TY - JOUR
T1 - 1100 days in the life of the supernova 2018ibb - The best pair-instability supernova candidate, to date⋆
AU - Fransson, Claes
AU - Kozyreva, Alexandra
AU - Chen, Ting-Wan
AU - Yaron, Ofer
AU - Jerkstrand, Anders
AU - Gal-Yam, Avishay
AU - Sollerman, Jesper
AU - Yan, Lin
AU - Kangas, Tuomas
AU - Leloudas, Giorgos
AU - Omand, Conor M. B.
AU - Smartt, Stephen J.
AU - Nicholl, Matt
AU - Sarin, Nikhil
AU - Yao, Yuhan
AU - Brink, Thomas G.
AU - Sharon, Amir
AU - Rossi, Andrea
AU - Chen, Ping
AU - Chen, Zhihao
AU - Cikota, Aleksandar
AU - De, Kishalay
AU - Drake, Andrew J.
AU - Filippenko, Alexei V.
AU - Fremling, Christoffer
AU - Fréour, Laurane
AU - Fynbo, Johan P. U.
AU - Ho, Anna Y. Q.
AU - Inserra, Cosimo
AU - Irani, Ido
AU - Kuncarayakti, Hanindyo
AU - Lunnan, Ragnhild
AU - Mazzali, Paolo
AU - Ofek, Eran O.
AU - Palazzi, Eliana
AU - Perley, Daniel A.
AU - Pursiainen, Miika
AU - Rothberg, Barry
AU - Shingles, Luke J.
AU - Smith, Ken
AU - Taggart, Kirsty
AU - Tartaglia, Leonardo
AU - Zheng, WeiKang
AU - Anderson, Joseph P.
AU - Cassara, Letizia
AU - Christensen, Eric
AU - George Djorgovski, S.
AU - Galbany, Lluís
AU - Gkini, Anamaria
AU - Graham, Matthew J.
AU - Gromadzki, Mariusz
AU - Groom, Steven L.
AU - Hiramatsu, Daichi
AU - Andrew Howell, D.
AU - Kasliwal, Mansi M.
AU - McCully, Curtis
AU - Müller-Bravo, Tomás E.
AU - Paiano, Simona
AU - Paraskeva, Emmanouela
AU - Pessi, Priscila J.
AU - Polishook, David
AU - Rau, Arne
AU - Rigault, Mickael
AU - Rusholme, Ben
N1 - We thank the referee for a careful reading of the manuscript and for helpful comments that improved this paper. We thank Stéphane Blondin (Laboratoire d’Astrophysique de Marseille, France), Luc Dessart (Sorbonne Université, France), Sebastian Gomez (Space Telescope Science Institute, USA), Ryosuke Hirai (Monash University, Australia), Boaz Katz (Weizmann Institute of Science, Israel), Keiichi Maeda (Kyoto University, Japan), Ilya Mandel (Monash University, Australia), and Kanji Mori (Fukuoka University, Japan) for fruitful discussions. U.C. Berkeley undergraduate students Nachiket Girish, Andrew Hoffman, Evelyn Liu, Shaunak Modak, Jackson Sipple, Samantha Stegman, Kevin Tang, and Keto Zhang helped obtain data with the Lick/Nickel telescope. Z. C. acknowledges support from the China Scholarship Council. A. V. Filippenko’s supernova group at U.C. Berkeley received financial support from the Christopher R. Redlich Fund, Gary & Cynthia Bengier, Clark & Sharon Winslow, Sanford Robertson, Frank and Kathleen Wood (T. G. Brink is a Wood Specialist in Astronomy), Alan Eustace (W. Zheng is a Eustace Specialist in Astronomy), and numerous other donors. C. F. acknowledges support from the Swedish Research Council and the Swedish National Space Board. J. P. U. F. acknowledges support from the Carlsberg Foundation. The Cosmic Dawn Center (DAWN) is funded by the Danish National Research Foundation under grant No. 140. M. G. is supported by the EU Horizon 2020 research and innovation programme under grant agreement No. 101004719. A. J. acknowledges support from the European Research Council (ERC) under the European Union’s Horizon 2020 Research and Innovation Programme (ERC Starting Grant No. [803189]). H. K. was funded by the Academy of Finland projects 324504 and 328898. G. L. and M. P. are supported by a research grant (19054) from VILLUM FONDEN. R. L. is supported by the European Research Council (ERC) under the European Union’s Horizon Europe research and innovation programme (grant agreement No. 10104229 – TransPIre). T. E. M.-B. and L. G. acknowledge financial support from the Spanish Ministerio de Ciencia e Innovación (MCIN), the Agencia Estatal de Investigación (AEI) 10.13039/501100011033, the European Social Fund (ESF) “Investing in your future”, and the European Union Next Generation EU/PRTR funds under the PID2020-115253GA-I00 HOSTFLOWS project, the 2019 Ramón y Cajal program RYC2019-027683-I, the 2021 Juan de la Cierva program FJC2021-047124-I, and from Centro Superior de Investigaciones Científicas (CSIC) under the PIE project 20215AT016, and the program Unidad de Excelencia María de Maeztu CEX2020-001058-M. M. N. is supported by the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (grant agreement No. 948381) and by a Fellowship from the Alan Turing Institute. D. P. is grateful for the Wise Observatory staff. A. R. acknowledges support from Premiale LBT 2013. M. R. has received funding from the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation programme (grant agreement No. 759194 – USNAC). N. S. is supported by a Nordita Fellowship. Nordita is funded in part by NordForsk. S. S. acknowledges support from the G.R.E.A.T. research environment, funded by Vetenskapsrådet, the Swedish Research Council, project number 2016-06012. L. J. S. acknowledges support by the European Research Council (ERC) under the European Union’s Horizon 2020 research and innovation program (ERC Advanced Grant KILONOVA No. 