{
  "id": "astro-ph/9910548",
  "version": "v1",
  "published": "1999-10-29T19:21:55.000Z",
  "updated": "1999-10-29T19:21:55.000Z",
  "title": "Resolved Spectroscopy of the Narrow-Line Region in NGC 1068. II. Physical Conditions Near the NGC 1068 ``Hot-Spot''",
  "authors": [
    "S. B. Kraemer",
    "D. M. Crenshaw"
  ],
  "comment": "42 pages, Latex, includes 5 figures (postscript), to appear in the Astrophysical Journal",
  "doi": "10.1086/308572",
  "categories": [
    "astro-ph"
  ],
  "abstract": "The physical conditions near the optical continuum peak (``hot spot'') in the inner narrow line region (NLR) of the Seyfert 2 galaxy, NGC 1068. Spectra were taken with HST/STIS through the 0.1X52 arcsec slit, covering the full STIS 1200 to 10000 Angstrom waveband, and are from a region that includes the hot spot, extending 0.2, or ~ 14 pc (for H= 75 km/sec/Mpc). Perhaps the most striking feature of these spectra is the presence of strong coronal emission lines, including [S XII] 7611 which has hitherto only been identified in spectra of the solar corona. There is an apparent correlation between ionization energy and velocity of the emission lines with respect to the systemic velocity of the host galaxy, with the coronal lines blueshifted, most other high excitation lines near systemic, and some of the low ionization lines redshifted. From the results of our modeling, we find that the emission-line gas consists of three principal components: 1) one in which most of the strong emission-lines, such as [O III] 5007, [Ne V] 3426, C IV 1550, arise, 2) a more tenuous, highly ionized component, which is the source of the coronal-line emission, and 3) a component, which is not co-planar with the other two, in which the low ionization and neutral lines, such as [N II] 6548 and [O I] 6300, are formed. The first two components are directly ionized by the EUV-Xray continuum emitted by the central source, while the low ionization gas is ionized by a combination of highly absorbed continuum radiation and a small fraction of unabsorbed continuum scattered by free electrons associated with the hot spot. The combination of covering factor and Thomson optical depth of the high ionization components is insufficient to scatter the observed fraction of continuum radiation into our line-of-sight.",
  "revisions": [
    {
      "version": "v1",
      "updated": "1999-10-29T19:21:55.000Z"
    }
  ],
  "analyses": {
    "keywords": [
      "physical conditions",
      "narrow-line region",
      "resolved spectroscopy",
      "low ionization",
      "hot spot"
    ],
    "tags": [
      "journal article"
    ],
    "note": {
      "typesetting": "LaTeX",
      "pages": 42,
      "language": "en",
      "license": "arXiv",
      "status": "editable",
      "inspire": 520063
    }
  }
}