2024ApJ...977..196H


Query : 2024ApJ...977..196H

2024ApJ...977..196H - Astrophys. J., 977, 196 (2024/December-3)

Rethinking Thorne-Żytkow Object Formation: The Fate of X-Ray Binary LMC X-4 and Implications for Ultra-long Gamma-Ray Bursts.

HUTCHINSON-SMITH T., EVERSON R.W., TWUM A.A., BATTA A., YARZA R., LAW-SMITH J.A.P., VIGNA-GOMEZ A. and RAMIREZ-RUIZ E.

Abstract (from CDS):

We present a start-to-end simulation aimed at studying the long-term fate of high-mass X-ray binaries and whether a Thorne-Żytkow object (TŻO) might ultimately be assembled. We analyze results from a 3D hydrodynamical simulation that models the eventual fate of LMC X-4, a compact high-mass X-ray binary system, after the primary fills its Roche lobe and engulfs the neutron star companion. We discuss the outcome of this engulfment within the standard paradigm of TŻO formation. The post-merger angular momentum content of the stellar core is a key ingredient, as even a small amount of rotation can break spherical symmetry and produce a centrifugally supported accretion disk. Our findings suggest the inspiraling neutron star, upon merging with the core, can accrete efficiently via a disk at high rates (≈10–2M⊙ s–1), subsequently collapsing into a black hole and triggering a bright transient with a luminosity and duration typical of an ultra-long gamma-ray burst. We propose that the canonical framework for TŻO formation via common envelope needs to be revised, as the significant post-merger accretion feedback will unavoidably unbind the vast majority of the surrounding envelope.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Transient sources - Close binary stars - Interacting binary stars - Stellar mergers - Hydrodynamical simulations - Late stellar evolution - Stellar interiors - X-ray binary stars - High mass x-ray binary stars - Gamma-ray bursts

Simbad objects: 19

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Number of rows : 19
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 GRB 101225A gB 00 00 47.48 +44 36 01.0           ~ 163 0
2 AT 2018bwo ev 00 14 01.680 -23 11 35.38           ~ 22 0
3 M31N 2015-01a No* 00 42 07.99 +40 55 01.1           ~ 70 0
4 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 12317 1
5 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
6 SV* HV 2112 Mi* 01 10 03.8526682872 -72 36 52.585541676 18.72 18.39 16.59 15.80 11.06 M5II-III 51 2
7 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
8 GRB 121027A gB 04 14 23.450 -58 49 47.17           ~ 136 0
9 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
10 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0 14.290   O8III 714 0
11 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
12 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1159 0
13 NAME M101 OT2015-1 SN? 14 02 16.78 +54 26 20.5   19.19 17.57 16.92 16.26 ~ 51 0
14 AT 2014ib SN? 14 59 59.47 +01 54 26.6           ~ 43 1
15 V* QV Nor HXB 15 42 23.3633146128 -52 23 09.577395960   16.3 14.5     B0.2Ia 455 1
16 2MASS J17004888-4139214 HXB 17 00 48.884 -41 39 21.46           Ofpe/WN9 272 0
17 HD 153919 HXB 17 03 56.7725629224 -37 50 38.913331452 6.06 6.78 6.51 6.08 5.90 O6Iafcp 851 0
18 SAX J1802.7-2017 HXB 18 02 41.9407199832 -20 17 17.312648064   17.4 16.4     B1Ib 100 0
19 XTE J1855-026 HXB 18 55 30.4058947392 -02 36 16.737653700   16.451 14.512 14.056   B0Iaep 104 0

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