2000MNRAS.312..151R


Query : 2000MNRAS.312..151R

2000MNRAS.312..151R - Mon. Not. R. Astron. Soc., 312, 151-158 (2000/February-2)

RXTE observations of Galactic microquasar XTE J1748-288 during its 1998 outburst.

REVNIVTSEV M.G., TRUDOLYUBOV S.P. and BOROZDIN K.N.

Abstract (from CDS):

We present an analysis of the RXTE observations of the recently discovered Galactic microquasar XTE J1748-288 during its 1998 outburst. General spectral and temporal properties of the source and their evolution were very typical for the Galactic black hole candidates (BHC) and, in particular, black hole X-ray novae.

The spectral evolution of the source during the outburst can be considered a sequence of qualitatively distinct states. During the first observations, corresponding to a maximum of the X-ray flux, the spectrum of the source consisted of a dominating hard power-law component and a soft thermal component, which can be described by a model for the multicolour-disc emission. The hard component contributed ≥80per cent to the X-ray luminosity in the 3-25keV energy band. Overall the two-component spectral shape is an attribute of the very high state observed previously in BHC, but the domination of the hard component is unusual. Later on, as the X-ray source faded, its energy spectrum qualitatively changed, showing high and then low states, both typical for black hole binaries.

As the energy spectrum changed, the fast variability also evolved dramatically. Initially the power-density spectrum was formed by a dominating band-limited noise component, quasi periodical oscillation features at 20-30Hz and at ∼0.5Hz, and a very low-frequency noise component. After a significant decrease of the contribution of the hard spectral component, the amplitude of the fractional variability decreased by an order of magnitude and the power-density spectrum adopted a power-law shape with a broad quasi periodical oscillation peak around 0.03Hz. When the system switched to the low state, the power-density spectrum shape changed again and the quasi periodical oscillations have not been detected since.

When the source was observed in the very high state, a clear correlation between quasi periodical oscillation parameters and X-ray flux was seen. Such a correlation gives an insight into our understanding of the accretion process in X-ray black hole binaries.


Abstract Copyright: 2000, Royal Astronomical Society

Journal keyword(s): black hole physics - binaries: general - stars: individual: XTE J1748-288 - novae, cataclysmic variables - X-rays: general

Errata: Erratum vol. 315, p. 655 (2000)

Simbad objects: 18

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Number of rows : 18
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 X LMC X-1 HXB 05 39 38.8284304464 -69 44 35.531553624   14.8 14.5 14.924   O8(f)p 700 0
3 1A 0620-00 HXB 06 22 44.5423857312 -00 20 44.290460544           K3V-K7V 1144 0
4 V* MM Vel HXB 10 13 36.3431303106 -45 04 31.128938218           G5V-M0V 211 1
5 V* GU Mus HXB 11 26 26.5961559600 -68 40 32.877752952           K3V-K7V 734 1
6 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
7 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
8 GRS G175.80 -25.80 Rad 17 09 -25.9           ~ 4 0
9 AX J1733.9-3112 LXB 17 33 32.00 -31 13 00.0           ~ 54 0
10 V* V2606 Oph CV* 17 42 40.030 -27 44 52.70     23.2     ~ 163 0
11 2E 3938 HXB 17 43 54.7 -29 44 44           ~ 693 1
12 X Sgr X-1 LXB 17 47 56.3 -26 33 47           ~ 402 0
13 AX J1748.0-2829 LXB 17 48 05.060 -28 28 25.80     13.60     ~ 189 0
14 4U 1758-25 LXB 18 01 09.7308060816 -25 04 44.120221284     11.08     ~ 705 1
15 2S 1803-245 LXB 18 06 50.72 -24 35 28.6           ~ 84 0
16 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
17 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
18 V* QZ Vul HXB 20 02 49.5220407111 +25 14 10.631666444           K3V-K6V 432 0

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