2019ApJ...875L..19Y


Query : 2019ApJ...875L..19Y

2019ApJ...875L..19Y - Astrophys. J., 875, L19-L19 (2019/April-3)

Second repeating FRB 180814.J0422+73 ten-year Fermi-LAT upper limits and implications.

YANG Y.-H., ZHANG B.-B. and ZHANG B.

Abstract (from CDS):

The second repeating fast radio burst source, FRB 180814.J0422+73, was detected recently by the CHIME collaboration. We use the ten-year Fermi Large Area Telescope archival data to place a flux upper limit in the energy range of 100 MeV-10 GeV at the position of the source, which is ∼1.1 x 10–11 erg cm–2 s–1 for a six-month time bin on average, and ∼2.4 x 10–12 erg cm–2 s–1 for the entire ten-year time span. For the maximum redshift of z = 0.11, the ten-year upper limit of luminosity is ∼7.3 x 1043 erg s–1. We utilize these upper limits to constrain the fast radio burst (FRB) progenitor and central engine. For the rotation-powered young magnetar model, the upper limits can pose constraints on the allowed parameter space for the initial rotational period and surface magnetic field of the magnetar. We also place significant constraints on the kinetic energy of a relativistic external shock wave, ruling out the possibility that there existed a gamma-ray burst (GRB) beaming toward Earth during the past ten years as the progenitor of the repeater. The case of an off-beam GRB is also constrained if the viewing angle is not much greater than the jet opening angle. All of these constraints are more stringent if FRB 180814.J0422+73 is at a closer distance.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): pulsars: general - radiation mechanisms: non-thermal - stars: magnetars - stars: magnetic field

Simbad objects: 3

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Number of rows : 3
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 NAME FRB 180814.J0422+73 rB 04 22 44.0 +73 39 52           ~ 112 0
2 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
3 FRB 131104 rB 06 44 10.4 -51 16 40           ~ 83 0

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