2000MNRAS.317....1F


Query : 2000MNRAS.317....1F

2000MNRAS.317....1F - Mon. Not. R. Astron. Soc., 317, 1-8 (2000/September-1)

The radio luminosity of persistent X-ray binaries.

FENDER R.P. and HENDRY M.A.

Abstract (from CDS):

We summarize all the reported detections of, and upper limits to, the radio emission from persistent (i.e. non-transient) X-ray binaries. A striking result is a common mean observed radio luminosity from the black hole candidates (BHCs) in the low/hard X-ray state and the neutron star Z sources on the horizontal X-ray branch. This implies a common mean intrinsic radio luminosity to within a factor of 25 (or less, if there is significant Doppler boosting of the radio emission). Unless coincidental, these results imply a physical mechanism for jet formation that requires neither a black hole event horizon nor a neutron star surface. As a whole the populations of Atoll and X-ray pulsar systems are less luminous by factors of ≳5 and ≳10 at radio wavelengths than the BHCs and Z sources (while some Atoll sources have been detected, no high-field X-ray pulsar has ever been reliably detected as a radio source). We suggest that all of the persistent BHCs and the Z sources generate, at least sporadically, an outflow with physical dimensions ≥1012cm; that is, significantly larger than the binary separations of most of the systems. We compare the physical conditions of accretion in each of the types of persistent X-ray binary and conclude that a relatively low (≤1010G) magnetic field associated with the accreting object, and a high (≥0.1 Eddington) accretion rate and/or dramatic physical change in the accretion flow, are required for formation of a radio-emitting outflow or jet.

Abstract Copyright: 2000, Royal Astronomical Society

Journal keyword(s): binaries: close - ISM: jets and outflows - radio continuum: stars

Simbad objects: 51

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Number of rows : 51
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 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11152 1
2 SK 160 HXB 01 17 05.1457288392 -73 26 36.014808156 12.23 13.00 13.15   13.17 O9.7Ia+ 858 0
3 V* V635 Cas HXB 01 18 31.9704955824 +63 44 33.072603144 17.05 16.64 15.19 14.34 13.22 B0.2Ve 744 0
4 V* X Per HXB 03 55 23.0777456088 +31 02 45.039836148 6.090 6.840 6.720     O9.5III 978 0
5 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17438 0
6 X LMC X-4 HXB 05 32 49.5556042296 -66 22 13.202721768   13.9 14.0     O8III 669 0
7 RX J0535.6-6651 HXB 05 35 40.9970566152 -66 51 53.547559416   13.7 13.8     B0.5IIIe 287 0
8 X LMC X-3 HXB 05 38 56.6323605504 -64 05 03.317937504   17 17.2     B2.5Ve 675 0
9 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5     O8(f)p 640 2
10 Ginga 0834-430 HXB 08 35 54.9956514920 -43 11 17.497095048     20.4     B0-2III-Ve 104 0
11 V* GP Vel HXB 09 02 06.8608812864 -40 33 16.899168060 6.85 7.37 6.87 6.31 6.05 B0.5Ia 1505 0
12 2E 2336 HXB 10 50 08.93 -59 53 19.9           Be 405 0
13 WRAY 15-793 HXB 11 20 57.1736884968 -61 55 00.166078020 12.81 13.06 12.12     O9.5III/Ve 208 0
14 V* V779 Cen HXB 11 21 15.0920532528 -60 37 25.630264596   14.4 12.27     O9III/Veq 1098 0
15 1E 1145.1-6141 HXB 11 47 28.5598257552 -61 57 13.426997544   13.08       B2Iae 149 0
16 HD 102567 HXB 11 48 00.0214464120 -62 12 24.902384760 8.24 9.06 9.00 9.62   B1Vne 319 0
17 V* BP Cru HXB 12 26 37.5605188992 -62 46 13.261044684   12.482 10.803 10.304   B1Ia+ 688 0
18 1H 1238-599 HXB 12 42 01.7 -60 12 06     13.80     ~ 32 0
19 4U 1416-62 HXB 14 21 12.1560262026 -62 41 56.089360085   17.9 17.2     B1:V:e 156 0
20 V* BR Cir HXB 15 20 40.8532547060 -57 10 00.206639033   21.4 21.4     ~ 781 1
21 V* QX Nor LXB 16 12 43.0 -52 25 23           ~ 905 1
22 V* V818 Sco LXB 16 19 55.0692669024 -15 38 25.017666540 11.60 12.40 11.1     Oev 1643 0
23 V* KZ TrA LXB 16 32 16.79 -67 27 39.3 17.40 18.60 18.5     ~ 582 1
24 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 870 1
25 4U 1642-45 LXB 16 45 47.7 -45 36 40     14.30     ~ 417 1
26 V* HZ Her LXB 16 57 49.8110126616 +35 20 32.486555472 11.90 14.89 13.63 13.88   B3/6ep 2076 0
27 NAME OAO 1657-41 HXB 17 00 48.884 -41 39 21.46           Ofpe/WN9 248 0
28 V* V821 Ara HXB 17 02 49.3876391280 -48 47 23.087954544 16.20 16.30 15.5     ~ 2079 0
29 V* V1101 Sco LXB 17 05 44.4916006152 -36 25 23.049324480   20.10 18.6     ~ 439 0
30 X Ara X-1 LXB 17 06 15.314 -43 02 08.69           ~ 268 1
31 4U 1705-44 LXB 17 08 54.470 -44 06 07.35           ~ 389 0
32 V* V2216 Oph LXB 17 31 44.17 -16 57 40.9 16.40 17.10 16.8     ~ 293 1
33 NAME Slow Burster LXB 17 31 57.73 -33 50 02.5     15.50     ~ 824 1
34 V* V2116 Oph Sy* 17 32 02.1532435416 -24 44 44.129169096   20.78 18.4     M6IIIe 692 1
35 V* V926 Sco LXB 17 38 58.2384053021 -44 27 00.699118812 16.90 17.70 17.5     ~ 456 0
36 NAME Great Annihilator LXB 17 43 54.83 -29 44 42.6           ~ 674 1
37 X Sgr X-1 LXB 17 47 56.0 -26 33 49           ~ 375 0
38 4U 1758-25 LXB 18 01 09.7308060816 -25 04 44.120221284     11.08     ~ 655 1
39 2XMM J180112.4-254436 LXB 18 01 12.40 -25 44 36.1           ~ 392 1
40 X Sgr X-3 LXB 18 01 32.3 -20 31 44           ~ 235 1
41 V* V4580 Sgr LXB 18 08 27.54 -36 58 44.3   16.81 16.51     ~ 984 0
42 V* V5512 Sgr LXB 18 14 31.55 -17 09 26.7     12.73     K5III 392 0
43 V* NP Ser LXB 18 16 01.389 -14 02 10.62   18.8       K 642 2
44 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 992 1
45 V* MM Ser LXB 18 39 57.56 +05 02 09.6   19.2 19.2     ~ 349 0
46 4U 1850-086 LXB 18 53 04.89 -08 42 19.7 20.40 21.20 21.0     ~ 252 1
47 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A3/7I 2124 4
48 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2628 0
49 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4337 0
50 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 1940 2
51 V* V1341 Cyg LXB 21 44 41.1544345272 +38 19 17.066570988 15.00 15.13 14.68 15.00   A9III 1155 1

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