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Published February 10, 2022 | public
Journal Article

The Early Phases of Supernova 2020pni: Shock Ionization of the Nitrogen-enriched Circumstellar Material

Abstract

We present multiwavelength observations of the Type II SN 2020pni. Classified at ∼1.3 days after explosion, the object showed narrow (FWHM intensity <250 km s⁻¹) recombination lines of ionized helium, nitrogen, and carbon, as typically seen in flash-spectroscopy events. Using the non-LTE radiative transfer code CMFGEN to model our first high-resolution spectrum, we infer a progenitor mass-loss rate of Ṁ = (3.5-5.3) × 10⁻³ M_⊙ yr⁻¹ (assuming a wind velocity of v_w = 200 km s⁻¹), estimated at a radius of Rᵢₙ = 2.5 × 10¹⁴ cm. In addition, we find that the progenitor of SN 2020pni was enriched in helium and nitrogen (relative abundances in mass fractions of 0.30–0.40 and 8.2 × 10⁻³, respectively). Radio upper limits are also consistent with dense circumstellar material (CSM) and a mass-loss rate of Ṁ > 5 × 10⁻⁴ Ṁ yr⁻¹. During the initial 4 days after first light, we also observe an increase in velocity of the hydrogen lines (from ∼250 to ∼1000 km s⁻¹), suggesting complex CSM. The presence of dense and confined CSM, as well as its inhomogeneous structure, indicates a phase of enhanced mass loss of the progenitor of SN 2020pni during the last year before explosion. Finally, we compare SN 2020pni to a sample of other shock-photoionization events. We find no evidence of correlations among the physical parameters of the explosions and the characteristics of the CSM surrounding the progenitors of these events. This favors the idea that the mass loss experienced by massive stars during their final years could be governed by stochastic phenomena and that, at the same time, the physical mechanisms responsible for this mass loss must be common to a variety of different progenitors.

Additional Information

© 2022. 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. Any further distribution of this work must maintain attribution to the author(s) and the title of the work, journal citation and DOI. W.J.-G. is supported by the National Science Foundation (NSF) Graduate Research Fellowship Program under grant DGE-1842165 and the Data Science Initiative Fellowship from Northwestern University. M.R.S. is supported by the NSF Graduate Research Fellowship Program under grant 1842400. R.M. acknowledges support by the NSF under grants AST-1909796 and AST-1944985. She is a CIFAR Azrieli Global Scholar in the Gravity & the Extreme Universe Program (2019) and an Alfred P. Sloan Fellow in Physics (2019). Her team at Northwestern University is partially funded by the Heising-Simons Foundation under grant 2018-0911 (PI Margutti). The Northwestern team is partially supported by National Aeronautics and Space Administration (NASA) grant 80NSSC20K1575. Support for D.O.J. was provided by NASA through Hubble Fellowship grant HF2-51462.001 awarded by the Space Telescope Science Institute (STScI), which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS5-26555. The UCSC team is supported in part by NASA grant 80NSSC20K0953, NSF grant AST-1815935, the Gordon & Betty Moore Foundation, the Heising-Simons Foundation, and a fellowship from the David and Lucile Packard Foundation to R.J.F. C.G. is supported by a VILLUM FONDEN Young Investigator Grant (project #25501). H.P. is indebted to the Danish National Research Foundation (DNRF132) and the Hong Kong government (GRF grant HKU27305119) for support. K.E. was supported by an NSF graduate research fellowship. Y.Z. is supported by the CHE Israel Excellence Fellowship. A.V.F.'s group at U.C. Berkeley has been supported by the Christopher R. Redlich Fund, the Miller Institute for Basic Research in Science (where A.V.F. is a Senior Miller Fellow), and many individual donors. The Pan-STARRS1 Surveys (PS1) and the PS1 public science archive have been made possible through contributions by the Institute for Astronomy, the University of Hawaii, the Pan-STARRS Project Office, the Max-Planck Society and its participating institutes, the Max Planck Institute for Astronomy, Heidelberg and the Max Planck Institute for Extraterrestrial Physics, Garching, Johns Hopkins University, Durham University, the University of Edinburgh, the Queen's University Belfast, the Harvard-Smithsonian Center for Astrophysics, the Las Cumbres Observatory Global Telescope Network Incorporated, the National Central University of Taiwan, STScI, NASA under grant NNX08AR22G issued through the Planetary Science Division of the NASA Science Mission Directorate, NSF grant AST-1238877, the University of Maryland, Eotvos Lorand University (ELTE), the Los Alamos National Laboratory, and the Gordon and Betty Moore Foundation. Some of the data presented herein were obtained at the W. M. Keck Observatory, which is operated as a scientific partnership among the California Institute of Technology, the University of California, and NASA. The Observatory was made possible by the generous financial support of the W. M. Keck Foundation. The authors wish to recognize and acknowledge the very significant cultural role and reverence that the summit of Maunakea has always had within the indigenous Hawaiian community. We are most fortunate to have the opportunity to conduct observations from this mountain. W. M. Keck Observatory and MMT Observatory access was supported by Northwestern University and the Center for Interdisciplinary Exploration and Research in Astrophysics (CIERA). A major upgrade of the Kast spectrograph on the Shane 3 m telescope at Lick Observatory was made possible through generous gifts from the Heising-Simons Foundation and William and Marina Kast. Research at Lick Observatory is partially supported by a generous gift from Google. Based in part on observations obtained with the Samuel Oschin 48-inch Telescope at the Palomar Observatory as part of the Zwicky Transient Facility project. ZTF is supported by the NSF under grant AST-1440341 and a collaboration including Caltech, IPAC, the Weizmann Institute for Science, the Oskar Klein Center at Stockholm University, the University of Maryland, the University of Washington, Deutsches Elektronen-Synchrotron and Humboldt University, Los Alamos National Laboratories, the TANGO Consortium of Taiwan, the University of Wisconsin at Milwaukee, and the Lawrence Berkeley National Laboratory. Operations are conducted by the Caltech Optical Observatories (COO), the Infrared Processing and Analysis Center (IPAC), and the University of Washington (UW). We acknowledge the use of public data from the Neil Gehrels Swift Observatory data archive. Parts of this research were supported by the Australian Research Council Centre of Excellence for All Sky Astrophysics in 3 Dimensions (ASTRO 3D), through project No. CE170100013. The National Radio Astronomy Observatory is a facility of the NSF operated under cooperative agreement by Associated Universities, Inc. Facilities: Gemini - , Keck - , LCO - , MMT - , NOT - , Pan-STARRS - , Lick Shane 3 m - , Swift - , VLA - , ZTF. - Software: APLpy (v1.1.1; Robitaille & Bressert 2012), Astropy (v2.0.1; Astropy Collaboration et al. 2013, 2018), CASA (v5.4.1; McMullin et al. 2007b), DAOPHOT (v2.14.1; Stetson 1987), HEAsoft (v6.22; HEASARC 2014), IRAF (v2.16; Tody 1986, 1993), NumPy (v1.13.1; Oliphant 2006), Matplotlib (v2.0.2; Hunter 2007), PypeIt (v1.0.6; Prochaska et al. 2020), SciPy (v0.19.1; Jones et al. 2001), SNOoPY (Cappellaro, E. 2014; http://sngroup.oapd.inaf.it/snoopy.html), Source Extractor (v2.19.5; Bertin & Arnouts 1996).

Additional details

Created:
August 22, 2023
Modified:
October 24, 2023