Astronomy:List of gravitational wave observations
This page contains a list of observed/candidate gravitational wave events.
Origin and nomenclature
Direct observation of gravitational waves, which commenced with the detection of an event by LIGO in 2015,[1] plays a key role in gravitational wave astronomy. LIGO has been involved in all subsequent detections to date, with Virgo joining in August 2017.[2]
Joint observation runs of LIGO and VIRGO, designated "O1, O2, etc." span many months, with months of maintenance and upgrades in-between designed to increase the instruments sensitivity and range. Within these run periods, the instruments are capable of detecting gravitational waves.
The first run, O1, ran from September 12, 2015, to January 19, 2016, and succeeded in its first gravitational wave detection. O2 ran for a greater duration, from November 30, 2016, to August 25, 2017.[3] O3 began on April 1, 2019, which was briefly suspended on September 30, 2019, for maintenance and upgrades, thus O3a. O3b marks resuming of the run and began on November 1, 2019. Due to the COVID-19 pandemic[4] O3 was forced to end prematurely.[5] O4 began on May 24, 2023; initially planned for March, the project needed more time to stabilize the instruments.
The O4 observing run has been extended from one year to 18 months, following plans to make further upgrades for the O5 run.[2][6] Updated observing plans are published on the official website, containing the latest information on these runs.[6] There is a two month commissioning break planned from January to March 2024, after which observations will resume for the remainder of O4.[7]
Gravitational wave events are named starting with the prefix GW, while observations that trigger an event alert but have not (yet) been confirmed are named starting with the prefix S.[8] Six digits then indicate the date of the event, with the two first digits representing the year, the two middle digits the month and two final digits the day of observation. This is similar to the systematic naming for other kinds of astronomical event observations, such as those of gamma-ray bursts.
Probable detections that are not confidently identified as gravitational wave events are designated LVT ("LIGO-Virgo trigger"). Known gravitational wave events come from the merger of two black holes (BH), two neutron stars (NS), or a black hole and a neutron star (BHNS).[9][10] Some objects are in the mass gap between the largest predicted neutron star masses (Tolman–Oppenheimer–Volkoff limit) and the smallest known black holes.
List of gravitational wave events
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Script error: No such module "Chart". |
GW event and time (UTC)[n 1] |
Date published |
Location area[n 2] (deg2) |
Signal to Noise Ratio (SNR) |
Luminosity distance (Mpc)[n 3] |
Energy radiated/c2 (M☉) [n 4] |
Chirp mass (M☉) [n 5] |
Effective spin[n 6] | Primary | Secondary | Remnant | Notes | Ref. | ||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Type | Mass (M☉) | Type | Mass (M☉) | Type | Mass (M☉) | Spin[n 7] | ||||||||||
GW150914 09:50:45 |
2016-02-11 | 179; mostly to the south
|
24.4+0.8
−0.8 |
430+150
−170 |
3.1+0.4
−0.4 |
28.6+1.6
−1.5 |
−0.01+0.12
−0.13 |
BH [n 8] |
35.6+4.8
−3.0 |
BH [n 9] |
30.6+3.0
−4.4 |
BH
|
63.1+3.3
−3.0 |
0.69+0.05
−0.04 |
First GW detection; first BH merger observed |
[18][19][17] |
GW151012 (fr) 09:54:43 |
2016-06-15 | 1555
|
10.0+0.5
−0.5 |
1060+540
−480 |
1.5+0.5
−0.5 |
15.2+2.0
−1.1 |
0.04+0.28
−0.19 |
BH
|
23.3+14.0
−5.5 |
BH
|
13.6+4.1
−4.8 |
BH
|
35.7+9.9
−3.8 |
0.67+0.13
−0.11 |
Formerly candidate LVT151012; accepted as astrophysical since February 2019 |
[20][12][11] |
GW151226 03:38:53 |
2016-06-15 | 1033
|
13.1+0.0
−1.2 |
440+180
−190 |
1.0+0.1
−0.2 |
8.9+0.3
−0.3 |
0.18+0.20
−0.12 |
BH
|
13.7+8.8
−3.2 |
BH
|
7.7+2.2
−2.6 |
BH
|
20.5+6.4
−1.5 |
0.74+0.07
−0.05 |
[21][22] | |
GW170104 10:11:58 |
2017-06-01 | 924
|
13.0+0.0
−0.0 |
960+430
−410 |
2.2+0.5
−0.5 |
21.5+2.1
−1.7 |
−0.04+0.17
−0.20 |
BH
|
31.0+7.2
−5.6 |
BH
|
20.1+4.9
−4.5 |
BH
|
49.1+5.2
−3.5 |
0.66+0.08
−0.10 |
||
GW170608 02:01:16 |
2017-11-16 | 396; to the north
|
14.9+0.5
−0.8 |
320+120
−110 |
0.9+0.0
−0.1 |
7.9+0.2
−0.2 |
0.03+0.19
−0.07 |
BH
|
10.9+5.3
−1.7 |
BH
|
7.6+1.3
−2.1 |
BH
|
17.8+3.2
−0.7 |
0.69+0.04
−0.04 |
Smallest BH progenitor masses to date |
[23] |
GW170729 18:56:29 |
2018-11-30 | 1033
|
10.2+0.6
−0.4 |
2750+1350
−1320 |
4.8+1.7
−1.7 |
35.7+6.5
−4.7 |
0.36+0.21
−0.25 |
BH
|
50.6+16.6
−10.2 |
BH
|
34.3+9.1
−10.1 |
BH
|
80.3+14.6
−10.2 |
0.81+0.07
−0.13 |
Largest progenitor masses until GW190521 | [12] |
GW170809 08:28:21 |
2018-11-30 | 340; towards Cetus
|
12.4+0.0
−0.2 |
990+320
−380 |
2.7+0.6
−0.6 |
25.0+2.1
−1.6 |
0.07+0.16
−0.16 |
BH
|
35.2+8.3
−6.0 |
BH
|
23.8+5.2
−5.1 |
BH
|
56.4+5.2
−3.7 |
0.70+0.08
−0.09 |
[12] | |
GW170814 10:30:43 |
2017-09-27 | 87; towards Eridanus
|
16.3+0.9
−0.4 |
580+160
−210 |
2.7+0.4
−0.3 |
24.2+1.4
−1.1 |
0.07+0.12
−0.11 |
BH
|
30.7+5.7
−3.0 |
BH
|
25.3+2.9
−4.1 |
BH
|
53.4+3.2
−2.4 |
0.72+0.07
−0.05 |
First announced detection by three observatories; first polarization measurement |
[24][25] |
GW170817 12:41:04 |
2017-10-16 | 16; NGC 4993
|
33.0+0.0
−2.1 |
40±10
|
≥ 0.04
|
1.186+0.001
−0.001 |
0.00+0.02
−0.01 |
NS
|
1.46+0.12
−0.10 |
NS
|
1.27+0.09
−0.09 |
NS [n 10] |
≤ 2.8[n 11] | ≤ 0.89
|
First NS merger observed in GW; first detection of EM counterpart (GRB 170817A; AT 2017gfo); nearest event to date |
[16][28][29] |
GW170818 02:25:09 |
2018-11-30 | 39; towards Pegasus
|
11.3+0.0
−0.0 |
1020+430
−360 |
2.7+0.5
−0.5 |
26.7+2.1
−1.7 |
−0.09+0.18
−0.21 |
BH
|
35.5+7.5
−4.7 |
BH
|
26.8+4.3
−5.2 |
BH
|
59.8+4.8
−3.8 |
0.67+0.07
−0.08 |
[12] | |
GW170823 13:13:58 |
2018-11-30 | 1651
|
11.1+0.4
−0.3 |
1850±840
|
3.3+0.9
−0.8 |
29.3+4.2
−3.2 |
0.08+0.20
−0.22 |
BH
|
39.6+10.0
−6.6 |
BH
|
29.4+6.3
−7.1 |
BH
|
65.6+9.4
−6.6 |
0.71+0.08
−0.10 |
[12] | |
GW190408_181802 2019-04-08 |
2020-10-27 | 140
|
15.3+0.2
−0.3 |
1580+400
−590 |
18.3+1.4
−1.2 |
−0.03+0.13
−0.19 |
BH
|
24.5+5.1
−3.4 |
BH
|
18.3+3.2
−3.5 |
BH
|
41.0+3.8
−2.7 |
0.67+0.06
−0.07 |
Originally designated S190408an. | [30] | |
GW190412 2019-04-12 05:30:44 |
2020-04-17 | 18.9+0.2
−0.3 |
730+140
−170 |
13.3+0.4
−0.3 |
0.25+0.08
−0.11 |
BH
|
29.7+5.0
−5.3 |
BH
|
8.4+1.8
−1.0 |
BH
|
37.0+4.1
−3.9 |
0.67+0.05
−0.07 |
First possible observation of a merger of two black holes of very different masses. Originally designated S190412m. | [31][32] | ||
GW190413_052954 2019-04-13 |
2020-10-27 | 1400
|
8.9+0.4
−0.7 |
4100+2410
−1890 |
24.0+5.4
−3.7 |
0.01+0.29
−0.33 |
BH
|
33.4+12.4
−7.4 |
BH
|
23.4+6.7
−6.3 |
BH
|
54.3+12.4
−8.4 |
0.69+0.12
−0.13 |
[30] | ||
GW190413_134308 2019-04-13 |
2020-10-27 | 520
|
10.0+0.4
−0.5 |
5150+2440
−2340 |
31.9+7.3
−4.6 |
−0.01+0.24
−0.28 |
BH
|
45.4+13.6
−9.6 |
BH
|
30.9+10.2
−9.6 |
BH
|
72.8+15.2
−10.3 |
0.69+0.10
−0.12 |
[30] | ||
GW190421_213856 2019-04-21 |
2020-10-27 | 1000
|
10.7+0.2
−0.4 |
3150+1370
−1420 |
30.7+5.5
−6.6 |
−0.05+0.23
−0.26 |
BH
|
40.6+10.4
−6.6 |
BH
|
31.4+7.5
−8.2 |
BH
|
68.6+11.7
−8.1 |
0.68+0.10
−0.11 |
Originally designated S190421ar. | [30] | |
GW190424_180648 2019-04-24 18:06:48 |
2020-10-27 | 26000
|
10.4+0.2
−0.4 |
2550+1560
−1330 |
30.3+5.7
−4.2 |
0.15+0.22
−0.22 |
BH
|
39.5+10.9
−6.9 |
BH
|
31.0+7.4
−7.3 |
BH
|
67.1+12.5
−9.2 |
0.75+0.08
−0.09 |
[30] | ||
GW190425 2019-04-25 08:18:05 |
2020-01-06 | 12.4+0.3
−0.4 |
159+69
−72 |
1.44+0.02
−0.02 |
0.012+0.01
−0.01 |
NS
|
1.60 - 1.87
|
NS
|
1.46 - 1.69
|
?
|
Originally designated S190425z (z:26th trigger|UTC day), this trigger was detected by a single LIGO instrument (of three LVC stations), and is considered by some scientists to have been confirmed as a binary neutron star merger.[34]
It was published in 2020 that a gamma-ray burst was detected (GRB 190425) ~0.5 seconds after the LIGO trigger, lasting 6 seconds and bearing similarities to GRB170817 (such as weakness [most power in sub-100 keV, or soft X-rays) bands], elevated energetic photon background levels [signal exceeding background by less than a factor of 2], and similar differences from other transients classified as short GRBs). Confidence was established for interpretation of a set of peaks through a control interval of only 2 days prior to the LIGO-Livingston trigger in INTEGRAL Electronic anticoincidence, could not be corroborated by other instruments and wasn't initially noted as a significant event. Non-detection in other instruments may be a consequence of an Earth-occulted source as the Fermi telescope attempted follow-up.[33] |
[35][36] | ||||
GW190426_152155 2019-04-26 15:21:55 |
2020-10-27 | 1300
|
8.7+0.5
−0.6 |
370+180
−160 |
2.41+0.08
−0.08 |
−0.03+0.32
−0.30 |
?
|
5.7+3.9
−2.3 |
NS
|
1.5+0.8
−0.5 |
?
