2024A&A...683A.243Q


Query : 2024A&A...683A.243Q

2024A&A...683A.243Q - Astronomy and Astrophysics, volume 683A243 (2024/3-1)

Probing a magnetar origin for the population of extragalactic fast X-ray transients detected by Chandra.

QUIROLA-VASQUEZ J., BAUER F.E., JONKER P.G., BRANDT W.N., EAPPACHEN D., LEVAN A.J., LOPEZ E., LUO B., RAVASIO M.E., SUN H., XUE Y.Q., YANG G. and ZHENG X.C.

Abstract (from CDS):

Context. Twenty-two extragalactic fast X-ray transients (FXTs) have now been discovered from two decades of Chandra data (analyzing ∼259 Ms of data), with 17 associated with distant galaxies (≳100 Mpc). Different mechanisms and progenitors have been proposed to explain their properties; nevertheless, after analyzing their timing, spectral parameters, host-galaxy properties, luminosity function, and volumetric rates, their nature remains uncertain.
Aims. We interpret a sub-sample of nine FXTs that show a plateau or a fast-rise light curve within the framework of a binary neutron star (BNS) merger magnetar model.
Methods. We fit their light curves and derive magnetar (magnetic field and initial rotational period) and ejecta (ejecta mass and opacity) parameters. This model predicts two zones: an orientation-dependent free zone (where the magnetar spin-down X-ray photons escape freely to the observer) and a trapped zone (where the X-ray photons are initially obscured and only escape freely once the ejecta material becomes optically thin). We argue that six FXTs show properties consistent with the free zone and three FXTs with the trapped zone.
Results. This sub-sample of FXTs has a similar distribution of magnetic fields and initial rotation periods to those inferred for short gamma-ray bursts, suggesting a possible association. We compare the predicted ejecta emission fed by the magnetar emission (called merger-nova) to the optical and near-infrared upper limits of two FXTs, XRT 141001 and XRT 210423 where contemporaneous optical observations are available. The non-detections place lower limits on the redshifts of XRT 141001 and XRT 210423 of z ≳ 1.5 and ≳0.1, respectively.
Conclusions. If the magnetar remnants lose energy via gravitational waves (GWs), it should be possible to detect similar objects with the current advanced LIGO detectors out to a redshift z ≲ 0.03, while future GW detectors will be able to detect them out to z ≈ 0.5.

Abstract Copyright: © The Authors 2024

Journal keyword(s): gamma-ray burst: general - stars: magnetars - X-rays: bursts - X-rays: general

Simbad objects: 27

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Number of rows : 27
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 CXO J010344.5-214845 X 01 03 44.59 -21 48 45.9           ~ 8 0
2 [BTS2017] CDF-S XT2 G 03 32 18.38112 -27 52 23.8692   26.509     24.598 ~ 46 0
3 NAME XRT 150322 ? 03 32 18.41 -27 52 24.4           ~ 7 0
4 NAME Chandra Deep Field-South reg 03 32 28.0 -27 48 30           ~ 2282 1
5 NAME XRT 100831 ? 03 32 38.78 -27 51 33.8           ~ 5 0
6 [BTS2017] CDF-S XT1 G 03 32 38.8 -27 51 34           ~ 40 0
7 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
8 GRB 230307A gB 04 03 26.24 -75 22 43.8           ~ 221 0
9 CXO J050706.7-315210 X 05 07 06.76 -31 52 10.8           ~ 9 0
10 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
11 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
12 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
13 PSR J0952-0607 Psr 09 52 08.319 -06 07 23.49           ~ 103 0
14 SDSS J112848.22+170418.5 G 11 28 48.22989 +17 04 18.5014           ~ 393 0
15 NAME XRT 000519 X 12 25 31.64 +13 03 58.8           ~ 19 0
16 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
17 ACO 1795 ClG 13 48 47.4 +26 34 55           ~ 1330 0
18 NAME XRT 210423 ev 13 48 56.46 +26 39 44.3           ~ 22 0
19 NAME XRT 191127 ? 13 49 23.31 +26 35 03.2           ~ 5 0
20 NAME XRT 110103 ev 14 08 28.89 -27 03 29.4           ~ 8 0
21 SDSS J140910.47+275320.8 G 14 09 10.47535 +27 53 20.8393           ~ 279 0
22 NAME XRT 140507 ? 15 34 56.39 +23 28 06.6           ~ 4 0
23 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
24 GRB 060614 G 21 23 32.140 -53 01 36.10           ~ 714 0
25 GRB 191019A gB 22 40 05.87 -17 19 40.8           ~ 55 0
26 NVSS J230126-385839 rG 23 01 26.7650 -38 58 40.422   22.22 21.22 21   ~ 325 1
27 CXO J234503.4-423841 X 23 45 03.44 -42 38 41.7           ~ 11 0

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