2016ApJ...829L..22S


Query : 2016ApJ...829L..22S

2016ApJ...829L..22S - Astrophys. J., 829, L22-L22 (2016/October-1)

Stronger reflection from black hole accretion disks in soft X-ray states.

STEINER J.F., REMILLARD R.A., GARCIA J.A. and McCLINTOCK J.E.

Abstract (from CDS):

We analyze 15,000 spectra of 29 stellar-mass black hole (BH) candidates collected over the 16 year mission lifetime of Rossi X-ray Timing Explorer using a simple phenomenological model. As these BHs vary widely in luminosity and progress through a sequence of spectral states, which we broadly refer to as hard and soft, we focus on two spectral components: the Compton power law and the reflection spectrum it generates by illuminating the accretion disk. Our proxy for the strength of reflection is the equivalent width of the Fe-K line as measured with respect to the power law. A key distinction of our work is that for all states we estimate the continuum under the line by excluding the thermal disk component and using only the component that is responsible for fluorescing the Fe-K line, namely, the Compton power law. We find that reflection is several times more pronounced (∼3) in soft compared to hard spectral states. This is most readily caused by the dilution of the Fe line amplitude from Compton scattering in the corona, which has a higher optical depth in hard states. Alternatively, this could be explained by a more compact corona in soft (compared to hard) states, which would result in a higher reflection fraction.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): accretion, accretion disks - black hole physics - X-rays: binaries - X-rays: binaries

Simbad objects: 30

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Number of rows : 30
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 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
2 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 722 0
3 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
4 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
5 V* BW Cir HXB 13 58 09.7227337579 -64 44 05.257858491           ~ 256 0
6 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
7 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
8 X Nor X-1 LXB 16 34 01.610 -47 23 34.80           ~ 579 0
9 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60           K4V 422 0
10 XTE J1652-453 XB* 16 52 20.330 -45 20 39.99           ~ 56 1
11 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
12 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 274 0
13 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
14 IGR J17091-3624 LXB 17 09 07.61 -36 24 25.7           ~ 320 1
15 V* V1228 Sco LXB 17 19 58.990 -31 45 01.11           ~ 122 1
16 V* V2606 Oph CV* 17 42 40.030 -27 44 52.70     23.2     ~ 163 0
17 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 805 0
18 AX J1748.0-2829 LXB 17 48 05.060 -28 28 25.80     13.60     ~ 189 0
19 RX J1749.8-3312 LXB 17 49 48.940 -33 12 11.60           ~ 64 0
20 XTE J1752-223 LXB 17 52 15.090 -22 20 32.36           ~ 229 0
21 2MAXI J1753-013 LXB 17 53 28.2898766424 -01 27 06.256555272 15.30 16.73 16.46 16.15 15.64 ~ 384 0
22 [KRL2007b] 312 LXB 18 17 43.537 -33 01 07.80           ~ 177 0
23 XTE J1818-245 LXB 18 18 24.430 -24 32 17.96           ~ 43 0
24 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654 13.479 13.139 B9III 530 0
25 MAXI J1836-194 XB* 18 35 43.440 -19 19 10.48           ~ 163 0
26 V* V406 Vul HXB 18 58 41.49127200 +22 39 29.7746640           G5V-K0V 409 0
27 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
28 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
29 V* V1408 Aql LXB 19 59 24.0074252040 +11 42 29.859773292 18.40 18.97 18.95 18.70 18.66 ~ 234 0
30 INTREF 1012 LXB 20 12 37.7592785736 +38 11 00.770922096     21.33     ~ 78 0

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