|
The primary object, being between 3.4 and 9.6 solar masses, is either a black hole or an object in the mass gap. Originally designated S230426c. | [30] | |||
GW190503_185404 2019-05-03 18:54:04 |
2020-10-27 | 12.4+0.2
−0.3 |
1450+690
−630 |
30.2+4.2
−4.2 |
−0.03+0.20
−0.26 |
BH
|
43.3+9.1
−8.2 |
BH
|
28.4+7.7
−8.0 |
BH
|
68.6+8.8
−7.7 |
0.66+0.09
−0.12 |
Originally designated S230503bf. | [30] | ||
GW190512_180714 2019-05-12 18:07:14 |
2020-10-27 | 220; towards Scorpius or Ophiuchus
|
12.2+0.2
−0.4 |
1430+550
−550 |
14.6+1.3
−1.0 |
0.03+0.12
−0.13 |
BH
|
23.3+5.3
−3.8 |
BH
|
12.6+3.6
−2.5 |
BH
|
34.5+3.8
−3.5 |
0.65+0.07
−0.07 |
Originally designated S230512at. | [30] | |
GW190513_205428 2019-05-13 20:54:28 |
2020-10-27 | 12.9+0.3
−0.4 |
2060+880
−800 |
21.6+3.8
−1.9 |
0.11+0.28
−0.17 |
BH
|
35.7+9.5
−9.2 |
BH
|
18.0+7.7
−4.2 |
BH
|
51.6+8.2
−5.8 |
0.68+0.14
−0.12 |
Originally designated S230513bm. | [30] | ||
GW190514_065416 2019-05-14 06:54:16 |
2020-10-27 | 3000
|
8.2+0.3
−0.6 |
4100+2700
−2200 |
28.5+7.9
−4.8 |
−0.19+0.29
−0.32 |
BH
|
39.0+14.7
−8.2 |
BH
|
28.4+9.3
−8.8 |
BH
|
65+18
−10 |
0.63+0.11
−0.15 |
[30] | ||
GW190517_055101 2019-05-17 06:54:16 |
2020-10-27 | 470
|
10.7+0.4
−0.6 |
1860+1620
−840 |
26.6+4.0
−4.0 |
0.52+0.19
−0.19 |
BH
|
37.4+11.7
−7.6 |
BH
|
25.3+7.0
−7.3 |
BH
|
59.3+9.1
−8.9 |
0.87+0.05
−0.07 |
Originally designated S190517h. | [30] | |
GW190519_153544 2019-05-19 15:35:44 |
2020-10-27 | 860
|
15.6+0.2
−0.3 |
2530+1830
−920 |
44.5+6.4
−7.1 |
0.31+0.20
−0.22 |
BH
|
66+11
−12 |
BH
|
41+11
−11 |
BH
|
101+12
−14 |
0.79+0.07
−0.13 |
Originally designated S190519bj. | [30] | |
GW190521 2019-05-21 03:02:29 |
2020-09-02 | 14.2+0.3
−0.3 |
5300+2400
−2600 |
7.6+2.2
−1.9 |
64+13
−8 |
0.08+0.27
−0.36 |
BH
|
85+21
−14 |
BH
|
66+17
−18 |
BH
|
142+28
−16 |
0.72+0.09
−0.12 |
Originally designated S190521g. Largest progenitor masses to date. | [37][38] | |
GW190521_074359 2019-05-21 07:43:59 |
2020-10-27 | 550
|
25.8+0.1
−0.2 |
1240+400
−570 |
32.1+3.2
−2.5 |
0.09+0.10
−0.13 |
BH
|
42.2+5.9
−4.8 |
BH
|
32.8+5.4
−6.4 |
BH
|
71.0+6.5
−4.4 |
0.72+0.05
−0.07 |
Originally designated S190521r. | [30] | |
GW190527_092055 2019-05-27 09:20:55 |
2020-10-27 | 3700
|
8.1+0.3
−0.9 |
2500+2500
−1200 |
24.3+9.2
−4.1 |
0.11+0.28
−0.28 |
BH
|
36.5+16.4
−9.0 |
BH
|
22.6+10.5
−8.1 |
BH
|
56.4+20.2
−9.3 |
0.71+0.12
−0.16 |
[30] | ||
GW190602_175927 2019-06-02 17:59:27 |
2020-10-27 | 690
|
12.8+0.2
−0.3 |
2700+1800
−1100 |
49.1+9.1
−8.5 |
0.07+0.25
−0.24 |
BH
|
69+16
−13 |
BH
|
48+14
−17 |
BH
|
111+18
−15 |
0.70+0.10
−0.14 |
Originally designated S190602aq. | [30] | |
GW190620_030421 2019-06-20 03:04:21 |
2020-10-27 | 7200
|
12.1+0.3
−0.4 |
2800+1700
−1300 |
38.3+8.3
−6.5 |
0.33+0.22
−0.25 |
BH
|
57+16
−13 |
BH
|
36+12
−12 |
BH
|
87+17
−12 |
0.79+0.08
−0.15 |
[30] | ||
GW190630_185205 2019-06-30 18:52:05 |
2020-10-27 | 1200
|
15.6+0.2
−0.3 |
890+560
−370 |
24.9+2.1
−2.1 |
0.10+0.12
−0.13 |
BH
|
35.1+6.9
−5.6 |
BH
|
23.7+5.2
−5.1 |
BH
|
56.4+4.4
−4.6 |
0.70+0.05
−0.07 |
Originally designated S190630ag. | [30] | |
GW190701_203306 2019-07-01 20:33:06 |
2020-10-27 | 11.3+0.2
−0.3 |
2060+760
−730 |
40.3+5.4
−4.9 |
−0.07+0.23
−0.29 |
BH
|
53.9+11.8
−8.0 |
BH
|
40.8+8.7
−12.0 |
BH
|
90.2+11.3
−8.9 |
0.66+0.09
−0.13 |
Originally designated S190701ah. | [30] | ||
GW190706_222641 2019-07-06 22:26:41 |
2020-10-27 | 650
|
12.6+0.2
−0.4 |
4400+2600
−1900 |
42.7+10.0
−7.0 |
0.28+0.26
−0.29 |
BH
|
67+15
−16 |
BH
|
38+15
−13 |
BH
|
99+18
−14 |
0.78+0.09
−0.18 |
Originally designated S190706ai. | [30] | |
GW190707_093326 2019-07-07 09:33:26 |
2020-10-27 | 1300
|
13.3+0.2
−0.4 |
770+380
−270 |
8.5+0.7
−0.6 |
−0.05+0.10
−0.08 |
BH
|
11.6+3.3
−1.7 |
BH
|
8.4+1.4
−1.7 |
BH
|
19.2+1.9
−1.3 |
0.66+0.03
−0.04 |
Originally designated S190707q. | [30] | |
GW190708_232457 2019-07-08 23:24:57 |
2020-10-27 | 14000
|
13.1+0.2
−0.3 |
880+330
−390 |
13.2+0.9
−0.6 |
0.02+0.08
−0.10 |
BH
|
17.6+4.7
−2.3 |
BH
|
13.2+2.0
−2.7 |
BH
|
29.5+2.5
−1.8 |
0.69+0.04
−0.04 |
[30] | ||
GW190719_215514 2019-07-09 21:55:14 |
2020-10-27 | 2900
|
8.3+0.3
−0.8 |
3900+2600
−2000 |
23.5+6.5
−4.0 |
0.32+0.29
−0.31 |
BH
|
37+18
−10 |
BH
|
20.8+9.0
−7.2 |
BH
|
55+17
−10 |
0.78+0.11
−0.17 |
[30] | ||
GW190720_000836 2019-07-20 00:08:36 |
2020-10-27 | 460; mostly towards Cygnus
|
11.0+0.3
−0.7 |
790+690
−320 |
8.9+0.5
−0.8 |
0.18+0.14
−0.12 |
BH
|
13.4+6.7
−3.0 |
BH
|
7.8+2.3
−2.2 |
BH
|
20.4+4.5
−2.2 |
0.72+0.06
−0.05 |
Originally designated S190720a. | [30] | |
GW190727_060333 2019-07-27 06:03:33 |
2020-10-27 | 830
|
11.9+0.3
−0.5 |
790+690
−320 |
28.6+5.3
−3.7 |
0.11+0.26
−0.25 |
BH
|
38.0+9.5
−6.2 |
BH
|
29.4+7.1
−8.4 |
BH
|
63.8+10.9
−7.5 |
0.73+0.10
−0.10 |
Originally designated S190727h. | [30] | |
GW190728_064510 2019-07-28 06:45:10 |
2020-10-27 | 400
|
13.0+0.2
−0.4 |
870+260
−370 |
8.6+0.5
−0.3 |
0.12+0.20
−0.07 |
BH
|
12.3+7.2
−2.2 |
BH
|
8.1+1.7
−2.6 |
BH
|
19.6+4.7
−1.3 |
0.71+0.04
−0.04 |
Originally designated S190728q. | [30] | |
GW190731_140936 2019-07-31 14:09:36 |
2020-10-27 | 3400
|
8.7+0.2
−0.5 |
3300+2400
−1700 |
29.5+7.1
−5.2 |
0.06+0.24
−0.24 |
BH
|
41.5+12.2
−9.0 |
BH
|
28.8+9.7
−9.5 |
BH
|
67+15
−11 |
0.70+0.10
−0.13 |
[30] | ||
GW190803_022701 2019-08-03 02:27:01 |
2020-10-27 | 1500
|
8.6+0.3
−0.5 |
3300+2000
−1600 |
27.3+5.7
−4.1 |
−0.03+0.24
−0.27 |
BH
|
37.3+10.6
−7.0 |
BH
|
27.3+7.8
−8.2 |
BH
|
61.7+11.8
−8.5 |
0.68+0.10
−0.11 |
[30] | ||
GW190814 2019-08-14 21:11:18 | 2020-06-23 | 24.9+0.1
−0.2 |
241+41
−45 |
6.09+0.06
−0.06 |
−0.002+0.06
−0.061 |
BH
|
23.2+1.1
−1.0 |
?
|
2.59+0.08
−0.09 |
BH
|
25.6+1.1
−0.9 |
0.28+0.02
−0.02 |
No optical counterpart was discovered despite an extensive search of the probability region. The mass of the lighter component is estimated to be 2.6 times the mass of the Sun, placing it in the mass gap between neutron stars and black holes.[39] | |||
GW190828_063405 2019-08-28 06:34:05 |
2020-10-27 | 520
|
16.2+0.2
−0.3 |
2130+660
−930 |
25.0+3.4
−2.1 |
0.19+0.15
−0.16 |
BH
|
32.1+5.8
−4.0 |
BH
|
26.2+4.6
−4.8 |
BH
|
54.9+7.2
−4.3 |
0.75+0.06
−0.07 |
Originally designated S190828j. | [30] | |
GW190828_065509 2019-08-28 06:55:09 |
2020-10-27 | 660
|
10.0+0.3
−0.5 |
1600+620
−600 |
13.3+1.2
−1.0 |
0.08+0.16
−0.16 |
BH
|
24.1+7.0
−7.2 |
BH
|
10.2+3.6
−2.1 |
BH
|
33.1+5.5
−4.5 |
0.65+0.08
−0.08 |
Originally designated S190828l. | [30] | |
GW190909_114149 2019-09-09 11:41:49 |
2020-10-27 | 4700
|
8.1+0.4
−0.6 |
3800+3300
−2200 |
30.9+17.2
−7.5 |
−0.06+0.37
−0.37 |
BH
|
46+53
−13 |
BH
|
28+13
−13 |
BH
|
72+55
−17 |
0.66+0.15
−0.20 |
[30] | ||
GW190910_112807 2019-09-10 11:28:07 |
2020-10-27 | 11000
|
14.1+0.2
−0.3 |
1460+1030
−580 |
34.3+4.1
−4.1 |
0.02+0.18
−0.18 |
BH
|
43.9+7.6
−6.1 |
BH
|
35.6+6.3
−7.2 |
BH
|
75.8+8.5
−8.6 |
0.70+0.08
−0.07 |
[30] | ||
GW190915_235702 2019-09-15 23:57:02 |
2020-10-27 | 13.6+0.2
−0.3 |
1620+710
−610 |
25.3+3.2
−2.7 |
0.02+0.20
−0.25 |
BH
|
35.3+9.5
−6.4 |
BH
|
24.4+5.6
−6.1 |
BH
|
57.2+7.1
−6.0 |
0.70+0.09
−0.11 |
Originally designated S230915ak. | [30] | ||
GW190924_021846 2019-09-24 02:18:46 |
2020-10-27 | 11.5+0.3
−0.4 |
570+220
−220 |
5.8+0.2
−0.2 |
0.03+0.30
−0.09 |
BH
|
8.9+7.0
−2.0 |
?
|
5.0+1.4
−1.9 |
BH
|
13.3+5.2
−1.0 |
0.67+0.05
−0.05 |
The secondary component, being between 3.1 and 6.4 solar masses, is either a black hole or an object in the mass gap. Originally designated S230924h. | [30] | ||
GW190929_012149 2019-09-29 01:21:49 |
2020-10-27 | 2200
|
10.1+0.6
−0.8 |
2100+3700
−1100 |
35.8+14.9
−8.2 |
0.01+0.34
−0.33 |
BH
|
81+33
−33 |
BH
|
24+19
−11 |
BH
|
102+34
−25 |
0.66+0.20
−0.31 |
[30] | ||
GW190930_133541 2019-09-30 13:35:41 |
2020-10-27 | 1700
|
9.5+0.3
−0.5 |
760+360
−320 |
8.5+0.5
−0.5 |
0.14+0.31
−0.15 |
BH
|
12.3+12.4
−2.3 |
?
