2024ApJ...972...29W


Query : 2024ApJ...972...29W

2024ApJ...972...29W - Astrophys. J., 972, 29 (2024/September-1)

High-redshift Merger Model for Low-frequency Gravitational Wave Background.

WU Z.-F. and GIANNIOS D.

Abstract (from CDS):

In 2023, the Pulsar Timing Array Collaborations announced the discovery of a gravitational wave background (GWB), predominantly attributed to supermassive black hole binary (SMBHB) mergers. However, the detected GWB is several times stronger than the default value expected from galactic observations at low and moderate redshifts. Recent findings by the James Webb Space Telescope have unveiled a substantial number of massive, high-redshift galaxies, suggesting more massive SMBHB mergers at these early epochs. Motivated by these findings, we propose an “early merger” model that complements the standard merger statistics by incorporating these early, massive galaxies. We compare the early and standard “late merger” models, which assume peak merger rates in the local Universe, and match both merger models to the currently detected GWB. Our analysis shows that the early merger model has a significantly lower detection probability for single binaries and predicts a ∼30% likelihood that the first detectable single source will be highly redshifted and remarkably massive with rapid frequency evolution. In contrast, the late merger model predicts a nearly monochromatic first source at low redshift. The future confirmation of an enhanced population of massive high-redshift galaxies and the detection of fast-evolving binaries would strongly support the early merger model, offering significant insights into the evolution of galaxies and SMBHs.

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

Journal keyword(s): Gravitational waves - Supermassive black holes - Galaxy evolution

Simbad objects: 25

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Number of rows : 25
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 J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
3 PSR J0610-2100 Psr 06 10 13.602953 -21 00 27.74435           ~ 116 0
4 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
5 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
6 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
7 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
8 PSR J1643-1224 Psr 16 43 38.16612 -12 24 58.6334           ~ 260 2
9 PSR J1705-1903 Psr 17 05 43.84864 -19 03 41.4140           ~ 17 0
10 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
11 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
12 PSR J1744-1134 Psr 17 44 29.4220844 -11 34 54.801320           ~ 323 1
13 PSR J1745+1017 Psr 17 45 33.8371 +10 17 52.523           ~ 70 0
14 PSR J1747-4036 Psr 17 47 48.715690 -40 36 54.79950           ~ 83 0
15 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
16 PSR J1853+1303 Psr 18 53 57.3183 +13 03 44.088           ~ 107 1
17 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
18 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
19 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
20 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
21 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
22 PSR J1946+3417 Psr 19 46 25.13182 +34 17 14.6770           ~ 64 0
23 PSR B1953+29 Psr 19 55 27.8680959374 +29 08 43.499227152           ~ 303 1
24 PSR B2145-07.8 Psr 21 45 50.45590 -07 50 18.5900           ~ 336 0
25 PSR J2234+06 Psr 22 34 22 +06 11.0           ~ 76 0

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