
Supernovae in deep Hubble Space Telescope galaxy cluster fields: cluster rates and field counts
Author(s) -
GalYam Avishay,
Maoz Dan,
Sharon Keren
Publication year - 2002
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1046/j.1365-8711.2002.05274.x
Subject(s) - physics , astrophysics , redshift , galaxy , supernova , hubble deep field , luminosity , astronomy , cluster (spacecraft) , advanced camera for surveys , galaxy cluster , hubble space telescope , intracluster medium , observational cosmology , computer science , programming language
We have searched for high‐redshift supernova (SN) candidates in multiple deep Hubble Space Telescope ( HST ) archival images of nine galaxy cluster fields. We detect six apparent SNe, with 21.6 I 814 28.4 mag . There is roughly 1 SN per deep ( I 814 >26 mag) , doubly‐imaged WFPC2 cluster field. Two SNe are associated with cluster galaxies (at redshifts z =0.18 and z =0.83) , three are probably in galaxies not in the clusters (at z =0.49 , z =0.60 , and z =0.98) , and one is at unknown z . After accounting for observational efficiencies and uncertainties (statistical and systematic) we derive the rate of type Ia SNe within the projected central of rich clusters: SNu in 0.18 z 0.37 clusters, and SNu in clusters at 0.83 z 1.27 (95 per cent confidence interval; 1 SNu≡1 SN century −1 per 10 10 L B⊙ ). Combining the two redshift bins, the mean rate is SNu. The upper bounds argue against SNe Ia being the dominant source of the large iron mass observed in the intracluster medium. We also compare our observed counts of field SNe (i.e. non‐cluster SNe of all types) to recent model predictions. The observed field count is N 1 SN with I 814 26 mag , and 1 N 3 SNe with I 814 27 mag . These counts are half of some of the predictions. Since the counts at these magnitudes are likely dominated by type II SNe, our observations may suggest obscuration of distant SNe II, or a SN II luminosity distribution devoid of a large high‐luminosity tail.