TY - JOUR
T1 - Unravelling the Asphericities in the Explosion and Multifaceted Circumstellar Matter of SN 2023ixf
AU - Singh, Avinash
AU - Teja, Rishabh Singh
AU - Moriya, Takashi J.
AU - Maeda, Keiichi
AU - Kawabata, Koji S.
AU - Tanaka, Masaomi
AU - Imazawa, Ryo
AU - Nakaoka, Tatsuya
AU - Gangopadhyay, Anjasha
AU - Yamanaka, Masayuki
AU - Swain, Vishwajeet
AU - Sahu, D. K.
AU - Anupama, G. C.
AU - Kumar, Brajesh
AU - Anche, Ramya M.
AU - Sano, Yasuo
AU - Raj, A.
AU - Agnihotri, V. K.
AU - Bhalerao, Varun
AU - Bisht, D.
AU - Bisht, M. S.
AU - Belwal, K.
AU - Chakrabarti, S. K.
AU - Fujii, Mitsugu
AU - Nagayama, Takahiro
AU - Matsumoto, Katsura
AU - Hamada, Taisei
AU - Kawabata, Miho
AU - Kumar, Amit
AU - Kumar, Ravi
AU - Malkan, Brian K.
AU - Smith, Paul
AU - Sakagami, Yuta
AU - Taguchi, Kenta
AU - Tominaga, Nozomu
AU - Watanabe, Arata
N1 - Publisher Copyright:
© 2024. The Author(s). Published by the American Astronomical Society.
PY - 2024/11/1
Y1 - 2024/11/1
N2 - We present a detailed investigation of photometric, spectroscopic, and polarimetric observations of the Type II SN 2023ixf. Earlier studies have provided compelling evidence for a delayed shock breakout from a confined dense circumstellar matter (CSM) enveloping the progenitor star. The temporal evolution of polarization in the SN 2023ixf phase revealed three distinct peaks in polarization evolution at 1.4 days, 6.4 days, and 79.2 days, indicating an asymmetric dense CSM, an aspherical shock front and clumpiness in the low-density extended CSM, and an aspherical inner ejecta/He-core. SN 2023ixf displayed two dominant axes, one along the CSM-outer ejecta and the other along the inner ejecta/He-core, showcasing the independent origin of asymmetry in the early and late evolution. The argument for an aspherical shock front is further strengthened by the presence of a high-velocity broad absorption feature in the blue wing of the Balmer features in addition to the P-Cygni absorption post-16 days. Hydrodynamical light-curve modeling indicated a progenitor mass of 10 M ⊙ with a radius of 470 R ⊙ and explosion energy of 2 × 1051 erg, along with 0.06 M ⊙ of 56 Ni, though these properties are not unique due to modeling degeneracies. The modeling also indicated a two-zone CSM: a confined dense CSM extending up to 5 × 1014 cm with a mass-loss rate of 10−2 M ⊙ yr−1 and an extended CSM spanning from 5 × 1014 to at least 1016 cm with a mass-loss rate of 10−4 M ⊙ yr−1, both assuming a wind-velocity of 10 km s−1. The early-nebular phase observations display an axisymmetric line profile of [O i], redward attenuation of the emission of Hα post 125 days, and flattening in the Ks-band, marking the onset of dust formation.
AB - We present a detailed investigation of photometric, spectroscopic, and polarimetric observations of the Type II SN 2023ixf. Earlier studies have provided compelling evidence for a delayed shock breakout from a confined dense circumstellar matter (CSM) enveloping the progenitor star. The temporal evolution of polarization in the SN 2023ixf phase revealed three distinct peaks in polarization evolution at 1.4 days, 6.4 days, and 79.2 days, indicating an asymmetric dense CSM, an aspherical shock front and clumpiness in the low-density extended CSM, and an aspherical inner ejecta/He-core. SN 2023ixf displayed two dominant axes, one along the CSM-outer ejecta and the other along the inner ejecta/He-core, showcasing the independent origin of asymmetry in the early and late evolution. The argument for an aspherical shock front is further strengthened by the presence of a high-velocity broad absorption feature in the blue wing of the Balmer features in addition to the P-Cygni absorption post-16 days. Hydrodynamical light-curve modeling indicated a progenitor mass of 10 M ⊙ with a radius of 470 R ⊙ and explosion energy of 2 × 1051 erg, along with 0.06 M ⊙ of 56 Ni, though these properties are not unique due to modeling degeneracies. The modeling also indicated a two-zone CSM: a confined dense CSM extending up to 5 × 1014 cm with a mass-loss rate of 10−2 M ⊙ yr−1 and an extended CSM spanning from 5 × 1014 to at least 1016 cm with a mass-loss rate of 10−4 M ⊙ yr−1, both assuming a wind-velocity of 10 km s−1. The early-nebular phase observations display an axisymmetric line profile of [O i], redward attenuation of the emission of Hα post 125 days, and flattening in the Ks-band, marking the onset of dust formation.
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U2 - 10.3847/1538-4357/ad7955
DO - 10.3847/1538-4357/ad7955
M3 - Article
AN - SCOPUS:85208147089
SN - 0004-637X
VL - 975
JO - Astrophysical Journal
JF - Astrophysical Journal
IS - 1
M1 - 132
ER -