2023ApJ...943....3T


Query : 2023ApJ...943....3T

2023ApJ...943....3T - Astrophys. J., 943, 3 (2023/January-3)

Discussions on the Nature of GLEAM-X J162759.5-523504.3.

TONG H.

Abstract (from CDS):

The nature of the long-period radio transient GLEAM-X J162759.5-523504.3 (hereafter GLEAM-X J1627) is discussed. We try to understand both its radio emission and pulsation in the neutron star scenario as an alternative to the white dwarf model. We think that (1) from the radio emission point of view, GLEAM-X J1627 can be a radio-loud magnetar; (2) from the rotational evolution point of view, GLEAM-X J1627 is unlikely to be an isolated magnetar; (3) the 1091 s period is unlikely to be the precession period; (4) GLEAM-X J1627 may be a radio-loud magnetar spun down by a fallback disk; (5) the pulsar death line is modified due to the presence of a fallback disk or a twisted magnetic field. In both cases, a higher maximum acceleration potential can be obtained. This may explain why GLEAM-X J1627 is still radioactive with such a long pulsation period; and (6) general constraints on the neutron star magnetic field and initial disk mass are given analytically. Possible ways to discriminate between different modelings are also discussed.

Abstract Copyright: © 2023. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Magnetars - Pulsars - Radio pulsars

Simbad objects: 9

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Number of rows : 9
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 PSR J0146+6145 Psr 01 46 22.21 +61 45 03.8   28.100 25.620     ~ 613 0
2 PSR J0250+5854 Psr 02 50 17.78 +58 54 01.3           ~ 51 0
3 PSR J0901-4046 Psr 09 01 29.2490 -40 46 02.984           ~ 48 0
4 AJG 44 Psr 16 17 33.000 -51 02 00.00           ~ 552 3
5 PSR J1622-4950 Psr 16 22 44.80000 -49 50 54.5000           ~ 169 0
6 GLEAM-X J162759.5-523504 Psr 16 27 59.50 -52 35 04.3           ~ 51 0
7 AX J1809.8-1943 Psr 18 09 51.07 -19 43 51.8           ~ 532 0
8 PSR B1828-10 Psr 18 30 47.566 -10 59 27.90           ~ 190 1
9 2E 4673 HXB 23 01 08.14 +58 52 44.5           ~ 673 1

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