2010MNRAS.403...61D


Query : 2010MNRAS.403...61D

2010MNRAS.403...61D - Mon. Not. R. Astron. Soc., 403, 61-82 (2010/March-3)

A global spectral study of black hole X-ray binaries.

DUNN R.J.H., FENDER R.P., KORDING E.G., BELLONI T. and CABANAC C.

Abstract (from CDS):

We report on a consistent and comprehensive spectral analysis of the X-ray emission of 25 black hole X-ray binaries. All publicly available observations of the black hole binaries in the RXTE archive were analysed. Three different types of model were fitted to investigate the spectral changes occurring during an outburst. For the population, as well as for each binary and each outburst from each binary, we construct two diagnostic diagrams. The hardness intensity/luminosity diagram (HID/HLD), the X-ray colour against the flux/luminosity of the binary, is most useful when studying a single binary. However, to compare different binary systems, the disc fraction luminosity diagram (DFLD) is more useful. The DFLD uses the luminosities of the disc and power-law components to calculate the ratio of the disc luminosity to the total luminosity, resulting in a more physical value, which is analogous to the X-ray colour calculated for X-ray binaries. The tracks of the outbursts populate the DFLD more evenly than the HLD. We discuss the limitations of both diagnostic diagrams for the study of the X-ray binary outbursts and clearly illustrate how the two diagrams map on to each other for real outburst data. The similarity of the X-ray colour and disc fraction behaviour over time during an outburst originally seen in GX 339-4 data is seen in other sources' outbursts. We extract the peak luminosities in a single outburst, as well as the luminosities at the transitions away from and returning to the power-law-dominated state for each outburst. The distribution of the luminosities at the transition from the power-law to the disc-dominated state peaks at around 0.3LEdd, the same as the peak of the distribution of the peak luminosities in an outburst. Using the disc fraction to calculate the transition luminosities shows that the distributions of the luminosities for the transitions away from and returning to the power-law-dominated state are both broad and appear to overlap. Using the change in disc fraction to calculate the date when a transition occurred is not drastically different from obtaining the dates from changes in the timing behaviour of the X-ray binary. In addition, we calculate the rate of motion of an X-ray binary through the DFLD during an outburst, a diagnostic which has the potential to be used as a comparison with populations of active galactic nuclei. The fastest rate of motion is on the egress and ingress from the power-law-dominated state. A further region of increased speed through the diagram occurs in the disc-dominated state on the return to the power-law-dominated state. Finally, we compare the measured X-ray luminosities with a small number of contemporaneous radio measurements. Overall, this is the most comprehensive and uniform global study of black hole X-ray binaries to date.

Abstract Copyright: © 2010 The Authors. Journal compilation © 2010 RAS

Journal keyword(s): accretion, accretion discs - binaries: general - ISM: jets and outflows - X-rays: binaries

Simbad objects: 27

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Number of rows : 27
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 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 677 0
2 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5     O8(f)p 643 2
3 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 824 0
4 V* BW Cir HXB 13 58 09.700 -64 44 05.80 17.90 18.00 16.9     ~ 239 1
5 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760     11.96     ~ 496 1
6 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000   17.95 16.6     K3III 1176 0
7 X Nor X-1 LXB 16 34 01.610 -47 23 34.80           ~ 522 0
8 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60     11.89     K4V 398 0
9 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1889 1
10 V* V821 Ara HXB 17 02 49.3876391280 -48 47 23.087954544 16.20 16.30 15.5     ~ 2091 0
11 SAX J1711.6-3808 XB* 17 11 37.1 -38 07 06           ~ 44 0
12 V* V1228 Sco LXB 17 19 58.990 -31 45 01.11           ~ 115 1
13 AX J1740.1-3102 X 17 40 09.000 -31 02 24.00           ~ 40 1
14 V* V2606 Oph CV* 17 42 40.030 -27 44 52.70     23.2     ~ 151 0
15 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 747 0
16 AX J1748.0-2829 LXB 17 48 05.060 -28 28 25.80     13.60     ~ 184 0
17 RX J1749.8-3312 LXB 17 49 48.940 -33 12 11.60           ~ 59 0
18 INTREF 866 LXB 17 55 28.6 -32 28 39     10.79     ~ 42 0
19 2XMM J180112.4-254436 LXB 18 01 12.40 -25 44 36.1           ~ 393 1
20 [KRL2007b] 312 LXB 18 17 43.537 -33 01 07.80           ~ 171 0
21 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654   13.092 B9III 476 1
22 V* V406 Vul HXB 18 58 41.580 +22 39 29.40 15.00 15.65 15.31     G5V-K0V 380 0
23 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4350 0
24 V* V1408 Aql LXB 19 59 24.0074252040 +11 42 29.859773292 18.40 18.97 18.95 18.70 18.66 ~ 201 0
25 INTREF 1012 LXB 20 12 37.7592785736 +38 11 00.770922096     21.33     ~ 72 0
26 V* V404 Cyg HXB 20 24 03.8254458776 +33 52 01.962185735           G9/K0III/V 1278 0
27 NAME Galactic Ridge ? ~ ~           ~ 500 1

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