The Deepest Radio Observations of Nearby Type IA Supernovae: Constraining Progenitor Types and Optimizing Future Surveys
Draft version January 20, 2020 Typeset using LATEX default style in AASTeX63 The Deepest Radio Observations of Nearby Type IA Supernovae: Constraining Progenitor Types and Optimizing Future Surveys Peter Lundqvist,1, 2 Esha Kundu,1, 2, 3 Miguel A. Pérez-Torres,4, 5 Stuart D. Ryder,6, 7 Claes-Ingvar Björnsson,1 Javier Moldon,8 Megan K. Argo,8, 9 Robert J. Beswick,8 Antxon Alberdi,4 and Erik C. Kool1, 2, 6, 7 1Department of Astronomy, AlbaNova University Center, Stockholm University, SE-10691 Stockholm, Sweden 2The Oskar Klein Centre, AlbaNova, SE-10691 Stockholm, Sweden 3Curtin Institute of Radio Astronomy, Curtin University, GPO Box U1987, Perth WA 6845, Australia 4Instituto de Astrofísica de Andalucía, Glorieta de las Astronomía, s/n, E-18008 Granada, Spain 5Visiting Scientist: Departamento de Física Teorica, Facultad de Ciencias, Universidad de Zaragoza, Spain 6Dept. of Physics and Astronomy, Macquarie University, Sydney NSW 2109, Australia 7Australian Astronomical Observatory, 105 Delhi Rd, North Ryde, NSW 2113, Australia 8Jodrell Bank Centre for Astrophysics, School of Physics and Astronomy, University of Manchester, M13 9PL, UK 9Jeremiah Horrocks Institute, University of Central Lancashire, Preston PR1 2HE, UK (Received December 30, 2019; Revised January 15, 2020; Accepted January 16, 2020) ABSTRACT We report deep radio observations of nearby Type Ia Supernovae (SNe Ia) with the electronic Multi-Element Radio Linked Interferometer Net-work (e-MERLIN), and the Australia Telescope Compact Array (ATCA). No detections were made. With standard assumptions for the energy densities of relativistic electrons going into a power-law energy distribution, and the magnetic field strength (e = B = 0:1), we arrive at the upper limits on mass-loss rate for the progenitor system of SN 2013dy (2016coj, 2018gv, 2018pv, 2019np), to be Û −8 −1 −1 M ∼< 12 ¹2:8; 1:3; 2:1; 1:7º × 10 M yr ¹vw/100 km s º, where vw is the wind speed of the mass loss.
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