2022ApJ...929..137C


Query : 2022ApJ...929..137C

2022ApJ...929..137C - Astrophys. J., 929, 137-137 (2022/April-3)

Anatomy of Pulsar XTE J1829-098: Ultramassive SXFT with a Dominant Nondipolar Magnetic Field, or the Third Canonical HMXB Caught at the Bottom of the Corbet Gap?.

CHRISTODOULOU D.M., BHATTACHARYA S., LAYCOCK S.G.T. and KAZANAS D.

Abstract (from CDS):

The X-ray binary pulsar XTE J1829-098 has been observed at extremely low luminosities for its spin period of 7.8448 s. Although its distance is uncertain by a factor of 4, the lowest observed X-ray fluxes may not correspond to its minimal-accretion propeller state or to nonaccreting states occurring at even lower X-ray luminosities, in which case the source has been caught at the bottom of the Corbet gap. We analyze all proposed distances D to the binary and the lowest X-ray fluxes, and we find only two physically acceptable solutions: (a) For D = 4.5 kpc (if the companion is a main-sequence B0 star), the neutron star is canonical with mass 1.41 M☉, radius 10.1 km, and a purely dipolar magnetic field as indicated by a cyclotron absorption line detected at 15 keV. In this case, the source has been observed at the bottom of the Corbet gap, the third high-mass X-ray binary pulsar to be caught in this state after the "twins" 4U 0115+63 and V 0332+53 found by Tsygankov et al. (b) For D = 18 kpc (if the companion is a B0.5Ib supergiant), the neutron star is ultramassive with mass 2.62 M☉, radius 18.7 km, and a dominant nondipolar magnetic field Bmul = 1.26 TG (versus a dipolar component of only Bdip = 0.43 TG). In this case, the source has been observed in its propeller state.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Magnetic fields - Stellar accretion disks - X-ray binary stars

Simbad objects: 8

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Number of rows : 8
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 J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 GrW 190814 GWE 00 55.8 -27 05           ~ 433 0
3 V* V635 Cas HXB 01 18 31.9704955824 +63 44 33.072603144 17.05 16.64 15.19 14.34 13.22 B0.2Ve 791 0
4 V* BQ Cam HXB 03 34 59.9116110096 +53 10 23.296879776   17.16 15.42 14.26 13.04 O8.5Ve 525 1
5 [HP99] 946 Be* 05 20 30.9009 -69 31 54.999   14.41 14.40     O8e 72 0
6 GrW 170817 GWE 13 09 48.0850 -23 22 53.343           ~ 2683 0
7 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
8 2CXO J182943.9-095123 HXB 18 29 44.01 -09 51 23.0           ~ 44 1

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