TY - JOUR
T1 - Early Spectroscopy and Dense Circumstellar Medium Interaction in SN 2023ixf
AU - Bostroem, K. Azalee
AU - Pearson, Jeniveve
AU - Shrestha, Manisha
AU - Sand, David J.
AU - Valenti, Stefano
AU - Jha, Saurabh W.
AU - Andrews, Jennifer E.
AU - Smith, Nathan
AU - Terreran, Giacomo
AU - Green, Elizabeth
AU - Dong, Yize
AU - Lundquist, Michael
AU - Haislip, Joshua
AU - Hoang, Emily T.
AU - Hosseinzadeh, Griffin
AU - Janzen, Daryl
AU - Jencson, Jacob E.
AU - Kouprianov, Vladimir
AU - Paraskeva, Emmy
AU - Meza Retamal, Nicolas E.
AU - Reichart, Daniel E.
AU - Arcavi, Iair
AU - Bonanos, Alceste Z.
AU - Coughlin, Michael W.
AU - Dobson, Ross
AU - Farah, Joseph
AU - Galbany, Lluís
AU - Gutiérrez, Claudia
AU - Hawley, Suzanne
AU - Hebb, Leslie
AU - Hiramatsu, Daichi
AU - Howell, D. Andrew
AU - Iijima, Takashi
AU - Ilyin, Ilya
AU - Jhass, Kiran
AU - McCully, Curtis
AU - Moran, Sean
AU - Morris, Brett M.
AU - Mura, Alessandra C.
AU - Müller-Bravo, Tomás E.
AU - Munday, James
AU - Newsome, Megan
AU - Pabst, Maria Th
AU - Ochner, Paolo
AU - Gonzalez, Estefania Padilla
AU - Pastorello, Andrea
AU - Pellegrino, Craig
AU - Piscarreta, Lara
AU - Ravi, Aravind P.
AU - Reguitti, Andrea
AU - Salo, Laura
AU - Vinkó, József
AU - de Vos, Kellie
AU - Wheeler, J. C.
AU - Williams, G. Grant
AU - Wyatt, Samuel
N1 - Publisher Copyright:
© 2023. The Author(s). Published by the American Astronomical Society.
PY - 2023/10/1
Y1 - 2023/10/1
N2 - 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.
AB - 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.
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U2 - 10.3847/2041-8213/acf9a4
DO - 10.3847/2041-8213/acf9a4
M3 - Article
AN - SCOPUS:85175084699
SN - 2041-8205
VL - 956
JO - Astrophysical Journal Letters
JF - Astrophysical Journal Letters
IS - 1
M1 - L5
ER -