885281). L. T. acknowledges support from MIUR (PRIN 2017 grant 20179ZF5KS). Y. Y. acknowledges support from a Benoziyo Prize Postdoctoral Fellowship and the Bengier-Winslow-Robertson Fellowship. This work was funded by ANID, Millennium Science Initiative, ICN12_009. Based in part on observations at the European Southern Observatory, Program IDs 199.D-0143, 0105.D-0380, 0106.D-0524, 1103.D-0328, 2102.D-5026, and 2104.D-5006 (PIs C. Inserra, S. Schulze, and S. J. Smartt); Gemini-South, Program ID 2021B-Q-901 (PI A. Gal-Yam); Hubble Space Telescope, Program ID GO-16657 (PI C. Fremling); Keck, Program IDs C323, U023, U025 (PIs S. R. Kulkarni, A. V. Filippenko); Large Binocular Telescope, Program ID DDT_2019B_13 (PI E. Palazzi); Las Cumbres Observatory, Program IDs FTPEPO2017AB-001, KEY2017AB-001, SUPA2019A-001, SUPA2019A-002, SUPA2019B-007, and NOAO2020B-012 (PIs P. J. Brown, K. De); Liverpool Telescope, Program IDs JL18B06, JL18B07, JL19A24, JL19B11, and JL20B15 (PI D. A. Perley); Nordic Optical Telescope, Program IDs 57-502, 58-802, and 61-606, (PIs G. Leloudas, J. Sollerman); P200 (PI L. Yan); and XMM-Newton, Program ID 08221501 (PI R. Margutti). We thank the staffs of the many observatories at which we conducted observations. This work has made use of data from the European Space Agency (ESA) mission Gaia, processed by the Gaia Data Processing and Analysis Consortium (DPAC). Funding for the DPAC has been provided by national institutions, in particular the institutions participating in the Gaia Multilateral Agreement. Part of the funding for GROND (both hardware as well as personnel) was generously granted from the Leibniz-Prize to Prof. G. Hasinger (DFG grant HA 1850/28-1). This work is based in part on observations made with the Large Binocular Telescope (LBT). The LBT is an international collaboration among institutions in Italy, the United States, and Germany. LBT Corporation partners are Istituto Nazionale di Astrofisica, Italy; The University of Arizona on behalf of the Arizona university system; LBT Beteiligungsgesellschaft, Germany, representing the Max Planck Society, the Astrophysical Institute Potsdam, and Heidelberg University; The Ohio State University; and The Research Corporation on behalf of The University of Notre Dame, University of Minnesota, and University of Virginia. Some of the observations with the Las Cumbres Observatory data have been obtained via OPTICON proposals and as part of the Global Supernova Project. The OPTICON project has received funding from the European Union’s Horizon 2020 research and innovation programme under grant agreement No. 730890. This work made use of data supplied by the UK Swift Science Data Centre at the University of Leicester. CRTS is supported by the U.S. National Science Foundation (NSF) under grants AST-0909182, AST-1313422, and AST-1413600. The Catalina Sky Survey (CSS) is a NASA-funded project supported by the Near Earth Object Observation Program (NEOO) under the Planetary Defense Coordination Office (PDCO). This publication makes use of data products from the Two Micron All Sky Survey, which is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California Institute of Technology, funded by NASA and the U.S. NSF. Based in part on observations obtained with the Samuel Oschin Telescope 48-inch and the 60-inch Telescope at the Palomar Observatory as part of the Zwicky Transient Facility project. ZTF is supported by the U.S. NSF under grant AST-1440341 and a collaboration including Caltech, IPAC, the Weizmann Institute of 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 Lawrence Berkeley National Laboratories. Operations are conducted by COO, IPAC, and UW. The SED Machine is based upon work supported by the U.S. NSF under grant 1106171. Partially based on observations made with the Nordic Optical Telescope, owned in collaboration by the University of Turku and Aarhus University, and operated jointly by Aarhus University, the University of Turku and the University of Oslo, representing Denmark, Finland and Norway, the University of Iceland and Stockholm University at the Observatorio del Roque de los Muchachos, La Palma, Spain, of the Instituto de Astrofisica de Canarias. This work makes use of observations from the Las Cumbres Observatory network. The Las Cumbres Observatory team is supported by NSF grants AST-1911225 and AST-1911151. 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. KAIT, and its ongoing operation were made possible by donations from Sun Microsystems, Inc., the Hewlett-Packard Company, AutoScope Corporation, the Lick Observatory, the U.S. NSF, the University of California, the Sylvia & Jim Katzman Foundation, and the TABASGO Foundation. A major upgrade of the Kast spectrograph on the Shane 3 m telescope at Lick Observatory was made possible through generous gifts from William and Marina Kast as well as the Heising-Simons Foundation. Research at Lick Observatory is partially supported by a generous gift from Google.
