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Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material
Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material
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Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material
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Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material
Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material

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Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material
Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material
Paper

Late-time Hubble Space Telescope Ultraviolet Spectra of SN 2023ixf and SN 2024ggi Show Ongoing Interaction with Circumstellar Material

2025
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Overview
We present far- and near-ultraviolet (UV) spectra of the Type II supernovae (SNe) SN~2023ixf from days 199 to 722 and SN~2024ggi at days 41 and 232. Both supernovae show broad, blueshifted, and asymmetric UV emission lines with an initial maximum velocity of \\(\\sim9000\\,km\\,s^{-1}\\) and narrow unresolved emission in CIV. We compare the optical and UV emission-line profiles, showing that they evolve from two distinct velocity profiles to a single profile tracing the UV emission. We interpret this as shock power from interaction with circumstellar material coming to dominate over the radioactive-decay power from the inner ejecta. Comparing our observations to radiative transfer models with injected shock power, we find SN~2024ggi is best matched by \\(P_{\\mathrm{shock, abs}}=1\\times10^{41}\\,erg\\,s^{-1}\\) at day 40, SN~2023ixf at day 300 and SN~2024ggi at day 200 are best matched by \\(P_{\\mathrm{shock,abs}}=1\\times10^{40}\\,erg\\,s^{-1}\\), and SN~2023ixf at day 600 is best matched by \\(P_{\\mathrm{shock,abs}}=5\\times10^{39}\\,erg\\,s^{-1}\\). From these models, we find the mass-loss rate of both supernovae increased just before explosion. For SN~2023ixf our mass-loss rates go from \\(4\\times10^{-5}\\,M_{\\odot}\\,yr^{-1}\\) at 600 yr before explosion to \\(2\\times10^{-2}\\,M_{\\odot}\\,yr^{-1}\\) at 15 yr prior to explosion. For SN~2024ggi, we find a mass-loss rate of \\(9\\times10^{-5}\\,M_{\\odot}\\,yr^{-1}\\) at 150 yr before explosion and \\(1\\times10^{-3}\\,M_{\\odot}\\,yr^{-1}\\) at 30 yr before explosion.