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Analysis reveals gamma-ray emitting regions within the jet of FSRQ 4C+01.28, suggesting new emission models.
The FSRQ 4C+01.28 is a bright and highly variable radio and $γ$-ray emitter. We aim to pinpoint the location of the $γ$-ray emitting region within its jet in order to derive strong constraints on $γ$-ray emission models for blazar jets. We use radio and $γ$-ray data obtained with ALMA, OVRO, SMA and Fermi/LAT to study the cross-correlation between $γ$-ray and multi-frequency radio light curves. Moreover, we employ VLBA observations at 43 GHz over a period of around nine years to study the parsec-scale jet kinematics. To pinpoint the location of the $γ$-ray emitting region, we use a model in which outbursts shown in the $γ$-ray and radio light curves are produced when moving jet components pass through the $γ$-ray emitting and the radio core regions. We find two bright and compact newly ejected jet components that are likely associated with a high activity period visible in the $γ$-ray and radio light curves. The kinematic analysis of the VLBA observations leads to a maximum apparent jet speed of βₐₚₚ=19±10 and an upper limit on the viewing angle of $ϕ$ < 4 deg. We determine the power law indices that are characterizing the jet geometry, brightness temperature distribution, and core shift to be l=0.974±0.098, s=-3.31±0.31, and kᵣ=1.09±0.17, which are in agreement with a conical jet in equipartition. A cross-correlation analysis shows that the radio light curves follow the $γ$-ray light curve. We pinpoint the location of the $γ$-ray emitting region with respect to the jet base to the range of 2.6\,pc≤ d_γ≤20\,pc. Our derived observational limits places the location of $γ$-ray production in 4C+01.28 beyond the expected extent of the broad-line region (BLR) and therefore challenges blazar-emission models that rely on inverse Compton up-scattering of seed photons from the BLR.
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Rösch et al. (2025) studied this question.
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