FinlandM. TornikoskiMetsähovi Radio Obs., Helsinki Univ. of Technology, FinlandC. TrigilioINAF, Osservatorio Astrofisico di Catania, ItalyKyle UckertDepartment of Physics and Astronomy, Ohio Univ., OH, USAG. UmanaINAF, Osservatorio Astrofisico di Catania, ItalyA. ValchevaInst. of Astronomy, Bulgarian Academy of Sciences, Sofia, BulgariaA. E. VolvachRadio Astronomy Lab. of Crimean Astrophysical Observatory, Ukraine
2009en
ABI

Аннотация

<i>Context. <i/>BL Lacertae is the prototype of the blazar subclass named after it. Yet, it has occasionally shown a peculiar behaviour that has questioned a simple interpretation of its broad-band emission in terms of synchrotron plus synchrotron self-Compton (SSC) radiation.<i>Aims. <i/>In the 2007–2008 observing season we carried out a new multiwavelength campaign of the Whole Earth Blazar Telescope (WEBT) on BL Lacertae, involving three pointings by the XMM-Newton satellite in July and December 2007, and January 2008, to study its emission properties, particularly in the optical-X-ray energy range.<i>Methods. <i/>The source was monitored in the optical-to-radio bands by 37 telescopes. The brightness level was relatively low. Some episodes of very fast variability were detected in the optical bands. Flux changes had larger amplitude at the higher radio frequencies than at longer wavelengths.<i>Results. <i/>The X-ray spectra acquired by the EPIC instrument onboard XMM-Newton are well fitted by a power law with photon index and photoelectric absorption exceeding the Galactic value. However, when taking into account the presence of a molecular cloud on the line of sight, the EPIC data are best fitted by a double power law, implying a concave X-ray spectrum. The spectral energy distributions (SEDs) built with simultaneous radio-to-X-ray data at the epochs of the XMM-Newton observations suggest that the peak of the synchrotron emission lies in the near-IR band, and show a prominent UV excess, besides a slight soft-X-ray excess. A comparison with the SEDs corresponding to previous observations with X-ray satellites shows that the X-ray spectrum is very variable, since it can change from extremely steep to extremely hard, and can be more or less curved in intermediate states. We ascribe the UV excess to thermal emission from the accretion disc, and the other broad-band spectral features to the presence of two synchrotron components, with their related SSC emission. We fit the thermal emission with a black body law and the non-thermal components by means of a helical jet model. The fit indicates a disc temperature and a luminosity .

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