2026MNRAS.545f1997U


Query : 2026MNRAS.545f1997U

2026MNRAS.545f1997U - Mon. Not. R. Astron. Soc., 545, part no 6, 1997 (2026/January-2)

A depolarization census of ASKAP fast radio bursts.

UTTARKAR P.A., SHANNON R.M., GOURDJI K., DELLER A.T., DIAL T., GLOWACKI M., BERA A., GORDON A.C., RYDER S.D., TEJOS N., BHANDARI S. and WANG Y.

Abstract (from CDS):

Fast radio bursts (FRBs) are luminous, dispersed pulses of extragalactic origin. The physics of the emission mechanism, the progenitor environment, and their origin are unclear. Some repeating FRBs exhibit a frequency-dependent decrease in linear polarization fraction. This has been attributed to multipath propagation in a surrounding complex magneto-ionic environment. In this framework, the depolarization magnitude can be quantified using the parameter $\sigma ^{\prime }_{\rm RM}$, which can be used to model the magneto-ionic complexity of the medium. In addition to depolarization, some repeating sources (specifically, those with complex magneto-ionic environments) have been identified to have co-located persistent radio sources (PRS). Searches for depolarization of non-repeating sources are challenging due to the limited bandwidth of most FRB detection systems. However, even with a limited bandwidth, such depolarization can be identified if it lies within the $\sigma ^{\prime }_{\rm RM}$ sensitivity window of the telescope. In this paper, we present a search for depolarization in 12 one-off FRBs detected by the Australian SKA Pathfinder. We report on a strongly depolarized (apparently) non-repeating FRB detected by ASKAP (FRB 20230526A). The source shows a decrease in linear polarization fraction from $\sim$60 per cent at 1440 MHz to $\sim$20 per cent at 1110 MHz. We also report constraints on the presence of a PRS coincident with FRB 20230526A using observations obtained with the Australia Telescope Compact Array. We use this to study the relationship between $\sigma ^{\prime }_{\rm RM}$ and PRS luminosity. Our investigation supports a scenario in which repeaters and non-repeaters share a common origin and where non-repeaters represent an older population relative to repeating FRB sources.

Abstract Copyright: © The Author(s) 2025. Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): polarization - techniques: polarimetric - fast radio bursts

Simbad objects: 25

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Number of rows : 25
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 FRB 20230526A rB 01 29 27.500 -52 46 07.70           ~ 12 0
2 QSO B0131-522 Bla 01 33 05.76250002 -52 00 03.9454078   18.68 20.3 18.63   ~ 129 1
3 FRB 20180916B rB 01 58 00.750 +65 43 00.30           ~ 457 0
4 FRB 20221106A rB 03 46 38.100 -25 39 44.90           ~ 12 0
5 FRB 20201124A rB 05 07 57.600 +26 11 24.00           ~ 307 0
6 FRB 20210407E rB 05 14 46.300 +27 04 12.30           ~ 4 0
7 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
8 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
9 FRB 180301 rB 06 12 43.40 +04 33 44.8           ~ 125 0
10 FRB 20190217A rB 06 19 31.2000 +43 06 36.000           ~ 8 0
11 FRB 20230718A rB 08 32 38.804 -40 27 06.33           ~ 12 0
12 FRB 210320 rB 13 37 16.800 -15 24 37.30           ~ 29 0
13 NAME Lupus SN SNR 15 02 22.1 -42 05 49           ~ 1407 1
14 FRB 200430 rB 15 18 49.54 +12 22 36.8           ~ 59 0
15 FRB 20190520B rB 16 02 04.270 -11 17 17.32           ~ 211 0
16 ICRF J193925.0-634245 Sy2 19 39 25.0245304992 -63 42 45.640373400   18.87 18.37 17.64   ~ 1332 2
17 FRB 20240114A rB 21 27 39.8350 +04 19 45.634           ~ 66 0
18 FRB 191001 rB 21 33 24.373 -54 44 51.40           ~ 64 0
19 FRB 20190711A rB 21 57 40.7 -80 21 29           ~ 114 0
20 FRB 20220725A rB 22 27 00.000 +34 53 00.00           ~ 13 0
21 FRB 20210117A rB 22 39 55.015 -16 09 05.45           ~ 49 0
22 FRB 191228 rB 22 57 43.30 -29 35 38.7           ~ 37 0
23 FRB 210912 rB 23 23 10.35 -30 24 19.2           ~ 12 0
24 FRB 20220610A rB 23 24 17.569 -33 30 49.37           ~ 31 0
25 FRB 20220501C rB 23 29 50.000 -32 27 00.00           ~ 12 0

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