---
title: 'SN 2023ixf: A Nearby Type II Supernova'
url: https://www.emergentmind.com/topics/sn-2023ixf
type: topic
---

# SN 2023ixf: A Nearby Type II Supernova

SN 2023ixf is a Type II supernova in Messier 101, at a distance quoted as \(6.85\)–\(6.9\) Mpc, discovered on 2023 May 19 and followed from within about a day of first light into the nebular phase. Because it was the closest supernova in the last decade and because pre-explosion HST, Spitzer, and ground-based imaging exist at its site, SN 2023ixf quickly became a central case for studying flash spectroscopy, delayed shock breakout in dense circumstellar material (CSM), red-supergiant progenitors, asymmetric mass loss, and late-time dust formation [2507.08078, 2306.04721].

## 1. Discovery, rise, and photometric classification

SN 2023ixf was discovered by Itagaki on 2023 May 19.727 UTC at an unfiltered magnitude of \(14.9\pm0.1\), with first light constrained to \(\mathrm{MJD}\ 60082.743 \pm 0.083\) in one analysis and to \(\mathrm{MJD}=60082.788^{+0.02}_{-0.05}\) in another [2307.03165, 2503.13974]. A globally distributed follow-up effort produced unusually dense coverage. In particular, the Unistellar Network assembled 252 observations from 115 telescopes beginning 2 days before the first known detection, and measured a peak \(M_V=-18.18\pm0.09\) at 2023-05-25 21:37 UTC [2307.14347]. Other studies reported a luminous peak near \(M_V\approx-18.2\) mag, a rapid rise of about 5 days, and an early plateau near \(M_V\approx-17.6\) mag with a decline rate of about \(0.03\) mag day\(^{-1}\) during the first month [2307.03165].

The light curve was brighter than that of typical Type II supernovae at early times. One early analysis reported peak absolute magnitudes \(M_u=-18.6\) mag and \(M_g=-18.4\) mag, more than \(2\) mag brighter than typical Type II supernovae, and interpreted that photometric boost as consistent with shock power supplied by CSM interaction [2306.04721]. Later studies variously described SN 2023ixf as a possible II-L subtype, a fast-decliner or IIL event with a relatively short plateau of fewer than \(\sim 70\) days, and also as a normal Type II-P supernova in terms of explosion parameters and photospheric-phase modeling [2503.13974, 2310.14407]. A common point across these classifications is that the spectrum was only briefly IIn-like: very narrow flash-ionization features dominated for less than a week and then faded, unlike genuine SNe IIn with prolonged interaction [2503.13974].

## 2. Early flash spectroscopy and the confined inner CSM

The earliest optical spectra showed the characteristic “flash” phenomenon. Emission lines of H I, He I/II, C IV, and N III/IV/V exhibited narrow cores plus broad, symmetric electron-scattering wings, and these profiles persisted for \(\sim 8\) days with respect to first light [2306.04721]. During the first \(\sim 2\) days the ionization state increased, while the \(U-V\) color evolved blueward from \(-0.86\pm0.03\) mag at 1.26 d to \(-1.01\pm0.04\) mag at 3.39 d, corresponding approximately to a temperature increase from \(\sim 12{,}000\) K to \(\sim 16{,}000\) K [2307.03165]. These results were interpreted as evidence for delayed shock breakout inside dense CSM rather than at the bare stellar surface.

The radial extent of the densest inner CSM was inferred to be compact. From the disappearance of flash features and the onset of broad ejecta lines, one study placed the dense CSM at \(r=(0.5-1)\times10^{15}\) cm and found a reduction in CSM density at \(r\gtrsim10^{15}\) cm [2306.04721]. Another study inferred a compact extent of \(\sim(3-7)\times10^{14}\) cm from the timescale of CSM interaction [2307.03165]. CMFGEN and HERACLES comparisons suggested dense, solar-metallicity CSM and a progenitor mass-loss rate of \(\dot{M}=10^{-2}\ M_\odot\,\mathrm{yr}^{-1}\); for an assumed wind velocity of \(v_w=50\

Source: https://www.emergentmind.com/topics/sn-2023ixf