2015MNRAS.454.1371W


Query : 2015MNRAS.454.1371W

2015MNRAS.454.1371W - Mon. Not. R. Astron. Soc., 454, 1371-1386 (2015/December-1)

Low-level accretion in neutron star X-ray binaries.

WIJNANDS R., DEGENAAR N., ARMAS PADILLA M., ALTAMIRANO D., CAVECCHI Y., LINARES M., BAHRAMIAN A. and HEINKE C.O.

Abstract (from CDS):

We search the literature for reports on the spectral properties of neutron star low-mass X-ray binaries when they have accretion luminosities between 1034 and 1036 erg/s, corresponding to roughly 0.01-1 percent of the Eddington accretion rate for a neutron star. We found that in this luminosity range the photon index (obtained from fitting a simple absorbed power law in the 0.5-10 keV range) increases with decreasing 0.5-10 keV X-ray luminosity (i.e. the spectrum softens). Such behaviour has been reported before for individual sources, but here we demonstrate that very likely most (if not all) neutron star systems behave in a similar manner and possibly even follow a universal relation. When comparing the neutron star systems with black hole systems, it is clear that most black hole binaries have significantly harder spectra at luminosities of 1034-1035 erg/s. Despite a limited number of data points, there are indications that these spectral differences also extend to the 1035-1036 erg/s range, but above a luminosity of 1035 erg/s the separation between neutron star and black hole systems is not as clear as below. In addition, the black hole spectra only become softer below luminosities of 1034 erg/s compared to 1036 erg/s for the neutron star systems. This observed difference between the neutron star binaries and black hole ones suggests that the spectral properties (between 0.5 and 10 keV) at 1034-1035 erg/s can be used to tentatively determine the nature of the accretor in unclassified X-ray binaries. More observations in this luminosity range are needed to determine how robust this diagnostic tool is and whether or not there are (many) systems that do not follow the general trend. We discuss our results in the context of properties of the accretion flow at low luminosities and we suggest that the observed spectral differences likely arise from the neutron star surface becoming dominantly visible in the X-ray spectra. We also suggest that both the thermal component and the non-thermal component might be caused by low-level accretion on to the neutron star surface for luminosities below a few times 1034 erg/s.

Abstract Copyright: © 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2015)

Journal keyword(s): accretion, accretion discs - binaries: close - X-rays: binaries

CDS comments: Probable misprints : AX J1548.3-5541 = AX J1538.3-5541, Swift J1753.5-0217 = Swift J1753.5-0127, XTE J1706-267 = XTE J1709-267.

Simbad objects: 44

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Number of rows : 44
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 267 1
2 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 822 0
3 CRTS J135716.8-093238 HXB 13 57 16.8357790008 -09 32 38.796487512           M4.5V 170 0
4 V* V822 Cen LXB 14 58 21.9347842080 -31 40 07.515432768 11.95 12.85 12.8     K3-K7V 544 0
5 AX J1538.3-5541 LXB 15 38 18.24 -55 56 16.8           ~ 11 0
6 V* KZ TrA LXB 16 32 16.79 -67 27 39.3 17.40 18.60 18.5     ~ 582 1
7 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1887 1
8 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 251 0
9 IGR J17062-6143 LXB 17 06 16.2820758768 -61 42 40.593758076           ~ 87 0
10 4U 1705-32 LXB 17 08 54.40 -32 18 57.5           ~ 59 0
11 RX J1709.5-2639 LXB 17 09 34 -26 39.9           ~ 122 0
12 RX J1718.4-4029 LXB 17 18 24.13 -40 29 30.4           ~ 43 0
13 XMMSL1 J171900.4-353217 X 17 19 00.4 -35 32 17           ~ 13 0
14 XTE J1719-291 XB* 17 19 16.970 -29 04 10.35           ~ 18 0
15 [KRL2007b] 241 LX? 17 28 38.97 -29 21 44.9           ~ 37 0
16 RX J1735.3-3540 LX? 17 35 23.0 -35 40 13           ~ 25 0
17 IGR J17361-4441 gam 17 36 17.418 -44 44 05.98           ~ 27 0
18 NGC 6388 GlC 17 36 17.461 -44 44 08.34           ~ 914 1
19 3FHL J1746.2-2852 LXB 17 44 33.09 -28 44 27.0           ~ 532 0
20 KS 1741-293 LXB 17 44 51.63 -29 20 42.8           ~ 102 0
21 2XMM J174502.1-285450 LXB 17 45 02.33 -28 54 49.7           ~ 133 0
22 AX J1745.6-2901 LXB 17 45 35.6400 -29 01 33.888           ~ 172 1
23 NAME Galactic Center reg 17 45 39.60213 -29 00 22.0000           ~ 14415 0
24 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 745 0
25 [KRL2007b] 275 LXB 17 47 02.60 -28 52 58.9     14.20     ~ 177 0
26 2XMM J174716.1-281047 LXB 17 47 16.17 -28 10 48.2           ~ 50 0
27 Cl Terzan 5 Cl* 17 48 05.00 -24 46 48.0           ~ 847 1
28 NAME TER 5 X-1 LXB 17 48 05.225 -24 46 47.66           ~ 217 1
29 MAXI J1747-249 LXB 17 48 05.3 -24 46 37           ~ 43 0
30 IGR J17494-3030 LXB 17 48 23.62 -30 29 59.0           ~ 28 0
31 [HAC2010] NGC 6440 X-2 LXB 17 48 52.76 -20 21 24.0           ~ 72 0
32 2XMM J174931.6-280805 LXB 17 49 31.940 -28 08 05.80           ~ 98 0
33 SAX J1750.8-2900 LXB 17 50 24.42 -29 02 15.4           ~ 139 0
34 2MAXI J1753-013 LXB 17 53 28.2898766424 -01 27 06.256555272 15.30 16.73 16.46 16.15 15.64 ~ 364 0
35 [OKM2018] SWIFT J1753.7-2382 LXB 17 53 31.896 -23 49 14.86           ~ 33 0
36 [KRL2007b] 294 LXB 17 54 14.60 -27 54 34.3           ~ 33 0
37 V* V4580 Sgr LXB 18 08 27.54 -36 58 44.3   16.81 16.51     ~ 984 0
38 IGR J18245-2452 LXB 18 24 32.50 -24 52 07.8           ~ 224 0
39 M 28 GlC 18 24 32.89 -24 52 11.4           ~ 770 0
40 V* V691 CrA LXB 18 25 46.8185061768 -37 06 18.529336656 14.30 15.20 15.1     ~ 436 0
41 2XMM J182833.7-103700 LXB 18 28 33.7753501392 -10 37 03.710934228           ~ 35 0
42 SWIFT J185003.2-005627 X 18 50 03.2 -00 56 27           ~ 20 0
43 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1136 1
44 2MAXI J1922-171 LXB 19 22 37.0 -17 17 03           ~ 36 0

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