Abstract

BL Lacertae objects constitute a rare class of active galactic nuclei with extreme observational features attributed to the Doppler-boosted emission from a relativistic jet, closely aligned to our line-of-sight. Their spectral energy distribution, extending over 17–19 orders of frequency from radio to the TeV energy range, is of non-thermal origin and shows a typical two-component structure. The lower-energy component, ranging from the radio to X-rays in the high-energy peaked BL Lacertae sources, is widely accepted to be a synchrotron radiation emitted by ultra-relativistic charged particles, to be initially accelerated via the Blandford–Znajek mechanism or magneto-hydrodynamic processes in the vicinity of the central super-massive black hole. However, the accelerated particles should lose the energy, sufficient for the emission of the keV-GeV photons, very quickly and the source can maintain its flaring state on the daily-weekly timescales only if some additional acceleration mechanisms are continuously at work. According to different studies and simulations,the particles can gain tremendous energies due to the propagation of relativistic shocks through the jet: By means of first-order Fermi mechanism at the shock front, or they undergo an efficient stochastic (second-order Fermi) acceleration close to the shock front, in the turbulent jet medium. Our intensive X-ray spectral study of TeV-detected, bright BL Lacertae objects (Mrk 421, 1ES 1959+650, Mrk 501) often show the signatures of the stochastic acceleration, while those related to the first-order Fermi process arefound relatively rarely. The TeV-undetected sources (1H 1516+660, BZB J1341+3959, BZB J1237+6258) mostly do not show the signatures of the efficient stochastic acceleration in their jets.

Highlights

  • The BL Lacertae objects constitute an extreme class of active galactic nuclei (AGNs) featuring non-thermal continuum emission stretching from radio to TeV-band (17–19 orders of frequency), absence of emission lines, strong flux variability in all spectral bands, compact and flat-spectrum radio emission, apparent superluminal motion of some components, high and variable radio/optical polarization, strong X-ray and γ-ray emissions [1]

  • These properties are explained by the presence of a super-massive black hole (SMBH; with masses M~108 –109 MJ ) in the center of the elliptical host galaxy, along with the inherent accretion disc (AD) and relativistic jet closely aligned to the observer

  • The lower-frequency spectral energy distribution (SED) component is explained via synchrotron radiation emitted by relativistic electrons in the jet, while there is a variety of models for the origin of the higher-energy bump, with the three most frequently considered scenarios: An inverse Compton (IC)

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Summary

Introduction

The BL Lacertae objects constitute an extreme class of active galactic nuclei (AGNs) featuring non-thermal continuum emission stretching from radio to TeV-band (17–19 orders of frequency), absence of emission lines, strong flux variability in all spectral bands, compact and flat-spectrum radio emission, apparent superluminal motion of some components, high and variable radio/optical polarization, strong X-ray and γ-ray emissions [1] These properties are explained by the presence of a super-massive black hole (SMBH; with masses M~108 –109 MJ ) in the center of the elliptical host galaxy, along with the inherent accretion disc (AD) and relativistic jet closely aligned to the observer (see Reference [2], and references therein).

The Origin of X-ray Spectral Curvature
First-Order Fermi Acceleration
The a-b a-b correlation
Discussion and Conclusions
The SS p
HR-flux the of of
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