2011A&A...534A.101C


Query : 2011A&A...534A.101C

2011A&A...534A.101C - Astronomy and Astrophysics, volume 534A, 101-101 (2011/10-1)

The 2008 outburst of IGR J17473-2721: evidence for a disk corona ?

CHEN Y.-P., ZHANG S., TORRES D.F., ZHANG S.-N., LI J., KRETSCHMAR P. and WANG J.-M.

Abstract (from CDS):

The 2008 outburst of the atoll source IGR J17473-2721 was observed by INTEGRAL, RXTE and Swift. Tens of type-I X-ray bursts were found in this outburst. Joint observations by INTEGRAL, RXTE, and Swift provide sufficient data to look into the behavior of IGR J17473-2721 at the rising part of the 2008 outburst. The relation between the duration of the bursts and the accretion rate and the nature of the corona producing the observed power-law component can therefore be studied in detail. We analyze observational data of IGR J17473-2721, focusing on the spectral evolution during the state transition from quiescent to low hard state (LHS), and on the flux dependence of the type-I X-ray bursts along the outburst. We find that the joint INTEGRAL, RXTE and Swift energy spectrum can be well fitted with a model composed of a blackbody and a cutoff power-law, with a cutoff energy decreasing from ∼150keV to ∼40keV as the source leaves the quiescent state toward the low hard state. This fits into a scenario in which the corona is cooled by the soft X-rays along the outburst evolution, as observed in several other atoll sources. Fifty-seven type-I bursts were reported in the 2008 outburst of IGR J17473-2721. By using the flux measured in the 1.5-30keV band, we find that the linear relationship between the burst duration and the flux still holds for those bursts that occur at the decaying part of the low hard state, but with a different slope than the overall one that was estimated with the bursts happening in the whole extent of, and for the rest of the low hard state. The significance of such a dichotomy in the type-I X-ray bursts is ∼3σ under an F-test. Similar results are hinted at as well with the broader energy-band that was adopted recently. This dichotomy may be understood in a scenario where part of the accreting material forms a corona on the way of falling onto the surface of the neutron star during the decaying part of the low hard state.Based on the accretion rates of the preceding LHS, estimated from type-I X-ray bursts and from persistent emission, at least for IGR J17473-2721, most of the accretion material may fall on the neutron star (NS) surface in the LHS. Considering the burst behavior in the context of the outburst indicates a corona formed on top of the disk rather than on the NS surface.

Abstract Copyright:

Journal keyword(s): X-rays: binaries - X-rays: bursts

Simbad objects: 16

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Number of rows : 16
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 V* V518 Per HXB 04 21 42.7227473352 +32 54 26.939156184 13.00 13.50 13.2     M4.5V 651 1
2 V* MM Vel HXB 10 13 36.4108035720 -45 04 32.553865524   14.84 14.71     G5V-M0V 198 0
3 V* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760     11.96     ~ 493 1
4 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000   17.95 16.6     K3III 1172 0
5 V* QX Nor LXB 16 12 43.0 -52 25 23           ~ 905 1
6 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 869 1
7 V* V1033 Sco HXB 16 54 00.137 -39 50 44.90   15.20 14.2 16.14   F5IV 1886 1
8 V* V821 Ara HXB 17 02 49.3876391280 -48 47 23.087954544 16.20 16.30 15.5     ~ 2078 0
9 V* V2293 Oph LXB 17 19 36.9201835128 -25 01 04.121601456   17.55 16.65     ~ 190 0
10 V* V2116 Oph Sy* 17 32 02.1532435416 -24 44 44.129169096   20.78 18.4     M6IIIe 692 1
11 [KRL2007b] 277 LXB 17 47 18.06 -27 20 38.9           ~ 78 0
12 GRO J1750-27 HXB 17 49 12.969 -26 38 38.93           Be? 70 1
13 4U 1758-25 LXB 18 01 09.7308060816 -25 04 44.120221284     11.08     ~ 655 1
14 2XMM J180112.4-254436 LXB 18 01 12.40 -25 44 36.1           ~ 391 1
15 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1136 1
16 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2627 0

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