<?xml version="1.0" encoding="UTF-8"?><rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:dcq="http://purl.org/dc/terms/"><records count="1" morepages="false" start="1" end="1"><record rownumber="1"><dc:product_type>Journal Article</dc:product_type><dc:title>Seven Years of SN 2014C: A Multiwavelength Synthesis of an Extraordinary Supernova</dc:title><dc:creator>Thomas, Benjamin P.; Wheeler, J. Craig; Dwarkadas, Vikram V.; Stockdale, Christopher; Vinkó, Jozsef; Pooley, David; Xu, Yerong; Zeimann, Greg; MacQueen, Phillip</dc:creator><dc:corporate_author/><dc:editor/><dc:description>Abstract                          SN 2014C was originally classified as a Type Ib supernova, but at phase              ϕ              = 127 days, post-explosion strong H              α              emission was observed. SN 2014C has since been observed in radio, infrared, optical and X-ray bands. Here we present new optical spectroscopic and photometric data spanning              ϕ              = 947–2494 days post-explosion. We address the evolution of the broadened H              α              emission line, as well as broad [O              iii              ] emission and other lines. We also conduct a parallel analysis of all publicly available multiwavelength data. From our spectra, we find a nearly constant H              α              FWHM velocity width of ∼2000 km s              −1              that is significantly lower than that of other broadened atomic transitions (∼3000–7000 km s              −1              ) present in our spectra ([O              i              ]              λ              6300; [O              iii              ]              λ              λ              4959, 5007; He              i              λ              7065; [Ca              ii              ]              λ              λ              7291, 7324). The late radio data demand a fast forward shock (∼10,000 km s              −1              at              ϕ              = 1700 days) in rarified matter that contrasts with the modest velocity of the H              α              . We propose that the infrared flux originates from a toroidal-like structure of hydrogen surrounding the progenitor system, while later emission at other wavelengths (radio, X-ray) likely originates predominantly from the reverse shock in the ejecta and the forward shock in the quasi-spherical progenitor He-wind. We propose that the H              α              emission arises in the boundary layer between the ejecta and torus. We also consider the possible roles of a pulsar and a binary companion.</dc:description><dc:publisher/><dc:date>2022-05-01</dc:date><dc:nsf_par_id>10347651</dc:nsf_par_id><dc:journal_name>The Astrophysical Journal</dc:journal_name><dc:journal_volume>930</dc:journal_volume><dc:journal_issue>1</dc:journal_issue><dc:page_range_or_elocation>57</dc:page_range_or_elocation><dc:issn>0004-637X</dc:issn><dc:isbn/><dc:doi>https://doi.org/10.3847/1538-4357/ac5fa6</dc:doi><dcq:identifierAwardId>1911061; 1813825; 1814178</dcq:identifierAwardId><dc:subject/><dc:version_number/><dc:location/><dc:rights/><dc:institution/><dc:sponsoring_org>National Science Foundation</dc:sponsoring_org></record></records></rdf:RDF>