2013ApJ...767..160T


Query : 2013ApJ...767..160T

2013ApJ...767..160T - Astrophys. J., 767, 160 (2013/April-3)

Spectral state evolution of 4U 1820-30: the stability of the spectral index of the comptonization tail.

TITARCHUK L., SEIFINA E. and FRONTERA F.

Abstract (from CDS):

We analyze the X-ray spectra and their timing properties of the compact X-ray binary 4U 1820-30. We establish spectral transitions in this source seen with BeppoSAX and the Rossi X-ray Timing Explorer (RXTE). During the RXTE observations (1996-2009), the source was in the soft state approximately ∼75% of the time making the lower banana and upper banana transitions combined with long-term low-high state transitions. We reveal that all of the X-ray spectra of 4U 1820-30 are fit by a combination of a thermal (Blackbody) component, a Comptonization component (COMPTB), and a Gaussian-line component. Thus, using this spectral analysis, we find that the photon power-law index Γ of the Comptonization component is almost unchangeable (Γ ∼ 2), while the electron temperature kTe changes from 2.9 to 21 keV during these spectral events. We also establish that for these spectral events the normalization of the COMPTB component (which is proportional to the mass accretion rate {dot}M) increases by a factor of eight when kTe decreases from 21 keV to 2.9 keV. Previously, this index stability effect was also found analyzing X-ray data for the Z-source GX 340+0 and for the atolls 4U 1728-34 and GX 3+1. Thus, we can suggest that this spectral stability property is a spectral signature of an accreting neutron star source. On the other hand, in a black hole binary Γ monotonically increases with {dot}M and ultimately its value saturates at large {dot}M.

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Journal keyword(s): accretion, accretion disks - black hole physics - radiation mechanisms: non-thermal - stars: individual: 4U 1820-30

Simbad objects: 27

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Number of rows : 27
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* IL Lup HXB 15 47 08.2768672752 -47 40 10.284587760         15.624 ~ 532 1
2 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
3 V* QX Nor LXB 16 12 43.0 -52 25 26           ~ 946 1
4 V* V818 Sco LXB 16 19 55.0692669024 -15 38 25.017666540 11.60 12.40 11.1     Oev 1730 0
5 4U 1642-45 LXB 16 45 48.1 -45 36 42           ~ 467 1
6 [GHJ2008] 3 HXB 16 50 00.980 -49 57 43.60           K4V 422 0
7 V* V1033 Sco HXB 16 54 00.1423963019 -39 50 44.761701340       16.14   F3-6IV 1980 0
8 MXB 1658-298 LXB 17 02 06.54 -29 56 44.1 18.35 18.75 18.3     ~ 381 0
9 V* V821 Ara LXB 17 02 49.3876391280 -48 47 23.087954544         15.322 ~ 2237 0
10 V* V1101 Sco LXB 17 05 44.4916006152 -36 25 23.049324480   20.10 18.6     ~ 473 0
11 4U 1722-30 LXB 17 27 33.25 -30 48 07.4     12.50     ~ 278 1
12 V* V2216 Oph LXB 17 31 44.17 -16 57 40.9 16.40 17.10 16.8     ~ 329 1
13 NAME Slow Burster LXB 17 31 58.0 -33 49 58     15.50     ~ 865 1
14 NAME XTE J17464-3213 LXB 17 46 15.59637 -32 14 00.8600           ~ 805 0
15 X Sgr X-1 LXB 17 47 56.3 -26 33 47           ~ 402 0
16 X Sgr X-3 LXB 18 01 32.6 -20 31 45           ~ 254 1
17 V* V5512 Sgr LXB 18 14 31.3 -17 09 23     12.73     K5III 449 0
18 V* NP Ser LXB 18 16 01.7 -14 02 09   18.8       K 683 2
19 NGC 6624 GlC 18 23 40.51 -30 21 39.7           ~ 939 1
20 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
21 V* V4634 Sgr LXB 18 29 28.8 -23 47 48 18.90 19.40 19     ~ 399 0
22 V* V406 Vul HXB 18 58 41.49127200 +22 39 29.7746640           G5V-K0V 409 0
23 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1
24 SS 433 HXB 19 11 49.5647697480 +04 58 57.827127648   16.854 14.643     A7Ib 2253 4
25 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
26 HD 226868 HXB 19 58 21.6757355952 +35 12 05.784512688 9.38 9.72 8.91 8.42   O9.7Iabpvar 4590 0
27 V* V1341 Cyg LXB 21 44 41.1544345272 +38 19 17.066570988 15.00 15.13 14.68 15.00   A9III 1229 1

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