2016ApJ...826...98U


Query : 2016ApJ...826...98U

2016ApJ...826...98U - Astrophys. J., 826, 98-98 (2016/July-3)

Investigation of primordial black hole bursts using interplanetary network gamma-ray bursts.

UKWATTA T.N., HURLEY K., MacGIBBON J.H., SVINKIN D.S., APTEKAR R.L., GOLENETSKII S.V., FREDERIKS D.D., PAL'SHIN V.D., GOLDSTEN J., BOYNTON W., KOZYREV A.S., RAU A., VON KIENLIN A., ZHANG X., CONNAUGHTON V., YAMAOKA K., OHNO M., OHMORI N., FEROCI M., FRONTERA F., GUIDORZI C., CLINE T., GEHRELS N., KRIMM H.A. and McTIERNAN J.

Abstract (from CDS):

The detection of a gamma-ray burst (GRB) in the solar neighborhood would have very important implications for GRB phenomenology. The leading theories for cosmological GRBs would not be able to explain such events. The final bursts of evaporating primordial black holes (PBHs), however, would be a natural explanation for local GRBs. We present a novel technique that can constrain the distance to GRBs using detections from widely separated, non-imaging spacecraft. This method can determine the actual distance to the burst if it is local. We applied this method to constrain distances to a sample of 36 short-duration GRBs detected by the Interplanetary Network (IPN) that show observational properties that are expected from PBH evaporations. These bursts have minimum possible distances in the 1013-1018 cm (7-105 au) range, which are consistent with the expected PBH energetics and with a possible origin in the solar neighborhood, although none of the bursts can be unambiguously demonstrated to be local. Assuming that these bursts are real PBH events, we estimate lower limits on the PBH burst evaporation rate in the solar neighborhood.

Abstract Copyright: © 2016. The American Astronomical Society. All rights reserved.

Journal keyword(s): black hole physics - methods: observational

Simbad objects: 36

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Number of rows : 36
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 GRB 090523 gB 02 00 +11.0           ~ 5 0
2 GRB 000607 gB 02 33 58.7 +17 08 51           ~ 25 1
3 GRB 001204 gB 02 41 08.6 +12 53 46           ~ 20 1
4 GRB 110802A gB 02 58 09.50 +32 34 44.5           ~ 7 0
5 GRB 080203 gB 03 12 50.06 +24 19 44.0           ~ 3 0
6 GRB 101009 gB 05 03 43.66 -33 51 11.5           ~ 3 0
7 GRB 100223A gB 06 58 +03.7           ~ 23 0
8 GRB 090228 gB 07 07.2 -24 18           ~ 45 0
9 2B 920414 gB 07 30.0 -73 43           ~ 20 0
10 GRB 001025 gB 08 36.6 -13 04           ~ 47 1
11 Fermi bn101129652 gB 10 23 41 -17 38.7           ~ 33 0
12 GRB 110705A gB 10 24 +40.1           ~ 22 0
13 GRB 121127A gB 11 46 -52.4           ~ 14 0
14 GRB 120519A gB 12 01 +20.5           ~ 16 0
15 GRB 080530A gB 12 24 +00.0           ~ 5 0
16 Fermi bn131126163 gB 14 22 +53.5           ~ 14 0
17 GRB 100629A gB 15 25 +27.8           ~ 15 0
18 GRB 970921 gB 15 43 31.8 -24 49 52           ~ 5 0
19 GRB 120811A gB 17 08 44.10 -22 44 06.7           ~ 15 0
20 Fermi bn141011282 gB 17 11 45.0 -09 40 52           ~ 11 0
21 GRB 010104 gB 17 49 45 +18 13.6           ~ 8 0
22 GRB 981102 gB 18 28 12.34 -48 20 07.4           ~ 4 0
23 GRB 010119 gB 18 53 46.17 +11 59 47.0           ~ 20 0
24 Fermi bn120222119 gB 19 58 +26.5           ~ 14 0
25 GRB 140906C gB 20 59.8 +01 56           ~ 7 0
26 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 262 1
27 GRB 100811A gB 23 04 +15.9           ~ 16 0
28 Fermi bn130504314 gB 23 12 -05.7           ~ 12 0
29 GRB 970902 gB 23 24 06.22 +07 19 45.8           ~ 4 0
30 GRB 121023 gB ~ ~           ~ 1 0
31 GRB 110510 gB ~ ~           ~ 2 0
32 GRB 140807 gB ~ ~           ~ 2 0
33 GRB 130501 gB ~ ~           ~ 2 0
34 GRB 140414B gB ~ ~           ~ 2 0
35 GRB 910206 gB ~ ~           ~ 4 0
36 GRB 080222 gB ~ ~           ~ 2 0

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