2015ApJ...812..143M


Query : 2015ApJ...812..143M

2015ApJ...812..143M - Astrophys. J., 812, 143 (2015/October-3)

Pulsar J0453+1559: a double neutron star system with a large mass asymmetry.

MARTINEZ J.G., STOVALL K., FREIRE P.C.C., DENEVA J.S., JENET F.A., McLAUGHLIN M.A., BAGCHI M., BATES S.D. and RIDOLFI A.

Abstract (from CDS):

To understand the nature of supernovae and neutron star (NS) formation, as well as binary stellar evolution and their interactions, it is important to probe the distribution of NS masses. Until now, all double NS (DNS) systems have been measured as having a mass ratio close to unity (q ≥ 0.91). Here, we report the measurement of the individual masses of the 4.07-day binary pulsar J0453+1559 from measurements of the rate of advance of periastron and Shapiro delay: the mass of the pulsar is Mp= 1.559±0.005 M{#8857} and that of its companion is M{#8857}; q = 0.75. If this companion is also an NS, as indicated by the orbital eccentricity of the system (e = 0.11), then its mass is the smallest precisely measured for any such object. The pulsar has a spin period of 45.7 ms and a spin period derivative of = (1.8616±0.0007)x10–19 s/s; from these, we derive a characteristic age of ∼ 4.1x109 years and a magnetic field of ∼ 2.9x109 G, i.e., this pulsar was mildly recycled by the accretion of matter from the progenitor of the companion star. This suggests that it was formed with (very approximately) its current mass. Thus, NSs form with a wide range of masses, which is important for understanding their formation in supernovae. It is also important for the search for gravitational waves released during an NS-NS merger: it is now evident that we should not assume that all DNS systems are symmetric.

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Journal keyword(s): gravitational waves - pulsars: general - pulsars: individual: J0453+1559

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 J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
2 PSR J0453+1559 Psr 04 53 45.41372 +15 59 21.3000           ~ 92 0
3 PSR J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
4 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
5 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
6 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
7 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
8 PSR J1727-2946 Psr 17 27 15.09493 -29 46 36.7970           ~ 19 0
9 PSR J1738+0333 Psr 17 38 53.966386 +03 33 10.87200           ~ 191 1
10 PSR J1753-2240 Psr 17 53 39.847 -22 40 42.00           ~ 53 1
11 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
12 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
13 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 64 0
14 PSR B1809-17.6 Psr 18 11 55.034 -17 36 37.70           ~ 114 1
15 PSR J1829+2456 Psr 18 29 34.6668 +24 56 18.193           ~ 89 1
16 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
17 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
18 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
19 PSR J1930-1852 Psr 19 30 29.7156 -18 51 46.270           ~ 54 0
20 PSR J2129+1209C Psr 21 30 01.2030 +12 10 38.159           ~ 215 2

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