2003ApJ...595.1058T


Query : 2003ApJ...595.1058T

2003ApJ...595.1058T - Astrophys. J., 595, 1058-1065 (2003/October-1)

X-ray bursts in neutron star and black hole binaries from unconventional stellar aspect experiment and Rossi X-ray Timing Explorer data: detections and upper limits.

TOURNEAR D., RAFFAUF E., BLOOM E.D., FOCKE W., GIEBELS B., GODFREY G., SAZ PARKINSON P.M., REILLY K.T., WOOD K.S., RAY P.S., WOLFF M.T., BANDYOPADHYAY R.M., LOVELLETTE M.N. and SCARGLE J.D.

Abstract (from CDS):

Narayan & Heyl have developed a theoretical framework to convert suitable upper limits on type I X-ray bursts from accreting black hole candidates (BHCs) into evidence for an event horizon. However, no appropriate observational limit exists in the literature. In this paper we survey 2101.2 ks of data from the Unconventional Stellar Aspect (USA) X-ray timing experiment and 5142 ks of data from the Rossi X-Ray Timing Explorer (RXTE) experiment to obtain a formal constraint of this type. We find that 1122 ks of neutron star data yield a population-averaged mean burst rate of (1.7±0.4)x10–5 bursts/s, while 6081 ks of BHC data yield a 95% confidence level upper limit of 4.9x10–7 bursts/s. This is the first published limit of this type for BHCs. Applying the theoretical framework of Narayan & Heyl, we calculate regions of unstable luminosity, where the neutron stars are expected to burst and the BHCs would be expected to burst if they had a surface. In this unstable luminosity region, 464 ks of neutron star data yield an averaged mean burst rate of (4.1±0.8)x10–5 bursts/s, and 1512 ks of BHC data yield a 95% confidence level upper limit of 2.0x10–6 bursts/s and a strong limit that BHCs do not burst with a rate similar to the rate of neutron stars in these unstable regions. This gives further evidence that BHCs do not have surfaces unless there is some new physics occurring on their surface.


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Journal keyword(s): Black Hole Physics - Stars: Neutron - X-Rays: Binaries - X-Rays: Bursts

Simbad objects: 26

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Number of rows : 26
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* CM Tau Psr 05 34 31.9474694616 +22 00 52.153698024           ~ 5476 0
3 V* V1055 Ori LXB 06 17 07.3565603963 +09 08 13.515857360   18.80 18.5     ~ 594 1
4 V* UY Vol LXB 07 48 33.71 -67 45 07.7 16.10 17.00 16.9 16.7 17.05 ~ 660 0
5 V* KV UMa HXB 11 18 10.7930420496 +48 02 12.314730120           K5V-M1V 865 0
6 V* GR Mus LXB 12 57 37.1833002949 -69 17 18.996899563   19.40 19.1     ~ 275 0
7 V* BR Cir HXB 15 20 40.8532547060 -57 10 00.206639033   21.4 21.4     B5-A0I 849 1
8 V* V381 Nor HXB 15 50 58.6637920704 -56 28 35.258385000           K3III 1254 0
9 V* V818 Sco LXB 16 19 55.0692669024 -15 38 25.017666540 11.60 12.40 11.1     Oev 1730 0
10 X Nor X-1 LXB 16 34 01.610 -47 23 34.80           ~ 579 0
11 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 921 0
12 4U 1642-45 LXB 16 45 48.1 -45 36 42           ~ 467 1
13 MXB 1658-298 LXB 17 02 06.54 -29 56 44.1 18.35 18.75 18.3     ~ 381 0
14 V* V1101 Sco LXB 17 05 44.4916006152 -36 25 23.049324480   20.10 18.6     ~ 473 0
15 NAME Slow Burster LXB 17 31 58.0 -33 49 58     15.50     ~ 865 1
16 NAME Rapid Burster LXB 17 33 24.0 -33 23 19           ~ 429 2
17 V* V926 Sco LXB 17 38 58.2384053021 -44 27 00.699118812 16.90 17.70 17.5     ~ 480 0
18 X Sgr X-1 LXB 17 47 56.3 -26 33 47           ~ 402 0
19 4U 1758-25 LXB 18 01 09.7308060816 -25 04 44.120221284     11.08     ~ 705 1
20 V* NP Ser LXB 18 16 01.7 -14 02 09   18.8       K 683 2
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 Granat 1915+105 HXB 19 15 11.55576 +10 56 44.9052           ~ 2810 0
25 V* V1521 Cyg HXB 20 32 25.78 +40 57 27.9           WN4/5-6/7 2035 2
26 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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