TY - JOUR
T1 - SN 2017gci
T2 - a nearby Type I Superluminous Supernova with a bumpy tail
AU - Fiore, A
AU - Chen, T-W
AU - Jerkstrand, A
AU - Benetti, S
AU - Ciolfi, R
AU - Inserra, C
AU - Cappellaro, E
AU - Pastorello, A
AU - Leloudas, G
AU - Schulze, S
AU - Berton, M
AU - Burke, J
AU - McCully, C
AU - Fong, W
AU - Galbany, L
AU - Gromadzki, M
AU - Gutiérrez, C P
AU - Hiramatsu, D
AU - Hosseinzadeh, G
AU - Howell, D A
AU - Kankare, E
AU - Lunnan, R
AU - Müller-Bravo, T E
AU - O’ Neill, D
AU - Nicholl, M
AU - Rau, A
AU - Sollerman, J
AU - Terreran, G
AU - Valenti, S
AU - Young, D R
PY - 2021/4
Y1 - 2021/4
N2 - We present and discuss the optical spectrophotometric observations of the nearby (z = 0.087) Type I superluminous supernova (SLSN I) SN 2017gci, whose peak K-corrected absolute magnitude reaches Mg = −21.5 mag. Its photometric and spectroscopic evolution includes features of both slow- and of fast-evolving SLSN I, thus favoring a continuum distribution between the two SLSN-I subclasses. In particular, similarly to other SLSNe I, the multiband light curves (LCs) of SN 2017gci show two re-brightenings at about 103 and 142 d after the maximum light. Interestingly, this broadly agrees with a broad emission feature emerging around 6520 Å after ∼51 d from the maximum light, which is followed by a sharp knee in the LC. If we interpret this feature as Hα, this could support the fact that the bumps are the signature of late interactions of the ejecta with a (hydrogen-rich) circumstellar material. Then we fitted magnetar- and CSM-interaction-powered synthetic LCs on to the bolometric one of SN 2017gci. In the magnetar case, the fit suggests a polar magnetic field Bp ≃ 6 × 1014 G, an initial period of the magnetar Pinitial ≃ 2.8 ms, an ejecta mass Mejecta≃9M⊙ and an ejecta opacity κ≃0.08cm2g−1. A CSM-interaction scenario would imply a CSM mass ≃5M⊙ and an ejecta mass ≃12M⊙. Finally, the nebular spectrum of phase + 187 d was modeled, deriving a mass of ∼10M⊙ for the ejecta. Our models suggest that either a magnetar or CSM interaction might be the power sources for SN 2017gci and that its progenitor was a massive (40M⊙) star.
AB - We present and discuss the optical spectrophotometric observations of the nearby (z = 0.087) Type I superluminous supernova (SLSN I) SN 2017gci, whose peak K-corrected absolute magnitude reaches Mg = −21.5 mag. Its photometric and spectroscopic evolution includes features of both slow- and of fast-evolving SLSN I, thus favoring a continuum distribution between the two SLSN-I subclasses. In particular, similarly to other SLSNe I, the multiband light curves (LCs) of SN 2017gci show two re-brightenings at about 103 and 142 d after the maximum light. Interestingly, this broadly agrees with a broad emission feature emerging around 6520 Å after ∼51 d from the maximum light, which is followed by a sharp knee in the LC. If we interpret this feature as Hα, this could support the fact that the bumps are the signature of late interactions of the ejecta with a (hydrogen-rich) circumstellar material. Then we fitted magnetar- and CSM-interaction-powered synthetic LCs on to the bolometric one of SN 2017gci. In the magnetar case, the fit suggests a polar magnetic field Bp ≃ 6 × 1014 G, an initial period of the magnetar Pinitial ≃ 2.8 ms, an ejecta mass Mejecta≃9M⊙ and an ejecta opacity κ≃0.08cm2g−1. A CSM-interaction scenario would imply a CSM mass ≃5M⊙ and an ejecta mass ≃12M⊙. Finally, the nebular spectrum of phase + 187 d was modeled, deriving a mass of ∼10M⊙ for the ejecta. Our models suggest that either a magnetar or CSM interaction might be the power sources for SN 2017gci and that its progenitor was a massive (40M⊙) star.
KW - Transients: supernovae
KW - supernova: general
KW - supernovae: individual: SN 2017gci
UR - http://www.scopus.com/inward/record.url?scp=85115843692&partnerID=8YFLogxK
U2 - 10.1093/mnras/staa4035
DO - 10.1093/mnras/staa4035
M3 - Article
SN - 0035-8711
VL - 502
SP - 2120
EP - 2139
JO - Monthly Notices of the Royal Astronomical Society
JF - Monthly Notices of the Royal Astronomical Society
IS - 2
ER -