{
  "id": "2301.00172",
  "version": "v1",
  "published": "2022-12-31T10:29:31.000Z",
  "updated": "2022-12-31T10:29:31.000Z",
  "title": "Near-infrared evolution of the equatorial ring of SN 1987A",
  "authors": [
    "T. Kangas",
    "A. Ahola",
    "C. Fransson",
    "J. Larsson",
    "P. Lundqvist",
    "S. Mattila",
    "B. Leibundgut"
  ],
  "comment": "17 pages, 16 figures. Submitted to Astronomy & Astrophysics",
  "categories": [
    "astro-ph.SR",
    "astro-ph.GA",
    "astro-ph.HE"
  ],
  "abstract": "We use adaptive-optics imaging and integral field spectroscopy from the Very Large Telescope, together with images from the \\emph{Hubble Space Telescope}, to study the near-infrared (NIR) evolution of the equatorial ring (ER) of SN~1987A. We study the NIR line and continuum flux and morphology over time in order to lay the groundwork for \\emph{James Webb Space Telescope} observations of the system. We also study the differences in the interacting ring structure and flux between optical, NIR and other wavelengths, and between line and continuum emission, to constrain the underlying physical processes. Mostly the evolution is similar in the NIR and optical. The morphology of the ER has been skewed toward the west side (with roughly 2/3 of the NIR emission originating there) since around 2010. A steady decline in the ER flux, broadly similar to the MIR and the optical, is ongoing since roughly this time as well. The expansion velocity of the ER hotspots in the NIR is fully consistent with the optical. However, continuum emission forms roughly 70 per cent of the NIR luminosity, and is relatively stronger outside the hotspot-defined extent of the ER than the optical emission or NIR line emission since 2012--2013, suggesting a faster-expanding continuum component. We find that this outer NIR emission can have a significant synchrotron contribution. Even if emission from hot ($\\sim$2000~K) dust is dominant within the ER, the mass of this dust must be vanishingly small (a few $\\times10^{-12}$~M$_\\odot$) compared to the total dust mass in the ER ($\\gtrsim10^{-5}$~M$_\\odot$) to account for the observed $HKs$ flux. The location of the NIR continuum emission is different, however, from that of the 180-K dust that dominates in the MIR, and the same hot dust component cannot account for the $J$-band emission.",
  "revisions": [
    {
      "version": "v1",
      "updated": "2022-12-31T10:29:31.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "sn 1987a",
      "equatorial ring",
      "near-infrared evolution",
      "continuum emission",
      "nir line"
    ],
    "note": {
      "typesetting": "TeX",
      "pages": 17,
      "language": "en",
      "license": "arXiv",
      "status": "editable"
    }
  }
}