2014MNRAS.440.1917D


Query : 2014MNRAS.440.1917D

2014MNRAS.440.1917D - Mon. Not. R. Astron. Soc., 440, 1917-1924 (2014/May-3)

On the lack of X-ray bright Type IIP supernovae.

DWARKADAS V.V.

Abstract (from CDS):

Type IIP supernovae (SNe) are expected to arise from red supergiant stars (RSGs). These stars have observed mass-loss rates that span more than two orders of magnitude, from less than 10^-6 M_☉/yr to almost 10^-4 M_☉/yr. Thermal bremsstrahlung X-ray emission from at least some IIPs should reflect the larger end of the high mass-loss rates. Strangely, no IIP SNe are seen where the X-ray luminosity is large enough to suggest mass-loss rates greater than about 10^-5 M_☉/yr. We investigate if this could be due to absorption of the X-ray emission. After carefully studying all the various aspects, we conclude that absorption would not be large enough to prevent us from having detected X-ray emission from high mass-loss rate IIPs. This leads us to the conclusion that there may be an upper limit of ∼ 10^-5 M_☉/yr to the mass-loss rate of Type IIP progenitors, and therefore to the luminosity of RSGs that explode to form Type IIPs. This in turn suggests an upper limit of \lesssim 19 M_☉ for the progenitor mass of a Type IIP SN. This limit is close to that obtained by direct detection of IIP progenitors, as well as that suggested by recent stellar evolution calculations. Although the statistics need to be improved, many current indicators support the notion that RSGs above ∼ 19 M_☉ do not explode to form Type IIP SNe.

Abstract Copyright: © 2014 The Author Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): shock waves - circumstellar matter - stars: massive - supernovae: general - stars: winds, outflows - X-rays: ISM

Simbad objects: 32

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Number of rows : 32
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 SN 2003gd SN* 01 36 42.65 +15 44 19.9     13.2     SNIIP 267 2
2 SN 2012ec SN* 02 45 59.89 -07 34 25.0         22.32 SNIIP 92 3
3 SN 2001du SN* 03 33 29.11 -36 08 32.5     14.0     SNIIP 58 1
4 SN 2009bw SN* 03 56 06.92 +72 55 40.9           SNII 70 1
5 SN 1999em SN* 04 41 27.04 -02 51 45.2   13.79 13.7     SNIIP 727 1
6 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 19090 0
7 SN 2006bc SN* 07 21 16.50 -68 59 57.3   17.6 16.0     SNIIP 52 1
8 2MASS J07371703+6535579 HXB 07 37 17.0432126424 +65 35 57.826001220           SNIIP 317 1
9 SN 2003Z SN* 09 07 32.46 +60 29 17.5     16.7     SNIIP 83 1
10 SN 1993J SN* 09 55 24.77476 +69 01 13.7026   10.8 12.0     SNIIb 1507 1
11 CXOU J095546.6+694037 HXB 09 55 46.6536476856 +69 40 37.899496056           SNIIP 51 1
12 SN 1999gi SN* 10 18 16.66 +41 26 28.2   14.8       SNIIP 248 1
13 SN 2012A SN* 10 25 07.39 +17 09 14.6           SNIIP 135 0
14 SN 2012aw SN* 10 43 53.735 +11 40 17.63       15   SNIIP 252 1
15 SN 2007aa SN* 12 00 27.69 -01 04 51.6 16.9 16.4 5.8     SNIIP 78 1
16 SN 1999an SN* 12 01 10.57 +14 06 12.3     15     SNII 29 1
17 SN 2003ie SN* 12 03 18.15 +44 31 34.6     15.2     SNIIP 40 1
18 SN 1999ev SN* 12 19 48.21336 +29 37 21.3492     14.4     SNIIP 47 1
19 SN 2006ov SN* 12 21 55.30 +04 29 16.7     14.9     SNIIP 88 1
20 SN 2008in SN* 12 22 01.77 +04 28 47.5           SNIIP 117 1
21 SN 2006my SN* 12 43 40.74 +16 23 14.1     15.3     SNIIP 64 1
22 SN 1999br SN* 13 00 41.80 +02 29 45.8     17.5     SNIIPp 171 1
23 SN 2011ja SN* 13 05 11.12 -49 31 27.0           SNIIP 48 0
24 SN 2005cs SN* 13 29 53.37 +47 10 28.2   14.5       SNIIP 450 1
25 SN 2004dg SN* 14 59 58.96 +01 53 25.6     17.1     SNIIP 40 1
26 SN 2000cb SN* 16 01 32.15 +01 42 23.0     18.0     SNII 57 1
27 SN 2009kf SN* 16 12 54.00 +55 38 13.8           SNIIP 53 1
28 SN 2004A SN* 16 43 01.90 +36 50 12.5     15.7     SNIIP 90 1
29 SN 2002hh SN* 20 34 44.29 +60 07 19.0     17.18     SNIIP 158 1
30 SN 2004et SN* 20 35 25.33 +60 07 17.7   12.88       SNIIP 547 1
31 SN 2007od SN* 23 55 48.68 +18 24 54.8       14.4   SNIIP 147 1
32 SN 2008bk SN* 23 57 50.42 -32 33 21.5           SNIIP 167 2

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