2016A&A...594A..54P


Query : 2016A&A...594A..54P

2016A&A...594A..54P - Astronomy and Astrophysics, volume 594A, 54-54 (2016/10-1)

High-redshift supernova rates measured with the gravitational telescope A 1689.

PETRUSHEVSKA T., AMANULLAH R., GOOBAR A., FABBRO S., JOHANSSON J., KJELLSSON T., LIDMAN C., PAECH K., RICHARD J., DAHLE H., FERRETTI R., KNEIB J.P., LIMOUSIN M., NORDIN J. and STANISHEV V.

Abstract (from CDS):

Aims. We present a ground-based, near-infrared search for lensed supernovae behind the massive cluster Abell 1689 at z = 0.18, which is one of the most powerful gravitational telescopes that nature provides.
Methods. Our survey was based on multi-epoch J-band observations with the HAWK-I instrument on VLT, with supporting optical data from the Nordic Optical Telescope.
Results. Our search resulted in the discovery of five photometrically classified, core-collapse supernovae with high redshifts of 0.671<z<1.703 and magnifications in the range Δm=-0.31 to -1.58mag, as calculated from lensing models in the literature. Owing to the power of the lensing cluster, the survey had the sensitivity to detect supernovae up to very high redshifts, z∼3, albeit for a limited region of space. We present a study of the core-collapse supernova rates for 0.4≤z<2.9, and find good agreement with previous estimates and predictions from star formation history. During our survey, we also discovered two Type Ia supernovae in A 1689 cluster members, which allowed us to determine the cluster Ia rate to be 0.14+0.19–0.09±0.01SNuB.h2 (SNuB∼10–12SNe/L☉,B/yr), where the error bars indicate 1σ confidence intervals, statistical and systematic, respectively. The cluster rate normalized by the stellar mass is 0.10+0.13–0.096±0.02 in SNuM.h2 (SNuM∼10–12SNe/M/yr). Furthermore, we explore the optimal future survey for improving the core-collapse supernova rate measurements at z≥2 using gravitational telescopes, and for detections with multiply lensed images, and we find that the planned WFIRST space mission has excellent prospects.
Conclusions. Massive clusters can be used as gravitational telescopes to significantly expand the survey range of supernova searches, with important implications for the study of the high-z transient Universe.

Abstract Copyright: © ESO, 2016

Journal keyword(s): supernovae: general - gravitational lensing: strong - galaxies: star formation - galaxies: clusters: individual: A 1689 - techniques: photometric

VizieR on-line data: <Available at CDS (J/A+A/594/A54): list.dat A1689_J.fits>

Nomenclature: Table 3: [PAG2016] CAND-NNNNN N=8 among (Nos 669-10662), [PAG2016] CAND-ISAAC N=1.

CDS comments: Table 3 : Cand 1208 is SN 2010lw in Simbad

Simbad objects: 19

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Number of rows : 19
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2023
#notes
1 ACO 2744 ClG 00 14 20.03 -30 23 17.8           ~ 749 0
2 SN 2007if SN* 01 10 51.37 +15 27 39.9   23.3 19.5     SNIap 124 1
3 NGC 3690 IG 11 28 31.0 +58 33 41   13.19 12.86     ~ 966 4
4 MCS J1149.5+2223 ClG 11 49 35.8 +22 23 55           ~ 441 0
5 NAME SN Refsdal SN* 11 49 36.010 +22 23 48.13           ~ 88 0
6 SN 2010lw SN* 13 11 21.57 -01 21 41.2           SNIa 4 1
7 [PAG2016] CAND-10658 SN* 13 11 22.31 -01 21 45.0           SNIIn 2 0
8 [PAG2016] CAND-10662 SN* 13 11 24.82 -01 19 42.9           SNIIP 2 0
9 [PAG2016] CAND-821 SN* 13 11 26.43 -01 21 31.2           SNIIn 2 0
10 [PAG2016] CAND-ISAAC SN* 13 11 28.01 -01 19 25.0           SNIIP 2 0
11 ACO 1689 ClG 13 11 29.5 -01 20 28           ~ 1109 0
12 [PAG2016] CAND-1392 SN* 13 11 29.69 -01 22 12.0           SNIIP 2 0
13 [AGC2011] SN SN* 13 11 30.0 -01 20 28           ~ 2 0
14 [PAG2016] CAND-7169 SN* 13 11 31.21 -01 21 24.0           SNIa 1 0
15 [PAG2016] CAND-802 SN* 13 11 32.14 -01 22 36.4           SNIa 1 0
16 [PAG2016] CAND-669 SN* 13 11 33.45 -01 23 42.9           SNIIL 2 0
17 NAME Subaru Deep Field NGP reg 13 24 21.3 +27 29 23           ~ 320 1
18 ACO 1835 ClG 14 01 02.07 +02 52 43.2           ~ 680 1
19 ACO S 1077 ClG 22 58 52.34 -34 46 54.6           ~ 185 0

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2023.09.26-01:27:59

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