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Unveiling the bent-jet structure and polarization of OJ 287 at 1.7 GHz with space VLBI

  • Ilje Cho
  • , José L. Gómez
  • , Rocco Lico
  • , Guang Yao Zhao
  • , Efthalia Traianou
  • , Rohan Dahale
  • , Antonio Fuentes
  • , Teresa Toscano
  • , Marianna Foschi
  • , Yuri Y. Kovalev
  • , Andrei Lobanov
  • , Alexander B. Pushkarev
  • , Leonid I. Gurvits
  • , Jae-Young Kim
  • , Mikhail Lisakov
  • , Petr Voitsik
  • , Ioannis Myserlis
  • , Felix Pötzl
  • , Eduardo Ros
  • CSIC - Institute of Astrophysics of Andalusia
  • National Institute for Astrophysics
  • Max Planck Institute for Radio Astronomy
  • RAS - P.N. Lebedev Physics Institute
  • Moscow Institute of Physics and Technology
  • Russian Academy of Sciences
  • Joint Institute for VLBI ERIC (JIVE)
  • Delft University of Technology
  • Institut de Radioastronomie Millimétrique
  • Foundation for Research and Technology-Hellas

Research output: Contribution to journalArticlepeer-review

5 Scopus citations

Abstract

We present total intensity and linear polarization images of OJ 287 at 1.68 GHz, obtained through space-based very long baseline interferometry (VLBI) observations with RadioAstron on April 16, 2016. The observations were conducted using a ground array consisting of the Very Long Baseline Array (VLBA) and the European VLBI Network (EVN). Ground-space fringes were detected with a maximum projected baseline length of ∼5.6 Earth's diameter, resulting in an angular resolution of ∼530 μas. With this unprecedented resolution at such a low frequency, the progressively bending jet structure of OJ 287 has been resolved up to ∼10 parsec of the projected distance from the radio core. In comparison with close-in-time VLBI observations at 15, 43, 86 GHz from MOJAVE and VLBA-BU-BLAZAR monitoring projects, we obtain the spectral index map showing the opaque core and optically thin jet components. The optically thick core has a brightness temperature of ∼1013 K, and is further resolved into two sub-components at higher frequencies labeled C1 and C2. These sub-components exhibit a transition from optically thick to thin, with a synchrotron self-absorption (SSA) turnover frequency estimated to be ∼33 and ∼11.5 GHz, and a turnover flux density ∼4 and ∼0.7 Jy, respectively. Assuming a Doppler boosting factor of 10, the SSA values provide the estimate of the magnetic field strengths from SSA of ∼3.4 G for C1 and ∼1.0 G for C2. The magnetic field strengths assuming equipartition arguments are also estimated as ∼2.6 G and ∼1.6 G, respectively. The integrated degree of linear polarization is found to be approximately ∼2.5%, with the electric vector position angle being well aligned with the local jet direction at the core region. This alignment suggests a predominant toroidal magnetic field, which is in agreement with the jet formation model that requires a helical magnetic field anchored to either the black hole ergosphere or the accretion disk. Further downstream, the jet seems to be predominantly threaded by a poloidal magnetic field.

Original languageEnglish
Article numberA248
JournalAstronomy and Astrophysics
Volume683
DOIs
StatePublished - 1 Mar 2024

Keywords

  • Galaxies: active
  • Galaxies: jets
  • Quasars: supermassive black holes
  • Radio continuum: galaxies

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