2014A&A...562A..16I


Query : 2014A&A...562A..16I

2014A&A...562A..16I - Astronomy and Astrophysics, volume 562A16-16 (2014/2-1)

The cooling rate of neutron stars after thermonuclear shell flashes.

IN'T ZAND J.J.M., CUMMING A., TRIEMSTRA T.L., MATEIJSEN R.A.D.A. and BAGNOLI T.

Abstract (from CDS):

Thermonuclear shell flashes on neutron stars are detected as bright X-ray bursts. Traditionally, their decay is modeled with an exponential function. However, this is not what theory predicts. The expected functional form for luminosities below the Eddington limit, at times when there is no significant nuclear burning, is a power law. We tested the exponential and power-law functional forms against the best data available: bursts measured with the high-throughput Proportional Counter Array (PCA) onboard the Rossi X-ray Timing Explorer. We selected a sample of 35 ``clean'' and ordinary (i.e., shorter than a few minutes) bursts from 14 different neutron stars that 1) show a wide dynamic range in luminosity; 2) are the least affected by disturbances by the accretion disk; and 3) lack prolonged nuclear burning through the rp-process. We find indeed that for every burst a power law is a better description than an exponential function. We also find that the decay index is steep, 1.8 on average, and different for every burst. This may be explained by contributions from degenerate electrons and photons to the specific heat capacity of the ignited layer and by deviations from the Stefan-Boltzmann law due to changes in the opacity with density and temperature. Detailed verification of this explanation yields inconclusive results. While the values for the decay index are consistent, the predicted dependency of the decay index with the burst time scale, as a proxy of ignition depth, is not supported by the data.

Abstract Copyright: ∼

Journal keyword(s): X-rays: binaries - X-rays: bursts - stars: neutron - dense matter

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 4U 0513-40 LXB 05 14 06.59 -40 02 37.0           ~ 176 1
2 V* UY Vol LXB 07 48 33.71 -67 45 07.7 16.10 17.00 16.9 16.7 17.05 ~ 660 0
3 4U 0919-54 LXB 09 20 26.4818170056 -55 12 24.512806404 20.40 21.30 21.0     ~ 175 0
4 V* QX Nor LXB 16 12 43.0 -52 25 26           ~ 946 1
5 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 921 0
6 X Ara X-1 LXB 17 06 15.2 -43 02 11           ~ 296 1
7 1RXS J170855.6-440653 LXB 17 08 54.346 -44 06 08.38           ~ 406 1
8 4U 1722-30 LXB 17 27 33.25 -30 48 07.4     12.50     ~ 278 1
9 NAME Slow Burster LXB 17 31 58.0 -33 49 58     15.50     ~ 865 1
10 IGR J17480-2446 LXB 17 48 04.831 -24 46 48.87           ~ 204 0
11 IGR J17511-3057 LXB 17 51 08.55 -30 57 41.7           ~ 114 1
12 SAX J1808.4-3658 LXB 18 08 27.58 -36 58 43.9           ~ 1051 0
13 XTE J1810-189 LXB 18 10 20.86 -19 04 11.2           ~ 64 0
14 V* V4722 Sgr LXB 18 10 44.47 -26 09 01.2   21.5     18.449 ~ 99 0
15 X Sgr X-4 LXB 18 23 40.57 -30 21 40.6   19.06 18.81     ~ 1056 1
16 V* V4634 Sgr LXB 18 29 28.8 -23 47 48 18.90 19.40 19     ~ 399 0
17 2MAXI J1900-248 LXB 19 00 08.65 -24 55 13.7     18.09     ~ 226 0
18 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1

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