2018MNRAS.479.3563F


Query : 2018MNRAS.479.3563F

2018MNRAS.479.3563F - Mon. Not. R. Astron. Soc., 479, 3563-3581 (2018/September-3)

The rate of Type-Ia supernovae in galaxy clusters and the delay-time distribution out to redshift 1.75.

FRIEDMANN M. and MAOZ D.

Abstract (from CDS):

The observed delay-time distribution (DTD) of Type-Ia supernovae (SNe Ia) is a valuable probe of SN Ia progenitors and physics, and of the role of SNe Ia in cosmic metal enrichment. The SN Ia rate in galaxy clusters as a function of cluster redshift is an almost-direct measure of the DTD, but current estimates have been limited out to a mean redshift <z> = 1.1, corresponding to time delays, after cluster star formation, of >=3.2 Gyr. We analyze data from a Hubble Space Telescope monitoring project of 12 galaxy clusters at z = 1.13-1.75, where we discover 29 SNe, and present their multiband light curves. Based on the SN photometry and the apparent host galaxies, we assess cluster membership and SN type, finding 11cases that are likely SNe Ia in cluster galaxies and 4 more cases, which are possible but not certain cluster SNe Ia. We conduct simulations to estimate the SN detection efficiency, the experiment's completeness, and the photometric errors, and perform photometry of the cluster galaxies to derive the cluster stellar masses. With this input, we obtain a mean <z> = 1.35 cluster rest-frame SN Ia rate per unit formed stellar mass of R_ Ia, m*_=2.6^+ 3.2^_- 1.5_ ×10–13 yr–1 M☉–1. Separating the cluster sample into high-z and low-z bins, the rates are 2.2^+ 2.6^_- 1.3_ ×10–13 yr–1 M☉–1 at <z> = 1.25, and 3.5^+ 6.6^_- 2.8_ ×10–13 yr–1 M☉–1 at <z> = 1.58. Combining our results with previous cluster SN Ia rates, we fit the DTD, now down to delays of 1.5 Gyr, with a power-law dependence, tα, with α=-1.30+0.23–0.16. We confirm previous indications for a SN Ia production efficiency that is several times higher in galaxy clusters than in the field, perhaps caused by a peculiar stellar initial mass function in clusters, or by a higher incidence of binaries that will evolve into SNe Ia.

Abstract Copyright: © 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Society

Journal keyword(s): surveys - supernovae: general - galaxies: clusters

VizieR on-line data: <Available at CDS (J/MNRAS/479/3563): table2.dat table3.dat>

Nomenclature: Fig. 2, Table 2: [FM2018] SN FMNN (Nos FM01-FM29).

Simbad objects: 42

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Number of rows : 42
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 [FM2018] SN FM20 SN? 00 35 47.60 -43 11 57.5           ~ 2 0
2 SpARCS J003550-431224 ClG 00 35 50.0 -43 12 24           ~ 35 0
3 [FM2018] SN FM19 SN? 00 35 52.10 -43 12 24.0           ~ 2 0
4 [FM2018] SN FM29 SN? 00 44 02.90 -20 33 50.0           SN.Ia 4 0
5 NAME XMMU J0044.0-2033 ClG 00 44 05.20 -20 33 59.7           ~ 40 0
6 [FM2018] SN FM25 SN? 02 05 46.20 -58 28 54.8           SN.Ia 4 0
7 ACT-CL J0205.7-5829 ClG 02 05 46.5 -58 29 08           ~ 54 0
8 [FM2018] SN FM24 SN? 02 05 48.00 -58 29 26.5           SN.Ia 4 0
9 [FM2018] SN FM22 SN? 02 05 51.00 -58 29 27.2           SN.Ia 4 0
10 [FM2018] SN FM23 SN? 02 05 51.00 -58 29 26.6           SN.Ia 4 0
11 [FM2018] SN FM21 SN? 02 05 52.30 -58 29 40.0           ~ 4 0
12 [FM2018] SN FM15 SN? 02 24 26.20 -03 23 32.2           ~ 3 0
13 SpARCS J022426-032331 ClG 02 24 26.32 -03 23 30.7           ~ 17 0
14 [FM2018] SN FM16 SN? 02 24 27.60 -03 22 57.4           ~ 4 0
15 [FM2018] SN FM18 SN? 03 30 53.50 -28 42 34.8           ~ 2 0
16 SpARCS J033056-284300 ClG 03 30 55.87 -28 42 59.7           ~ 18 0
17 [FM2018] SN FM17 SN? 03 30 55.90 -28 42 45.8           SN.Ia 4 0
18 NAME Hubble Ultra Deep Field reg 03 32 39.0 -27 47 29           ~ 1900 0
19 [FM2018] SN FM13 SN? 10 14 04.00 +00 38 11.4           SN.Ia 4 0
20 SCP 16C3 SN* 10 14 06.37 +00 38 25.5           SNIa 5 0
21 ACT-CL J1014.1+0038 ClG 10 14 07.49 +00 38 30.2           ~ 23 0
22 [FM2018] SN FM11 SN? 10 14 07.60 +00 38 08.3           ~ 4 0
23 [FM2018] SN FM10 SN? 10 14 09.10 +00 37 48.9           ~ 2 0
24 SpARCS J104922+564032 ClG 10 49 22.60 +56 40 32.5           ~ 37 0
25 ACT-CL J1142.7+1527 ClG 11 42 43.9 +15 27 07           ~ 22 0
26 [FM2018] SN FM14 SN? 11 42 44.90 +15 27 52.1           ~ 2 0
27 IDCS J1426.5+3508 ClG 14 26.5 +35 08           ~ 64 0
28 [FM2018] SN FM06 SN? 14 26 31.70 +35 09 02.0           ~ 2 0
29 [FM2018] SN FM05 SN? 14 26 32.00 +35 07 37.3           ~ 2 0
30 [FM2018] SN FM04 SN? 14 26 34.80 +35 07 46.5           ~ 2 0
31 [FM2018] SN FM03 SN? 14 26 35.20 +35 08 35.0           ~ 2 0
32 [FM2018] SN FM02 SN? 14 26 35.30 +35 07 31.7           ~ 2 0
33 [FM2018] SN FM01 SN? 14 26 38.30 +35 08 26.6           ~ 2 0
34 [FM2018] SN FM08 SN? 14 32 13.90 +32 53 23.1           ~ 2 0
35 [FM2018] SN FM07 SN? 14 32 16.10 +32 52 49.4           ~ 2 0
36 [FM2018] SN FM09 SN? 14 32 18.00 +32 52 56.3           ~ 2 0
37 ISCS J1432.3+3253 ClG 14 32 18.30 +32 53 07.8           ~ 11 0
38 [FM2018] SN FM27 SN? 20 40 58.80 -44 51 01.6           ~ 4 0
39 ACT-CL J2040.9-4452 ClG 20 40 59.23 -44 51 35.6           ~ 41 0
40 [FM2018] SN FM26 SN? 20 40 59.70 -44 52 04.1           ~ 4 0
41 [FM2018] SN FM28 SN? 21 05 57.10 -58 45 11.9           ~ 2 0
42 ACT-CL J2106.0-5844 ClG 21 06 04.3 -58 44 32           ~ 103 0

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