Early Spectroscopy and Dense Circumstellar Medium Interaction in SN 2023ixf
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Author
Bostroem, K.A.Pearson, J.
Shrestha, M.
Sand, D.J.
Valenti, S.
Jha, S.W.
Andrews, J.E.
Smith, N.
Terreran, G.
Green, E.
Dong, Y.
Lundquist, M.
Haislip, J.
Hoang, E.T.
Hosseinzadeh, G.
Janzen, D.
Jencson, J.E.
Kouprianov, V.
Paraskeva, E.
Meza, Retamal, N.E.
Reichart, D.E.
Arcavi, I.
Bonanos, A.Z.
Coughlin, M.W.
Dobson, R.
Farah, J.
Galbany, L.
Gutiérrez, C.
Hawley, S.
Hebb, L.
Hiramatsu, D.
Howell, D.A.
Iijima, T.
Ilyin, I.
Jhass, K.
McCully, C.
Moran, S.
Morris, B.M.
Mura, A.C.
Müller-Bravo, T.E.
Munday, J.
Newsome, M.
Pabst, M.T.
Ochner, P.
Gonzalez, E.P.
Pastorello, A.
Pellegrino, C.
Piscarreta, L.
Ravi, A.P.
Reguitti, A.
Salo, L.
Vinkó, J.
de Vos, K.
Wheeler, J.C.
Williams, G.G.
Wyatt, S.
Affiliation
Steward Observatory, University of ArizonaIssue Date
2023-10-06
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American Astronomical SocietyCitation
K. Azalee Bostroem et al 2023 ApJL 956 L5Journal
Astrophysical Journal LettersRights
© 2023. The Author(s). Published by the American Astronomical Society. Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence.Collection Information
This item from the UA Faculty Publications collection is made available by the University of Arizona with support from the University of Arizona Libraries. If you have questions, please contact us at repository@u.library.arizona.edu.Abstract
We present the optical spectroscopic evolution of SN 2023ixf seen in subnight cadence spectra from 1.18 to 15 days after explosion. We identify high-ionization emission features, signatures of interaction with material surrounding the progenitor star, that fade over the first 7 days, with rapid evolution between spectra observed within the same night. We compare the emission lines present and their relative strength to those of other supernovae with early interaction, finding a close match to SN 2020pni and SN 2017ahn in the first spectrum and SN 2014G at later epochs. To physically interpret our observations, we compare them to CMFGEN models with confined, dense circumstellar material around a red supergiant (RSG) progenitor from the literature. We find that very few models reproduce the blended N iii (λλ4634.0,4640.6)/C iii (λλ4647.5,4650.0) emission lines observed in the first few spectra and their rapid disappearance thereafter, making this a unique diagnostic. From the best models, we find a mass-loss rate of 10−3-10−2 M ⊙ yr−1, which far exceeds the mass-loss rate for any steady wind, especially for an RSG in the initial mass range of the detected progenitor. These mass-loss rates are, however, similar to rates inferred for other supernovae with early circumstellar interaction. Using the phase when the narrow emission features disappear, we calculate an outer dense radius of circumstellar material R CSM,out ≈ 5 × 1014 cm, and a mean circumstellar material density of ρ = 5.6 × 10−14 g cm−3. This is consistent with the lower limit on the outer radius of the circumstellar material we calculate from the peak Hα emission flux, R CSM,out ≳ 9 × 1013 cm. © 2023. The Author(s). Published by the American Astronomical Society.Note
Open access journalISSN
2041-8205Version
Final Published Versionae974a485f413a2113503eed53cd6c53
10.3847/2041-8213/acf9a4
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Except where otherwise noted, this item's license is described as © 2023. The Author(s). Published by the American Astronomical Society. Original content from this work may be used under the terms of the Creative Commons Attribution 4.0 licence.

