2022ApJ...927..224S


Query : 2022ApJ...927..224S

2022ApJ...927..224S - Astrophys. J., 927, 224-224 (2022/March-2)

Luminosity Function and Event Rate Density of XMM-Newton-selected Supernova Shock Breakout Candidates.

SUN H., LIU H.-Y., PAN H.-W., LIU Z., ALP D., HU J., LI Z., ZHANG B. and YUAN W.

Abstract (from CDS):

A dozen X-ray supernova shock breakout (SN SBO) candidates were reported recently based on XMM-Newton archival data, which increased the X-ray-selected SN SBO sample by an order of magnitude. Assuming that they are genuine SN SBOs, we study the luminosity function (LF) by improving on the method used in our previous work. The light curves and the spectra of the candidates were used to derive the maximum volume within which these objects could be detected with XMM-Newton by simulation. The results show that the SN SBO LF can be described by either a broken power law (BPL) with indices (at the 68% confidence level) of 0.48 ± 0.28 and 2.11 ± 1.27 before and after the break luminosity at log(L_\/erg {s}^{-1}) = 45.32 ± 0.55 or a single power law (SPL) with an index of 0.80 ± 0.16. The local event rate densities of SN SBOs above 5 x 1042 erg s–1 are consistent for two models, i.e., {4.6}_{-1.3}^{+1.7}×{10}^{4} Gpc–3 yr–1 and {4.9}_{-1.4}^{+1.9}×{10}^{4} Gpc–3 yr–1 for BPL and SPL models, respectively. The number of fast X-ray transients of SN SBO origin can be significantly increased by wide-field X-ray telescopes such as the Einstein Probe.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Time domain astronomy - X-ray transient sources - Luminosity function - Core-collapse supernovae

Simbad objects: 23

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Number of rows : 23
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 [AL2020] XT 070618 SN? 01 37 06.05 -12 57 10.1           ~ 4 0
2 3XMM J015709.1+373739 SN? 01 57 09.16 +37 37 38.4           ~ 5 0
3 EXMM J023135.0-603743 SN? 02 31 35.0 -60 37 43           ~ 7 0
4 [AL2020] XT 140811 SN? 02 54 36.85 +41 04 27.5           ~ 3 0
5 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
6 [BTS2017] CDF-S XT2 G 03 32 18.38112 -27 52 23.8692   26.509     24.598 ~ 46 0
7 [BTS2017] CDF-S XT1 G 03 32 38.8 -27 51 34           ~ 40 0
8 SN 1987A SN* 05 35 27.98840 -69 16 11.1134           SNIIpec 5203 2
9 SN 2010bh SN* 07 10 30.63 -56 15 19.7           SNIc 336 1
10 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
11 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
12 SN 2008D SN* 09 09 30.625 +33 08 20.16     17.5     SNIb 458 1
13 GRB 061218 gB 09 56 57.000 -35 13 15.90           ~ 26 0
14 [AL2020] XT 151128 SN? 11 08 18.69 -05 04 30.6           ~ 4 0
15 SN 2017iuk SN* 11 09 39.49 -12 35 18.7           SNII 210 0
16 [AL2020] XT 040610 SN? 11 18 08.70 +07 42 09.6           ~ 3 0
17 3XMM J113407.5+005223 SN? 11 34 07.43 +00 52 24.7           ~ 5 0
18 [AL2020] XT 060207 SN? 13 07 19.60 -40 27 38.3           ~ 5 0
19 [AL2020] XT 160220 SN? 13 36 47.98 -41 20 14.5           ~ 3 0
20 [AL2020] XT 161028 SN? 17 32 56.79 +43 30 45.0           ~ 3 0
21 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
22 [AL2020] XT 050925 SN? 20 45 44.94 -67 38 49.3           ~ 2 0
23 [AL2020] XT 100424 SN? 21 27 11.21 -12 02 20.6           ~ 3 0

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