PY - 2024/3/1
Y1 - 2024/3/1
N2 - Stars with zero-age main sequence masses between 140 and 260 M⊙ are thought to explode as pair-instability supernovae (PISNe). During their thermonuclear runaway, PISNe can produce up to several tens of solar masses of radioactive nickel, resulting in luminous transients similar to some superluminous supernovae (SLSNe). Yet, no unambiguous PISN has been discovered so far. SN 2018ibb is a hydrogen-poor SLSN at z = 0.166 that evolves extremely slowly compared to the hundreds of known SLSNe. Between mid 2018 and early 2022, we monitored its photometric and spectroscopic evolution from the UV to the near-infrared (NIR) with 2–10 m class telescopes. SN 2018ibb radiated > 3 × 1051 erg during its evolution, and its bolometric light curve reached > 2 × 1044 erg s−1 at its peak. The long-lasting rise of > 93 rest-frame days implies a long diffusion time, which requires a very high total ejected mass. The PISN mechanism naturally provides both the energy source (56Ni) and the long diffusion time. Theoretical models of PISNe make clear predictions as to their photometric and spectroscopic properties. SN 2018ibb complies with most tests on the light curves, nebular spectra and host galaxy, and potentially all tests with the interpretation we propose. Both the light curve and the spectra require 25–44 M⊙ of freshly nucleosynthesised 56Ni, pointing to the explosion of a metal-poor star with a helium core mass of 120–130 M⊙ at the time of death. This interpretation is also supported by the tentative detection of [Co II] λ 1.025 μm, which has never been observed in any other PISN candidate or SLSN before. We observe a significant excess in the blue part of the optical spectrum during the nebular phase, which is in tension with predictions of existing PISN models. However, we have compelling observational evidence for an eruptive mass-loss episode of the progenitor of SN 2018ibb shortly before the explosion, and our dataset reveals that the interaction of the SN ejecta with this oxygen-rich circumstellar material contributed to the observed emission. That may explain this specific discrepancy with PISN models. Powering by a central engine, such as a magnetar or a black hole, can be excluded with high confidence. This makes SN 2018ibb by far the best candidate for being a PISN, to date.
AB - Stars with zero-age main sequence masses between 140 and 260 M⊙ are thought to explode as pair-instability supernovae (PISNe). During their thermonuclear runaway, PISNe can produce up to several tens of solar masses of radioactive nickel, resulting in luminous transients similar to some superluminous supernovae (SLSNe). Yet, no unambiguous PISN has been discovered so far. SN 2018ibb is a hydrogen-poor SLSN at z = 0.166 that evolves extremely slowly compared to the hundreds of known SLSNe. Between mid 2018 and early 2022, we monitored its photometric and spectroscopic evolution from the UV to the near-infrared (NIR) with 2–10 m class telescopes. SN 2018ibb radiated > 3 × 1051 erg during its evolution, and its bolometric light curve reached > 2 × 1044 erg s−1 at its peak. The long-lasting rise of > 93 rest-frame days implies a long diffusion time, which requires a very high total ejected mass. The PISN mechanism naturally provides both the energy source (56Ni) and the long diffusion time. Theoretical models of PISNe make clear predictions as to their photometric and spectroscopic properties. SN 2018ibb complies with most tests on the light curves, nebular spectra and host galaxy, and potentially all tests with the interpretation we propose. Both the light curve and the spectra require 25–44 M⊙ of freshly nucleosynthesised 56Ni, pointing to the explosion of a metal-poor star with a helium core mass of 120–130 M⊙ at the time of death. This interpretation is also supported by the tentative detection of [Co II] λ 1.025 μm, which has never been observed in any other PISN candidate or SLSN before. We observe a significant excess in the blue part of the optical spectrum during the nebular phase, which is in tension with predictions of existing PISN models. However, we have compelling observational evidence for an eruptive mass-loss episode of the progenitor of SN 2018ibb shortly before the explosion, and our dataset reveals that the interaction of the SN ejecta with this oxygen-rich circumstellar material contributed to the observed emission. That may explain this specific discrepancy with PISN models. Powering by a central engine, such as a magnetar or a black hole, can be excluded with high confidence. This makes SN 2018ibb by far the best candidate for being a PISN, to date.
UR - http://www.scopus.com/inward/record.url?scp=85193033597&partnerID=8YFLogxK
U2 - 10.1051/0004-6361/202346855
DO - 10.1051/0004-6361/202346855
M3 - Article
SN - 0004-6361
VL - 683
JO - Astronomy and Astrophysics
JF - Astronomy and Astrophysics
M1 - A223
ER -