2024MNRAS.527.6055C


Query : 2024MNRAS.527.6055C

2024MNRAS.527.6055C - Mon. Not. R. Astron. Soc., 527, 6055-6064 (2024/January-3)

On the possibility to detect gravitational waves from post-merger supermassive neutron stars with a kilohertz detector.

CHEN Y., LIU B., AI S., LAN L., GAO H., YUAN Y. and ZHU Z.-H.

Abstract (from CDS):

The detection of a secular post-merger gravitational wave (GW) signal in a binary neutron star (BNS) merger serves as strong evidence for the formation of a long-lived post-merger neutron star (NS), which can help constrain the maximum mass of NSs and differentiate NS equations of state. We specifically focus on the detection of GW emissions from rigidly rotating NSs formed through BNS mergers, using several kilohertz GW detectors that have been designed. We simulate the BNS mergers within the detecting limit of LIGO-Virgo-KARGA O4 and attempt to find out on what fraction the simulated sources may have a detectable secular post-merger GW signal. For kilohertz detectors designed in the same configuration of LIGO A+, we find that the design with peak sensitivity at approximately 2 kHz is most appropriate for such signals. The fraction of sources that have a detectable secular post-merger GW signal would be approximately $0.94{\!-\!}11~{{ \rm per\ cent}}$ when the spin-downs of the post-merger rigidly rotating NSs are dominated by GW radiation, while it would be approximately $0.46{\!-\!}1.6~{{ \rm per\ cent}}$ when the contribution of electromagnetic (EM) radiation to the spin-down processes is non-negligible. We also estimate this fraction based on other well-known proposed kilohertz GW detectors and find that, with advanced design, it can reach approximately $12{\!-\!}45~{{ \rm per\ cent}}$ for the GW-dominated spin-down case and $4.7{\!-\!}16~{{\rm per\ cent}}$ when both the GW and EM radiations are considered.

Abstract Copyright: © 2023 The Author(s). Published by Oxford University Press on behalf of Royal Astronomical Society.

Journal keyword(s): gravitational waves - neutron star mergers

Simbad objects: 38

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Number of rows : 38
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 Fermi bn100117879 G 00 45 04.6610 -01 35 42.020           ~ 155 0
2 GRB 100625A gB 01 03 10.98 -39 05 18.3           ~ 124 0
3 GRB 180805B gB 01 43 07.59 -17 29 36.4           ~ 32 0
4 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
5 Fermi bn081024245 gB 01 51 33.80 +61 21 08.2           ~ 75 0
6 GRB 120305A gB 03 10 08.73 +28 29 30.9           ~ 56 0
7 GRB 200411A gB 03 10 39.39 -52 19 03.3           ~ 31 0
8 GRB 070714B G 03 51 22.2720 +28 17 50.943           ~ 248 0
9 GRB 071227A G 03 52 31.0260 -55 59 00.890           ~ 201 0
10 GRB 101219A gB 04 58 20.45 -02 32 23.1           ~ 152 0
11 GRB 200907B G 05 56 06.9510 +06 54 22.637           ~ 24 0
12 GRB 061006 G 07 24 07.8080 -79 11 55.188           ~ 214 0
13 GRB 051227 gB 08 20 58.107 +31 55 32.01           ~ 127 0
14 GRB 120521A gB 09 54 53.91 -49 25 02.4           ~ 41 0
15 UCAC4 217-047923 * 10 19 02.5992684123 -46 40 11.294771086   13.795 12.458 12.114   ~ 54 0
16 GRB 090515 gB 10 56 41.0 +14 27 22           ~ 122 0
17 GRB 181123B G 12 17 27.9100 +14 35 52.270           ~ 47 0
18 GRB 210726A G 12 53 09.8200 +19 11 25.032           ~ 36 0
19 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
20 GRB 060801 G 14 12 01.2620 +16 58 55.970           ~ 172 0
21 GRB 150423A gB 14 46 18.96 +12 17 00.6           ~ 79 0
22 Fermi bn150301045 gB 16 17 13.13 -48 42 47.2           ~ 31 0
23 GRB 100702A gB 16 22 47.26 -56 31 53.8           ~ 53 0
24 UGCS J162444.39-273226.8 G 16 24 44.38275 -27 32 26.8381     19.70     ~ 469 1
25 Fermi bn180402406 gB 16 47 43.90 -14 58 12.1           ~ 31 0
26 GRB 080919 gB 17 40 53.00 -42 22 29.5           ~ 49 0
27 Fermi bn160821937 gB 18 39 54.550 +62 23 30.35           ~ 190 0
28 GRB 191031D gB 18 53 09.57 +47 38 38.5           ~ 46 0
29 Fermi bn080905499 G 19 10 42.0450 -18 52 54.510           ~ 200 0
30 GRB 080702A gB 20 52 12.21 +72 18 46.7           ~ 47 0
31 GRB 051210 gB 22 00 40.930 -57 36 47.10           ~ 138 0
32 Fermi bn160624477 gB 22 00 46.21 +29 38 37.8           ~ 69 0
33 GRB 061201 gB 22 08 32.060 -74 34 47.90           ~ 205 0
34 Fermi bn090510016 G 22 14 12.6230 -26 34 58.550           ~ 548 0
35 Fermi bn200219317 G 22 50 33.1080 -59 07 11.579           ~ 42 0
36 GRB 180727A G 23 06 40.0380 -63 03 07.088           ~ 29 0
37 GRB 190425 GWE ~ ~           ~ 438 0
38 GrW 150914 GWE ~ ~           ~ 674 1

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