|
7.8+1.7
−3.3 |
BH
|
19.4+9.2
−1.5 |
0.72+0.07
−0.06 |
The secondary component, being between 4.5 and 9.5 solar masses, is either a black hole or an object in the mass gap. Originally designated S190930s. | [30] | |
GW191103 2019-11-03 01:25:49 |
2021-11-17 | 2500
|
8.9+0.3
−0.5 |
990+500
−470 |
8.34+0.66
−0.57 |
0.21+0.16
−0.10 |
BH
|
11.8+6.2
−2.2 |
BH
|
7.9+1.7
−2.4 |
BH
|
19.0+3.8
−1.7 |
0.75+0.06
−0.05 |
[40] | ||
GW191105 2019-11-05 14:35:21 |
2021-11-17 | 640
|
9.7+0.3
−0.5 |
1150+430
−480 |
7.82+0.61
−0.45 |
−0.02+0.13
−0.09 |
BH
|
10.7+3.7
−1.6 |
BH
|
7.7+1.4
−1.9 |
BH
|
17.6+2.1
−1.2 |
0.67+0.04
−0.05 |
Originally designated S191105e. | [40] | |
GW191109 2019-11-09 01:07:17 |
2021-11-17 | 1600
|
17.3+0.5
−0.5 |
1290+1130
−650 |
47.5+9.6
−7.5 |
−0.29+0.42
−0.31 |
BH
|
65+11
−11 |
BH
|
47+15
−13 |
BH
|
107+18
−15 |
0.61+0.18
−0.19 |
Originally designated S191109d. | [40] | |
GW191113 2019-11-13 07:17:53 |
2021-11-17 | 3600
|
7.9+0.5
−1.1 |
1290+1130
−650 |
10.7+1.1
−1.0 |
0.00+0.37
−0.29 |
BH
|
29+12
−14 |
BH
|
5.9+4.4
−1.3 |
BH
|
34+11
−10 |
0.45+0.33
−0.11 |
[40] | ||
GW191126 2019-11-26 11:52:59 |
2021-11-17 | 1400
|
8.3+0.2
−0.5 |
1620+740
−740 |
8.65+0.95
−0.71 |
0.21+0.15
−0.11 |
BH
|
12.1+5.5
−2.2 |
BH
|
8.3+1.9
−2.4 |
BH
|
19.6+3.5
−2.0 |
0.75+0.06
−0.05 |
[40] | ||
GW191127 2019-11-27 05:02:27 |
2021-11-17 | 980
|
9.2+0.7
−0.6 |
3400+3100
−1900 |
29.9+11.7
−9.1 |
0.18+0.34
−0.36 |
BH
|
53+47
−20 |
BH
|
24+17
−14 |
BH
|
76+31
−29 |
0.75+0.13
−0.29 |
[40] | ||
GW191129 2019-11-29 13:40:29 |
2021-11-17 | 850
|
13.1+0.2
−0.3 |
790+260
−330 |
7.31+0.43
−0.28 |
0.06+0.18
−0.06 |
BH
|
10.7+4.1
−2.1 |
BH
|
6.7+1.5
−1.7 |
BH
|
16.8+2.5
−1.2 |
0.69+0.03
−0.05 |
Originally designated S191129u. | [40] | |
GW191204_110529 2019-12-04 11:05:29 |
2021-11-17 | 3700
|
8.8+0.4
−0.6 |
1800+1700
−1100 |
19.8+3.6
−3.3 |
0.05+0.26
−0.27 |
BH
|
27.3+11.0
−6.0 |
BH
|
19.3+5.6
−6.0 |
BH
|
45.0+8.6
−7.6 |
0.71+0.12
−0.11 |
[40] | ||
GW191204_171526 2019-12-04 17:15:26 |
2021-11-17 | 17.5+0.2
−0.2 |
650+190
−250 |
8.55+0.38
−0.27 |
0.16+0.08
−0.05 |
BH
|
11.9+3.3
−1.8 |
BH
|
8.2+1.4
−1.6 |
BH
|
19.21+1.79
−0.95 |
0.73+0.03
−0.03 |
Originally designated S191204r. | [40] | ||
GW191215 2019-12-15 22:30:52 |
2021-11-17 | 530
|
11.2+0.3
−0.4 |
1930+890
−860 |
18.4+2.2
−1.7 |
−0.04+0.17
−0.21 |
BH
|
24.9+7.1
−4.1 |
BH
|
18.1+3.8
−4.1 |
BH
|
41.4+5.1
−4.1 |
0.68+0.07
−0.07 |
Originally designated S191215w. | [40] | |
GW191216 2019-12-16 21:33:38 |
2021-11-17 | 490
|
18.6+0.2
−0.2 |
340+120
−130 |
8.33+0.22
−0.19 |
0.11+0.13
−0.06 |
BH
|
12.1+4.6
−2.3 |
BH
|
7.7+1.6
−1.9 |
BH
|
18.87+2.80
−0.94 |
0.70+0.03
−0.04 |
Originally designated S191216ap. | [40] | |
GW191219 2019-12-19 16:31:20 |
2021-11-17 | 1500
|
9.1+0.5
−0.8 |
550+250
−160 |
4.32+0.12
−0.17 |
0.00+0.07
−0.09 |
BH
|
31.1+2.2
−2.8 |
NS
|
1.17+0.07
−0.06 |
BH
|
32.2+2.2
−2.7 |
0.14+0.06
−0.06 |
The event is unconfirmed due to difficulty accurately modelling the extreme mass ratio. | [40] | |
GW191222 2019-12-22 03:35:37 |
2021-11-17 | 2000
|
12.5+0.2
−0.3 |
3000+1700
−1700 |
33.8+7.1
−5.0 |
−0.04+0.20
−0.25 |
BH
|
45.1+10.9
−8.0 |
BH
|
34.7+9.3
−10.5 |
BH
|
75.5+15.3
−9.9 |
0.67+0.08
−0.11 |
Originally designated S191222n. | [40] | |
GW191230 2019-12-30 18:04:58 |
2021-11-17 | 1100
|
10.4+0.3
−0.4 |
4300+2100
−1900 |
36.5+8.2
−5.6 |
−0.05+0.26
−0.31 |
BH
|
49.4+14.0
−9.6 |
BH
|
37+11
−12 |
BH
|
82+17
−11 |
0.68+0.11
−0.13 |
[40] | ||
GW200105 2020-01-05 16:24:26 |
2021-06-29 | 7200
|
13.7+0.2
−0.4 |
280±110
|
3.41+0.08
−0.07 |
−0.01+0.11
−0.15 |
BH
|
8.9+1.2
−1.5 |
NS
|
1.9+0.3
−0.2 |
BH
|
10.4+2.7
−2.0 |
0.43+0.04
−0.03 |
First event confirmed to be a black hole and neutron star merger. Originally designated S200105ae. | [41][42] | |
GW200112 2020-01-12 15:58:38 |
2021-11-17 | 4300
|
19.8+0.1
−0.2 |
1250+430
−460 |
27.4+2.6
−2.1 |
0.06+0.15
−0.15 |
BH
|
35.6+6.7
−4.5 |
BH
|
28.3+4.4
−5.9 |
BH
|
60.8+5.3
−4.3 |
0.71+0.06
−0.06 |
Originally designated S200112r. | [40] | |
GW200114 2020-01-14 02:08:08 |
2022-08-18 | 1250+1500
−400 |
68+6
−4 |
−0.75+0.50
−0.15 |
BH
|
78+10
−10 |
BH
|
70+10
−10 |
BH
|
140+15
−15 |
Originally designated S200114f. The event was initially published as an unmodeled gravitational wave burst, and different studies have offered conflicting interpretations. One study suggested it was a nearby high-mass black hole merger with component masses of 118+10 −12 and 89+18 −8 Msun which was poorly modeled because of its high mass.[43] Another study interpreted it as a somewhat smaller black hole merger taking place at the same time as a detector glitch.[44] Both studies conclude the signal is most likely a real event, and the latter model is included in the table. |
[43][44] | ||||
GW200115 2020-01-15 04:23:09 |
2021-06-29 | 600
|
11.3+0.3
−0.5 |
300+150
−100 |
2.42+0.05
−0.07 |
−0.19+0.23
−0.35 |
BH
|
5.7+1.8
−2.1 |
NS
|
1.5+0.7
−0.3 |
BH
|
7.8+1.4
−1.6 |
0.38+0.04
−0.03 |
Second event confirmed to be a black hole and neutron star merger. Originally designated S200115j. | [41][45] | |
GW200128 2020-01-28 02:20:11 |
2021-11-17 | 2600
|
10.6+0.3
−0.4 |
3400+2100
−1800 |
32.0+7.5
−5.5 |
0.12+0.24
−0.25 |
BH
|
42.2+11.6
−8.1 |
BH
|
32.6+9.5
−9.2 |
BH
|
71+16
−11 |
0.74+0.10
−0.10 |
Originally designated S200128d. | [40] | |
GW200129 2020-01-29 06:54:58 |
2021-11-17 | 26.8+0.2
−0.2 |
900+290
−380 |
27.2+2.1
−2.3 |
0.11+0.11
−0.16 |
BH
|
34.5+9.9
−3.2 |
BH
|
28.9+3.4
−9.3 |
BH
|
60.3+4.0
−3.3 |
0.73+0.06
−0.05 |
Originally designated S200129m. | [40] | ||
GW200202 2020-02-02 15:43:12 |
2021-11-17 | 170
|
10.8+0.2
−0.4 |
410+150
−160 |
7.49+0.24
−0.20 |
0.04+0.13
−0.06 |
BH
|
10.1+3.5
−1.4 |
BH
|
7.3+1.1
−1.7 |
BH
|
16.76+1.87
−0.66 |
0.69+0.03
−0.04 |
[40] | ||
GW200208_130117 2020-02-08 13:01:17 |
2021-11-17 | 30; towards Pyxis or Antlia
|
10.8+0.3
−0.4 |
2230+1000
−850 |
27.7+3.6
−3.1 |
−0.07+0.22
−0.27 |
BH
|
37.8+9.2
−8.2 |
BH
|
27.5+6.1
−7.4 |
BH
|
62.5+7.3
−6.4 |
0.66+0.09
−0.13 |
Originally designated S200208q. | [40] | |
GW200208_222617 2020-02-08 22:26:17 |
2021-11-17 | 2000
|
7.4+1.4
−1.2 |
4100+4400
−1900 |
19.6+10.7
−5.1 |
0.45+0.43
−0.44 |
BH
|
51+104
−30 |
BH
|
12.3+9.0
−5.7 |
BH
|
61+100
−25 |
0.83+0.14
−0.27 |
[40] | ||
GW200209 2020-02-09 08:54:52 |
2021-11-17 | 730
|
9.6+0.4
−0.5 |
3400+1900
−1800 |
26.7+6.0
−4.2 |
−0.12+0.24
−0.30 |
BH
|
35.6+10.5
−6.8 |
BH
|
27.1+7.8
−7.8 |
BH
|
59.9+13.1
−8.9 |
0.66+0.10
−0.12 |
[40] | ||
GW200210 2020-02-10 09:22:54 |
2021-11-17 | 1800
|
8.4+0.5
−0.7 |
940+430
−340 |
6.56+0.38
−0.40 |
0.02+0.22
−0.21 |
BH
|
24.1+7.5
−4.6 |
?
|
2.83+0.47
−0.42 |
BH
|
26.7+7.2
−4.3 |
0.34+0.13
−0.08 |
The secondary component, being between 2.41 and 3.30 solar masses, is an object in the mass gap. | [40] | |
GW200216 2020-02-16 22:08:04 |
2021-11-17 | 2900
|
8.1+0.4
−0.5 |
3800+3000
−2000 |
32.9+9.3
−8.5 |
0.10+0.34
−0.36 |
BH
|
51+22
−13 |
BH
|
30+14
−16 |
BH
|
78+19
−13 |
0.70+0.14
−0.24 |
[40] | ||
GW200219 2020-02-19 09:44:15 |
2021-11-17 | 700
|
10.7+0.3
−0.5 |
3400+1700
−1500 |
27.6+5.6
−3.8 |
−0.08+0.23
−0.29 |
BH
|
37.5+10.1
−6.9 |
BH
|
27.9+7.4
−8.4 |
BH
|
62.2+11.7
−7.8 |
0.66+0.10
−0.13 |
Originally designated S200219ac. | [40] | |
GW200220_061928 2020-02-20 06:19:28 |
2021-11-17 | 3000
|
7.2+0.4
−0.7 |
6000+4800
−3100 |
62+23
−15 |
0.06+0.40
−0.38 |
BH
|
87+40
−23 |
BH
|
61+26
−25 |
BH
|
141+51
−31 |
0.71+0.15
−0.17 |
[40] | ||
GW200220_124850 2020-02-20 12:48:50 |
2021-11-17 | 3200
|
8.5+0.3
−0.5 |
4000+2800
−2200 |
28.2+7.3
−5.1 |
−0.07+0.27
−0.33 |
BH
|
38.9+14.1
−8.6 |
BH
|
27.9+9.2
−9.0 |
BH
|
64+16
−11 |
0.67+0.11
−0.14 |
[40] | ||
GW200224 2020-02-24 22:22:34 |
2021-11-17 | 20.0+0.2
−0.2 |
1710+490
−640 |
31.1+3.2
−2.6 |
0.10+0.15
−0.15 |
BH
|
40.0+6.9
−4.5 |
BH
|
32.5+5.0
−7.2 |
BH
|
68.6+6.6
−4.7 |
0.73+0.07
−0.07 |
Originally designated S200224ca. | [40] | ||
GW200225 2020-02-25 06:04:21 |
2021-11-17 | 370; towards Ursa Minor or Cepheus
|
12.5+0.3
−0.4 |
1150+510
−530 |
14.2+1.5
−1.4 |
−0.12+0.17
−0.28 |
BH
|
19.3+5.0
−3.0 |
BH
|
14.0+2.8
−3.5 |
BH
|
32.1+3.5
−2.8 |
0.66+0.07
−0.13 |
Originally designated S200225q. | [40] | |
GW200302 2020-03-02 01:58:11 |
2021-11-17 | 6000
|
10.8+0.3
−0.4 |
1480+1020
−700 |
23.4+4.7
−3.0 |
0.01+0.25
−0.26 |
BH
|
37.8+8.7
−8.5 |
BH
|
20.0+8.1
−5.7 |
BH
|
55.5+8.9
−8.6 |
0.66+0.13
−0.15 |
Originally designated S200302c. | [40] | |
GW200306 2020-03-06 09:37:14 |
2021-11-17 | 4600
|
7.8+0.4
−0.6 |
2100+1700
−1100 |
17.5+3.5
−3.0 |
0.32+0.28
−0.46 |
BH
|
28.3+17.1
−7.7 |
BH
|
14.8+6.5
−6.4 |
BH
|
41.7+12.3
−6.9 |
0.78+0.11
−0.26 |
[40] | ||
GW200308 2020-03-08 17:36:09 |
2021-11-17 | 2000
|
7.1+0.5
−0.5 |
5400+2700
−2600 |
19.0+4.8
−2.8 |
0.65+0.21
−0.17 |
BH
|
36.4+11.2
−9.6 |
BH
|
13.8+7.2
−3.3 |
BH
|
47.4+11.1
−7.7 |
0.91+0.03
−0.08 |
[40] | ||
GW200311 2020-03-11 11:58:53 |
2021-11-17 | 35; towards Cetus
|
17.8+0.2
−0.2 |
1170+280
−400 |
26.6+2.4
−2.0 |
−0.02+0.16
−0.20 |
BH
|
34.2+6.4
−3.8 |
BH
|
27.7+4.1
−5.9 |
BH
|
59.0+4.8
−3.9 |
0.69+0.07
−0.08 |
Originally designated S200311bg. | [40] | |
GW200316 2020-03-16 21:57:56 |
2021-11-17 | 190
|
10.3+0.4
−0.7 |
1120+470
−440 |
8.75+0.62
−0.55 |
0.13+0.27
−0.10 |
BH
|
13.1+10.2
−2.9 |
BH
|
7.8+1.9
−2.9 |
BH
|
20.2+7.4
−1.9 |
0.70+0.04
−0.04 |
Originally designated S200316bj. | [40] | |
GW200322 2020-03-22 09:11:33 |
2021-11-17 | 6500
|
6.0+1.7
−1.2 |
3600+7000
−2000 |
15.5+15.7
−3.7 |
0.24+0.45
−0.51 |
BH
|
34+48
−18 |
BH
|
14.0+16.8
−8.7 |
BH
|
53+38
−26 |
0.78+0.16
−0.17 |
[40] |
Candidate events and marginal detections
There is possible detection of nanohertz waves by observation of the timing of pulsars, but they have not been confirmed at the 5 sigma level of confidence, (As of 2023).[46]
Marginal detections from O1 and O2
In addition to well-constrained detections listed above, a number of low-significance detections of possible signals were made by LIGO and Virgo. Their characteristics are listed below, only including detections with a <50% chance of being noise:
Candidate event |
Detection time (UTC) |
Date published |
Luminosity distance (Mpc)[n 12] |
Detector [n 13] |
False alarm rate (year) |
Effective spin | Primary | Secondary | Probability of terrestrial noise | Notes | Ref | ||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Type | Mass (M☉) | Type | Mass (M☉) | ||||||||||
151205 | 2015-12-05 19:55:25 | 2019-10-11 | 3000+2400 −1600 |
H,L | 0.61 | 0.14+0.40 −0.38 |
BH |
67+28 −17 |
BH |
42+16 −19 |
0.47 | [47] | |
170121 | 2017-01-21 21:25:36 | 2019-04-15 | H,L | −0.3±0.3 | BH |
29+4 −3 |
BH |
<0.01 | [48] | ||||
170304 | 2017-03-04 16:37:53 | 2019-10-11 | 2300+1600 −1200 |
H,L | 2.5 | 0.11+0.29 −0.27 |
BH |
44.9+17.6 −9.4 |
BH |
31.8+9.5 −11.6 |
0.30 | [47] | |
170402 | 2017-04-02 21:51:50 | 2019-10-21 | H,L | 0.32 | [49] | ||||||||
170727 | 2017-07-27 01:04:30 | 2019-10-11 | 2200+1500 −1100 |
H,L | 180 | −0.05+0.25 −0.30 |
BH |
41.6+12.8 −7.9 |
BH |
30.4+7.9 −8.2 |
0.006 | [47] | |
170817A | 2017-08-17 03:02:46 | 2019-10-21 | H,L,V | 11.5 | 0.5±0.2 | BH |
56+16 −10 |
BH |
40+10 −11 |
0.14 | [49] |
Observation candidates from O3/2019
From observation run O3/2019 on, observations are published as Open Public Alerts to facilitate multi-messenger observations of events.[50][51][52] Candidate event records can be directly accessed at the Gravitational-Wave Candidate Event Database (GraceDB).[53] On 1 April 2019, the start of the third observation run was announced with a circular published in the public alerts tracker.[54] The first O3/2019 binary black hole detection alert was broadcast on 8 April 2019. A significant percentage of O3 candidate events detected by LIGO are accompanied by corresponding triggers at Virgo.
