Making the invisible visible: Magnetic fields in accretion flows revealed by X-ray polarization
Samuel Barnier, Chris Done
arXiv:2404.12815v1 Announce Type: new
Abstract: Large scale, strong magnetic fields are often evoked in black hole accretion flows, for jet launching in the low/hard state and to circumvent the thermal instability in the high/soft state. Here we show how these ideas are strongly challenged by X-ray polarization measurements from IXPE. Quite general arguments show that equipartition fields in the accretion flow should be of order $10^{6-8}$ G. These produce substantial Faraday rotation and/or depolarization for photons escaping the flow in the 2-8 keV IXPE bandpass, which is not consistent with the observed data. While we stress that Faraday rotation should be calculated for each individual simulation (density, field geometry and emissivity), it seems most likely that there are no equipartition strength large scale ordered fields inside the photosphere of the X-ray emitting gas. Strong poloidal fields can still be present if they thread the black hole horizon rather than the X-ray emitting flow, so Blandford-Znajek jets are still possible, but an alternative solution is that the low/hard state jet is dominated by pairs so can be accelerated by lower fields. Fundamentally, polarization data from IXPE means that magnetic fields in black hole accretion flows are no longer invisible and unconstrained.arXiv:2404.12815v1 Announce Type: new
Abstract: Large scale, strong magnetic fields are often evoked in black hole accretion flows, for jet launching in the low/hard state and to circumvent the thermal instability in the high/soft state. Here we show how these ideas are strongly challenged by X-ray polarization measurements from IXPE. Quite general arguments show that equipartition fields in the accretion flow should be of order $10^{6-8}$ G. These produce substantial Faraday rotation and/or depolarization for photons escaping the flow in the 2-8 keV IXPE bandpass, which is not consistent with the observed data. While we stress that Faraday rotation should be calculated for each individual simulation (density, field geometry and emissivity), it seems most likely that there are no equipartition strength large scale ordered fields inside the photosphere of the X-ray emitting gas. Strong poloidal fields can still be present if they thread the black hole horizon rather than the X-ray emitting flow, so Blandford-Znajek jets are still possible, but an alternative solution is that the low/hard state jet is dominated by pairs so can be accelerated by lower fields. Fundamentally, polarization data from IXPE means that magnetic fields in black hole accretion flows are no longer invisible and unconstrained.