2018MNRAS.478.1377A


Query : 2018MNRAS.478.1377A

2018MNRAS.478.1377A - Mon. Not. R. Astron. Soc., 478, 1377-1391 (2018/July-3)

Evidence for a maximum mass cut-off in the neutron star mass distribution and constraints on the equation of state.

ALSING J., SILVA H.O. and BERTI E.

Abstract (from CDS):

We infer the mass distribution of neutron stars in binary systems using a flexible Gaussian mixture model and use Bayesian model selection to explore evidence for multimodality and a sharp cut-off in the mass distribution. We find overwhelming evidence for a bimodal distribution, in agreement with previous literature, and report for the first time positive evidence for a sharp cut-off at a maximum neutron star mass. We measure the maximum mass to be 2.0 M☉ < mmax < 2.2 M☉ (68 per cent), 2.0 M☉ < mmax < 2.6 M☉ (90 per cent), and evidence for a cut-off is robust against the choice of model for the mass distribution and to removing the most extreme (highest mass) neutron stars from the data set. If this sharp cut-off is interpreted as the maximum stable neutron star mass allowed by the equation of state of dense matter, our measurement puts constraints on the equation of state. For a set of realistic equations of state that support >2 M☉ neutron stars, our inference of mmax is able to distinguish between models at odds ratios of up to 12:1, whilst under a flexible piecewise polytropic equation-of-state model our maximum mass measurement improves constraints on the pressure at 3-7x the nuclear saturation density by ∼30-50 per cent compared to simply requiring mmax > 2 M☉. We obtain a lower bound on the maximum sound speed attained inside the neutron star of c_ s_max > 0.63c (99.8 per cent), ruling out c_ s_max < c/sqrt(3)at high significance. Our constraints on the maximum neutron star mass strengthen the case for neutron star-neutron star mergers as the primary source of short gamma-ray bursts.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): equation of state - stars: neutron

CDS comments: Table 1: J1740-5350 is a misprint for J1740-5340.

