2026ApJ...998...70F


Query : 2026ApJ...998...70F

2026ApJ...998...70F - Astrophys. J., 998, 70 (2026/February-2)

Mass-Radius Constraints for 2S 0918-549 from an RXTE Superexpansion Burst: A Direct Cooling-tail Analysis.

FAN H., LIU H., LI Z., CHEN Y., BAN S., LU G., DOHI A., ZHU C. and XU R.

Abstract (from CDS):

Thermonuclear (Type I) X-ray bursts from accreting neutron stars (NSs) offer a means to determine NS mass (M) and radius (R) and thereby probe the properties of matter at supranuclear density. A subset of these events, photospheric radius-expansion bursts, provide a particularly powerful tool to constrain the NS M and R. Here, we apply the direct cooling-tail method to 2S 0918-549, using a rare superexpansion burst observed by Rossi X-ray Timing Explorer. We fit only the posttouchdown data within F/Ftd ∈ [0.6, 0.95], employing modern atmosphere models (pure-He and metal-enriched). The pure-He atmosphere yields a good description of the cooling tail (χ2/ν = 18.12/14), whereas metal-rich models fail; information-criterion tests (Akaike information criterion/Bayesian information criterion) disfavor adding a free absorption edge in every time bin, indicating that heavy-element ashes are unnecessary. The joint fit gives a distance d = 4.1-5.3 kpc and mass-radius constraints M = 1-2 M⊙ and R = 9.7-11.9 km (99% confidence). These results suggest that representative families of both gravity-bound and self-bound equations of state remain viable at the 1σ confidence level.

Abstract Copyright: © 2026. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Low-mass X-ray binary stars - X-ray bursts - Neutron stars

Simbad objects: 12

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Number of rows : 12
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 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
2 V* V1055 Ori LXB 06 17 07.3565603963 +09 08 13.515857360   18.80 18.5     ~ 594 1
3 4U 0919-54 LXB 09 20 26.4818170056 -55 12 24.512806404 20.40 21.30 21.0     ~ 175 0
4 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
5 V* QV Nor HXB 15 42 23.3633146128 -52 23 09.577395960   16.3 14.5     B0.2Ia 455 1
6 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
7 4U 1722-30 LXB 17 27 33.25 -30 48 07.4     12.50     ~ 278 1
8 Granat 1747-312 LXB 17 50 46.862 -31 16 28.86           ~ 135 0
9 V* V4722 Sgr LXB 18 10 44.47 -26 09 01.2   21.5     18.449 ~ 99 0
10 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
11 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
12 CXOU J212958.1+121002 XB* 21 29 58.06 +12 10 02.6     16.6     ~ 87 1

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