2023A&A...678A.187C


Query : 2023A&A...678A.187C

2023A&A...678A.187C - Astronomy and Astrophysics, volume 678A187 (2023/10-1)

The MPIfR-MeerKAT Galactic Plane Survey II. The eccentric double neutron star system PSR J1208-5936 and a neutron star merger rate update.

COLOM I BERNADICH M., BALAKRISHNAN V., BARR E., BEREZINA M., BURGAY M., BUCHNER S., CHAMPION D.J., CHEN W., DESVIGNES G., FREIRE P.C.C., GRUNTHAL K., KRAMER M., MEN Y., PADMANABH P.V., PARTHASARATHY A., PILLAY D., RAMMALA I., SENGUPTA S. and VENKATRAMAN KRISHNAN V.

Abstract (from CDS):

The MPIfR-MeerKAT Galactic Plane survey at L-band (MMGPS-L) is the most sensitive pulsar survey in the Southern Hemisphere, providing 78 discoveries in an area of 900 sq. deg. Here, we present a follow-up study of one of these new discoveries, PSR J1208-5936, a 28.71-ms recycled pulsar in a double neutron star system with an orbital period of Pb = 0.632 days and an eccentricity of e = 0.348, merging within the Hubble time. Through timing of almost one year of observations, we detected the relativistic advance of periastron (ω̇ = 0.918(1) deg yr–1), resulting in a total system mass of Mt = 2.586(5) M⊙. We also achieved low-significance constraints on the amplitude of the Einstein delay and Shapiro delay, in turn yielding constraints on the pulsar mass ($ M_{\mathrm{p}}=1.26^{+0.13}_{-0.25}\,M_\odot $), the companion mass ($ M_{\mathrm{c}}=1.32^{+0.25}_{-0.13}\,M_\odot $), and the inclination angle (i = 57 ± 12°). This system is highly eccentric compared to other Galactic field double neutron stars with similar periods, possibly hinting at a larger-than-usual supernova kick during the formation of the second-born neutron star. The binary will merge within 7.2(2) Gyr due to the emission of gravitational waves, making it a progenitor of the neutron star merger events seen by ground-based gravitational wave observatories. With the improved sensitivity of the MMGPS-L, we updated the Milky Way neutron star merger rate to be $ \mathcal{R}_{\mathrm{MW}}^{\mathrm{new}}=25^{+19}_{-9} $ Myr–1 within 90% credible intervals, which is lower than previous studies based on known Galactic binaries owing to the lack of further detections despite the highly sensitive nature of the survey. This implies a local cosmic neutron star merger rate of $ \mathcal{R}_{\mathrm{local}}^{\mathrm{new}}=293^{+222}_{-103} $ Gpc–3 yr–1, which is consistent with LIGO and Virgo O3 observations. With this, we also predict the observation of $ 10^{+8}_{-4} $ neutron star merger events during the LIGO-Virgo-KAGRA O4 run. We predict the uncertainties on the component masses and the inclination angle will be reduced to 5 × 10–3 M⊙ and 0.4° after two decades of timing, and that in at least a decade from now the detection of Ṗb and the sky proper motion will serve to make an independent constraint of the distance to the system.

Abstract Copyright: © The Authors 2023

Journal keyword(s): binaries: close - ephemerides - gravitational waves - stars: neutron - celestial mechanics - stars: fundamental parameters

Simbad objects: 25

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Number of rows : 25
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 J0737-3039A Psr 07 37 51.24669 -30 39 40.6895           ~ 317 1
4 PSR J0737-3039 Psr 07 37 51.248 -30 39 40.83           ~ 445 1
5 PSR J0737-3039B Psr 07 37 51.24927 -30 39 40.7195           ~ 222 1
6 PSR J1018-1523 Psr 10 18 12.72 -15 23 10.2           ~ 10 0
7 PSR J1155-6529 Psr 11 55 13.26 -65 29 18.5           ~ 5 0
8 PSR J1208-5936 Psr 12 08 27.03010 -59 36 20.3812           ~ 8 0
9 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
10 PSR J1325-6253 Psr 13 25 04.8907 -62 53 39.594           ~ 14 0
11 PSR J1411+2551 Psr 14 11 18.866 +25 51 08.39           ~ 50 0
12 PSR J1518+4904 Psr 15 18 16.832 +49 04 34.19           ~ 201 1
13 PSR B1534+11 Psr 15 37 09.9603 +11 55 55.554           ~ 453 1
14 PSR J1753-2240 Psr 17 53 39.847 -22 40 42.00           ~ 53 1
15 PSR J1755-25 Psr 17 55 38.400 -25 50 22.00           ~ 34 0
16 PSR J1756-2251 Psr 17 56 46.63 -22 51 59.4           ~ 153 1
17 PSR J1757-1854 Psr 17 57 03.78438 -18 54 03.3760           ~ 67 0
18 PSR J1759+5036 Psr 17 59 45.672 +50 36 56.96           ~ 17 0
19 PSR B1809-17.6 Psr 18 11 55.034 -17 36 37.70           ~ 114 1
20 PSR J1829+2456 Psr 18 29 34.6668 +24 56 18.193           ~ 89 1
21 PSR J1906+0749 Psr 19 06 48.67 +07 46 28.6           ~ 172 1
22 PSR J1913+1102 Psr 19 13 29.0542 +11 02 05.741           ~ 64 0
23 PSR J1915+1606 Psr 19 15 27.99999 +16 06 27.4034     22.5     ~ 1032 1
24 PSR J1930-1852 Psr 19 30 29.7156 -18 51 46.270           ~ 54 0
25 PSR J1946+2052 Psr 19 46 14.1438633037 +20 52 24.333605451           ~ 65 0

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