Simbad objects: 69

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Number of rows : 69
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 J0024-72H Psr 00 24 06.686 -72 04 06.74           ~ 64 1
2 PSR J0045-7319 HXB 00 45 35.2606875816 -73 19 03.269105220   15.97 16.18   16.30 B0.5-B2IV-V 193 0
3 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
4 ChASeM33 J013236.84+303229.0 X 01 32 36.95 +30 32 30.1           ~ 15 0
5 PSR J0337+1715 Psr 03 37 43.8210968640 +17 15 14.886499572           ~ 113 0
6 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
7 PSR J0437-47 Psr 04 37 15.7994581776 -47 15 08.544351636           DC 1032 0
8 PSR J0453+1559 Psr 04 53 45.41372 +15 59 21.3000           ~ 92 0
9 PSR J0514-4002A Psr 05 14 06.6927 -40 02 48.897           ~ 69 1
10 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0 14.290   O8III 714 0
11 PSR J0621+10 Psr 06 21 22.11108 +10 02 38.7410           ~ 128 1
12 PSR J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
13 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
14 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
15 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
16 V* V395 Car LXB 09 22 34.6761959832 -63 17 41.355773520 15.40 16.104 15.455     K0III 143 0
17 PSR J1012+5307 Psr 10 12 33.4345449600 +53 07 02.548542576     19.5     DA 419 1
18 PSR J1023+0038 Psr 10 23 47.6841824712 +00 38 41.005893516     17.31     GV 470 0
19 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1159 0
20 PSR J1141-6545 Psr 11 41 07.00060 -65 45 19.0500     25.08 24.38   ~ 207 1
21 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
22 PSR J1311-3430 Psr 13 11 45.7292612136 -34 30 30.294149760   21.0   18.8   ~ 181 1
23 PSR J1518+0204B Psr 15 18 31.458 +02 05 15.47           ~ 46 1
24 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
25 V* QV Nor HXB 15 42 23.3633146128 -52 23 09.577395960   16.3 14.5     B0.2Ia 455 1
26 PSR J1600-3053 Psr 16 00 51.902514 -30 53 49.45343           ~ 218 0
27 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
28 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
29 2MASS J17004888-4139214 HXB 17 00 48.884 -41 39 21.46           Ofpe/WN9 272 0
30 HD 153919 HXB 17 03 56.7725629224 -37 50 38.913331452 6.06 6.78 6.51 6.08 5.90 O6Iafcp 851 0
31 PSR J1713+0747 Psr 17 13 49.5367813 +07 47 37.450240           ~ 530 1
32 PSR J1723-2837 Psr 17 23 23.1937506912 -28 37 57.210408048   16.81 15.77 15.71   ~ 105 0
33 2MASS J17251139-3616575 HXB 17 25 11.392 -36 16 57.53     14.30     B0-1Ia 140 2
34 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
35 PSR J1740-5340 Psr 17 40 44.589 -53 40 40.90   17.43   16.25   ~ 157 2
36 PSR J1748-2446I Psr 17 48 04.870 -24 46 46.48           ~ 37 0
37 PSR J1748-2446J Psr 17 48 04.9 -24 46 45           ~ 30 0
38 PSR J1748-2446ad Psr 17 48 04.9 -24 46 04           ~ 141 1
39 PSR J1748-2021B Psr 17 48 52.95290 -20 21 38.8600           ~ 34 0
40 PSR J1750-3703A Psr 17 50 13.8016 -37 03 10.950           ~ 14 1
41 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
42 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
43 SAX J1802.7-2017 HXB 18 02 41.9407199832 -20 17 17.312648064   17.4 16.4     B1Ib 100 0
44 PSR J1802-07 Psr 18 04 49.8954 -07 35 24.690     12.33     ~ 101 2
45 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 64 0
46 PSR J1816+4510 Psr 18 16 35.9342957160 +45 10 33.917516328           ~ 126 0
47 PSR J1824-2452C Psr 18 24 32.8 -24 52 11           ~ 23 1
48 V* V691 CrA LXB 18 25 46.8185061768 -37 06 18.529336656 14.30 15.20 15.1     ~ 461 0
49 XTE J1855-026 HXB 18 55 30.4058947392 -02 36 16.737653700   16.451 14.512 14.056   B0Iaep 104 0
50 PSR B1855+09 Psr 18 57 36.390620 +09 43 17.20712           DA 569 1
51 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
52 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
53 PSR J1909-3744 Psr 19 09 47.42820 -37 44 14.7740           ~ 343 2
54 PSR J1910-5959A Psr 19 11 42.7562 -59 58 26.900 22.02 22.13 22.03     DA5 99 1
55 PSR J1913+1102 Psr 19 13 29.0542 +11 02 05.741           ~ 64 0
56 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
57 PSR J1918-0642 Psr 19 18 48.027685 -06 42 34.95735           ~ 146 0
58 PSR J1946+3417 Psr 19 46 25.13182 +34 17 14.6770           ~ 64 0
59 PSR J1949+3106 Psr 19 49 29.63851 +31 06 03.8289           ~ 42 0
60 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
61 PSR J2043+1711 Psr 20 43 20.8828 +17 11 28.941           ~ 129 1
62 PSR J2045+3633 Psr 20 45 01.50504 +36 33 01.4033           ~ 18 0
63 PSR J2053+4650 Psr 20 53 52.62804 +46 50 51.7181           ~ 17 0
64 V* LZ Aqr LXB 21 23 14.54 -05 47 52.9 15.90 16.78 16.8     ~ 154 0
65 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 215 2
66 V* V1341 Cyg LXB 21 44 41.1544345272 +38 19 17.066570988 15.00 15.13 14.68 15.00   A9III 1229 1
67 PSR J2222-0137 Psr 22 22 06.00015 -01 37 15.7827           ~ 78 0
68 PSR J2234+06 Psr 22 34 22 +06 11.0           ~ 76 0
69 PSR J2305+4707 Psr 23 05 55.842 +47 07 45.32           ~ 227 1

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