2021ApJ...908...51F


Query : 2021ApJ...908...51F

2021ApJ...908...51F - Astrophys. J., 908, 51-51 (2021/February-2)

Early-time light curves of Type Ia supernovae observed with TESS.

FAUSNAUGH M.M., VALLELY P.J., KOCHANEK C.S., SHAPPEE B.J., STANEK K.Z., TUCKER M.A., RICKER G.R., VANDERSPEK R., LATHAM D.W., SEAGER S., WINN J.N., JENKINS J.M., BERTA-THOMPSON Z.K., DAYLAN T., DOTY J.P., FURESZ G., LEVINE A.M., MORRIS R., PAL A., SHA L., TING E.B. and WOHLER B.

Abstract (from CDS):

We present the early-time light curves of Type Ia supernovae (SNe Ia) observed in the first six sectors of Transiting Exoplanet Survey Satellite (TESS) data. Ten of these SNe were discovered by ASAS-SN, seven by ATLAS, six by ZTF, and one by Gaia. For nine of these objects with sufficient dynamic range (>3.0 mag from detection to peak), we fit power-law models and searched for signatures of companion stars. We found a diversity of early-time light-curve shapes, although most of our sources are consistent with fireball models where the flux increases as ∝t2. Three SNe displayed a flatter rise with flux ∝t. We did not find any obvious evidence for additional structures, such as multiple power-law components, in the early rising light curves. For assumptions about the SN properties and the observer viewing angle (ejecta mass of 1.4 M☉, expansion velocity of 104 km s–1, opacity of 0.2 cm2 g–1, and viewing angle of 45°) and a further assumption that any companion stars would be in Roche lobe overflow, it is possible to place upper limits on the radii of any companion stars. Six of the nine SNe had complete coverage of the early-time light curves, and we placed upper limits on the radii of companion stars of <=32 R☉ for these SNe, <=20 R☉ for five of the six, and <=4 R☉ for two of the six. The small sample size did not allow us to put limits on the occurrence rate of companion stars in the progenitors of SNe Ia. However, we expect that TESS observed enough SNe in its two-year primary mission (26 sectors) to either detect the signature of a large companion (R > 20 R☉) or constrain the occurrence rate of such systems, at least for the fiducial SN properties adopted here. We also show that TESS is capable of detecting emission from a 1 R☉ companion for an SN Ia within 50 Mpc and has a reasonable chance of doing so after about six years.

Abstract Copyright: © 2021. The American Astronomical Society. All rights reserved.

Journal keyword(s): Type Ia supernovae - Supernovae

VizieR on-line data: <Available at CDS (J/ApJ/908/51): table1.dat table2.dat table5.dat refs.dat>

Simbad objects: 46

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Number of rows : 46
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 2018hka SN* 00 39 20.075 -10 28 44.29           SNIa 4 0
2 SN 2018fub SN* 00 40 30.650 -50 41 15.14           SNIa 4 0
3 SN 2018hgc SN* 00 42 04.560 -02 37 44.51           SNIa 7 0
4 SN 2018hkb SN* 01 02 38.399 -06 23 33.44           SNIa 5 0
5 SN 2018hlp SN* 01 27 34.852 -12 26 43.71           SNIa 2 0
6 SN 2018hrs SN* 01 55 09.981 +02 29 04.75           SNIa 3 0
7 SN 2018fvi SN* 01 57 42.560 -67 11 12.80           SNIa 6 0
8 SN 2018ieu SN* 02 07 10.870 -09 01 28.65           SNIa 4 0
9 SN 2018huc SN* 02 22 19.361 -12 09 10.87           SNIa 4 0
10 SN 2018hyy SN* 02 31 55.420 +03 07 33.78           SNIa 3 0
11 SN 2018hib SN* 02 56 21.270 -32 11 08.77           SNIa 6 0
12 SN 2018hpu SN* 03 18 21.293 -41 36 34.85           SNIa 4 0
13 SN 2012fr SN* 03 33 35.99 -36 07 37.7           SNIa-norm 178 1
14 SN 2018hsz SN* 03 56 20.719 -54 00 40.14           SNIa 3 0
15 SN 2018hkx SN* 04 00 53.810 -66 40 30.61           SNIa 4 0
16 SN 2018hzh SN* 04 07 12.870 -37 03 10.44           SNIa 2 0
17 SN 2018hss SN* 04 13 00.250 -53 59 31.27           SNIa 3 0
18 SN 2018jeb SN* 04 13 55.028 -06 16 35.77           SNIa 3 0
19 SN 2018fhw SN* 04 18 06.266 -63 36 54.25           SNIa 47 0
20 SN 2018ioa SN* 04 20 32.120 -38 57 35.89           SNIa 4 0
21 SN 2018itr SN* 04 30 18.842 -05 42 11.31           SNIa 5 0
22 SN 2018iyx SN* 04 33 32.450 -01 38 51.06           SNIa 5 0
23 SN 2018hdo SN* 04 42 37.960 -53 16 01.13           SNIa 2 0
24 SN 2018jnd SN* 04 49 25.498 -13 36 59.85           SNIa 3 0
25 SN 2018koy SN* 05 41 13.760 -13 13 27.12           SNIa 9 0
26 SN 2018kfv SN* 05 50 34.641 +13 17 57.13           SNIa 4 0
27 SN 2018lla SN* 05 58 17.006 +05 48 16.83           SNIa 2 0
28 SN 2018jwi SN* 06 18 39.283 -54 28 14.31           SNIa 6 0
29 AT 2019ahk ev 07 00 11.410 -66 02 25.16           ~ 57 0
30 SN 2018oh SN* 09 06 39.6 +19 20 18           SNIa-norm 91 0
31 SN 2014J SN* 09 55 42.12 +69 40 25.9           SNIa-norm 456 1
32 SN 2012cg SN* 12 27 12.83 +09 25 13.2           SNIa-norm 224 1
33 SN 2019yvq SN* 12 27 21.850 +64 47 59.82           SNIa 49 0
34 ASASSN -14bd SN* 12 52 44.8 +26 28 13           SNIa 102 0
35 SN 2016bln SN* 13 34 45.6 +13 51 14           SNIa-norm 62 0
36 SN 2011fe SN* 14 03 05.711 +54 16 25.22   10.12 10.06     SNIa-norm 747 1
37 SN 2017cbv SN* 14 32 34.420 -44 08 02.74           SNIa 146 0
38 NAME Kepler's SN SNR 17 30 40.51 -21 29 14.4           ~ 851 3
39 SN 2018eod SN* 20 53 19.66 -33 25 24.8           SNIa 3 0
40 SN 2018exc SN* 21 00 08.02 -40 21 30.9           SNIa 6 0
41 SN 2018evo SN* 21 48 38.420 -43 22 48.07           SNIa 2 0
42 SN 2013dy SN* 22 18 17.5 +40 34 09           SNIa-norm 128 0
43 SN 2018fqn SN* 22 39 38.020 -15 05 08.66           SNIa 6 0
44 SN 2018grv SN* 22 45 31.856 -16 07 05.64           SNIa 4 0
45 SN 2018fwi SN* 22 47 46.560 -31 15 33.70           SNIa 3 0
46 SN 2018fzi SN* 23 39 47.310 -23 55 12.81           SNIa 5 0

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