False alarm rates are mixed, with more than half of events assigned false alarm rates greater than 1 per 20 years, contingent on presence of glitches around signal, foreground electromagnetic instability, seismic activity, and operational status of any one of the three LIGO-Virgo instruments. For instance, events S190421ar and S190425z weren't detected by Virgo and LIGO's Hanford site, respectively.
The LIGO/Virgo collaboration took a short break from observing during the month of October 2019 to improve performance and prepare for future plans, with no signals detected in that month as a result.[55]
The Kamioka Gravitational Wave Detector (KAGRA) in Japan became operational on 25 February 2020,[56] likely improving the detection and localization of future gravitational wave signals.[57] However, KAGRA does not report their signals in real-time on GraceDB as LIGO and Virgo do, so the results of their observation run will likely not be published until the end of O3.
The LIGO-Virgo collaboration ended the O3 run early on March 27, 2020, due to health concerns from the COVID-19 pandemic.[5][58]
Script error: No such module "Chart". |
Script error: No such module "Chart". |
GW event | Detection time (UTC) |
Location area[n 14] (deg2) |
Luminosity distance (Mpc)[n 15] |
Detector [n 16] |
False alarm Rate (Hz) |
False alarm chance in O3[n 17] |
Classification | Notes | Ref | ||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
NS / NS [n 18] |
NS / BH [n 19] |
BH / BH [n 20] |
Mass gap [n 21] |
Terrestrial [n 22] | |||||||||
S190901ap | 2019-09-01 23:31:01 |
14753
|
241±79
|
L,V | 4.5093 7.0 10−9
|
0.181 | 0.861 | 0.0 | 0.0 | 0.0 | 0.139 | [59] | |
S190910d | 2019-09-10 01:26:19 |
2482
|
632±186
|
H,L | 8.5248 3.7 10−9
|
0.100 | 0.0 | 0.976 | 0.0 | 0.0 | 0.024 | [60] | |
S190910h | 2019-09-10 08:29:58 |
24264
|
230±88
|
L | 0.88402 3.6 10−8
|
0.642 | 0.612 | 0.0 | 0.0 | 0.0 | 0.388 | Detected by only the Livingston detector, resulting in a bad sky localization. | [61] |
S190923y | 2019-09-23 12:55:59 | 2107
|
438±133
|
H,L | 0.66251 4.8 10−8
|
0.746 | 0.0 | 0.677 | 0.0 | 0.0 | 0.322 | [62] | |
S190930t | 2019-09-30 14:34:07 | 24220
|
108±38
|
L | 2.0536 1.5 10−8
|
0.348 | 0.0 | 0.743 | 0.0 | 0.0 | 0.257 | Detected by only the Livingston detector, resulting in a bad sky localization; last detection of the O3a run. | [63] |
S191205ah | 2019-12-05 21:52:08 | 6378
|
385±164
|
H,L,V | 2.5383 1.2 10−8
|
0.290 | 0.0 | 0.932 | 0.0 | 0.0 | 0.068 | [64] | |
S191213g | 2019-12-13 04:34:08 | 4480
|
201±81
|
H,L,V | 0.89310 3.5 10−8
|
0.631 | 0.768 | 0.0 | 0.0 | 0.0 | 0.232 | [65] | |
S200213t | 2020-02-13 04:10:40 | 2326
|
201±80
|
H,L,V | 1.7934 1.8 10−8
|
0.401 | 0.629 | 0.0 | 0.0 | 0.0 | 0.371 | [66] |
Observation candidates from O4/2023
On 15 June 2022, LIGO announced to start the O4 observing run in March 2023.[67] As the date got closer, engineering challenges delayed the observing run to May 2023.[68] An engineering run to assess the sensitivity of LIGO, Virgo, and KAGRA began in April, with the Hanford detector's first operations beginning on April 29,[69] and the Livingston and Virgo detectors' first operations beginning on May 5.[70]
On March 7, 2023, a gamma-ray burst compatible with a neutron star merger was detected by the Fermi telescope and named GRB 230307A. The burst, identified as being from a host galaxy approximately 296 Mpc away, would likely have only been marginally detected at best by LIGO if it had been operating at the time, as the detectors would only later achieve a sensitivity of 160 Mpc for neutron star mergers by O4's beginning, 3 months later.
Near the end of the engineering run on 15 May 2023, LIGO announced that O4 would be beginning on 24 May 2023, running for 20 months with up to 2 months of maintenance. The LIGO detectors failed to achieve the hoped for 160-190 Mpc sensitivity for neutron star mergers, but did achieve an improved 130-150 Mpc sensitivity over O3's 100-140 Mpc, later improving to nearly 160 Mpc for both detectors by late 2023. Virgo was found to have both a damaged mirror and other new, unknown noise sources, limiting its sensitivity to just 31-35 Mpc (similar to its performance during O2 in 2017, and lower than O3's 40-50 Mpc.) As a result, Virgo spent most of 2023 in commissioning, with a deadline of March 2024 to improve its sensitivity before joining O4. KAGRA achieved its planned 1 Mpc sensitivity before returning to commissioning in July, with plans to rejoin at an improved 10 Mpc sensitivity by early 2024. However, the title|Moment mag. scale|Mw|dotted=no}}7.5 2024 Noto earthquake occurred on 1 January 2024 only 103 kilometres (64 mi) from KAGRA, damaging the detector's sensitive instruments and delaying its development by at least several months.
On 18 May 2023, near the end of the engineering run and shortly before O4 proper, the first candidate gravitational wave event was detected. Four more were detected before the official beginning of the run. In October, LIGO announced a planned pause between January and March 2024, for a mid-run commissioning break intended to reduce noise and improve the uptime of the detectors.
Script error: No such module "Chart". |
Script error: No such module "Chart". |
GW event | Detection time (UTC) |
Location area[n 23] (deg2) |
Luminosity distance (Mpc)[n 24] |
Detector [n 25] |
False Alarm Rate (Hz) |
False Alarm chance in O4[n 26] |
Classification | Notes | Ref | ||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|
NS / NS [n 27] |
NS / BH [n 28] |
BH / BH [n 29] |
Mass gap [n 30] |
Terrestrial [n 31] | |||||||||
S230518h | 2023-05-18 12:59:07 |
460; near the galactic plane
|
204±57
|
H,L | 66.6 3.2 10−10
|
0.015 | 0.0 | 0.864 | 0.037 | 0.0 | 0.099 | Detected during the engineering phase, before the official start of O4. | [71] |
S230520ae | 2023-05-20 22:48:41 |
1702
|
2014±663
|
H,L | 7.00 3.1 10−9
|
0.133 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 1.4e-7 | [72] | |
S230522a | 2023-05-22 09:38:04 |
24219
|
3102±1032
|
L | 2.07 1.0 10−8
|
0.383 | 0.0 | 0.0 | 0.99973 | 0.00071 | 0.00027 | [73] | |
S230522n | 2023-05-22 15:30:32 |
29021
|
2221±870
|
L | 3.31 6.5 10−9
|
0.261 | 0.0 | 0.0 | 0.993 | 0.0041 | 0.0069 | [74] | |
S230524b | 2023-05-24 06:13:20 |
24224
|
2437±891
|
L | 0.026 8.3 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.725 | 0.0041 | 0.275 | [75] | |
S230525a | 2023-05-25 02:38:17 |
24219
|
1166±390
|
L | 0.029 7.5 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.724 | 0.0082 | 0.276 | Detected by only the Livingston detector, resulting in a bad sky localization. | [76] |
S230527bv | 2023-05-27 17:25:29 |
3876±2027
|
H,L | 0.103 2.1 10−7
|
0.9999[n 34] | 0.0 | 0.0 | 0.882 | 0.0 | 0.118 | [77] | ||
S230528a | 2023-05-28 02:27:14 |
1787
|
261±108
|
H,L | 0.071 3.0 10−7
|
1.0 ~1.0 | 0.0053 | 0.011 | 0.0 | 0.626 | 0.357 | The other component is a neutron star. | [78] |
S230528bt | 2023-05-28 14:51:29 |
6597
|
7412±2488
|
H,L | 0.075 2.9 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.880 | 0.043 | 0.120 | [79] | |
S230529ay | 2023-05-29 18:15:00 |
25022
|
201±63
|
L | 109 2.0 10−10
|
0.0092 | 0.0043 | 0.0089 | 0.0 | 0.916 | 0.070 | The other component is a neutron star. Detected by only the Livingston detector, resulting in a bad sky localization. | [80] |
S230601bf | 2023-06-01 22:41:34 |
2531
|
3565±1260
|
H,L | 12504000 1.7 10−15
|
7.8 10−8 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0022 | 6.4e-9 | [81] | |
S230604z | 2023-06-04 09:20:31 |
2481
|
392±201
|
H,L | 0.080 2.7 10−7
|
1.0 ~1.0 | 0.0 | 0.042 | 0.706 | 0.017 | 0.252 | [82] | |
S230605o | 2023-06-05 06:53:43 |
1077
|
1067±333
|
H,L | 4.74 4.5 10−9
|
0.190 | 0.0 | 0.0 | 0.988 | 0.0 | 0.012 | [83] | |
S230606d | 2023-06-06 00:43:05 |
1221
|
2545±874
|
H,L | 1.88 1.1 10−8
|
0.412 | 0.0 | 0.0 | 0.99928 | 0.0 | 0.00072 | [84] | |
S230606z | 2023-06-06 06:53:20 |
5989
|
4497±2023
|
H,L | 0.052 4.2 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.835 | 0.0 | 0.165 | [85] | |
S230608as | 2023-06-08 20:50:47 |
1694
|
3447±1079
|
H,L | 157 1.4 10−10
|
0.0064 | 0.0 | 0.0 | 0.99981 | 0.0 | 0.00019 | [86] | |
S230609a | 2023-06-09 01:08:24 |
3507
|
4537±1433
|
H,L | 0.268 8.0 10−8
|
0.976 | 0.0 | 0.0 | 0.956 | 0.043 | 0.044 | [87] | |
S230609u | 2023-06-09 06:49:58 |
1287
|
3390±1125
|
H,L | 2.13 1.0 10−8
|
0.374 | 0.0 | 0.0 | 0.961 | 0.0 | 0.038 | [88] | |
S230615av | 2023-06-15 16:08:26 |
7017
|
12726±4301
|
H,L | 0.148 1.4 10−7
|
0.9988[n 39] | 0.0 | 0.0 | 0.912 | 0.026 | 0.088 | [89] | |
S230615az | 2023-06-15 17:50:08 |
4416
|
260±133
|
H,L | 0.144 1.5 10−7
|
0.9991[n 40] | 0.847 | 0.0 | 0.0 | 0.0069 | 0.153 | [90] | |
S230623at | 2023-06-23 17:18:09 |
736; towards Hydra
|
124±34
|
H,L | 0.110 2.0 10−7
|
0.9999[n 41] | 0.0 | 0.00080 | 0.634 | 0.072 | 0.293 | [91] | |
S230624av | 2023-06-24 11:31:03 |
1718
|
2556±787
|
H,L | 1.65 1.3 10−8
|
0.455 | 0.0 | 0.0 | 0.953 | 0.0 | 0.047 | [92] | |
S230627c | 2023-06-27 01:53:37 |
278±68
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.365 | 0.354 | 0.251 | 0.030 | [93] | ||
S230628aj | 2023-06-28 16:42:24 |
1861
|
421±125
|
H,L | 0.102 2.1 10−7
|
0.9999[n 42] | 0.0 | 0.00085 | 0.679 | 0.014 | 0.306 | [94] | |
S230628ax | 2023-06-28 23:12:00 |
705
|
2047±585
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.4e-5 | [95] | |
S230630am | 2023-06-30 12:58:06 |
3642
|
8710±2735
|
H,L | 0.889 2.4 10−8
|
0.676 | 0.0 | 0.0 | 0.941 | 0.042 | 0.017 | [96] | |
S230630bq | 2023-06-30 23:45:32 |
1975
|
1150±360
|
H,L | 2.77 7.7 10−9
|
0.303 | 0.0 | 0.00076 | 0.890 | 0.079 | 0.031 | [97] | |
S230702an | 2023-07-02 18:54:53 |
2267
|
2428±849
|
H,L | 14000 1.5 10−12
|
7.2 10−5 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.8e-5 | [98] | |
S230704f | 2023-07-04 02:12:11 |
1948
|
2965±978
|
H,L | 7.61 2.8 10−9
|
0.123 | 0.0 | 0.0 | 0.997 | 0.0 | 0.0026 | [99] | |
S230704bd | 2023-07-04 21:26:16 |
6293
|
15450±5072
|
H,L | 0.036 5.9 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.735 | 0.020 | 0.245 | [100] | |
S230706ah | 2023-07-06 10:43:33 |
1553
|
2143±684
|
H,L | 0.503 4.3 10−8
|
0.863 | 0.0 | 0.0 | 0.939 | 0.035 | 0.027 | [101] | |
S230707ai | 2023-07-07 12:40:47 |
2714
|
3766±1135
|
H,L | 1.56 1.4 10−8
|
0.474 | 0.0 | 0.0 | 0.951 | 0.0 | 0.049 | [102] | |
S230708t | 2023-07-08 05:37:05 |
1227
|
3010±988
|
H,L | 0.495 4.3 10−8
|
0.867 | 0.0 | 0.0 | 0.973 | 0.0041 | 0.027 | [103] | |
S230708z | 2023-07-08 07:18:59 |
3373
|
4647±1696
|
