2012ApJ...761...26J


Query : 2012ApJ...761...26J

2012ApJ...761...26J - Astrophys. J., 761, 26 (2012/December-2)

Supernova remnant progenitor masses in M31.

JENNINGS Z.G., WILLIAMS B.F., MURPHY J.W., DALCANTON J.J., GILBERT K.M., DOLPHIN A.E., FOUESNEAU M. and WEISZ D.R.

Abstract (from CDS):

Using Hubble Space Telescope photometry, we age-date 59 supernova remnants (SNRs) in the spiral galaxy M31 and use these ages to estimate zero-age main-sequence masses (MZAMS) for their progenitors. To accomplish this, we create color-magnitude diagrams (CMDs) and employ CMD fitting to measure the recent star formation history of the regions surrounding cataloged SNR sites. We identify any young coeval population that likely produced the progenitor star, then assign an age and uncertainty to that population. Application of stellar evolution models allows us to infer the MZAMS from this age. Because our technique is not contingent on identification or precise location of the progenitor star, it can be applied to the location of any known SNRs. We identify significant young star formation around 53 of the 59 SNRs and assign progenitor masses to these, representing a factor of ∼2 increase over currently measured progenitor masses. We consider the remaining six SNRs as either probable Type Ia candidates or the result of core-collapse progenitors that have escaped their birth sites. In general, the distribution of recovered progenitor masses is bottom-heavy, showing a paucity of the most massive stars. If we assume a single power-law distribution, dN/dM∝M α, then we find a distribution that is steeper than a Salpeter initial mass function (IMF) (α = -2.35). In particular, we find values of α outside the range -2.7 ≥ α ≥ -4.4 to be inconsistent with our measured distribution at 95% confidence. If instead we assume a distribution that follows a Salpeter IMF up to some maximum mass, then we find that values of MMax> 26 are inconsistent with the measured distribution at 95% confidence. In either scenario, the data suggest that some fraction of massive stars may not explode. The result is preliminary and requires more SNRs and further analysis. In addition, we use our distribution to estimate a minimum mass for core collapse between 7.0 and 7.8 M☉.

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Journal keyword(s): galaxies: individual: M31 - supernovae: general

Nomenclature: Table 1: [JWM2012] BW-NNN N=27 among (Nos 11-110).

