2001MNRAS.324..923F


Query : 2001MNRAS.324..923F

2001MNRAS.324..923F - Mon. Not. R. Astron. Soc., 324, 923-930 (2001/July-2)

On the peak radio and X-ray emission from neutron star and black hole candidate X-ray transients.

FENDER R.P. and KUULKERS E.

Abstract (from CDS):

We have compiled and analysed reports from the literature of (quasi-)simultaneous observations of X-ray transients at radio and X-ray wavelengths and compared them with each other and with more unusual radio-bright sources such as Cygnus X-3, GRS 1915+105 and Circinus X-1. There exists a significant (>97 per cent likelihood) positive (rank) correlation between the peak X-ray flux PX and radio flux density PR for the black hole candidate (BHC) systems, and a marginally significant positive (rank) correlation for the neutron star (NS) systems. This is further evidence for a coupling between accretion and outflows in X-ray binary systems, in this case implying a relation between peak disc-accretion rate and the number of synchrotron-emitting electrons ejected. However, we also show that the distribution of `radio loudness', PR/PX, is significantly different for the two samples, in the sense that the BHCs generally have a higher PR/PX ratio. The origin of this discrepancy is uncertain, but probably reflects differences in the energetics and/or radiative efficiency of flows around the neutron stars and black holes; we briefly discuss some of these possibilities. Furthermore, the data for the two recently discovered `fast transients' (FTs), XTE J0421+560/CI Cam and SAX J1819.3-2525/V4641 Sgr are entirely compatible with the distribution of BHCs. As at least three of the BHCs and both FTs have been directly resolved into mildly relativistic jets, it seems likely that such outflows are the origin of the radio emission in all BHC and FT transients, and probably also for the NS transients. We further note that the range of X-ray and radio fluxes observed from the unusual superluminal source GRS 1915+105 is also entirely compatible with the distribution for transients, implying that there is nothing special about the physics of jet formation in that system. We conclude that these data point to the formation of a mildly relativistic jet whose luminosity is a function of the accretion rate in the majority, if not all, X-ray transient outbursts, but whose relation to the observed X-ray emission is dependent on the nature of the accreting compact object.

Abstract Copyright: The Royal Astronomical Society

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

Simbad objects: 31

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Number of rows : 31
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* CI Cam HXB 04 19 42.1355996520 +55 59 57.706599192 12.13 12.41 11.77 10.79 9.99 B0/2I[e] 271 0
2 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184           M4.5V 670 0
3 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
4 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
5 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 734 1
6 V* BW Cir HXB 13 58 09.7227337579 -64 44 05.257858491           ~ 256 0
7 V* V822 Cen LXB 14 58 21.9347842080 -31 40 07.515432768 11.95 12.85 12.8     K3-K7V 555 0
8 V* BR Cir HXB 15 20 40.8532547060 -57 10 00.206639033   21.4 21.4     B5-A0I 849 1
9 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
10 X Nor X-1 LXB 16 34 01.610 -47 23 34.80           ~ 579 0
11 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
12 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
13 V* V2293 Oph LXB 17 19 36.9201835128 -25 01 04.121601456   17.55 16.65     ~ 208 0
14 NAME Rapid Burster LXB 17 33 24.0 -33 23 19           ~ 429 2
15 V* V2606 Oph CV* 17 42 40.030 -27 44 52.70     23.2     ~ 163 0
16 AX J1745.6-2901 LXB 17 45 35.6400 -29 01 33.888           ~ 191 1
17 1A 1742-289 X 17 45 37.1832 -29 01 04.656           ~ 93 1
18 MXB 1743-29 LXB 17 45 47 -29 17.2           ~ 54 2
19 AX J1748.0-2829 LXB 17 48 05.060 -28 28 25.80     13.60     ~ 189 0
20 INTREF 866 LXB 17 55 28.6 -32 28 39     10.79     ~ 46 0
21 2S 1803-245 LXB 18 06 50.72 -24 35 28.6           ~ 84 0
22 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
23 V* V4641 Sgr HXB 18 19 21.6343259256 -25 24 25.849595952     13.654 13.479 13.139 B9III 530 0
24 V* V406 Vul HXB 18 58 41.49127200 +22 39 29.7746640           G5V-K0V 409 0
25 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1
26 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
27 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
28 V* QZ Vul HXB 20 02 49.5220407111 +25 14 10.631666444           K3V-K6V 432 0
29 INTREF 1012 LXB 20 12 37.7592785736 +38 11 00.770922096     21.33     ~ 78 0
30 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0
31 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 2035 2

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