2019PASP..131f4201Y


Query : 2019PASP..131f4201Y

2019PASP..131f4201Y - Publ. Astron. Soc. Pac., 131, part no 6, 4201-64201 (2019/June-0)

The classifications of double neutron stars and their correlations with the binary orbital parameters.

YANG Y.-Y., ZHANG C.-M., LI D., CHEN L., LINGHU R.-F. and ZHI Q.-J.

Abstract (from CDS):

The statistical distribution of the total mass of 14 double neutron star (DNS) systems (out of 18 pairs observed) is found to be very narrow, with the average and standard deviation as 2.65 ± 0.03 M☉. For the seven pairs of DNSs with the precisely measured masses of the recycled NSs (first formed) and their non-recycled companions (second formed), their masses are homogeneously distributed as 1.38 ± 0.02 M☉ and 1.29 ± 0.02 M☉, respectively. It is shown by the Anderson-Darling and Mann-Whitney-Wilcoxon tests that the first-born NSs share a same distribution, which should be formed by the supernova explosion; however, the second-formed NSs have the different statistical origins, which can be ascribed to three formation mechanisms after the further investigations of their orbital parameters and mass values, for instance, supernova explosion (e.g., PSR B1913+16), electron capture (e.g., PSR J0737-3039B), and ultra-stripped cores in close-orbit systems (e.g., PSR J1411+2551). In addition, by means of Fisher's discriminant method, through simulation of the two groups of DNS samples that originated from electron-capture supernova and core-collapse supernova, we obtained the linear discriminant equation (e = -4.5Porb(day) + 1.1) between the eccentricity and orbital period, which can divide the DNSs into two groups involved in NS formed by electron-capture supernova (core-collapse supernova) without (with) kick.

Abstract Copyright: © 2019. The Astronomical Society of the Pacific. All rights reserved.

Journal keyword(s):

Simbad objects: 20

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Number of rows : 20
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 J0453+1559 Psr 04 53 45.41372 +15 59 21.3000           ~ 92 0
2 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
3 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
4 PSR J0751+1807 Psr 07 51 09.1539 +18 07 38.335           ~ 316 1
5 PSR J1411+2551 Psr 14 11 18.866 +25 51 08.39           ~ 50 0
6 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
7 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
8 PSR J1753-2240 Psr 17 53 39.847 -22 40 42.00           ~ 53 1
9 PSR J1755-25 Psr 17 55 38.400 -25 50 22.00           ~ 34 0
10 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
11 PSR J1757-1854 Psr 17 57 03.78438 -18 54 03.3760           ~ 67 0
12 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 64 0
13 PSR B1809-17.6 Psr 18 11 55.034 -17 36 37.70           ~ 114 1
14 PSR J1829+2456 Psr 18 29 34.6668 +24 56 18.193           ~ 89 1
15 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
16 PSR J1913+1102 Psr 19 13 29.0542 +11 02 05.741           ~ 64 0
17 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
18 PSR J1930-1852 Psr 19 30 29.7156 -18 51 46.270           ~ 54 0
19 PSR J1946+2052 Psr 19 46 14.1438633037 +20 52 24.333605451           ~ 65 0
20 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 215 2

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