http://arxiv.org/abs/2202.13458
The repeating FRB 20190520B is localized to a galaxy at $z=0.241$, much closer than expected given its dispersion measure $\rm DM=1205\pm4 pc\ cm^{-3}$. Here we assess implications of the large DM and scattering observed from FRB 20190520B for the host galaxy’s plasma properties. Using a sample of 75 bursts detected with the Five-hundred-meter Aperture Spherical radio Telescope, we obtained a mean scattering time $\tau=10.9\pm1.5$ ms at 1.41 GHz, which can be attributed to the host galaxy. The mean scintillation bandwidth of $\Delta \nu_{\rm d}=0.21\pm0.01$ MHz at 1.41 GHz is consistent with Galactic diffractive interstellar scintillation. Balmer line measurements for the host imply an H$\alpha$ emission measure (galaxy frame) $\rm EM_s=620$ pc cm$^{-6} \times (T/10^4 {\rm K})^{0.9}$, implying $\rm DM_{\rm H\alpha}$ of order the value inferred from the FRB DM budget, $\rm DM_h=1121^{+89}{-138}$ pc cm$^{-3}$ for temperatures in excess of $10^4$ K. Combining $\tau$ and $\rm DM_h$ yields a nominal constraint on the scattering amplification from the host galaxy $\tilde{F} G=1.5^{+0.8}{-0.3}$ (pc$^2$ km)$^{-1/3}$, where $\tilde{F}$ describes turbulent density fluctuations and $G$ represents the geometric leverage to scattering that depends on the location of the scattering material. For a two-screen scattering geometry where $\tau$ arises from the host galaxy and $\Delta \nu_{\rm d}$ from the Milky Way, the implied distance between the FRB source and dominant scattering material is $\lesssim100$ pc. The host galaxy scattering and DM contributions support a novel technique for estimating FRB redshifts using the $\tau-\rm DM$ relation, and are consistent with previous findings that scattering of localized FRBs is largely dominated by plasma within host galaxies and the Milky Way.
S. Ocker, J. Cordes, S. Chatterjee, et. al.
Tue, 1 Mar 22
20/80
Comments: 13 pages, 9 figures, submitted to ApJ
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