2022A&A...665A..53S


Query : 2022A&A...665A..53S

2022A&A...665A..53S - Astronomy and Astrophysics, volume 665A53-53 (2022/9-1)

The eccentric millisecond pulsar, PSR J0955-6150. I. Pulse profile analysis, mass measurements, and constraints on binary evolution.

SERYLAK M., VENKATRAMAN KRISHNAN V., FREIRE P.C.C., TAURIS T.M., KRAMER M., GEYER M., PARTHASARATHY A., BAILES M., COLOM I BERNADICH M., BUCHNER S., BURGAY M., CAMILO F., KARASTERGIOU A., LOWER M.E., POSSENTI A., REARDON D.J., SHANNON R.M., SPIEWAK R., STAIRS I.H. and VAN STRATEN W.

Abstract (from CDS):


Context. PSR J0955-6150 is a member of an enigmatic class of eccentric millisecond pulsar (MSP) and helium white dwarf (He WD) systems (eMSPs), whose binary evolution is poorly understood and believed to be strikingly different to that of traditional MSP+He WD systems in circular orbits.
Aims. Measuring the masses of the stars in this system is important for testing the different hypotheses for the formation of eMSPs.
Methods. We carried out timing observations of this pulsar with the Parkes radio telescope using the 20 cm multibeam and ultra-wide bandwidth low-frequency (UWL) receivers, and the L-band receiver of the MeerKAT radio telescope. The pulse profiles were flux and polarisation calibrated, and a rotating-vector model (RVM) was fitted to the position angle of the linear polarisation of the combined MeerKAT data. Pulse times of arrival (ToAs) were obtained from these using standard pulsar analysis techniques and analysed using theTEMPO2 timing software.
Results. Our observations reveal a strong frequency evolution of this MSP's intensity, with a flux density spectral index (α) of -3.13(2). The improved sensitivity of MeerKAT resulted in a greater than tenfold improvement in the timing precision obtained compared to our older Parkes observations. This, combined with the eight-year timing baseline, has allowed precise measurements of a very small proper motion and three orbital post-Keplerian parameters, namely the rate of advance of periastron, ω = 0.00152(1) deg yr–1, and the orthometric Shapiro delay parameters, h3 = 0.89(7) µs and s = 0.88(2). Assuming general relativity, we obtain Mp = 1.71(2) M☉ for the mass of the pulsar and Mc = 0.254(2) M☉ for the mass of the companion; the orbital inclination is 83.2(4) degrees. Crucially, assuming that the position angle of the linear polarisation follows the RVM, we find that the spin axis has a misalignment relative to the orbital angular momentum of > 4.8deg at 99% confidence level.
Conclusions. While the value of Mp falls well within the wide range observed in eMSPs, Mc is significantly smaller than expected from several formation hypotheses proposed, which are therefore unlikely to be correct and can be ruled out; Mc is also significantly different from the expected value for an ideal low mass X-ray binary evolution scenario. If the misalignment between the spin axis of the pulsar and the orbital angular momentum is to be believed, it suggests that the unknown process that created the orbital eccentricity of the binary was also capable of changing its orbital orientation, an important evidence for understanding the origin of eMSPs.

Abstract Copyright: © ESO 2022

Journal keyword(s): stars: neutron - binaries: general - pulsars: individual: PSR J0955-6150

Simbad objects: 16

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Number of rows : 16
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 J0514-4002A Psr 05 14 06.6927 -40 02 48.897           ~ 69 1
2 MCG-02-24-007 LIN 09 18 05.66848602 -12 05 43.8060823   14.38 14.8     ~ 1077 1
3 PSR J0955-6150 Psr 09 55 20.847467 -61 50 16.89532           ~ 42 0
4 PSR J1007-6316 Psr 10 06 36.60 -63 11 41.2           ~ 8 0
5 PSR J1147-66 Psr 11 46 58.3731 -66 10 51.358           ~ 8 0
6 PSR J1618-3919 Psr 16 18 18.82500 -39 21 01.8320           ~ 32 0
7 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 16269 0
8 PSR J1807-2500B Psr 18 07 20.871209 -25 00 01.91500           ~ 64 0
9 PSR J1811-2405 Psr 18 11 19.854352 -24 05 18.42800           ~ 56 1
10 PSR J1823-3021G Psr 18 23 40.7213 -30 21 35.630           ~ 13 0
11 PSR J1835-3259A Psr 18 35 44.856 -32 59 25.08           ~ 22 0
12 PSR J1903+0327 Psr 19 03 05.7937 +03 27 19.222           ~ 187 1
13 PSR J1946+2052 Psr 19 46 14.1438633037 +20 52 24.333605451           ~ 65 0
14 PSR J1946+3417 Psr 19 46 25.13182 +34 17 14.6770           ~ 64 0
15 PSR J1950+2414 Psr 19 50 45.06390 +24 14 56.9638           ~ 34 0
16 PSR J2234+06 Psr 22 34 22 +06 11.0           ~ 76 0

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