H,L | 0.305 7.0 10−8
|
0.962 | 0.0 | 0.0 | 0.954 | 0.0041 | 0.046 | [104] | |
S230708cf | 2023-07-08 23:09:35 |
2525
|
2056±608
|
H,L | 1.38 1.6 10−8
|
0.515 | 0.0 | 0.0 | 0.989 | 0.0 | 0.011 | [105] | |
S230709bi | 2023-07-09 12:27:27 |
2644
|
4364±1585
|
H,L | 7.00 3.1 10−9
|
0.133 | 0.0 | 0.0 | 0.997 | 0.0 | 0.0028 | [106] | |
S230711b | 2023-07-11 02:07:05 |
4775
|
6214±2136
|
H,L | 0.045 4.8 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.758 | 0.034 | 0.208 | [107] | |
S230716o | 2023-07-16 03:01:19 |
2351
|
508±203
|
H,L | 0.043 5.0 10−7
|
1.0 ~1.0 | 0.0 | 0.0064 | 0.568 | 0.176 | 0.250 | [108] | |
S230723ac | 2023-07-23 10:18:23 |
1117
|
1551±436
|
H,L | 0.402 5.3 10−8
|
0.917 | 0.0 | 0.0 | 0.867 | 0.0 | 0.133 | [109] | |
S230725am | 2023-07-25 13:16:48 |
3415
|
613±203
|
H,L | 0.043 5.0 10−7
|
1.0 ~1.0 | 0.0 | 0.00057 | 0.454 | 0.047 | 0.498 | [110] | |
S230726a | 2023-07-26 00:29:40 |
27774
|
2132±714
|
L | 559000 3.8 10−14
|
1.8 10−6 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 1.4e-7 | Detected by only the Livingston detector, resulting in a bad sky localization. | [111] |
S230728ap | 2023-07-28 08:36:28 |
3495
|
2731±1445
|
H,L | 0.209 1.0 10−7
|
0.9917[n 47] | 0.0 | 0.0 | 0.940 | 0.0 | 0.060 | [112] | |
S230729z | 2023-07-29 08:23:17 |
1945
|
1495±444
|
H,L | 6.32 3.4 10−9
|
0.158 | 0.0 | 0.0 | 0.942 | 0.055 | 0.0030 | [113] | |
S230731an | 2023-07-31 21:53:07 |
599
|
1001±242
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.174 | 0.771 | 0.053 | 0.0022 | [114] | |
S230802aq | 2023-08-02 11:33:59 |
25885
|
576±246
|
H | 0.962 2.2 10−8
|
0.646 | 0.0 | 0.020 | 0.289 | 0.657 | 0.035 | The other component is a black hole. Detected by only the Hanford detector, resulting in a bad sky localization. | [115] |
S230805x | 2023-08-05 03:42:49 |
2235
|
3852±1193
|
H,L | 2.33 9.2 10−9
|
0.349 | 0.0 | 0.0 | 0.99975 | 0.0 | 0.00025 | [116] | |
S230806ak | 2023-08-06 20:40:41 |
3715
|
5423±1862
|
H,L | 7.25 3.0 10−9
|
0.129 | 0.0 | 0.0 | 0.997 | 0.0 | 0.0026 | [117] | |
S230807f | 2023-08-07 20:50:45 |
5436
|
5272±1900
|
H,L | 0.300 7.1 10−8
|
0.964 | 0.0 | 0.0 | 0.913 | 0.041 | 0.047 | [118] | |
S230811n | 2023-08-11 03:21:16 |
810
|
1905±672
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.2e-5 | [119] | |
S230814r | 2023-08-14 06:19:20 |
3389
|
3788±1416
|
H,L | 0.446 4.8 10−8
|
0.894 | 0.0 | 0.0 | 0.932 | 0.0 | 0.068 | [120] | |
S230814ah | 2023-08-14 23:09:01 |
25259
|
330±105
|
L | 11600000000000 1.7 10−21
|
8.6 10−14 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.0e-14 | Detected by only the Livingston detector, resulting in a bad sky localization. | [121] |
S230819ax | 2023-08-19 17:19:10 |
4044
|
4216±1645
|
H,L | 2.42 8.8 10−9
|
0.338 | 0.0 | 0.0 | 0.993 | 0.0 | 0.0072 | [122] | |
S230820bq | 2023-08-20 21:25:15 |
1373
|
3600±1437
|
H,L | 0.507 4.2 10−8
|
0.861 | 0.0 | 0.0 | 0.958 | 0.0 | 0.042 | [123] | |
S230822ac | 2023-08-22 04:39:49 |
5534
|
9962±3231
|
H,L | 0.060 3.6 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.778 | 0.035 | 0.187 | [124] | |
S230822bm | 2023-08-22 23:03:37 |
3974
|
5154±1771
|
H,L | 0.829 2.6 10−8
|
0.700 | 0.0 | 0.0 | 0.939 | 0.042 | 0.019 | [125] | |
S230824r | 2023-08-24 03:30:47 |
3279
|
4701±1563
|
H,L | 1310 1.6 10−11
|
0.00076 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.9e-5 | [126] | |
S230825k | 2023-08-25 04:13:34 |
3012
|
5283±2117
|
H,L | 8.98 2.4 10−9
|
0.105 | 0.0 | 0.0 | 0.939 | 0.059 | 0.0022 | [127] | |
S230830q | 2023-08-30 06:47:44 |
1677
|
3843±1289
|
H,L | 0.161 1.3 10−7
|
0.9980[n 49] | 0.0 | 0.0 | 0.923 | 0.0041 | 0.077 | [128] | |
S230831e | 2023-08-31 01:54:14 |
3803
|
4900±2126
|
H,L | 1.08 2.0 10−8
|
0.603 | 0.0 | 0.0 | 0.985 | 0.0073 | 0.015 | [129] | |
S230902af | 2023-09-02 15:03:25 |
7622
|
10221±3354
|
H,L | 0.054 4.0 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.764 | 0.034 | 0.202 | [130] | |
S230904n | 2023-09-04 05:10:13 |
2015
|
1095±327
|
H,L | 9.53 2.2 10−9
|
0.100 | 0.0 | 0.0007 | 0.927 | 0.064 | 0.009 | [131] | |
S230904bg | 2023-09-04 19:45:32 |
3059
|
4581±1531
|
H,L | 0.027 8.0 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.688 | 0.0073 | 0.312 | [132] | |
S230911ae | 2023-09-11 19:53:24 |
27759
|
1623±584
|
H | 11300 1.9 10−12
|
8.8 10−5 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 3.6e-6 | Detected by only the Hanford detector, resulting in a bad sky localization. | [133] |
S230914ak | 2023-09-14 11:14:01 |
1532
|
2676±827
|
H,L | 23.8 9.0 10−10
|
0.041 | 0.0 | 0.0 | 0.992 | 0.0 | 0.0083 | [134] | |
S230919bj | 2023-09-19 21:57:12 |
708
|
1491±402
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 0.99965 | 0.0 | 0.00035 | [135] | |
S230920al | 2023-09-20 07:11:24 |
2180
|
3139±1003
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 1.1e-5 | [136] | |
S230922g | 2023-09-22 02:03:44 |
324; towards Pisces Austrinus or Aquarius
|
1491±443
|
H,L | 11100000000000000 1.9 10−24
|
0.0 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 0.0 | [137] | |
S230922q | 2023-09-22 04:06:58 |
4658
|
6653±2348
|
H,L | 59.4 3.6 10−10
|
0.017 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.2e-5 | [138] | |
S230924an | 2023-09-24 12:44:53 |
835
|
2358±596
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 1.9e-5 | [139] | |
S230927l | 2023-09-27 04:37:29 |
1177
|
2966±1041
|
H,L | 1.99 1.1 10−8
|
0.394 | 0.0 | 0.0 | 0.976 | 0.0 | 0.024 | [140] | |
S230927be | 2023-09-27 15:38:32 |
298
|
1059±289
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 0.99966 | 0.0 | 0.00034 | [141] | |
S230928cb | 2023-09-28 21:58:27 |
3093
|
5604±1692
|
H,L | 22.6 9.5 10−10
|
0.043 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.8e-5 | [142] | |
S230930al | 2023-09-30 11:07:30 |
2799
|
5123±1615
|
H,L | 2.90 7.4 10−9
|
0.291 | 0.0 | 0.0 | 0.994 | 0.0041 | 0.0061 | [143] | |
S231001aq | 2023-10-01 14:02:20 |
3181
|
4425±1946
|
H,L | 4.32 5.0 10−9
|
0.207 | 0.0 | 0.0 | 0.996 | 0.0044 | 0.0040 | [144] | |
S231004bq | 2023-10-04 23:23:46 |
4742
|
7960±2738
|
H,L | 0.028 7.6 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.677 | 0.030 | 0.292 | [145] | |
S231005j | 2023-10-05 02:10:30 |
5480
|
6417±2246
|
H,L | 0.666 3.2 10−8
|
0.777 | 0.0 | 0.0 | 0.978 | 0.0 | 0.022 | [146] | |
S231005ah | 2023-10-05 09:15:49 |
2497
|
3707±1335
|
H,L | 10.5 2.0 10−9
|
0.091 | 0.0 | 0.0 | 0.998 | 0.0041 | 0.0015 | [147] | |
S231007w | 2023-10-07 13:47:20 |
2648
|
3721±1231
|
H,L | 0.035 6.1 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.746 | 0.0041 | 0.254 | [148] | |
S231008ap | 2023-10-08 14:25:21 |
3102
|
3531±1320
|
H,L | 14.0 1.5 10−9
|
0.069 | 0.0 | 0.0 | 0.9986 | 0.0 | 0.0014 | [149] | |
S231014r | 2023-10-14 04:05:48 |
1807
|
2857±903
|
H,L | 2.07 1.0 10−8
|
0.382 | 0.0 | 0.0 | 0.992 | 0.0 | 0.0080 | [150] | |
S231020ba | 2023-10-20 14:29:47 |
1339
|
1168±361
|
H,L | 16.9 1.3 10−9
|
0.057 | 0.0 | 0.076 | 0.851 | 0.066 | 0.0070 | [151] | |
S231020bw | 2023-10-20 18:05:09 |
386
|
2620±694
|
H,L | 62.1 3.5 10−10
|
0.016 | 0.0 | 0.0 | 0.99965 | 0.0 | 0.00035 | [152] | |
S231025a | 2023-10-25 03:11:24 |
2254
|
233±135
|
H,L | 0.022 9.3 10−7
|
1.0 ~1.0 | 0.587 | 0.0016 | 0.0 | 0.0 | 0.412 | [153] | |
S231025ap | 2023-10-25 14:23:06 |
4584
|
4394±1526
|
H,L | 0.058 3.7 10−7
|
1.0 ~1.0 | 0.0 | 0.0 | 0.794 | 0.035 | 0.170 | [154] | |
S231028bg | 2023-10-28 15:30:06 |
1207
|
4221±923
|
H,L | 28100000000000000000000 7.6 10−31
|
0.0 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 0.0 | [155] | |
S231029y | 2023-10-29 11:15:08 |
29972
|
3292±1313
|
L | 99.0 2.2 10−10
|
0.010 | 0.0 | 0.0 | 0.99977 | 0.0 | 0.00023 | Detected by only the Livingston detector, resulting in a bad sky localization. | [156] |
S231102w | 2023-11-02 07:17:36 |
2343
|
3493±1015
|
H,L | 367000000000000 5.8 10−23
|
0.0 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 3.3e-16 | [157] | |
S231104ac | 2023-11-04 13:34:18 |
759
|
1357±321
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0020 | 0.988 | 0.0088 | 0.0018 | [158] | |
S231108u | 2023-11-08 12:51:42 |
949
|
1986±494
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 0.99969 | 0.0 | 0.00032 | [159] | |
S231110g | 2023-11-10 04:03:20 |
636
|
1849±533
|
H,L | 1.11 1.9 10−8
|
0.593 | 0.0 | 0.0 | 0.968 | 0.0 | 0.032 | [160] | |
S231113bb | 2023-11-13 12:26:23 |
2172
|
3260±1181
|
H,L | 0.383 5.6 10−8
|
0.927 | 0.0 | 0.0 | 0.965 | 0.0041 | 0.035 | [161] | |
S231113bw | 2023-11-13 20:04:17 |
1713
|
1186±376
|
H,L | 1.57 1.4 10−8
|
0.470 | 0.0 | 0.161 | 0.743 | 0.056 | 0.040 | [162] | |
S231114n | 2023-11-14 04:32:11 |
1267
|
1317±407
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 0.99985 | 0.0095 | 0.00015 | [163] | |
S231118d | 2023-11-18 00:56:26 |
1063
|
2352±681
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 0.99981 | 0.0 | 0.00019 | [164] | |
S231118ab | 2023-11-18 07:14:02 |
3197
|
4531±1498
|
H,L | 1.13 1.9 10−8
|
0.587 | 0.0 | 0.0 | 0.985 | 0.0 | 0.015 | [165] | |
S231118an | 2023-11-18 09:06:02 |
1048
|
1396±377
|
H,L | 0.287 7.5 10−8
|
0.969 | 0.0 | 0.015 | 0.726 | 0.017 | 0.242 | [166] | |
S231119u | 2023-11-19 07:52:48 |
5211
|
6597±2556
|
H,L | 0.288 7.4 10−8
|
0.969 | 0.0 | 0.015 | 0.914 | 0.041 | 0.045 | [167] | |
S231123cg | 2023-11-23 13:54:30 |
2714
|
1148±338
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.015 | 0.99999 | 0.041 | 7.6e-6 | [168] | |
S231124z | 2023-11-24 02:49:18 |
2490
|
8008±2734
|
H,L | 0.021 1.0 10−6
|
1.0 ~1.0 | 0.0 | 0.0 | 0.630 | 0.017 | 0.353 | [169] | |
S231127cg | 2023-11-27 16:53:00 |
3450
|
4425±1718
|
H,L | 3.69 5.8 10−9
|
0.237 | 0.0 | 0.0 | 0.996 | 0.0063 | 0.0044 | [170] | |
S231129ac | 2023-11-29 08:17:45 |
3089
|
3964±1513
|
H,L | 1.21 1.8 10−8
|
0.561 | 0.0 | 0.0 | 0.986 | 0.0041 | 0.014 | [171] | |
S231206ca | 2023-12-06 23:31:34 |
2335
|
3230±1141
|
H,L | 67.7 3.2 10−10
|
0.015 | 0.0 | 0.0 | 0.99998 | 0.0 | 0.000018 | [172] | |
S231206cc | 2023-12-06 23:39:01 |
342
|
1467±264
|
H,L | 1110000000000000000000000000 1.9 10−35
|
0.0 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 0.0 | [173] | |
S231213ap | 2023-12-13 11:14:17 |
1469
|
3861±1257
|
H,L | 33.8 6.3 10−10
|
0.029 | 0.0 | 0.0 | 0.99998 | 0.0 | 0.000022 | [174] | |
S231223j | 2023-12-23 03:28:36 |
3520
|
4468±1602
|
H,L | 19.3 1.1 10−9
|
0.051 | 0.0 | 0.0 | 0.99905 | 0.000023 | 0.00095 | [175] | |
S231223bg | 2023-12-23 20:26:19 |
24219
|
917±309
|
H | 0.022 9.6 10−7
|
1.0 ~1.0 | 0.0 | 0.00031 | 0.689 | 0.011 | 0.310 | Detected by only the Hanford detector, resulting in a bad sky localization. | [176] |
