2010MNRAS.409..763V


Query : 2010MNRAS.409..763V

2010MNRAS.409..763V - Mon. Not. R. Astron. Soc., 409, 763-776 (2010/December-1)

Is the plateau state in GRS 1915+105 equivalent to canonical hard states ?

VAN OERS P., MARKOFF S., RAHOUI F., MAITRA D., NOWAK M., WILMS J., CASTRO-TIRADO A.J., RODRIGUEZ J., DHAWAN V. and HARLAFTIS E.

Abstract (from CDS):

GRS 1915+105 is a very peculiar black hole binary that exhibits accretion-related states that are not observed in any other stellar-mass black hole system. One of these states, however - referred to as the plateau state - may be related to the canonical hard state of black hole X-ray binaries. Both the plateau and hard state are associated with steady, relatively lower X-ray emission and flat/inverted radio emission, that is sometimes resolved into compact, self-absorbed jets. However, while generally black hole binaries quench their jets when the luminosity becomes too high, GRS 1915+105 seems to sustain them despite the fact that it accretes at near- or super-Eddington rates. In order to investigate the relationship between the plateau and the hard state, we fit two multiwavelength observations using a steady-state outflow-dominated model, developed for hard-state black hole binaries. The data sets consist of quasi-simultaneous observations in radio, near-infrared and X-ray bands. Interestingly, we find both significant differences between the two plateau states, as well as between the best-fitting model parameters and those representative of the hard state. We discuss our interpretation of these results, and the possible implications for GRS 1915+105's relationship to canonical black hole candidates.

Abstract Copyright: © 2010 The Authors. Journal compilation © 2010 RAS

Journal keyword(s): accretion, accretion discs - black hole physics - radiation mechanisms: general - galaxies: active - galaxies: jets - X-rays: binaries

Simbad objects: 15

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Number of rows : 15
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 3C 48 QSO 01 37 41.2996631208 +33 09 35.080388820   16.62 16.20     ~ 2815 2
2 M 1 SNR 05 34 30.9 +22 00 53           ~ 6192 1
3 V* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5260 0
4 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544 10.60 11.40 11.2     K3V-K7V 1113 0
5 M 81 Sy2 09 55 33.1726556496 +69 03 55.062505368   7.89 6.94     ~ 4450 3
6 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120     12.25     K5V-M1V 822 0
7 3C 286 Sy1 13 31 08.2883506368 +30 30 32.960091564   17.51 17.25     ~ 4341 2
8 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1887 1
9 V* V821 Ara HXB 17 02 49.3876391280 -48 47 23.087954544 16.20 16.30 15.5     ~ 2079 0
10 * 10 Aql a2* 18 58 46.9240671288 +13 54 23.941711692 6.23 6.14 5.89     A7VpSrEu_Ksn 285 0
11 GAL 045.5+00.0 HII 19 14 20.8 +11 09 04           ~ 139 0
12 CORNISH G045.4545+00.0591 HII 19 14 21.31 +11 09 11.7           ~ 154 1
13 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2628 0
14 NVSS J192234+153010 Rad 19 22 34.69936025 +15 30 10.0326112           ~ 60 0
15 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4337 0

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