2018ApJ...861...92D


Query : 2018ApJ...861...92D

2018ApJ...861...92D - Astrophys. J., 861, 92-92 (2018/July-2)

Progenitor mass distribution for core-collapse supernova remnants in M31 and M33.

DIAZ-RODRIGUEZ M., MURPHY J.W., RUBIN D.A., DOLPHIN A.E., WILLIAMS B.F. and DALCANTON J.J.

Abstract (from CDS):

Using the star formation histories (SFHs) near 94 supernova remnants (SNRs), we infer the progenitor mass distribution for core-collapse supernovae. We use Bayesian inference and model each SFH with multiple bursts of star formation (SF), one of which is assumed to be associated with the SNR. Assuming single-star evolution, the minimum mass of CCSNe is 7.33–0.16+0.02M☉, the slope of the progenitor mass distribution is α=-2.96–0.25+0.45, and the maximum mass is greater than M{max}> 59M☉ with a 68% confidence. While these results are consistent with previous inferences, they also provide tighter constraints. The progenitor distribution is somewhat steeper than a Salpeter initial mass function (α = -2.35). This suggests that either SNR catalogs are biased against the youngest SF regions, or the most massive stars do not explode as easily as lower mass stars. If SNR catalogs are biased, it will most likely affect the slope but not the minimum mass. The uncertainties are dominated by three primary sources of uncertainty, the SFH resolution, the number of SF bursts, and the uncertainty on SF rate in each age bin. We address the first two of these uncertainties, with an emphasis on multiple bursts. The third will be addressed in future work.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): galaxies: individual: (M31, M33) - ISM: supernova remnants - methods: statistical - stars: evolution - supernovae: general

