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Nebular-phase Spectra of Superluminous Supernovae: Physical Insights from Observational and Statistical Properties

M. NichollInstitute for Astronomy, University of Edinburgh, Royal Observatory, Blackford Hill, Edinburgh EH9 3HJ, UKE. BergerHarvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USAP. K. BlanchardHarvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USASebastián GómezHarvard-Smithsonian Center for Astrophysics, 60 Garden Street, Cambridge, MA 02138, USAR. ChornockAstrophysical Institute, Department of Physics and Astronomy, 251B Clippinger Lab, Ohio University, Athens, OH 45701, USA
2019en
ABI

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Abstract We study the spectroscopic evolution of superluminous supernovae (SLSNe) later than 100 days after maximum light. We present new data for Gaia16apd and SN 2017egm and analyze these with a larger sample comprising 41 spectra of 12 events. The spectra become nebular within 2–4 e -folding times after light-curve peak, with the rate of spectroscopic evolution correlated to the light-curve timescale. Emission lines are identified with well-known transitions of oxygen, calcium, magnesium, sodium, and iron. SLSNe are differentiated from other SNe Ic by a prominent O i λ 7774 line and higher ionization states of oxygen. The iron-dominated region around 5000 Å is more similar to broad-lined SNe Ic than to normal SNe Ic. Principal component analysis shows that five “eigenspectra” capture ≳70% of the variance, while a clustering analysis shows no clear evidence for multiple SLSN subclasses. Line velocities are 5000–8000 km s −1 and show stratification of the ejecta. O i λ 7774 likely arises in a dense inner region that also produces calcium emission, while [O i ] λ 6300 comes from farther out until 300–400 days. The luminosities of O i λ 7774 and Ca ii suggest significant clumping, in agreement with previous studies. Ratios of [Ca ii ] λ 7300/[O i ] λ 6300 favor progenitors with relatively massive helium cores, likely ≳6 , though more modeling is required here. SLSNe with broad light curves show the strongest [O i ] λ 6300, suggesting larger ejecta masses. We show how the inferred velocity, density, and ionization structure point to a central power source.

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