2024A&A...685A..71P


Query : 2024A&A...685A..71P

2024A&A...685A..71P - Astronomy and Astrophysics, volume 685A71 (2024/5-1)

New insight into the hard X-ray emission influenced by the type I bursts observed by Insight-HXMT during the outburst of 4U 1636-536.

PENG J.Q., ZHANG S., CHEN Y.P., KONG L.D., WANG P.J., ZHANG S.N., SHUI Q.C., JI L., ZHANG G.B., YAN Z., TAO L., QU J.L., GE M.Y., YU Z.L., LI J., CHANG Z., LI Z.S., ZHANG P., XIAO Y.X. and ZHAO S.J.

Abstract (from CDS):

Context. Thermonuclear bursts, also known as type I X-ray bursts, result from unstable nuclear burning of H/He accreted to the surface of neutron stars, lasting from tens to hundreds of seconds. Thermonuclear bursts have an important impact on accretion environments around the neutron stars, such as their disks and coronas, and are therefore a subject of extensive research. Thermonuclear bursts can be used as probes to gain a deeper understanding of the properties of their disks and coronas.
Aims. By analyzing the data from Insight-HXMT and NICER, we can determine the evolution of the significance of the hard shortage in 4U 1636-536 with its spectral state, as well as the evolution of the fraction of deficit with energy. Additionally, we investigate the possible geometry and evolution of the corona in 4U 1636-536 by combining our findings with the results of spectral analysis.
Methods. We extracted the light curves from the Insight-HXMT low-energy, medium-energy, and high-energy data and subtracted their pre-burst emission, which allowed us to estimate the significance of the hard shortages during the bursts. By fitting the spectra, the correlation between the persistent spectral parameters and the significance of the hard shortages could be established. The bursts were then grouped according to the spectral state in which they occurred, and the significance of the hard shortages was estimated. These in turn helped to investigate the evolution of the fraction of deficit with energy.
Results. We find that during the soft state the significance of possible hard X-ray shortage in bursts is almost zero. However, in the hard state, some bursts exhibit significant shortages (> 3σ), while others do not. We attempt to establish a correlation between the significance of the hard X-ray shortage and the spectral parameters, but the data quality and the limited number of bursts prevent us from finding a strong correlation. For bursts with insignificant shortages in the soft state, the fraction of the deficit remains small. However, in the hard state the fraction of deficit for all bursts increases with energy, regardless of the significance of the shortage of individual bursts. For bursts during the hard state, we investigated the evolution of the fraction of deficit during the bursts by stacking the peaks and decays of the bursts, and find that as the flux of the bursts decreases, the energy corresponding to the maximum of the fraction of deficit becomes progressively higher.
Conclusions. We explore the possible geometry and evolution of the corona suggested by the evolution of the fraction of deficit, which is obtained from the spectral and temporal analysis.

Abstract Copyright: © The Authors 2024

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

Simbad objects: 12

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Number of rows : 12
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 M 1 SNR 05 34 31.8 +22 01 03           ~ 6516 1
2 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 921 0
3 1RXS J170855.6-440653 LXB 17 08 54.346 -44 06 08.38           ~ 406 1
4 NAME Slow Burster LXB 17 31 58.0 -33 49 58     15.50     ~ 865 1
5 4U 1730-22 LXB 17 33 57.00 -22 02 07.0           ~ 64 0
6 KS 1731-260 LXB 17 34 13.46 -26 05 18.6       22.8 20.9 ~ 437 0
7 [KRL2007b] 277 LXB 17 47 18.06 -27 20 38.9           ~ 88 0
8 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
9 MAXI J1816-195 Psr 18 16 52.34478480 -19 37 55.8563160           ~ 48 1
10 V* V4634 Sgr LXB 18 29 28.8 -23 47 48 18.90 19.40 19     ~ 399 0
11 SWIFT J1858.6-0814 XB* 18 58 34.91 -08 14 14.8           ~ 76 0
12 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1

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