2021
DOI: 10.1051/0004-6361/202141053
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Identifying changing jets through their radio variability

Abstract: Context. Supermassive black holes can launch highly relativistic jets with velocities reaching Lorentz factors of as high as Γ >  50. How the jets accelerate to such high velocities and where along the jet they reach terminal velocity are open questions that are tightly linked to their structure as well as their launching and dissipation mechanisms. Aims. Changes in the beaming factor along the jets could potentially reveal jet acceleration, deceleration, or bending. We aim to (1) quantify the relativistic … Show more

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Cited by 3 publications
(2 citation statements)
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“…We used the results of Magnetron to compute the maximum observed brightness temperature distribution, which we compared to the intrinsic maximum brightness temperature of T int,max = 2.78×10 11 K . We find a Doppler factor of δ = 11.6 +11.1 −5.5 , which is consistent with previous estimates in the literature (Liodakis et al 2017(Liodakis et al , 2021. The uncertainties on δ are not statistical, but rather express the range of possible values over the ∼15 years of radio observations.…”
Section: Optical Circular Polarization Observations and Modelingsupporting
confidence: 91%
“…We used the results of Magnetron to compute the maximum observed brightness temperature distribution, which we compared to the intrinsic maximum brightness temperature of T int,max = 2.78×10 11 K . We find a Doppler factor of δ = 11.6 +11.1 −5.5 , which is consistent with previous estimates in the literature (Liodakis et al 2017(Liodakis et al , 2021. The uncertainties on δ are not statistical, but rather express the range of possible values over the ∼15 years of radio observations.…”
Section: Optical Circular Polarization Observations and Modelingsupporting
confidence: 91%
“…It is known that flat-spectrum radio sources exhibit flux density variability over timescales from days to years (Hovatta et al 2007;Chen et al 2013;Sadler et al 2014). Interstellar scintillation (Walker 1998;Said et al 2020) and variations in the Doppler boosting factor (Liodakis et al 2021;Kosogorov et al 2022) are two processes that may cause the observed flux density variability. For flat-spectrum radio sources, in particular the blazar subclass, this variability is often associated with flaring activity, and it is a major source of misidentification of Peaked Spectrum (PS) objects (Kovalev et al 2002;Jauncey et al 2003;Tinti et al 2005;Torniainen et al 2005;Orienti et al 2010), i.e., the radio spectrum becomes peaked where it is expected to be flat.…”
Section: Flux Density and Spectral Variabilitymentioning
confidence: 99%