2025ApJ...985...51N


Query : 2025ApJ...985...51N

2025ApJ...985...51N - Astrophys. J., 985, 51 (2025/May-3)

Dinosaur in a Haystack: X-Ray View of the Entrails of SN 2023ixf and the Radio Afterglow of Its Interaction with the Medium Spawned by the Progenitor Star (Paper I).

NAYANA A.J., MARGUTTI R., WISTON E., CHORNOCK R., CAMPANA S., LASKAR T., MURASE K., KRIPS M., MIGLIORI G., TSUNA D., ALEXANDER K.D., CHANDRA P., BIETENHOLZ M., BERGER E., CHEVALIER R.A., DE COLLE F., DESSART L., DIESING R., GREFENSTETTE B.W., JACOBSON-GALAN W.V., MAEDA K., MARCOTE B., MATTHEWS D., MILISAVLJEVIC D., RAY A.K., REGUITTI A. and POLZIN A.

Abstract (from CDS):

We present the results from our extensive hard-to-soft X-ray (NuSTAR, Swift-XRT, XMM-Newton, Chandra) and meter-to-millimeter-wave radio (Giant Metrewave Radio Telescope, Very Large Array, NOEMA) monitoring campaign of the very nearby (d = 6.9 Mpc) Type II supernova (SN) 2023ixf spanning ≈4-165 days post-explosion. This unprecedented data set enables inferences on the explosion's circumstellar medium (CSM) density and geometry. In particular, we find that the luminous X-ray emission is well modeled by thermal free-free radiation from the forward shock with rapidly decreasing photoelectric absorption with time. The radio spectrum is dominated by synchrotron radiation from the same shock. Similar to the X-rays, the level of free-free absorption affecting the radio spectrum rapidly decreases with time as a consequence of the shock propagation into the dense CSM. While the X-ray and the radio modeling independently support the presence of a dense medium corresponding to an effective mass-loss rate $\dot{M}\approx 1{0}^{-4}\,{M}_{\odot }\,{\mathrm{yr}}^{-1}$ at R = (0.4-14) × 1015 cm (for vw = 25 km s–1), our study points at a complex CSM density structure with asymmetries and clumps. The inferred densities are ≈10-100 times those of typical red supergiants, indicating an extreme mass-loss phase of the progenitor in the ≈200 yr preceding core collapse, which leads to the most X-ray luminous Type II SN and the one with the most delayed emergence of radio emission. These results add to the picture of the complex mass-loss history of massive stars on the verge of collapse and demonstrate the need for panchromatic campaigns to fully map their intricate environments.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Core-collapse supernovae - Radio transient sources - X-ray transient sources

Simbad objects: 13

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Number of rows : 13
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 2013ej SN* 01 36 48.16 +15 45 31.0           SNIIP 248 0
2 SN 1999em SN* 04 41 27.04 -02 51 45.2   13.79 13.7     SNIIP 727 1
3 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1169 0
4 2MASS J07371703+6535579 HXB 07 37 17.0432126424 +65 35 57.826001220           SNIIP 317 1
5 SN 1993J SN* 09 55 24.77476 +69 01 13.7026   10.8 12.0     SNIIb 1507 1
6 SN 2012aw SN* 10 43 53.735 +11 40 17.63       15   SNIIP 252 1
7 SN 2016X SN* 12 55 15.50 +00 05 59.7           SNIIb 61 0
8 M 101 GiP 14 03 12.583 +54 20 55.50   8.46 7.86 7.76   ~ 3138 2
9 SN 2023ixf SN* 14 03 38.562 +54 18 41.94           SNII 209 0
10 IRC +10420 pA* 19 26 48.0979492536 +11 21 16.758531216   13.98 11.66     F8Ia+e 492 0
11 SN 2017eaw SN* 20 34 44.238 +60 11 36.00           SNIIP 180 0
12 SN 2004et SN* 20 35 25.33 +60 07 17.7   12.88       SNIIP 547 1
13 SN 2014C SN* 22 37 05.60 +34 24 31.9           SNIb 167 1

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