S231224e | 2023-12-24 02:43:21 |
394
|
863±213
|
H,L | 14.0 1.5 10−9
|
0.069 | 0.0 | 0.00019 | 0.880 | 0.117 | 0.0034 | [177] | |
S231226av | 2023-12-26 10:15:20 |
199
|
1218±171
|
H,L | 1920000000000000000000000000000000000000000 1.1 10−50
|
0.0 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 0.0 | [178] | |
S231231ag | 2023-12-31 15:40:16 |
27061
|
1066±339
|
H | 2570000 8.4 10−15
|
3.9 10−7 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.9e-8 | Detected by only the Hanford detector, resulting in a bad sky localization. | [179] |
S240104bl | 2024-01-04 16:49:32 |
27948
|
1978±615
|
H | 603000000 3.6 10−17
|
6.8 10−10 | 0.0 | 0.0 | 1.0 ~1.0
|
0.0 | 2.2e-10 | Detected by only the Hanford detector, resulting in a bad sky localization. | [180] |
S240107b | 2024-01-07 01:32:15 |
3961
|
3890±1212
|
H,L | 0.367 5.8 10−8
|
0.934 | 0.0 | 0.0 | 0.966 | 0.0 | 0.034 | [181] | |
S240109a | 2024-01-09 05:04:31 |
28048
|
1594±567
|
H | 2.92 7.3 10−9
|
0.290 | 0.0 | 0.0 | 0.995 | 0.0 | 0.0053 | Detected by only the Hanford detector, resulting in a bad sky localization. | [182] |
S240116p | 2024-01-16 04:23:14 |
5236
|
148±97
|
H,L | 0.157 1.4 10−7
|
0.9983 | 0.0 | 0.0 | 0.632 | 0.078 | 0.291 | [183] |
See also
- GRB 150101B, a weak gamma-ray burst trigger observed prior to aLIGO O1 (beginning September 12, 2015), with claimed similarities to model-supported possible neutron star merger GW170817/GRB 170817A/AT2017gfo.
Notes
- ↑ The detection date of a GW event is indicated by its designation; i.e., event GW150914 was detected on 2015-09-14.
- ↑ The relatively large and distant area of the sky within which it is claimed to be possible to localize the source.
- ↑ 1 Mpc is approximately 3.26 Mly.
- ↑ c2M☉ is about 1.8×103 foe; 1.8×1047 J; 1.8×1054 erg; 4.3×1046 cal; 1.7×1044 BTU; 5.0×1040 kWh, or 4.3×1037 tonnes of TNT.
- ↑ The chirp mass is the binary parameter most relevant to the evolution of the inspiral gravitational waveform, and thus is the mass that can be measured most accurately. It is related to, but less than, the geometric mean [math]\displaystyle{ (m_{geo}) }[/math] of the binary masses, according to [math]\displaystyle{ m_{geo} \left(\frac{m_{geo}}{m_1 + m_2}\right)^{1/5} }[/math], thus ranging from ~87% of [math]\displaystyle{ m_{geo} }[/math] when the masses are the same to ~78% when they differ by an order of magnitude.
- ↑ The dimensionless effective inspiral spin parameter is: [math]\displaystyle{ \frac{m_1 a_1 cos \theta_{LS_1} + m_2 a_2 cos \theta_{LS_2}}{m_1 + m_2}, }[/math][13] where [math]\displaystyle{ m }[/math] is the mass of a black hole, [math]\displaystyle{ a }[/math] is its spin, and [math]\displaystyle{ \theta_{LS} }[/math] is the angle between the orbital angular momentum and a merging black hole's spin (ranging from [math]\displaystyle{ 0 }[/math] when aligned to [math]\displaystyle{ \pi }[/math] when antialigned). It is the mass-weighted linear combination of the components of the black holes' spins aligned with the orbital axis[13][12] and has values ranging from −1 to 1 (the extremes correspond to situations with both black hole spins exactly antialigned and aligned, respectively, with orbital angular momentum).[14] This is the spin parameter most relevant to the evolution of the inspiral gravitational waveform, and it can be measured more accurately than those of the premerger BHs.[15]
- ↑ Values of the dimensionless spin parameter [math]\displaystyle{ a = }[/math] cJ/GM2 for a black hole range from zero to a maximum of one. The macroscopic properties of an isolated astrophysical (uncharged) black hole are fully determined by its mass and spin. Values for other objects can potentially exceed one. The largest value known for a neutron star is ≤ 0.4, and commonly used equations of state would limit that value to < 0.7.[16]
- ↑ Spin estimate is 0.26+0.52
−0.24.[17] - ↑ Spin estimate is 0.32+0.54
−0.29.[17] - ↑ Based on a descending spin-down chirp observed in GW post-merger, a magnetar was produced that survived at least 5 seconds.[26]
- ↑ Besides the loss of mass due to GW emission that occurred during the merger, the event is thought to have ejected 0.05±0.02 M☉ of material.[27]
- ↑ 1 Mpc is approximately 3.26 Mly.
- ↑ Which instruments observed the event. (H = LIGO Hanford, L=LIGO Livingston, V=Virgo)
- ↑ The area of the sky within which it was possible to localize the source.
- ↑ 1 Mpc is approximately 3.26 Mly.
- ↑ Which instruments observed the event. (H = LIGO Hanford, L=LIGO Livingston, V=Virgo)
- ↑ The chance a random signal of this significance would occur at any point in O3's 11-month run. Calculated by 1 - (1-false alarm rate in Hz)28,512,000. This is not the chance of the given signal being 'real' or not: Background contamination (such as earthquakes) can cause statistically significant signals as well, and although four detections have a >50% chance to have occurred randomly in O3, there is only a 19.4% chance that none of these signals would be real.
- ↑ Probability that both components have mass < 3 M☉
- ↑ Probability that one component has mass < 3 M☉ and the other has mass > 5 M☉
- ↑ Probability that both components have mass > 5 M☉
- ↑ Probability that at least one component has a mass in the range 3-5 M☉, between those of known neutron stars and black holes, a range sometimes identified as the "lower" mass gap
- ↑ Probability that the source is terrestrial or non-cosmological (e.g. foreground noises and signals [e.g. "noise"] or a technical/systematic error ["glitch"])
- ↑ The area of the sky within which it was possible to localize the source.
- ↑ 1 Mpc is approximately 3.26 Mly.
- ↑ Which instruments observed the event. (H = LIGO Hanford, L=LIGO Livingston, V=Virgo)
- ↑ The chance a random signal of this significance would occur at any point in O4's 20-month run. Calculated by 1 - (1-false alarm rate in Hz)46,656,000. This is not the chance of the given signal being 'real' or not: Background contamination (such as earthquakes) can cause statistically significant signals as well.
- ↑ Probability that both components have mass < 3 M☉
- ↑ Probability that one component has mass < 3 M☉ and the other has mass > 5 M☉
- ↑ Probability that both components have mass > 5 M☉
- ↑ Probability that at least one component has a mass in the range 3-5 M☉, between those of known neutron stars and black holes, a range sometimes identified as the "lower" mass gap
- ↑ Probability that the source is terrestrial or non-cosmological (e.g. foreground noises and signals [e.g. "noise"] or a technical/systematic error ["glitch"])
- ↑ During O4, random noise is expected to be as significant as this event 39 times; 0.5 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 35 times; 0.5 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 10 times; 0.2 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 14 times; 0.3 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 13 times; 0.3 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 13 times; 0.4 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 19 times; 0.7 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 7 times; 0.4 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 7 times; 0.4 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 9 times; 0.6 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 10 times; 0.8 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 28 times; 2 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 22 times; 2 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 23 times; 3 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 23 times; 3 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 5 times; 0.6 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 17 times; 3 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 6 times; 1 time by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 19 times; 4 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 37 times; 8 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 36 times; 9 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 28 times; 7 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 44 times; 13 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 17 times; 5 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 47 times; 17 times by this point in the run.
- ↑ During O4, random noise is expected to be as significant as this event 45 times; 18 times by this point in the run.
References
- ↑ "GW150914 - The First Direct Detection of Gravitational Waves". https://www.ligo.org/detections/GW150914.php.
- ↑ 2.0 2.1 "LSC News". https://www.ligo.org/news/index.php#lvkO4updateJan23.
- ↑ The LIGO Scientific Collaboration; the Virgo Collaboration; Abbott, B. P.; Abbott, R.; Abbott, T. D.; Abraham, S.; Acernese, F.; Ackley, K. et al. (2019-09-04). "GWTC-1: A Gravitational-Wave Transient Catalog of Compact Binary Mergers Observed by LIGO and Virgo during the First and Second Observing Runs". Physical Review X 9 (3): 031040. doi:10.1103/PhysRevX.9.031040. ISSN 2160-3308. Bibcode: 2019PhRvX...9c1040A.
- ↑ Burtnyk, Kimberly (2019-10-01). "LIGO's Commissioning Break Commences". https://www.ligo.caltech.edu/news/ligo20191001.
- ↑ 5.0 5.1 "LIGO Suspends Third Observing Run (O3)". Caltech. https://www.ligo.caltech.edu/news/ligo20200326.
- ↑ 6.0 6.1 Ligo, Virgo and Kagra Observing Run Plans
- ↑ https://observing.docs.ligo.org/plan/
- ↑ "GCN/LVC Notices". https://gcn.gsfc.nasa.gov/lvc.html.
- ↑ Fragione, Giacomo (2019). "Black Hole and Neutron Star Mergers in Galactic Nuclei". Monthly Notices of the Royal Astronomical Society 488 (1): 47–63. doi:10.1093/mnras/stz1651. Bibcode: 2019MNRAS.488...47F.
- ↑ Strickland, Ashley (3 May 2019). "Scientists may have detected violent collision between neutron star, black hole". CNN. https://www.cnn.com/2019/05/02/world/gravitational-wave-neutron-star-black-hole-collisions-scn/index.html.
- ↑ 11.0 11.1 11.2 Nitz, Alexander H. (25 February 2019). "1-OGC: The first open gravitational-wave catalog of binary mergers from analysis of public Advanced LIGO data". Astrophysical Journal 872 (2): 195. doi:10.3847/1538-4357/ab0108. Bibcode: 2019ApJ...872..195N.
- ↑ 12.0 12.1 12.2 12.3 12.4 12.5 12.6 12.7 Abbott, B.P. (2019). "GWTC-1: A Gravitational-Wave Transient Catalog of Compact Binary Mergers Observed by LIGO and Virgo during the First and Second Observing Runs". Physical Review X 9 (3): 031040. doi:10.1103/PhysRevX.9.031040. Bibcode: 2019PhRvX...9c1040A.
