2022ApJ...924..129Q


Query : 2022ApJ...924..129Q

2022ApJ...924..129Q - Astrophys. J., 924, 129-129 (2022/January-2)

On the angular momentum transport efficiency within the star constrained from gravitational-wave observations.

QIN Y., WANG Y.-Z., WU D.-H., MEYNET G. and SONG H.

Abstract (from CDS):

The LIGO Scientific Collaboration and Virgo Collaboration (LIGO/Virgo) have recently reported in GWTC-2.1 eight additional candidate events with a probability of astrophysical origin greater than 0.5 in the LIGO/Virgo's deeper search on O3a running. In GWTC-2.1, the majority of the effective inspiral spins (χeff) show magnitudes consistent with zero, while two (GW190403–051519 and GW190805–211137) of the eight new events have χeff > 0 (at 90% credibility). We note that GW190403–051519 was reported with χeff = 0.70–0.27+0.15 and mass ratio q = 0.25–0.11+0.54. Assuming a uniform prior probability between 0 and 1 for each black hole's dimensionless spin magnitude, GW190403–051519 was reported with the dimensionless spin of the more massive black hole, χ1 = 0.92–0.22+0.07. This is the fastest black hole ever measured in all current gravitational-wave events. If the immediate progenitor of GW190403–051519 is a close binary system composed of a black hole and a helium star, which can be the natural outcome of the classical isolated binary evolution through the common envelope phase, this extremely high spin challenges, at least in that case, the existence of an efficient angular momentum transport mechanism between the stellar core and the radiative envelope of massive stars, as for instance predicted by the Tayler-Spruit dynamo or its revised version by Fuller et al.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Gravitational waves - Massive stars - Stellar rotation - Binary stars

Simbad objects: 58

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Number of rows : 58
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 GrW 190814 GWE 00 55.8 -27 05           ~ 433 0
2 NAME M33 X-7 HXB 01 33 34.13 +30 32 11.3 17.50 18.80 18.70     O 187 2
3 GrW 170814 GWE 03 11.0 -44 57           ~ 157 0
4 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
5 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
6 GrW 190412 GWE ~ ~           ~ 169 0
7 GrW 190413 134308 GWE ~ ~           ~ 32 0
8 GrW 190424 180648 GWE ~ ~           ~ 21 0
9 GrW 190503 185404 GWE ~ ~           ~ 40 0
10 GrW 190513 205428 GWE ~ ~           ~ 39 0
11 GrW 190517 055101 GWE ~ ~           ~ 64 0
12 GrW 190521 GWE ~ ~           ~ 409 0
13 GrW 190527 092055 GWE ~ ~           ~ 28 0
14 GrW 190620 030421 GWE ~ ~           ~ 49 0
15 GrW 190701 203306 GWE ~ ~           ~ 43 0
16 GrW 190707 093326 GWE ~ ~           ~ 38 0
17 GrW 190719 215514 GWE ~ ~           ~ 30 0
18 GrW 190725 174728 GWE ~ ~           ~ 23 0
19 GrW 190403 051519 GWE ~ ~           ~ 38 0
20 GrW 190803 022701 GWE ~ ~           ~ 34 0
21 GrW 190828 065509 GWE ~ ~           ~ 40 0
22 GrW 190910 112807 GWE ~ ~           ~ 34 0
23 GrW 190916 200658 GWE ~ ~           ~ 17 0
24 GrW 190924 021846 GWE ~ ~           ~ 50 0
25 GrW 190926 050336 GWE ~ ~           ~ 16 0
26 GrW 190930 133541 GWE ~ ~           ~ 44 0
27 GrW 150914 GWE ~ ~           ~ 674 1
28 GrW 151226 GWE ~ ~           ~ 275 1
29 GrW 170608 GWE ~ ~           ~ 127 0
30 GrW 170809 GWE ~ ~           ~ 69 0
31 GrW 170818 GWE ~ ~           ~ 75 0
32 GrW 190408 181802 GWE ~ ~           ~ 46 0
33 GrW 190413 052954 GWE ~ ~           ~ 29 0
34 GrW 190421 213856 GWE ~ ~           ~ 37 0
35 GrW 190426 190642 GWE ~ ~           ~ 30 0
36 GrW 190512 180714 GWE ~ ~           ~ 43 0
37 GrW 190514 065416 GWE ~ ~           ~ 26 0
38 GrW 190519 153544 GWE ~ ~           ~ 56 0
39 GrW 190521 074359 GWE ~ ~           ~ 40 0
40 GrW 190602 175927 GWE ~ ~           ~ 51 0
41 GrW 190630 185205 GWE ~ ~           ~ 40 0
42 GrW 190706 222641 GWE ~ ~           ~ 55 0
43 GrW 190708 232457 GWE ~ ~           ~ 34 0
44 GrW 190720 000836 GWE ~ ~           ~ 39 0
45 GrW 190727 060333 GWE ~ ~           ~ 40 0
46 GrW 190731 140936 GWE ~ ~           ~ 32 0
47 GrW 190805 211137 GWE ~ ~           ~ 20 0
48 GrW 190828 063405 GWE ~ ~           ~ 41 0
49 GrW 190915 235702 GWE ~ ~           ~ 41 0
50 GrW 190917 114630 GWE ~ ~           ~ 28 0
51 GrW 190925 232845 GWE ~ ~           ~ 23 0
52 GrW 190929 012149 GWE ~ ~           ~ 35 0
53 GrW 190728 GWE ~ ~           ~ 48 0
54 GrW 190909 114149 GWE ~ ~           ~ 18 0
55 GrW 151012 grv ~ ~           ~ 162 1
56 GrW 170104 GWE ~ ~           ~ 186 1
57 GrW 170729 GWE ~ ~           ~ 127 0
58 GrW 170823 GWE ~ ~           ~ 69 0

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