2011MNRAS.413.2269S


Query : 2011MNRAS.413.2269S

2011MNRAS.413.2269S - Mon. Not. R. Astron. Soc., 413, 2269-2280 (2011/May-3)

On the nature of the `radio-quiet' black hole binaries.

SOLERI P. and FENDER R.

Abstract (from CDS):

The coupling between accretion processes and ejection mechanisms in accreting black holes in binary systems can be investigated by empirical relations between the X-ray/radio and X-ray/optical-infrared luminosities. These correlations are valid over several orders of magnitude and were initially thought to be universal. However, recently, many black hole binaries have been found to produce jets that, given certain accretion-powered luminosities, are fainter than expected from the earlier correlations. This shows that black holes with similar accretion flows can produce a broad range of outflows in power, suggesting that some other parameters or factors might be tuning the accretion–ejection coupling. Recent work has already shown that this jet power does not correlate with the reported black hole spin measurements. Here we discuss whether fixed parameters of the binary system (orbital period, disc size, inclination), as well as the properties of the outburst, produce any effect on the energy output in the jet. No obvious dependence is found. We also show that there is no systematic variation in the slope of the radio–X-ray correlation with normalization. We define a jet-toy model in which the bulk Lorentz factor becomes larger than ∼1 above ∼0.1 per cent of the Eddington luminosity. With this model, if we assume random inclination angles which result in highly variable boosting at large Eddington ratios, we are able to reproduce qualitatively the scatter of the X-ray–radio correlation and the `radio-quiet' population. However, the model seems to be at odds with some other observed properties of the systems. We also compare the `radio-quiet' black holes with the neutron stars. We show that if a mass correction from the Fundamental Plane is applied, the possibility that they are statistically indistinguishable in the X-ray–radio plane cannot be completely ruled out. This result suggests that some of the outliers could actually be neutron stars or that the disc–jet coupling in the `radio-quiet' black holes is more similar to the one in neutron stars.

Abstract Copyright: 2011 The Authors Monthly Notices of the Royal Astronomical Society2011 RAS

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

CDS comments: In Table 5 : 4U 1728-4 is a misprint for 4U 1728-34, 4U 0614-091 is a misprint for 4U 0614+091.

Simbad objects: 34

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Number of rows : 34
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 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 283 1
2 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184           M4.5V 670 0
3 V* V1055 Ori LXB 06 17 07.3565603963 +09 08 13.515857360   18.80 18.5     ~ 594 1
4 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
5 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
6 V* BW Cir HXB 13 58 09.7227337579 -64 44 05.257858491           ~ 256 0
7 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
8 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
9 V* QX Nor LXB 16 12 43.0 -52 25 26           ~ 946 1
10 V* V818 Sco LXB 16 19 55.0692669024 -15 38 25.017666540 11.60 12.40 11.1     Oev 1730 0
11 4U 1642-45 LXB 16 45 48.1 -45 36 42           ~ 467 1
12 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60           K4V 422 0
13 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
14 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 274 0
15 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
16 V* V1101 Sco LXB 17 05 44.4916006152 -36 25 23.049324480   20.10 18.6     ~ 473 0
17 V* V1228 Sco LXB 17 19 58.990 -31 45 01.11           ~ 122 1
18 NAME Slow Burster LXB 17 31 58.0 -33 49 58     15.50     ~ 865 1
19 NAME Rapid Burster LXB 17 33 24.0 -33 23 19           ~ 429 2
20 2E 3938 HXB 17 43 54.7 -29 44 44           ~ 693 1
21 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 805 0
22 2MAXI J1753-013 LXB 17 53 28.2898766424 -01 27 06.256555272 15.30 16.73 16.46 16.15 15.64 ~ 384 0
23 4U 1758-25 LXB 18 01 09.7308060816 -25 04 44.120221284     11.08     ~ 705 1
24 2CXO J180112.3-254436 HXB 18 01 12.4783119670 -25 44 35.694663099           AV 417 1
25 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
26 V* V5512 Sgr LXB 18 14 31.3 -17 09 23     12.73     K5III 449 0
27 V* NP Ser LXB 18 16 01.7 -14 02 09   18.8       K 683 2
28 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
29 V* MM Ser LXB 18 39 57.8 +05 02 13   19.2 19.2     ~ 378 0
30 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1
31 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
32 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
33 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0
34 V* V1341 Cyg LXB 21 44 41.1544345272 +38 19 17.066570988 15.00 15.13 14.68 15.00   A9III 1229 1

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