Simbad objects: 67

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Number of rows : 67
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 [JWM2012] BW-11 SNR 00 40 59.2 +40 36 29           ~ 1 0
2 [MPV95] 2-016 HII 00 41 16.7 +40 57 19           ~ 2 0
3 BA 1-416 SNR 00 41 35.65 +41 06 56.8           ~ 27 0
4 [MPV95] 2-020 bub 00 41 48.2 +41 06 50           ~ 2 0
5 [MPV95] 2-021 HII 00 41 55.6 +40 46 49           ~ 5 0
6 [JWM2012] BW-19 SNR 00 42 09.8 +40 56 50           ~ 1 0
7 [AMB2011] HII 1547 SNR 00 42 10.39 +40 51 53.3           ~ 2 0
8 [MPV95] 2-024 HII 00 42 23.0 +41 00 13           ~ 2 0
9 [MPV95] 1-006 SNR 00 42 31.6 +41 06 02           ~ 1 0
10 [MPV95] 2-025 HII 00 42 34.8 +40 58 08           ~ 2 0
11 [MPV95] 2-026 HII 00 42 40.8 +41 02 41           ~ 2 0
12 M 31 AGN 00 42 44.330 +41 16 07.50 4.86 4.36 3.44     ~ 13622 1
13 [JWM2012] BW-31 SNR 00 42 55.6 +40 59 44           ~ 1 0
14 [JWM2012] BW-32 SNR 00 42 55.9 +40 58 18           ~ 1 0
15 [MPV95] 2-028 bub 00 42 57.0 +40 58 11           ~ 2 0
16 [MPV95] 1-008 SNR 00 43 04.2 +41 36 11           ~ 1 0
17 [JWM2012] BW-36 SNR 00 43 05.4 +41 22 30           ~ 1 0
18 [JWM2012] BW-39 SNR 00 43 10.4 +41 37 42           ~ 1 0
19 [MPV95] 1-009 SNR 00 43 11.4 +41 37 32           ~ 1 0
20 [MPV95] 1-010 SNR 00 43 11.5 +41 29 07           ~ 1 0
21 [JWM2012] BW-44 SNR 00 43 30.7 +41 41 18           ~ 1 0
22 [WB92a] 180 SNR 00 43 40.461 +41 10 53.20           ~ 8 0
23 [WB92a] 376 SNR 00 44 20.407 +41 34 49.58           ~ 8 0
24 [JWM2012] BW-60 SNR 00 44 21.2 +41 54 06           ~ 1 0
25 [AMB2011] HII 2888 SNR 00 44 25.30 +41 20 59.6           ~ 2 0
26 [WB92a] 446 HII 00 44 31.122 +41 21 25.88           ~ 8 0
27 [JWM2012] BW-65 SNR 00 44 35.7 +41 25 22           ~ 1 0
28 [JWM2012] BW-66 SNR 00 44 37.2 +41 52 00           ~ 2 0
29 [LL2014] 99 SNR 00 44 37.469 +41 24 47.80           ~ 8 0
30 [WB92a] 516 bub 00 44 40.772 +41 24 52.04           ~ 5 0
31 [WB92a] 526A SNR 00 44 41.3052 +41 27 55.058           ~ 8 0
32 [LL2014] 103 HII 00 44 43.5601 +41 26 15.702           ~ 8 0
33 [LL2014] 104 SNR 00 44 43.7622 +41 57 52.805           ~ 5 0
34 [WB92a] 527A bub 00 44 44.0 +41 26 47           ~ 6 0
35 [JWM2012] BW-71 SNR 00 44 47.0 +41 29 19           ~ 1 0
36 [MPV95] 2-044 HII 00 44 47.7 +41 27 55           ~ 2 0
37 [WB92a] 567 SNR 00 44 49.525 +41 53 05.57           ~ 11 0
38 [WB92a] 574 SNR 00 44 50.409 +41 27 53.77           ~ 10 0
39 2MASS J00445095+4129058 SNR 00 44 50.950 +41 29 05.86           ~ 17 0
40 USNO-B1.0 1319-00013971 SNR 00 44 52.815 +41 54 58.03           ~ 13 0
41 [JWM2012] BW-76 SNR 00 44 54.4 +41 30 44           ~ 1 0
42 [JWM2012] BW-77 SNR 00 44 54.4816828680 +41 31 48.182694744           ~ 3 0
43 [JWM2012] BW-81 SNR 00 45 08.6 +41 36 36           ~ 1 0
44 [AMB2011] HII 3365 SNR 00 45 09.41 +41 51 07.9           ~ 2 0
45 [MPV95] 2-046 HII 00 45 10.3 +41 35 57           ~ 2 0
46 BA 1-160 SNR 00 45 14.00 +41 36 14.1     21.42     ~ 32 0
47 [JWM2012] BW-84 SNR 00 45 15.9 +41 39 22           ~ 1 0
48 [MPV95] 2-049 bub 00 45 18.10 +41 52 04.4           ~ 3 0
49 [JWM2012] BW-86 SNR 00 45 21.3 +41 40 00           ~ 1 0
50 [JWM2012] BW-89 SNR 00 45 27.6 +41 54 13           ~ 1 0
51 [MPV95] 2-050 SNR 00 45 27.9 +41 52 11           ~ 1 0
52 [WB92a] 856A SNR 00 45 43.5 +41 55 53           ~ 3 1
53 [JWM2012] BW-102 SNR 00 45 52.2 +42 09 42           ~ 1 0
54 [LL2014] 145 bub 00 45 56.651 +42 11 13.56           ~ 10 0
55 [WB92a] 891 bub 00 46 09.725 +42 13 11.13           ~ 6 0
56 [LL2014] 148 SNR 00 46 29.553 +41 58 06.63           ~ 10 0
57 [JWM2012] BW-105 SNR 00 46 31.1 +41 59 19           ~ 1 0
58 [JWM2012] BW-106 SNR 00 46 34.0 +42 10 49           ~ 1 0
59 BA 1-679 SNR 00 46 35.206 +42 13 35.65           ~ 10 0
60 [WB92a] 947 SNR 00 46 40.523 +42 11 28.04           ~ 9 0
61 [WB92a] 956A SNR 00 46 43.002 +42 13 01.70           ~ 6 0
62 [AMB2011] HII 3934 SNR 00 46 45.60 +42 13 04.8           ~ 2 0
63 AT 2008jd ev 00 54 34.16 -37 38 28.6           ~ 134 1
64 M 33 GiG 01 33 50.8965749232 +30 39 36.630403128 6.17 6.27 5.72     ~ 6226 1
65 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
66 SN 2012aw SN* 10 43 53.735 +11 40 17.63       15   SNIIP 252 1
67 SN 2011dh SN* 13 30 05.10555 +47 10 10.9227           SNIIb 445 1

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