2025A&A...698A..78R


Query : 2025A&A...698A..78R

2025A&A...698A..78R - Astronomy and Astrophysics, volume 698A78 (2025/6-1)

A magnetar powers the luminous supernova 2023pel, which is associated with a long gamma-ray burst.

ROMAN AGUILAR L.M., SAEZ M.M., ERTINI K. and BERSTEN M.C.

Abstract (from CDS):

Aims. We explore supernova (SN) 2023pel, the most recent event associated with gamma-ray bursts (GRBs), specifically GRB 230812B. SN 2023pel has a high luminosity (∼1.5 × 1043 erg s–1 at the peak) and low expansion velocities (v ∼ 16 000 km s–1 at the peak) compared to other GRB-SNe. These properties seem difficult to reconcile with a single nickel power source. We searched for models that can explain the properties of this event.
Methods. We calculated a grid of hydrodynamic models based on pre-SN structures derived from evolutionary calculations. We compared our models with observations of SN 2023pel and selected our preferred model using statistical analysis, taking both light curves and expansion velocities into account. This allowed us to derive a set of physical properties for SN 2023pel.
Results. Our models suggest that the most probable scenario involves a millisecond magnetar as the primary power source, supplemented by energy from radioactive decay. Our preferred model has a spin period of P = 3.2 ms, a magnetic field of B = 28 × 1014 G, an explosion energy of 2.3 foe, a nickel mass of MNi = 0.24 M⊙, and an ejected mass of 3.4 M⊙. Alternatively, we find that a purely nickel-powered model also provides a good match with the observations, though MNi ≥ 0.8 M⊙ are always required. However, the combination of such high values of MNi and low Mej is difficult to reconcile, indicating that this scenario is less probable. We have also identified a specific region within the peak luminosity-velocity plane where an additional energy source beyond nickel may be necessary to power SNe with characteristics similar to SN 2023pel.
Conclusions. Our study indicates that an additional energy source beyond radioactive decay is essential to explain the high brightness and relatively low expansion velocities of SN 2023pel. A magnetar-powered model, similar to the models proposed for the very luminous GRB-SN 2011kl, aligns well with these characteristics.

Abstract Copyright: © The Authors 2025

Journal keyword(s): hydrodynamics - stars: magnetars - supernovae: individual: SN 2023pel - gamma rays: stars - gamma-ray burst: individual: GRB 230812B

Simbad objects: 18

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Number of rows : 18
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 CRTS MLS151203 J000922-000407 SN* 00 09 21.67 -00 04 06.5           SNIc 9 0
2 SN 2011kl SN* 00 57 22.64 -46 48 03.6           SNSLSN 268 1
3 SN 2002ap SN* 01 36 23.85 +15 45 13.2   13.11 14.54     SNIc-BL 587 1
4 SN 2006aj SN* 03 21 39.670 +16 52 02.27 17.96 19.11 17.40     SNIc-BL 1007 1
5 SN 2016jca SN* 06 06 51.36 -26 47 29.7           SNIc 140 0
6 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
7 SN 2012bz SN* 09 07 38.38 +14 01 07.5           SNIb/c 193 1
8 SN 2009bb SN* 10 31 33.92 -39 57 28.2           SNIc 185 1
9 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
10 SN 2013dx SN* 14 29 14.77 +15 46 26.6           ~ 178 0
11 SN 2020bvc SN* 14 33 57.009 +40 14 37.62           SNIc-BL 61 0
12 iPTF 14dby SN* 15 17 06.29 +25 21 11.4           SNIc 13 0
13 SN 2023pel SN* 16 36 31.483 +47 51 32.26           SNIc-BL 8 0
14 GRB 230812B gB 16 36 31.49 +47 51 31.3           ~ 89 0
15 PTF 10qts SN* 16 41 37.60 +28 58 21.1           SNIc 27 0
16 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
17 SN 2017dby SN* 20 04 44.89 -09 56 08.6           SNIa 2 0
18 SN 2003jd SN* 23 21 03.38 -04 53 45.5   16.34       SNIc-BL 147 1

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