2015ApJ...812...33S


Query : 2015ApJ...812...33S

2015ApJ...812...33S - Astrophys. J., 812, 33 (2015/October-2)

Extragalactic high-energy transients: event rate densities and luminosity functions.

SUN H., ZHANG B. and LI Z.

Abstract (from CDS):

Several types of extragalactic high-energy transients have been discovered, which include high-luminosity and low-luminosity long-duration gamma-ray bursts (GRBs), short-duration GRBs, supernova shock breakouts (SBOs), and tidal disruption events (TDEs) without or with an associated relativistic jet. In this paper, we apply a unified method to systematically study the redshift-dependent event rate densities and the global luminosity functions (GLFs; ignoring redshift evolution) of these transients. We introduce some empirical formulae for the redshift-dependent event rate densities for different types of transients and derive the local specific event rate density, which also represents its GLF. Long GRBs (LGRBs) have a large enough sample to reveal features in the GLF, which is best charaterized as a triple power law (PL). All the other transients are consistent with having a single-power-law (SPL) LF. The total event rate density depends on the minimum luminosity, and we obtain the following values in units of Gpc–3/yr: for high-luminosity LGRBs above 1050 erg/s; for low-luminosity LGRBs above 5x1046 erg/s; and above 1050 erg/s for short GRBs with three different merger delay models (Gaussian, lognormal, and PL); above 1044 erg/s for SBOs, for normal TDEs above 1044 erg/s; and above 1048 erg/s for TDE jets as discovered by Swift. Intriguingly, the GLFs of different kinds of transients, which cover over 12 orders of magnitude, are consistent with an SPL with an index of -1.6.

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Journal keyword(s): gamma-ray burst: general - stars: flare - stars: luminosity function, mass function - supernovae: individual: SN 2006aj

Simbad objects: 24

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Number of rows : 24
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 PSO J027.8085-18.5940 G 01 51 14.05011120 -18 35 38.4976680           ~ 192 0
2 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
3 GRB 080517 gB 06 48 58.00 +50 44 06.3           ~ 52 1
4 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
5 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
6 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
7 NGC 3599 GiP 11 15 26.9494646448 +18 06 37.428503940   13.0       ~ 226 0
8 GRB 060123 gB 11 58 47.83 +45 30 50.9           ~ 46 0
9 2MASS J12013602+3003052 G 12 01 36.0281668104 +30 03 05.576406012           ~ 47 0
10 GRB 070419A gB 12 10 58.830 +39 55 34.06 18.52         ~ 130 0
11 RX J1242.6-1119 PaG 12 42 36.9 -11 19 35           ~ 49 1
12 SDSS J131122.15-012345.6 G 13 11 22.15203 -01 23 45.6159           ~ 23 0
13 SDSS J132341.97+482701.3 G 13 23 41.9755425624 +48 27 01.261293624           ~ 34 0
14 PSO J203.7673-22.1424 G 13 35 04.16044560 -22 08 32.8717680           ~ 178 0
15 TDXF J134730.3-325451 X 13 47 30.330 -32 54 50.63           ~ 4 1
16 WINGS J134849.88+263557.5 G 13 48 49.88 +26 35 57.5   23.28 22.46     ~ 16 0
17 2MASS J14202436+5334117 BLL 14 20 24.3988020192 +53 34 11.158101156   20.49 20.03     ~ 40 0
18 NGC 5905 H2G 15 15 23.3280793632 +55 31 01.926808032   13.6       ~ 287 1
19 2MASX J16245665+7554560 BLL 16 24 56.5716973728 +75 54 55.975695048     16.60     ~ 59 0
20 SWIFT J164449.3+573451 G 16 44 47.81184000 +57 35 00.7113480           ~ 533 0
21 2MASS J18472513-6317252 G 18 47 25.1287042560 -63 17 25.304943912     16.67   15.56 ~ 16 0
22 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
23 SWIFT J2058.4+0516 X 20 58 19.898 +05 13 32.25           ~ 169 0
24 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 248 1

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