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March 14, 2026The Astrophysical Journal0 citationsOpen Access

Different Polarized Components of the Quasar 3C 286 Revealed by FAST

PTPengfu TianXCXiao ChenWuhan University of TechnologyWYWen YangYunnan Normal University

Key Points

  • To analyze the effects of interplanetary scintillation on the polarized emissions of quasar 3C 286.
  • Conducted high-time-resolution observations using the Five-hundred-meter Aperture Spherical radio Telescope.
  • Analyzed data from 2019 to 2023 to assess polarized flux densities.
  • Evaluated variations in Stokes I, Q, U, and V parameters.
  • Detected IPS affecting polarized flux densities in Stokes I, Q, and U.
  • Observed synchronous variations between Stokes I and U, with Stokes Q showing more randomness.
  • Estimated a 2.8 s time delay between Stokes I and Q, indicating different emission regions.

Abstract

Abstract 3C 286, a well-known radio calibrator, exhibits stability in both total flux density and polarization parameters. However, its stable and luminous interstellar radio signal may encounter interplanetary scintillation (IPS) due to density irregularities in the solar wind within the heliosphere. In this work, we analyze high-time-resolution observations of 3C 286 obtained with the Five-hundred-meter Aperture Spherical radio Telescope from 2019 to 2023. Our analysis reveals that IPS affects the polarized flux densities of the Stokes I , Q , and U parameters, whereas Stokes V shows no detectable IPS-induced variations. The IPS variations detected in Stokes I are synchronous with those in Stokes U , while those in Stokes Q exhibit greater randomness. The cross-correlation function results indicate no time delay between Stokes I and U but a delay of approximately 2.8 s between Stokes I and Q . This suggests that the different polarized radio emissions of 3C 286 originate from distinct emission regions, specifically the core and the southwestern jet. Furthermore, the projections of the radio core and jet component onto the scintillation screen at 1 au yield a solar wind plasma speed of ∼637 km s −1 .

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Cite This Study

Tian et al. (2026) studied this question.

synapsesocial.com/papers/69b4fb8db39f7826a300bc04https://doi.org/10.3847/1538-4357/ae4877
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