2016/08/24 by David M. Russell, D. M. Russell, T. Shahbaz +3
Physics and Astronomy · #Astronomy #Astrophysical Phenomena and Observations #Astrophysics #Astrophysics and Cosmic Phenomena #Galaxy #Infrared #Line-of-sight #Magnetic field #Optics #Physics #Polarimetry #Polarization (electrochemistry) #Position angle #Pulsars and Gravitational Waves Research #Scattering #Synchrotron #astro-ph.HE
paper · pdf · doi:10.1093/mnras/stw2166
Accepted to MNRAS
arxiv created 2016/08/24 · openalex publication_date 2016/08/26 · arxiv updated 2016/09/07 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We present near-infrared polarimetric observations of the black hole X-ray binaries Swift J1357.2−0933 and A0620−00. In both sources, recent studies have demonstrated the presence of variable infrared synchrotron emission in quiescence, most likely from weak compact jets. For Swift J1357.2−0933, we find that the synchrotron emission is polarized at a level of 8.0 ± 2.5 per cent (a 3.2σ detection of intrinsic polarization). The mean magnitude and rms variability of the flux (fractional rms of 19–24 per cent in KS band) agree with previous observations. These properties imply a continuously launched (stable on long time-scales), highly variable (on short time-scales) jet in the Swift J1357.2−0933 system in quiescence, which has a moderately tangled magnetic field close to the base of the jet. We find that for A0620–00, there are likely to be three components to the optical–infrared polarization; interstellar dust along the line of sight, scattering within the system, and an additional source that changes the polarization position angle in the reddest (H and KS) wavebands. We interpret this as a stronger contribution of synchrotron emission, and by subtracting the line-of-sight polarization, we measure an excess of ∼1.25 ± 0.28 per cent polarization and a position angle of the magnetic field vector that is consistent with being parallel with the axis of the resolved radio jet. These results imply that weak jets in low-luminosity accreting systems have magnetic fields which possess similarly tangled fields compared to the more luminous, hard state jets in X-ray binaries.