2014MNRAS.445..290G


Query : 2014MNRAS.445..290G

2014MNRAS.445..290G - Mon. Not. R. Astron. Soc., 445, 290-300 (2014/November-3)

The radio/X-ray domain of black hole X-ray binaries at the lowest radio luminosities.

GALLO E., MILLER-JONES J.C.A., RUSSELL D.M., JONKER P.G., HOMAN J., PLOTKIN R.M., MARKOFF S., MILLER B.P., CORBEL S. and FENDER R.P.

Abstract (from CDS):

We report on deep, coordinated radio and X-ray observations of the black hole X-ray binary XTE J1118+480 in quiescence. The source was observed with the Karl G. Jansky Very Large Array for a total of 17.5 h at 5.3 GHz, yielding a 4.8±1.4 µJy radio source at a position consistent with the binary system. At a distance of 1.7 kpc, this corresponds to an integrated radio luminosity between 4 and 8x1025erg/s, depending on the spectral index. This is the lowest radio luminosity measured for any accreting black hole to date. Simultaneous observations with the Chandra X-ray Telescope detected XTE J1118+480 at 1.2x10–14erg/s/ cm2 (1-10 keV), corresponding to an Eddington ratio of ∼ 4x10–9 for a 7.5 M☉ black hole. Combining these new measurements with data from the 2005 and 2000 outbursts available in the literature, we find evidence for a relationship of the form ℓr = α+βℓX (where ℓ denotes logarithmic luminosities), with β = 0.72±0.09. XTE J1118+480 is thus the third system - together with GX339-4 and V404 Cyg - for which a tight, non-linear radio/X-ray correlation has been reported over more than 5 dex in ℓX. Confirming previous results, we find no evidence for a dependence of the correlation normalization of an individual system on orbital parameters, relativistic boosting, reported black hole spin and/or black hole mass. We then perform a clustering and linear regression analysis on what is arguably the most up-to-date collection of coordinated radio and X-ray luminosity measurements from quiescent and hard-state black hole X-ray binaries, including 24 systems. At variance with previous results, a two-cluster description is statistically preferred only for random errors ≲ 0.3 dex in both ℓr and ℓX, a level which we argue can be easily reached when the known spectral shape/distance uncertainties and intrinsic variability are accounted for. A linear regression analysis performed on the whole data set returns a best-fitting slope β = 0.61±0.03 and intrinsic scatter σ0 = 0.31±0.03 dex.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): accretion, accretion discs - black hole physics - methods: statistical - ISM: jets and outflows - radio continuum: general - X-rays: binaries

Simbad objects: 13

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Number of rows : 13
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 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
2 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
3 NVSS J111820+475659 rG 11 18 20.5503821040 +47 56 58.880413032           ~ 6 1
4 6C 112412+453344 Bla 11 26 57.6549321696 +45 16 06.283693704   17.66 17.51 17.01   ~ 88 1
5 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4558 2
6 CRTS J135716.8-093238 HXB 13 57 16.8357790008 -09 32 38.796487512           M4.5V 187 0
7 MAXI J1659-152 LXB 16 59 01.680 -15 15 28.73           ~ 274 0
8 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
9 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 805 0
10 MAXI J1836-194 XB* 18 35 43.440 -19 19 10.48           ~ 163 0
11 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
12 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0
13 NAME Cyg X Cld 20 30 04.7973633 +40 51 36.002197           ~ 962 1

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