2019ApJ...880L...8A


Query : 2019ApJ...880L...8A

2019ApJ...880L...8A - Astrophys. J., 880, L8-L8 (2019/July-3)

Double neutron star populations and formation channels.

ANDREWS J.J. and MANDEL I.

Abstract (from CDS):

In the past five years, the number of known double neutron stars (DNSs) in the Milky Way has roughly doubled. We argue that the observed sample can be split into three distinct subpopulations based on their orbital characteristics: (i) short-period, low-eccentricity binaries; (ii) wide binaries; and (iii) short-period, high-eccentricity binaries. These subpopulations also exhibit distinct spin period and spindown rate properties. We focus on subpopulation (iii), which contains the Hulse-Taylor binary. Contrary to previous analysis, we demonstrate that, if they are the product of isolated binary evolution, the Porb and e distribution of these systems requires that the second-born NSs must have been formed with small natal kicks (<=25 km s–1) and have pre-SN masses narrowly distributed around 3.2 M☉. These constraints challenge binary evolution theory and further predict closely aligned spin and orbital axes, inconsistent with the Hulse-Taylor binary's measured spin-orbit misalignment angle of ≃20°. Motivated by the similarity of these DNSs to B2127+11C, a DNS residing in the globular cluster M15, we argue that this subpopulation is consistent with being formed in, and then ejected from, globular clusters. This scenario provides a pathway for the formation and merger of DNSs in stellar environments without recent star formation, as observed in the host galaxy population of short gamma-ray bursts and the recent detection by LIGO of a merging DNS in an old stellar population.

Abstract Copyright: © 2019. The American Astronomical Society. All rights reserved.

Journal keyword(s): binaries: close - stars: neutron - supernovae: general

Simbad objects: 23

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Number of rows : 23
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 J0509+3801 Psr 05 09 31.788 +38 01 18.10           ~ 41 0
3 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
4 NGC 4993 Sy2 13 09 47.6908761600 -23 23 02.314044636   13.34   11.92   ~ 397 0
5 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
6 PSR J1411+2551 Psr 14 11 18.866 +25 51 08.39           ~ 50 0
7 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
8 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
9 PSR J1753-2240 Psr 17 53 39.847 -22 40 42.00           ~ 53 1
10 PSR J1755-25 Psr 17 55 38.400 -25 50 22.00           ~ 34 0
11 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
12 PSR J1757-1854 Psr 17 57 03.78438 -18 54 03.3760           ~ 67 0
13 NGC 6544 GlC 18 07 20.58 -24 59 50.4   11.36 9.90     ~ 332 0
14 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 64 0
15 PSR B1809-17.6 Psr 18 11 55.034 -17 36 37.70           ~ 114 1
16 PSR J1829+2456 Psr 18 29 34.6668 +24 56 18.193           ~ 89 1
17 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
18 PSR J1913+1102 Psr 19 13 29.0542 +11 02 05.741           ~ 64 0
19 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
20 PSR J1930-1852 Psr 19 30 29.7156 -18 51 46.270           ~ 54 0
21 PSR J1946+2052 Psr 19 46 14.1438633037 +20 52 24.333605451           ~ 65 0
22 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
23 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 215 2

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