- ↑ 13.0 13.1 Cite error: Invalid
<ref>
tag; no text was provided for refs named50SM2017
- ↑ Farr, W. M.; Stevenson, S.; Miller, M. C.; Mandel, I.; F arr, B.; Vecchio, A. (2017). "Distinguishing spin-aligned and isotropic black hole populations with gravitational waves". Nature 548 (7667): 426–429. doi:10.1038/nature23453. PMID 28836595. Bibcode: 2017Natur.548..426F.
- ↑ Vitale, S.; Lynch, R.; Raymond, V.; Sturani, R.; Veitch, J.; Graff, P. (2017). "Parameter estimation for heavy binary-black holes with networks of second-generation gravitational-wave detectors". Physical Review D 95 (6): 064053. doi:10.1103/PhysRevD.95.064053. Bibcode: 2017PhRvD..95f4053V.
- ↑ 16.0 16.1 Abbott, B.P. (16 October 2017). "GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral". Physical Review Letters 119 (16): 161101. doi:10.1103/PhysRevLett.119.161101. PMID 29099225. Bibcode: 2017PhRvL.119p1101A.
- ↑ 17.0 17.1 17.2 The LIGO Scientific Collaboration and The Virgo Collaboration (3 June 2016). "An improved analysis of GW150914 using a fully spin-precessing waveform model". Physical Review X 6 (4): 041014. doi:10.1103/PhysRevX.6.041014. Bibcode: 2016PhRvX...6d1014A.
- ↑ Abbott, B.P. (11 February 2016). "Observation of Gravitational Waves from a Binary Black Hole Merger". Physical Review Letters 116 (6): 061102. doi:10.1103/PhysRevLett.116.061102. PMID 26918975. Bibcode: 2016PhRvL.116f1102A.
- ↑ Tushna Commissariat (11 February 2016). "LIGO detects first ever gravitational waves – from two merging black holes". Physics World. http://physicsworld.com/cws/article/news/2016/feb/11/ligo-detects-first-ever-gravitational-waves-from-two-merging-black-holes.
- ↑ Abbott, B.P. (21 October 2016). "Binary Black Hole Mergers in the first Advanced LIGO Observing Run". Physical Review X 6 (4): 041015. doi:10.1103/PhysRevX.6.041015. Bibcode: 2016PhRvX...6d1015A.
- ↑ Abbott, B.P. (15 June 2016). "GW151226: Observation of Gravitational Waves from a 22-Solar-Mass Binary Black Hole Coalescence". Physical Review Letters 116 (24): 241103. doi:10.1103/PhysRevLett.116.241103. PMID 27367379. Bibcode: 2016PhRvL.116x1103A.
- ↑ Nemiroff, R.; Bonnell, J., eds (15 June 2016). "GW151226: A Second Confirmed Source of Gravitational Radiation". Astronomy Picture of the Day. NASA. https://apod.nasa.gov/apod/ap160615.html.
- ↑ Abbott, B.P. (18 December 2017). "GW170608: Observation of a 19-solar-mass Binary Black Hole Coalescence". The Astrophysical Journal Letters 851 (2): L35. doi:10.3847/2041-8213/aa9f0c. Bibcode: 2017ApJ...851L..35A.
- ↑ Abbott, B.P. (2017-10-06). "GW170814: A three-detector observation of gravitational waves from a binary black hole coalescence". Phys. Rev. Lett. 119 (14): 141101. doi:10.1103/PhysRevLett.119.141101. PMID 29053306. Bibcode: 2017PhRvL.119n1101A. https://dcc.ligo.org/LIGO-P170814/public/main.
- "Gravitational waves from a binary black hole merger observed by LIGO and Virgo" (PDF). LIGO Scientific Collaboration (Press release).
- ↑ Overbye, Dennis (27 September 2017). "New Gravitational Wave Detection From Colliding Black Holes". The New York Times. https://www.nytimes.com/2017/09/27/science/black-holes-collision-ligo-virgo.html.
- ↑ van Putten, Maurice H.P.M.; Della Valle, Massimo (January 2019). "Observational evidence for extended emission to GW170817". Monthly Notices of the Royal Astronomical Society: Letters 482 (1): L46–L49. doi:10.1093/mnrasl/sly166. Bibcode: 2019MNRAS.482L..46V.
- ↑ Drout, M. R.; Piro, A. L.; Shappee, B. J. et al. (2017-10-16). "Light curves of the neutron star merger GW170817/SSS17a: Implications for r-process nucleosynthesis". Science 358 (6370): 1570–1574. doi:10.1126/science.aaq0049. PMID 29038375. Bibcode: 2017Sci...358.1570D.
- ↑ Abbott, B.P. (October 2017). "Multi-messenger Observations of a Binary Neutron Star Merger". The Astrophysical Journal 848 (2): L12. doi:10.3847/2041-8213/aa91c9. Bibcode: 2017ApJ...848L..12A. https://dcc.ligo.org/public/0145/P1700294/007/ApJL-MMAP-171017.pdf.
- ↑ Cho, Adrian (16 October 2017). "Merging neutron stars generate gravitational waves and a celestial light show". Science. https://www.science.org/content/article/merging-neutron-stars-generate-gravitational-waves-and-celestial-light-show.
- ↑ 30.00 30.01 30.02 30.03 30.04 30.05 30.06 30.07 30.08 30.09 30.10 30.11 30.12 30.13 30.14 30.15 30.16 30.17 30.18 30.19 30.20 30.21 30.22 30.23 30.24 30.25 30.26 30.27 30.28 30.29 30.30 30.31 30.32 30.33 30.34 The LIGO Scientific Collaboration; the Virgo Collaboration (2021). "GWTC-2: Compact Binary Coalescences Observed by LIGO and Virgo during the First Half of the Third Observing Run". Physical Review X 11 (2): 021053. doi:10.1103/PhysRevX.11.021053. Bibcode: 2021PhRvX..11b1053A.
- ↑ "Superevent info - S190412m". LIGO. https://gracedb.ligo.org/superevents/S190412m/view/.
- ↑ The LIGO Scientific Collaboration; the Virgo Collaboration; Abbott, R. et al. (17 April 2020). "GW190412: Observation of a Binary-Black-Hole Coalescence with Asymmetric Masses". Physical Review D 102 (4): 043015. doi:10.1103/PhysRevD.102.043015. Bibcode: 2020PhRvD.102d3015A.
- ↑ 33.0 33.1 Позаненко, А. С.; Минаев, П. Ю.; Гребенев, С. А.; Человеков, И. В. (2019). "Наблюдение в гамма-диапазоне второго связанного со слиянием нейтронных звезд события LIGO/Virgo S190425z" (in ru). Письма В Астрономический Журнал: Астрономия И Космическая Астрофизика 45 (11): 768–786. doi:10.1134/S032001081911007X.
- ↑ "Gravitational waves reveal a second neutron star collision". 8 January 2020. http://www.astronomy.com/news/2020/01/gravitational-waves-reveal-a-second-neutron-star-collision.
- ↑ "Superevent info - S190425z". LIGO. https://gracedb.ligo.org/superevents/S190425z/view/.
- ↑ The LIGO Scientific Collaboration; the Virgo Collaboration et al. (6 January 2020). "GW190425: Observation of a Compact Binary Coalescence with Total Mass ~ 3.4 M☉". The Astrophysical Journal 892 (1): L3. doi:10.3847/2041-8213/ab75f5. Bibcode: 2020ApJ...892L...3A.
- ↑ Abbott, R. (2 September 2020). "GW190521: A Binary Black Hole Merger with a Total Mass of 150 M ⊙" (in en). Physical Review Letters 125 (10): 101102. doi:10.1103/PhysRevLett.125.101102. PMID 32955328. Bibcode: 2020PhRvL.125j1102A.
- ↑ Abbott, R. (2 September 2020). "Properties and Astrophysical Implications of the 150 M ⊙ Binary Black Hole Merger GW190521". The Astrophysical Journal 900 (1): L13. doi:10.3847/2041-8213/aba493. Bibcode: 2020ApJ...900L..13A.
- ↑ "Black hole or neutron star?". June 23, 2020. https://news.psu.edu/story/623786/2020/06/23/research/black-hole-or-neutron-star.
- ↑ 40.00 40.01 40.02 40.03 40.04 40.05 40.06 40.07 40.08 40.09 40.10 40.11 40.12 40.13 40.14 40.15 40.16 40.17 40.18 40.19 40.20 40.21 40.22 40.23 40.24 40.25 40.26 40.27 40.28 40.29 40.30 40.31 40.32 40.33 The LIGO Scientific Collaboration et al. (17 November 2021). GWTC-3: Compact Binary Coalescences Observed by LIGO and Virgo During the Second Part of the Third Observing Run.
- ↑ 41.0 41.1 Abbott, R. et al. (2021). "Observation of Gravitational Waves from Two Neutron Star–Black Hole Coalescences". The Astrophysical Journal Letters 915 (1): L5. doi:10.3847/2041-8213/ac082e. Bibcode: 2021ApJ...915L...5A.
- ↑ "Superevent info - S200105ae". LIGO. https://gracedb.ligo.org/superevents/S200105ae/view/.
- ↑ 43.0 43.1 Bustillo, Juan Calderon; Sanchis-Gual, Nicolas; Leong, Samson H. W.; Chandra, Koustav; Torres-Forne, Alejandro; Font, Jose A.; Herdeiro, Carlos; Radu, Eugen; Wong, Isaac C. F.; Li, T. G. F. (2022). "Searching for vector boson-star mergers within LIGO-Virgo intermediate-mass black-hole merger candidates". arXiv:2206.02551 [gr-qc].
- ↑ 44.0 44.1 Hourihane, Sophie; Chatziioannou, Katerina; Wijngaarden, Marcella; Davis, Derek; Littenberg, Tyson; Cornish, Neil (15 August 2022). "Accurate modeling and mitigation of overlapping signals and glitches in gravitational-wave data". Physical Review D 106 (4): 042006. doi:10.1103/PhysRevD.106.042006. Bibcode: 2022PhRvD.106d2006H.
- ↑ "Superevent info - S200115j". LIGO. https://gracedb.ligo.org/superevents/S200115j/view/.
- ↑ Hartono, Naomi (29 June 2023). "15 Years of Radio Data Reveals Evidence of Space-Time Murmur". NASA. https://www.nasa.gov/feature/jpl/15-years-of-radio-data-reveals-evidence-of-space-time-murmur/.
- ↑ 47.0 47.1 47.2 Nitz, Alexander H.; Dent, Thomas; Davies, Gareth S.; Kumar, Sumit; Capano, Collin D.; Harry, Ian; Mozzon, Simone; Nuttall, Laura et al. (12 March 2020). "2-OGC: Open Gravitational-wave Catalog of Binary Mergers from Analysis of Public Advanced LIGO and Virgo Data". The Astrophysical Journal 891 (2): 123. doi:10.3847/1538-4357/ab733f. Bibcode: 2020ApJ...891..123N.
- ↑ Venumadhav, Tejaswi; Zackay, Barak; Roulet, Javier; Dai, Liang; Zaldarriaga, Matias (2020). "New Binary Black Hole Mergers in the Second Observing Run of Advanced LIGO and Advanced Virgo". Physical Review D 101 (8): 083030. doi:10.1103/PhysRevD.101.083030. Bibcode: 2020PhRvD.101h3030V.
- ↑ 49.0 49.1 Zackay, Barak; Dai, Liang; Venumadhav, Tejaswi; Roulet, Javier; Zaldarriaga, Matias (2021). "Detecting Gravitational Waves With Disparate Detector Responses: Two New Binary Black Hole Mergers" (in en). Phys. Rev. D 104 (8): 063030. doi:10.1103/PhysRevD.101.083030. Bibcode: 2020PhRvD.101h3030V.
- ↑ "Real-time alerts and circulars tracker". https://gcn.gsfc.nasa.gov/gcn3_archive.html.
- ↑ "Observing Plans and Public Alerts". LIGO Scientific Collaboration. October 2018. https://www.ligo.org/scientists/GWEMalerts.php.
- ↑ Singer, Leo P. (16 March 2017). "What constitutes an open, public alert?". LSC (LIGO Scientific Collaboration). https://wiki.gw-astronomy.org/pub/OpenLVEM/TownHallMeetings2018/what-is-an-opa.pdf.
- ↑ "GraceDB — Gravitational Wave Candidate Event Database". https://gracedb.ligo.org/latest/.
- ↑ "Real-time alerts and circulars tracker". https://gcn.gsfc.nasa.gov/gcn3/24045.gcn3.
- ↑ "LIGO Announces Commissioning Break". https://www.ligo.caltech.edu/news/ligo20190712.
- ↑ "KAGRA Gravitational-wave Telescope Starts Observation « KAGRA Large-scale Cryogenic Graviationai wave Telescope Project" (in ja). https://gwcenter.icrr.u-tokyo.ac.jp/en/archives/1381.
- ↑ "KAGRA to Join LIGO and Virgo in Hunt for Gravitational Waves". https://www.ligo.caltech.edu/news/ligo20191004.
- ↑ "LIGO Laboratory's Response to COVID-19". Caltech. https://www.ligo.caltech.edu/news/ligo20200317.
- ↑ "Superevent info - S190901ap". LIGO. https://gracedb.ligo.org/superevents/S190901ap/view/.
- ↑ "Superevent info - S190910d". LIGO. https://gracedb.ligo.org/superevents/S190910d/view/.
- ↑ "Superevent info - S190910h". LIGO. https://gracedb.ligo.org/superevents/S190910h/view/.
- ↑ "Superevent info - S190923y". LIGO. https://gracedb.ligo.org/superevents/S190923y/view/.
- ↑ "Superevent info - S190930t". LIGO. https://gracedb.ligo.org/superevents/S190930t/view/.
- ↑ "Superevent info - S191205ah". LIGO. https://gracedb.ligo.org/superevents/S191205ah/view/.
- ↑ "Superevent info - S191213g". LIGO. https://gracedb.ligo.org/superevents/S191213g/view/.
- ↑ "Superevent info - S200213t". LIGO. https://gracedb.ligo.org/superevents/S200213t/view/.
