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Multi-Wavelength Variability of BL Lacertae Measured with High Time Resolution

Z. R. WeaverInstitute for Astrophysical Research , Boston University , 725 Commonwealth Avenue , Boston , MA 02215 , USAKaren E. WilliamsonInstitute for Astrophysical Research , Boston University , 725 Commonwealth Avenue , Boston , MA 02215 , USASvetlana G. JorstadAlan P. MarscherInstitute for Astrophysical Research , Boston University , 725 Commonwealth Avenue , Boston , MA 02215 , USAV. M. LarionovMain (Pulkovo) Astronomical Observatory of RAS , Pulkovskoye shosse 60 , St. Petersburg 196149 , RussiaC. M. RaiteriINAF , Osservatorio Astrofisico di Torino , Via Osservatorio 20 , I-10025 Pino Torinese , ItalyM. VillataJ. A. Acosta‐PulidoR. BachevG. V. BaidaT. J. BalonekDepartment of Physics and Astronomy , Colgate University , 13 Oak Drive , Hamilton , New York 13346 , USAE. BenítezInstituto de Astronomía , Universidad Nacional Autónoma de México , Apdo. Postal 70-264 , CDMX 04510 , MéxicoГ. А. БорманCrimean Astrophysical Observatory RAS , P/O Nauchny , 298409 , RussiaV. BozhilovDepartment of Astronomy , Faculty of Physics , University of Sofia , BG-1164 Sofia , BulgariaM. I. CarnereroD. CarosatiEPT Observatories , Tijarafe , E-38780 La Palma , SpainWen-Ping ChenG. DamljanovićVinit DhimanDavid J. DoughertyDepartment of Physics and Astronomy , Colgate University , 13 Oak Drive , Hamilton , New York 13346 , USASh. A. EhgamberdievAryabhatta Research Institute of Observational Sciences (ARIES) , Manora Peak , Nainital -263 001 , IndiaT. S. GrishinaAlok C. GuptaMurdock HartD. HiriartH. Y. HsiaoS. IbryamovM. D. JonerG. N. KimeridzeE. N. KopatskayaAstronomical Institute , St. Petersburg State University , Universitetskij Pr. 28 , Petrodvorets , St. Petersburg 198504 , RussiaO. M. KurtanidzeSofia O. KurtanidzeЕ. Г. ЛарионоваKatsura MatsumotoAstronomical Institute , Osaka Kyoiku University , Osaka , 582-8582 , JapanR. MatsumuraAstronomical Institute , Osaka Kyoiku University , Osaka , 582-8582 , JapanM. MinevSofia University "St. Kliment Ohridski"D. O. MirzaqulovD. A. MorozovaA. A. NikiforovaM. G. NikolashviliAbastumani Observatory , Mt. Kanobili , 0301 Abastumani , GeorgiaE. OvcharovDepartment of Astronomy , Faculty of Physics , University of Sofia , BG-1164 Sofia , BulgariaN. RizziUniversity of Colorado DenverA. C. SadunС. С. СавченкоE. SemkovInstitute of Astronomy and National Astronomical Observatory , Bulgarian Academy of Sciences , 72 Tsarigradsko shosse Blvd. , 1784 Sofia , BulgariaJohn J. SlaterDepartment of Physics and Astronomy , Colgate University , 13 Oak Drive , Hamilton , New York 13346 , USAK. SmithM. StojanovićAstronomical Observatory , Volgina 7 , 11060 , Belgrade , SerbiaA. StrigachevYu. V. TroitskayaIvan S. TroitskyAstronomical Institute , St. Petersburg State University , Universitetskij Pr. 28 , Petrodvorets , St. Petersburg 198504 , RussiaAn-Li TsaiGraduate Institute of Astronomy , National Central University , 300 Jhongda Road , Zhongli , Taoyuan , 32001 , TaiwanO. VinceA. ValchevaA. A. VasilyevE. ZaharievaAlexey V. Zhovtan
2020en
ABI

Annotatsiya

In an effort to locate the sites of emission at different frequencies and physical processes causing variability in blazar jets, we have obtained high time-resolution observations of BL Lacertae over a wide wavelength range: with the \emph{Transiting Exoplanet Survey Satellite} (TESS) at 6,000-10,000 Å with 2-minute cadence; with the Neil Gehrels \emph{Swift} satellite at optical, UV, and X-ray bands; with the Nuclear Spectroscopic Telescope Array at hard X-ray bands; with the \emph{Fermi} Large Area Telescope at $γ$-ray energies; and with the Whole Earth Blazar Telescope for measurement of the optical flux density and polarization. All light curves are correlated, with similar structure on timescales from hours to days. The shortest timescale of variability at optical frequencies observed with TESS is $\sim 0.5$ hr. The most common timescale is $13\pm1$~hr, comparable with the minimum timescale of X-ray variability, 14.5 hr. The multi-wavelength variability properties cannot be explained by a change solely in the Doppler factor of the emitting plasma. The polarization behavior implies that there are both ordered and turbulent components to the magnetic field in the jet. Correlation analysis indicates that the X-ray variations lag behind the $γ$-ray and optical light curves by up to $\sim 0.4$ days. The timescales of variability, cross-frequency lags, and polarization properties can be explained by turbulent plasma that is energized by a shock in the jet and subsequently loses energy to synchrotron and inverse Compton radiation in a magnetic field of strength $\sim3$ G

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