2000ApJ...541..908B


Query : 2000ApJ...541..908B

2000ApJ...541..908B - Astrophys. J., 541, 908-917 (2000/October-1)

Coronal X-ray emission from the stellar companions to transiently accreting black holes.

BILDSTEN L. and RUTLEDGE R.E.

Abstract (from CDS):

Many neutron stars and black holes are in binaries where the mass transfer rate onto the compact object is highly variable. X-ray observations of these transients in quiescence (LX<1034 ergs.s–1) have found that the binaries harboring black holes are much fainter than those that contain a neutron star. Narayan and collaborators postulated that the faint X-ray emission from black hole binaries was powered by an advection- dominated accretion flow (ADAF). The subsequent ADAF modeling requires that an appreciable fraction of the constant Roche-lobe overflow into the outer disk proceeds into the black hole during ``quiescence''. A robust and nearly uniform quenching mechanism must then be hypothesized for the neutron star binaries, as comparably large accretion rates would lead to luminosities in excess of 1036 ergs.s–1 in quiescence. We explore an alternative explanation for the quiescent X-ray emission from the black hole systems: coronal emission from the rapidly rotating optical companion. This is commonly observed and well studied in other tidally locked binaries, such as the RS CVn, Algol, and By Dra systems. We show that two of the three X-ray detected black hole binaries (A0620-00 and GRO J1655-40) exhibit X-ray fluxes entirely consistent with coronal emission. The X-ray spectra of these objects should be best fitted with thermal Raymond-Smith models rich in lines when coronal emission predominates, a prediction that will be tested with Chandra and XMM-Newton observations. One black hole system (V404 Cyg) is too X-ray bright to be explained as coronal emission and remains a candidate for ADAFs in quiescence. The quiescent X-ray emission from all the neutron star binaries is far too bright for coronal emission. It might be that all soft X-ray transients have variable accretion rates in quiescence and that the basal quiescent X-ray flux is set by either coronal emission from the companion or–when present–by thermal emission from the neutron star. We have also searched for other indicators of coronal activity in these companion stars. For example, we show that the lithium abundances in the black hole systems are comparable to those in the RS CVns. Indeed, both the X-ray flux and lithium abundance from the K star in the binary V471 Tau match that of A0620-00. Though the production mechanisms for lithium in active coronae is still under debate, our work makes it clear that there is no longer a need for mechanisms that involve the compact object.

Abstract Copyright: ∼

Journal keyword(s): Accretion, Accretion Disks - Stars: Binaries: Close - Black Hole Physics - stars: individual (Aquila X-1, Centaurus X-4, 4U 1608-522, 4U 2129+47, A0620-00, GS 1124-68, GRO J1655-40, V404 Cygni, GS 2000+25, GRO J0422+32, 4U 1543-47, H1705-25) - X-Rays: Stars

Simbad objects: 21

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Number of rows : 21
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* HT Cas CV* 01 10 13.1213394144 +60 04 35.489642700     14.10     M5.5e 401 0
2 HD 22468 RS* 03 36 47.2904292073 +00 35 15.943692002 7.09 6.79 5.90     K2:Vnk 1206 0
3 Cl Melotte 22 OpC 03 46 38.0 +24 10 41           ~ 3679 0
4 V* V471 Tau SB* 03 50 24.9666549840 +17 14 47.430910716   10.258 9.373   8.393 K2V+DA 697 0
5 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184           M4.5V 670 0
6 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
7 NGC 2682 OpC 08 51 23.5 +11 48 54           ~ 2528 0
8 V* OY Car CV* 10 06 22.0793274312 -70 14 04.584660540           ~ 586 0
9 V* MM Vel HXB 10 13 36.3431303106 -45 04 31.128938218           G5V-M0V 211 1
10 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 734 1
11 HD 116160 PM* 13 21 41.6458462536 +02 05 14.060137272   5.732 5.687   5.64 A0V 79 0
12 V* V822 Cen LXB 14 58 21.9347842080 -31 40 07.515432768 11.95 12.85 12.8     K3-K7V 555 0
13 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
14 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
15 V* QX Nor LXB 16 12 43.0 -52 25 26           ~ 946 1
16 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
17 V* V2107 Oph HXB 17 08 14.5085716774 -25 05 30.159687978           K3V-K7V 235 0
18 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1
19 V* QZ Vul HXB 20 02 49.5220407111 +25 14 10.631666444           K3V-K6V 432 0
20 V* V404 Cyg HXB 20 24 03.8247037434 +33 52 01.961154861           G9/K0III/V 1370 0
21 V* V1727 Cyg LXB 21 31 26.2133156448 +47 17 24.512055396 16.75 17.05 16.4     ~ 250 0

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