2018RAA....18..128C


Query : 2018RAA....18..128C

2018RAA....18..128C - Research in Astron. and astroph., 18, 128-128 (2018/October-0)

A striking confluence between theory and observations of high-mass X-ray binary pulsars.

CHRISTODOULOU D., LAYCOCK S. and KAZANAS D.

Abstract (from CDS):

We analyze the most powerful X-ray outbursts from neutron stars in eleven Magellanic high-mass X-ray binaries and three pulsating ultraluminous X-ray sources. Most of the outbursts rise to $L_max$ which is about the level of the Eddington luminosity, while the remaining more powerful outbursts also appear to recognize that limit when their emissions are assumed to be anisotropic and beamed toward our direction. We use the measurements of pulsar spin periods $P_S$ and their derivatives ${dot}P_S$ to calculate the X-ray luminosities $L_p$ in their faintest accreting ("propeller-line") states. In five cases with unknown ${dot}P_S$, we use the lowest observed X-ray luminosities, which only adds to the heterogeneity of the sample. Then we calculate the ratios $L_p/L_max$ and we obtain an outstanding confluence of theory and observations from which we conclude that work done on both fronts is accurate and the results are trustworthy: sources known to reside on the lowest Magellanic propeller line are all located on/near that line, whereas other sources jump higher and reach higher-lying propeller lines. These jumps can be interpreted in only one way, higher-lying pulsars have stronger surface magnetic fields in agreement with previous empirical results in which ${dot}P_S$ and $L_p$ values were not used.

Abstract Copyright: ∼

Journal keyword(s): accretion, accretion disks - stars: magnetic fields - stars: neutron - X-rays: binaries

Simbad objects: 14

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Number of rows : 14
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 SXP 4.78 HXB 00 51 38.7742234656 -72 17 04.796861748 14.63 15.66 15.63   15.44 B0V-B1Ve 55 0
2 LIN 198 HXB 00 52 05.6251611744 -72 26 04.228773036 13.86 14.91 14.927 14.91 14.794 B0-5(II)e 187 0
3 LIN 203 HXB 00 52 13.9956976512 -73 19 18.812945496   14.66 14.67   14.534 O9.5IIIe/B0Ve 93 0
4 X SMC X-2 HXB 00 54 33.43 -73 41 01.3 13.77 16.40 16.38   14.67 O9.5III-V 143 0
5 SXP 5.05 HXB 00 57 02.1884332608 -72 25 55.431870600 14.77 15.76 15.993   15.960 B0.5e 42 0
6 SXP 6.85 HXB 01 02 53.3180253744 -72 44 35.166214716   14.51 14.59     O9.5-B0IV-V 66 0
7 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 918 0
8 AzV 503 HXB 01 21 40.6223488848 -72 57 30.906717444   14.23 14.3     B0-5(II)e 48 0
9 CAL E HXB 05 02 51.7474501824 -66 26 26.907946008   14.12 14.22 14.359   O9.5/B0III/Ve 37 0
10 [HP99] 946 Be* 05 20 30.9009 -69 31 54.999   14.41 14.40     O8e 72 0
11 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0 14.290   O8III 714 0
12 [KCF2005] M82 G ULX 09 55 51.040 +69 40 45.49           ~ 284 1
13 NAME NGC 5907 ULX ULX 15 15 58.60 +56 18 10.0           ~ 180 0
14 NAME NGC 7793 P13 ULX 23 57 50.90 -32 37 26.6           ~ 225 0

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