2012A&A...539A.113E


Query : 2012A&A...539A.113E

2012A&A...539A.113E - Astronomy and Astrophysics, volume 539A113-113 (2012/3-1)

The long γ-ray burst rate and the correlation with host galaxy properties.

ELLIOTT J., GREINER J., KHOCHFAR S., SCHADY P., JOHNSON J.L. and RAU A.

Abstract (from CDS):

To answer questions on the start and duration of the epoch of reionisation, periods of galaxy mergers and properties of other cosmological encounters, the cosmic star formation history, {dot}(ρ)* or CSFH, is of fundamental importance. Using the association of long-duration gamma-ray bursts (LGRBs) with the death of massive stars and their ultra-luminous nature (>1052erg/s), the CSFH can be probed to higher redshifts than current conventional methods. Unfortunately, no consensus has been reached on the manner in which the LGRB rate, {dot}(ρ)grb or LGRBR, traces the CSFH, leaving many of the questions mentioned mostly unexplored by this method. Observations by the gamma-ray burst near-infrared detector (GROND) over the past 4 years have, for the first time, acquired highly complete LGRB samples. Driven by these completeness levels and new evidence of LGRBs also occurring in more massive and metal rich galaxies than previously thought, the possible biases of the {dot}(ρ)grb-{dot}(ρ)* connection are investigated over a large range of galaxy properties. The CSFH is modelled using empirical fits to the galaxy mass function and galaxy star formation rates. Biasing the CSFH by means of metallicity cuts, mass range boundaries, and other unknown redshift dependencies of the form {dot}(ρ)grb∝{dot}(ρ)*(1+z)δ, a {dot}(ρ)grb is generated and compared to the highly complete GROND LGRB sample. It is found that there is no strong preference for a metallicity cut or fixed galaxy mass boundaries and that there are no unknown redshift effects (δ=0), in contrast to previous work which suggest values of Z/Z☉∼0.1-0.3. From the best-fit models obtained, we predict that ∼1.2% of the LGRB burst sample exists above z=6. The linear relationship between {dot}(ρ)grb and {dot}(ρ)* suggested by our results implies that redshift biases present in previous LGRB samples significantly affect the inferred dependencies of LGRBs on their host galaxy properties. Such biases can lead to, for example, an interpretation of metallicity limitations and evolving LGRB luminosity functions.

Abstract Copyright: ∼

Journal keyword(s): gamma-ray burst: general - cosmology: miscellaneous

Simbad objects: 39

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Number of rows : 39
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 GRB 071031 gB 00 25 37.40 -58 03 33.9           ~ 184 0
2 GRB 080710 gB 00 33 05.68 +19 30 05.8           ~ 136 0
3 GRB 081222 gB 01 30 57.76 -34 05 44.0           ~ 199 0
4 GRB 091018 gB 02 08 46 -57 33.0           ~ 169 0
5 GRB 080707 gB 02 10 28.48 +33 06 35.1           ~ 83 0
6 SN 2009nz SN* 02 26 19.87 -18 57 08.6           ~ 307 1
7 GRB 070802 gB 02 27 35.91 -55 31 39.1           ~ 168 0
8 GRB 080411 gB 02 31 54.82 -71 18 07.5           ~ 109 0
9 GRB 081228 gB 02 37 50.80 +30 51 09.2           ~ 43 0
10 Fermi bn090926914 gB 03 05 14.30 -38 59 50.9           ~ 149 1
11 Fermi bn091221870 gB 03 43 11.40 +23 14 28.0           ~ 66 0
12 GRB 091029 gB 04 00 40.00 -55 57 12.7           ~ 168 0
13 GRB 080913 gB 04 22 57.90 -25 07 38.6           ~ 213 0
14 GRB 081121 gB 05 57 07.70 -60 36 42.1           ~ 152 0
15 GRB 080129 gB 07 01 08.13 -07 50 47.8           ~ 85 0
16 GRB 080516 gB 08 02 34.16 -26 09 35.3           ~ 59 0
17 GRB 090102 gB 08 32 59.50 +33 06 25.7           ~ 253 0
18 GRB 100205A gB 09 25 33.00 +31 44 25.8           ~ 39 0
19 Fermi bn090519881 gB 09 29 16.20 +00 11 23.9           ~ 98 0
20 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
21 GRB 100316B gB 10 54 00 -45 28.0           ~ 62 0
22 GRB 080330 gB 11 17 06.70 +30 36 24.1           ~ 145 0
23 GRB 090313 gB 13 13 36.00 +08 05 10.7           ~ 149 0
24 GRB 090429B gB 14 02 40.10 +32 10 14.6           ~ 166 0
25 GRB 090814A gB 15 58 26.44 +25 37 52.4           ~ 56 0
26 GRB 080210 gB 16 45 04.03 +13 49 36.3           ~ 121 0
27 GRB 080605 gB 17 28 30.04 +04 00 56.9           ~ 198 0
28 Fermi bn090904058 gB 17 36 44.52 -25 12 45.9           ~ 56 0
29 Fermi bn081008832 gB 18 39 52.40 -57 25 58.8           ~ 224 0
30 GRB 080520 gB 18 40 46.50 -54 59 30.4           ~ 68 0
31 GRB 080413A gB 19 09 11.73 -27 40 39.6           ~ 163 0
32 GRB 071010A gB 19 12 14.42 -32 24 06.2           ~ 138 0
33 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
34 GRB 080805 gB 20 56 55.30 -62 25 58.8           ~ 102 0
35 GRB 080413B gB 21 44 34.62 -19 58 51.2           ~ 191 0
36 Fermi bn080804972 gB 21 54 41.90 -53 11 20.2           ~ 158 0
37 SN 2008hw SN* 22 39 50.39 -40 08 49.1           SNIc 197 1
38 GRB 081029 gB 23 07 06 -68 10.7           ~ 121 0
39 GRB 090812 gB 23 32 48.5 -10 36 17           ~ 165 0

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