- ↑ "LIGO, Virgo and Kagra Observing Run Plans". Caltech. https://observing.docs.ligo.org/plan/.
- ↑ Burtnyk, Kimberly. "Latest Update on Start of Next Observing Run (O4)". LIGO (Caltech). https://www.ligo.caltech.edu/news/ligo20220123.
- ↑ "Detector status - 29 April 2023". https://gwosc.org/detector_status/day/20230429/.
- ↑ "Detector status - 5 May 2023". https://gwosc.org/detector_status/day/20230505/.
- ↑ "Superevent info - S230518h". LIGO. https://gracedb.ligo.org/superevents/S230518h/view/.
- ↑ "Superevent info - S230520ae". LIGO. https://gracedb.ligo.org/superevents/S230520ae/view/.
- ↑ "Superevent info - S230522a". LIGO. https://gracedb.ligo.org/superevents/S230522a/view/.
- ↑ "Superevent info - S230522n". LIGO. https://gracedb.ligo.org/superevents/S230522n/view/.
- ↑ "Superevent info - S230524b". LIGO. https://gracedb.ligo.org/superevents/S230524b/view/.
- ↑ "Superevent info - S230525a". LIGO. https://gracedb.ligo.org/superevents/S230525a/view/.
- ↑ "Superevent info - S230527bv". LIGO. https://gracedb.ligo.org/superevents/S230527bv/view/.
- ↑ "Superevent info - S230528a". LIGO. https://gracedb.ligo.org/superevents/S230528a/view/.
- ↑ "Superevent info - S230528bt". LIGO. https://gracedb.ligo.org/superevents/S230528bt/view/.
- ↑ "Superevent info - S230529ay". LIGO. https://gracedb.ligo.org/superevents/S230529ay/view/.
- ↑ "Superevent info - S230601bf". LIGO. https://gracedb.ligo.org/superevents/S230601bf/view/.
- ↑ "Superevent info - S230604z". LIGO. https://gracedb.ligo.org/superevents/S230604z/view/.
- ↑ "Superevent info - S230605o". LIGO. https://gracedb.ligo.org/superevents/S230605o/view/.
- ↑ "Superevent info - S230606d". LIGO. https://gracedb.ligo.org/superevents/S230606d/view/.
- ↑ "Superevent info - S230606z". LIGO. https://gracedb.ligo.org/superevents/S230606z/view/.
- ↑ "Superevent info - S230608as". LIGO. https://gracedb.ligo.org/superevents/S230608as/view/.
- ↑ "Superevent info - S230609a". LIGO. https://gracedb.ligo.org/superevents/S230609a/view/.
- ↑ "Superevent info - S230609u". LIGO. https://gracedb.ligo.org/superevents/S230609u/view/.
- ↑ "Superevent info - S230615av". LIGO. https://gracedb.ligo.org/superevents/S230615av/view/.
- ↑ "Superevent info - S230615az". LIGO. https://gracedb.ligo.org/superevents/S230615az/view/.
- ↑ "Superevent info - S230623at". LIGO. https://gracedb.ligo.org/superevents/S230623at/view/.
- ↑ "Superevent info - S230624av". LIGO. https://gracedb.ligo.org/superevents/S230624av/view/.
- ↑ "Superevent info - S230627c". LIGO. https://gracedb.ligo.org/superevents/S230627c/view/.
- ↑ "Superevent info - S230628aj". LIGO. https://gracedb.ligo.org/superevents/S230628aj/view/.
- ↑ "Superevent info - S230628ax". LIGO. https://gracedb.ligo.org/superevents/S230628ax/view/.
- ↑ "Superevent info - S230630am". LIGO. https://gracedb.ligo.org/superevents/S230630am/view/.
- ↑ "Superevent info - S230630bq". LIGO. https://gracedb.ligo.org/superevents/S230630bq/view/.
- ↑ "Superevent info - S230702an". LIGO. https://gracedb.ligo.org/superevents/S230702an/view/.
- ↑ "Superevent info - S230704f". LIGO. https://gracedb.ligo.org/superevents/S230704f/view/.
- ↑ "Superevent info - S230704bd". LIGO. https://gracedb.ligo.org/superevents/S230704bd/view/.
- ↑ "Superevent info - S230706ah". LIGO. https://gracedb.ligo.org/superevents/S230706ah/view/.
- ↑ "Superevent info - S230707ai". LIGO. https://gracedb.ligo.org/superevents/S230707ai/view/.
- ↑ "Superevent info - S230708t". LIGO. https://gracedb.ligo.org/superevents/S230708t/view/.
- ↑ "Superevent info - S230708z". LIGO. https://gracedb.ligo.org/superevents/S230708z/view/.
- ↑ "Superevent info - S230708cf". LIGO. https://gracedb.ligo.org/superevents/S230708cf/view/.
- ↑ "Superevent info - S230709bi". LIGO. https://gracedb.ligo.org/superevents/S230709bi/view/.
- ↑ "Superevent info - S230711b". LIGO. https://gracedb.ligo.org/superevents/S230711b/view/.
- ↑ "Superevent info - S230716o". LIGO. https://gracedb.ligo.org/superevents/S230716o/view/.
- ↑ "Superevent info - S230723ac". LIGO. https://gracedb.ligo.org/superevents/S230723ac/view/.
- ↑ "Superevent info - S230725am". LIGO. https://gracedb.ligo.org/superevents/S230725am/view/.
- ↑ "Superevent info - S230726a". LIGO. https://gracedb.ligo.org/superevents/S230726a/view/.
- ↑ "Superevent info - S230728ap". LIGO. https://gracedb.ligo.org/superevents/S230728ap/view/.
- ↑ "Superevent info - S230729z". LIGO. https://gracedb.ligo.org/superevents/S230729z/view/.
- ↑ "Superevent info - S230731an". LIGO. https://gracedb.ligo.org/superevents/S230731an/view/.
- ↑ "Superevent info - S230802aq". LIGO. https://gracedb.ligo.org/superevents/S230802aq/view/.
- ↑ "Superevent info - S230805x". LIGO. https://gracedb.ligo.org/superevents/S230805x/view/.
- ↑ "Superevent info - S230806ak". LIGO. https://gracedb.ligo.org/superevents/S230806ak/view/.
- ↑ "Superevent info - S230807f". LIGO. https://gracedb.ligo.org/superevents/S230807f/view/.
- ↑ "Superevent info - S230811n". LIGO. https://gracedb.ligo.org/superevents/S230811n/view/.
- ↑ "Superevent info - S230814r". LIGO. https://gracedb.ligo.org/superevents/S230814r/view/.
- ↑ "Superevent info - S230814ah". LIGO. https://gracedb.ligo.org/superevents/S230814ah/view/.
- ↑ "Superevent info - S230819ax". LIGO. https://gracedb.ligo.org/superevents/S230819ax/view/.
- ↑ "Superevent info - S230820bq". LIGO. https://gracedb.ligo.org/superevents/S230820bq/view/.
- ↑ "Superevent info - S230822ac". LIGO. https://gracedb.ligo.org/superevents/S230822ac/view/.
- ↑ "Superevent info - S230822bm". LIGO. https://gracedb.ligo.org/superevents/S230822bm/view/.
- ↑ "Superevent info - S230824r". LIGO. https://gracedb.ligo.org/superevents/S230824r/view/.
- ↑ "Superevent info - S230825k". LIGO. https://gracedb.ligo.org/superevents/S230825k/view/.
- ↑ "Superevent info - S230830q". LIGO. https://gracedb.ligo.org/superevents/S230830q/view/.
- ↑ "Superevent info - S230831e". LIGO. https://gracedb.ligo.org/superevents/S230831e/view/.
- ↑ "Superevent info - S230902af". LIGO. https://gracedb.ligo.org/superevents/S230902af/view/.
- ↑ "Superevent info - S230904n". LIGO. https://gracedb.ligo.org/superevents/S230904n/view/.
- ↑ "Superevent info - S230904bg". LIGO. https://gracedb.ligo.org/superevents/S230904bg/view/.
- ↑ "Superevent info - S230911ae". LIGO. https://gracedb.ligo.org/superevents/S230911ae/view/.
- ↑ "Superevent info - S230914ak". LIGO. https://gracedb.ligo.org/superevents/S230914ak/view/.
- ↑ "Superevent info - S230919bj". LIGO. https://gracedb.ligo.org/superevents/S230919bj/view/.
- ↑ "Superevent info - S230920al". LIGO. https://gracedb.ligo.org/superevents/S230920al/view/.
- ↑ "Superevent info - S230922g". LIGO. https://gracedb.ligo.org/superevents/S230922g/view/.
- ↑ "Superevent info - S230922q". LIGO. https://gracedb.ligo.org/superevents/S230922q/view/.
- ↑ "Superevent info - S230924an". LIGO. https://gracedb.ligo.org/superevents/S230924an/view/.
- ↑ "Superevent info - S230927l". LIGO. https://gracedb.ligo.org/superevents/S230927l/view/.
- ↑ "Superevent info - S230927be". LIGO. https://gracedb.ligo.org/superevents/S230927be/view/.
- ↑ "Superevent info - S230928cb". LIGO. https://gracedb.ligo.org/superevents/S230928cb/view/.
- ↑ "Superevent info - S230930al". LIGO. https://gracedb.ligo.org/superevents/S230930al/view/.
- ↑ "Superevent info - S231001aq". LIGO. https://gracedb.ligo.org/superevents/S231001aq/view/.
- ↑ "Superevent info - S231004bq". LIGO. https://gracedb.ligo.org/superevents/S231004bq/view/.
- ↑ "Superevent info - S231005j". LIGO. https://gracedb.ligo.org/superevents/S231005j/view/.
- ↑ "Superevent info - S231005ah". LIGO. https://gracedb.ligo.org/superevents/S231005ah/view/.
- ↑ "Superevent info - S231007w". LIGO. https://gracedb.ligo.org/superevents/S231007w/view/.
- ↑ "Superevent info - S231008ap". LIGO. https://gracedb.ligo.org/superevents/S231008ap/view/.
- ↑ "Superevent info - S231014r". LIGO. https://gracedb.ligo.org/superevents/S231014r/view/.
- ↑ "Superevent info - S231020ba". LIGO. https://gracedb.ligo.org/superevents/S231020ba/view/.
- ↑ "Superevent info - S231020bw". LIGO. https://gracedb.ligo.org/superevents/S231020bw/view/.
- ↑ "Superevent info - S231025a". LIGO. https://gracedb.ligo.org/superevents/S231025a/view/.
- ↑ "Superevent info - S231025ap". LIGO. https://gracedb.ligo.org/superevents/S231025ap/view/.
- ↑ "Superevent info - S231028bg". LIGO. https://gracedb.ligo.org/superevents/S231028bg/view/.
- ↑ "Superevent info - S231029y". LIGO. https://gracedb.ligo.org/superevents/S231029y/view/.
- ↑ "Superevent info - S231102w". LIGO. https://gracedb.ligo.org/superevents/S231102w/view/.
- ↑ "Superevent info - S231104ac". LIGO. https://gracedb.ligo.org/superevents/S231104ac/view/.
- ↑ "Superevent info - S231108u". LIGO. https://gracedb.ligo.org/superevents/S231108u/view/.
- ↑ "Superevent info - S231110g". LIGO. https://gracedb.ligo.org/superevents/S231110g/view/.
- ↑ "Superevent info - S231113bb". LIGO. https://gracedb.ligo.org/superevents/S231113bb/view/.
- ↑ "Superevent info - S231113bw". LIGO. https://gracedb.ligo.org/superevents/S231113bw/view/.
- ↑ "Superevent info - S231114n". LIGO. https://gracedb.ligo.org/superevents/S231114n/view/.
- ↑ "Superevent info - S231118d". LIGO. https://gracedb.ligo.org/superevents/S231118d/view/.
- ↑ "Superevent info - S231118ab". LIGO. https://gracedb.ligo.org/superevents/S231118ab/view/.
- ↑ "Superevent info - S231118an". LIGO. https://gracedb.ligo.org/superevents/S231118an/view/.
- ↑ "Superevent info - S231119u". LIGO. https://gracedb.ligo.org/superevents/S231119u/view/.
- ↑ "Superevent info - S231123cg". LIGO. https://gracedb.ligo.org/superevents/S231123cg/view/.
- ↑ "Superevent info - S231124z". LIGO. https://gracedb.ligo.org/superevents/S231124z/view/.
- ↑ "Superevent info - S231127cg". LIGO. https://gracedb.ligo.org/superevents/S231127cg/view/.
- ↑ "Superevent info - S231129ac". LIGO. https://gracedb.ligo.org/superevents/S231129ac/view/.
- ↑ "Superevent info - S231206ca". LIGO. https://gracedb.ligo.org/superevents/S231206ca/view/.
- ↑ "Superevent info - S231206cc". LIGO. https://gracedb.ligo.org/superevents/S231206cc/view/.
- ↑ "Superevent info - S231213ap". LIGO. https://gracedb.ligo.org/superevents/S231213ap/view/.
- ↑ "Superevent info - S231223j". LIGO. https://gracedb.ligo.org/superevents/S231223j/view/.
- ↑ "Superevent info - S231223bg". LIGO. https://gracedb.ligo.org/superevents/S231223bg/view/.
- ↑ "Superevent info - S231224e". LIGO. https://gracedb.ligo.org/superevents/S231224e/view/.
- ↑ "Superevent info - S231226av". LIGO. https://gracedb.ligo.org/superevents/S231226av/view/.
- ↑ "Superevent info - S231231ag". LIGO. https://gracedb.ligo.org/superevents/S231231ag/view/.
- ↑ "Superevent info - S240104bl". LIGO. https://gracedb.ligo.org/superevents/S240104bl/view/.
- ↑ "Superevent info - S240107b". LIGO. https://gracedb.ligo.org/superevents/S240107b/view/.
- ↑ "Superevent info - S240109a". LIGO. https://gracedb.ligo.org/superevents/S240109a/view/.
- ↑ "Superevent info - S240116p". LIGO. https://gracedb.ligo.org/superevents/S240116p/view/.
External links
Original source: https://en.wikipedia.org/wiki/List of gravitational wave observations.
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