Lowly polarized light from a highly magnetized jet of GRB 190114C

TL;DR

This study presents early optical polarimetry of GRB 190114C, revealing low polarization likely dominated by dust and suggesting complex magnetic field structures in the jet, with implications for understanding GRB emission mechanisms.

Contribution

It provides the first detailed optical polarimetry of a TeV-detected GRB afterglow, highlighting low intrinsic polarization and challenging inverse Compton models for high-energy emission.

Findings

Polarization decreases from 7.7% to 2-4% and remains steady.

The afterglow is highly obscured with significant dust extinction.

Inverse Compton scattering models do not explain the low polarization.

Abstract

We report multi-color optical imaging and polarimetry observations of the afterglow of the first TeV- detected gamma-ray burst, GRB 190114C, using RINGO3 and MASTER II polarimeters. Observations begin 31 s after the onset of the GRB and continue until $\sim 7000\,$s post-burst. The light curves reveal a chromatic break at $\sim 400- 500\,$s, with initial temporal decay $\alpha = 1.669 \pm 0.013$ flattening to $\alpha \sim 1$ post-break, which we model as a combination of reverse and forward-shock components, with magnetization parameter $R_{\rm B} \sim 70$. The observed polarization degree decreases from $7.7 \pm 1.1\%$ to $2-4\%$ during $52-109\,$s post-burst and remains steady at this level for the subsequent $\sim 2000$-s, at constant position angle. Broadband spectral energy distribution modeling of the afterglow confirms GRB 190114C is highly obscured (A$_{\rm v, HG} = 1.49 \pm 0.12 \,$mag; N$_{\rm H, HG}= (9.0 \pm 0.3) \times 10^{22}\,$cm$^{-2}$). We interpret the measured afterglow polarization as intrinsically low and dominated by dust, in contrast to ${\rm P} >10\%$ measured previously for other GRB reverse shocks, with a small contribution from polarized prompt photons in the first minute. We test whether 1st and higher-order inverse Compton scattering in a magnetized reverse shock can explain the low optical polarization and the sub-TeV emission but conclude neither is explained in the reverse shock Inverse Compton model. Instead, the unexpectedly low intrinsic polarization degree in GRB 190114C can be explained if large-scale jet magnetic fields are distorted on timescales prior to reverse shock emission.