Simbad objects: 65

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Number of rows : 65
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 [LL2014] 8 SNR 00 40 14.1364 +40 37 15.290           ~ 4 0
2 [LL2014] 10 SNR 00 40 30.41 +40 43 16.7           ~ 5 0
3 [LL2014] 13 SNR 00 40 33.4444 +40 43 36.052           ~ 5 0
4 [LL2014] 14 SNR 00 40 33.6651 +40 32 47.130           ~ 5 0
5 [LL2014] 16 SNR 00 40 39.6545 +40 34 48.637           ~ 6 0
6 [LL2014] 32 SNR 00 41 34.0215 +41 14 52.199           ~ 4 0
7 BA 1-416 SNR 00 41 35.65 +41 06 56.8           ~ 27 0
8 [LL2014] 37 SNR 00 42 10.2894 +40 51 48.924           ~ 4 0
9 [LL2014] 42 SNR 00 42 25.4489 +40 52 24.575           ~ 4 0
10 [LL2014] 45 SNR 00 42 31.61 +41 06 04.7           ~ 5 0
11 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
12 [LL2014] 46 SNR 00 42 44.6995 +40 54 35.683           ~ 4 0
13 [LL2014] 47 SNR 00 42 47.1998 +41 01 20.366           ~ 4 0
14 [LL2014] 51 SNR 00 42 55.3954 +40 59 45.881           ~ 6 0
15 [WB92a] 86 SNR 00 43 03.775 +41 36 15.42           ~ 9 0
16 [LL2014] 59 SNR 00 43 08.7886 +41 03 06.588           ~ 4 0
17 [LL2014] 60 SNR 00 43 10.9843 +41 37 38.323           ~ 5 0
18 [LL2014] 62 SNR 00 43 14.5573 +40 54 32.731           ~ 4 0
19 [LL2014] 63 SNR 00 43 19.5039 +41 03 01.523           ~ 4 0
20 [LL2014] 64 SNR 00 43 22.7266 +41 06 35.438           ~ 4 0
21 [WB92a] 124 SNR 00 43 22.991 +41 05 53.17           ~ 5 0
22 [LL2014] 68 SNR 00 43 35.4206 +41 14 08.200           ~ 4 0
23 BA 1-55 PN 00 43 39.20 +41 26 52.9     20.35     ~ 35 1
24 [LL2014] 73 SNR 00 43 45.3305 +41 26 47.065           ~ 5 0
25 [LL2014] 75 SNR 00 43 47.3694 +41 12 52.834           ~ 4 0
26 [LL2014] 77 SNR 00 43 53.8644 +41 41 16.868           ~ 5 0
27 [LL2014] 82 SNR 00 44 01.10 +41 21 05.5     22.33     ~ 12 0
28 BA 1-83 SNR 00 44 05.0933 +41 27 18.857           ~ 7 0
29 [WB92a] 288 SNR 00 44 05.510 +41 20 12.26           ~ 7 0
30 [LL2014] 86 SNR 00 44 13.100 +41 50 28.21           ~ 7 0
31 [LL2014] 93 SNR 00 44 26.4294 +41 48 59.476           ~ 6 0
32 [WB92a] 425 SNR 00 44 28.157 +41 18 12.74           ~ 9 0
33 [LL2014] 95 SNR 00 44 29.5676 +41 52 44.105           ~ 6 0
34 [LL2014] 98 SNR 00 44 36.6165 +41 25 05.552           ~ 6 0
35 [LL2014] 100 SNR 00 44 38.8245 +41 25 26.810           ~ 6 0
36 [LL2014] 105 HII 00 44 46.00 +41 52 58.9     23.50     ~ 7 0
37 [WB92a] 567 SNR 00 44 49.525 +41 53 05.57           ~ 11 0
38 [LL2014] 109 SNR 00 44 50.5586 +41 54 22.925           ~ 4 0
39 [LL2014] 110 SNR 00 44 50.8584 +41 32 12.206           ~ 6 0
40 [LL2014] 113 SNR 00 44 54.4572 +41 31 52.320           ~ 6 0
41 [LL2014] 116 SNR 00 45 01.61 +41 59 29.8           ~ 6 0
42 [LL2014] 117 SNR 00 45 05.031 +41 38 51.70           ~ 9 0
43 [LL2014] 118 SNR 00 45 07.354 +41 35 44.17           ~ 8 0
44 [PAV78] 694 SNR 00 45 07.880 +41 32 23.26           ~ 7 0
45 [LL2014] 121 SNR 00 45 10.9152 +41 40 05.225           ~ 5 0
46 [LL2014] 122 SNR 00 45 12.1330 +41 50 17.506           ~ 6 0
47 [LL2014] 123 SNR 00 45 13.8437 +41 35 48.005           ~ 5 0
48 [LL2014] 125 SNR 00 45 15.2296 +41 34 24.618           ~ 6 0
49 USNO-B1.0 1317-00015312 SNR 00 45 25.899 +41 43 21.08           ~ 11 0
50 BA 1-187 SNR 00 45 27.853 +41 46 25.74           ~ 9 0
51 [LL2014] 136 SNR 00 45 28.7736 +41 46 31.350           ~ 5 0
52 [LL2014] 137 SNR 00 45 29.820 +41 47 33.69           ~ 7 0
53 [LL2014] 138 SNR 00 45 31.9270 +41 48 05.972           ~ 5 0
54 [LL2014] 139 SNR 00 45 35.5261 +41 58 08.202           ~ 6 0
55 [LL2014] 141 SNR 00 45 36.3963 +41 47 57.156           ~ 5 0
56 [LL2014] 142 SNR 00 45 37.8960 +41 50 21.034           ~ 5 0
57 [LL2014] 145 bub 00 45 56.651 +42 11 13.56           ~ 10 0
58 [LL2014] 146 SNR 00 46 04.1130 +41 50 12.095           ~ 5 0
59 [LL2014] 147 SNR 00 46 20.1 +41 53 04           ~ 7 0
60 BA 1-228 SNR 00 46 32.2920922344 +41 59 43.841736744     23.49     ~ 11 0
61 [LL2014] 151 SNR 00 46 33.7859 +41 59 36.474           ~ 3 0
62 [LL2014] 153 SNR 00 46 38.0940 +42 11 14.986           ~ 3 0
63 [LL2014] 154 SNR 00 46 39.0763 +42 07 17.364           ~ 4 0
64 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
65 SN 2003gd SN* 01 36 42.65 +15 44 19.9     13.2     SNIIP 267 2

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