2012ApJ...756...85S


Query : 2012ApJ...756...85S

2012ApJ...756...85S - Astrophys. J., 756, 85 (2012/September-1)

Formation of millisecond pulsars from intermediate- and low-mass X-ray binaries.

SHAO Y. and LI X.-D.

Abstract (from CDS):

We present a systematic study of the evolution of intermediate- and low-mass X-ray binaries consisting of an accreting neutron star of mass 1.0-1.8 M☉ and a donor star of mass 1.0-6.0 M☉. In our calculations we take into account physical processes such as unstable disk accretion, radio ejection, bump-induced detachment, and outflow from the L2point. Comparing the calculated results with the observations of binary radio pulsars, we report the following results. (1) The allowed parameter space for forming binary pulsars in the initial orbital period-donor mass plane increases with increasing neutron star mass. This may help explain why some millisecond pulsars with orbital periods longer than ∼60 days seem to have less massive white dwarfs than expected. Alternatively, some of these wide binary pulsars may be formed through mass transfer driven by planet/brown-dwarf-involved common envelope evolution. (2) Some of the pulsars in compact binaries might have evolved from intermediate-mass X-ray binaries with anomalous magnetic braking. (3) The equilibrium spin periods of neutron stars in low-mass X-ray binaries are in general shorter than the observed spin periods of binary pulsars by more than one order of magnitude, suggesting that either the simple equilibrium spin model does not apply or there are other mechanisms/processes spinning down the neutron stars.

Abstract Copyright: ∼

Journal keyword(s): binaries: general - pulsars: general - stars: neutron - X-rays: binaries

Simbad objects: 19

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Number of rows : 19
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 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
2 WD 0137-349 WD* 01 39 42.8531929464 -34 42 39.577891392 14.60 15.33 15.30     DA3 101 0
3 PSR J0218+42 Psr 02 18 06.3604 +42 32 17.365           ~ 365 2
4 PSR B0655+64 Psr 07 00 37.802 +64 18 11.20           ~ 250 1
5 PSR J0823+0159 Psr 08 23 09.78731 +01 59 12.6003           DA 244 0
6 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1588 0
7 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
8 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1159 0
9 PSR B1257+12 Psr 13 00 03.1075 +12 40 55.155           ~ 546 1
10 PSR J1435-60 Psr 14 35 20.2733756922 -61 00 57.545079751           ~ 58 1
11 V* QV Nor HXB 15 42 23.3633146128 -52 23 09.577395960   16.3 14.5     B0.2Ia 455 1
12 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
13 V* KZ TrA LXB 16 32 16.79 -67 27 39.3 17.40 18.60 18.5     ~ 626 1
14 PSR J1640+2224 Psr 16 40 16.744850 +22 24 08.84119           ~ 210 0
15 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2172 0
16 PSR J1756-5322 Psr 17 57 15.154960 -53 22 26.59604           ~ 56 0
17 PSR J1802-2124 Psr 18 02 05.334393 -21 24 03.67600           ~ 101 1
18 PSR J1841+0130 Psr 18 41 17.761 +01 30 19.60           ~ 16 1
19 PSR J1952+2630 Psr 19 52.6 +26 30           ~ 44 0

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