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The [NII] Line Ratio

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The map of Figure 3 contains only about 20% of our data ... diffuse (ne 100 cm-3) 'halo' component encompassing the entire complex ... – PowerPoint PPT presentation

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Title: The [NII] Line Ratio


1
Aurora over the South Pole August 22, 2005 (photo
by Stephen Parshley)
The SPIFI instrument mounted on the Nasmyth arm
of the AST/RO telescope.
  • Discussion
  • Prior ISO Results
  • ISO/LWS mapped much of the same regions in the
    OIII and NII 122 ?m lines (Mizutani, Onaka,
    and Shibai, 2002)
  • O takes 35 eV to form so it traces gas
    exposed to UV light from high mass stars. From
    the OIII lines, they find the highly ionized
    gas has two components
  • Relatively dense (ne 100 to 350 cm-3)
    component associated with the Carina I and II HII
    regions
  • Relatively diffuse (ne lt 100 cm-3) halo
    component encompassing the entire complex with a
    diameter of 30 pc
  • The NII Line Ratio
  • The ISO 122 ?m NII to SPIFI 205 ?m line ratio
    yields the density of the low ionization gas
    (Figure 5, blue line and circle)
  • The ratio is 1.2 ? ne 30 cm-3
  • Even with a 50 calibration uncertainty, it is
    clear that the NII lines (tracing low
    ionization gas) arise from a very low density
    medium 10 lt ne lt 100 cm-3
  • Therefore, the halo of emission seen in the
    OII lines also contains gas in lower ionization
    states
  • This low ionization, diffuse gas is similar to
    the warm ionized medium in the Galaxy as a whole
  • NII and CII
  • The CII line was mapped with ISO LWS and the
    KAO, and is both bright and widespread over the
    Carina Nebula (Mizutani, Onaka, and Shibai, 2004,
    Brooks et al. 2003)
  • In galaxies the CII line emission
    predominantly arises from the warm dense
    photodissociation regions (PDRs) on the far-UV
    exposed surfaces of molecular clouds (cf. Stacey
    et al. 1991)
  • -- However, CII can also arise from low
    density ionized gas
  • With an ionization potential of 14.5 eV, the
    205 ?m NII line only arises from ionized gas
    regions
  • Since the NII 205 ?m line has a nearly
    identical critical density for thermalization as
    CII in ionized regions ( 50 cm-3), the
    CII/NII 205 ?m line intensity ratio yields
    the fraction of the observed CII that arises
    from the ionized medium subject to relative C
    to N abundance estimates
  • Figure 5 displays the predicted CII/NII
    line intensity ratio (red line) for ionized gas
    as a function of gas density
  • The observed value (red dot) of 8 means that
    4/8 50 of the observed CII line emission
    arises from the ionized medium
  • This is a much larger fraction than the 10 to 25
    commonly assumed in neutral gas studies of
    external galaxies, and has implications for the
    modeling of photodissociation regions including
    gas density and temperature, and the strength of
    stellar radiation fields in these studies
  • Observations
  • The Carina Nebula was observed in the 205.178 ?m
    NII line with SPIFI (Bradford et al. 2002) on
    the 1.7 m AST/RO telescope (Stark et al. 2001) at
    the South Pole. The data presented here were
    obtained on 23 to 25 August 2005, near the middle
    of our 30 day run. We mapped the region outlined
    in red in Figure 1 in weather that was unusually
    poor for the South Pole site, with zenith
    transmission 7.6.
  • SPIFI-AST/RO Parameters
  • Beam size 54 (FWHM)
  • Field of view 325 ? 325
  • Resolving Power R ? ?/?? 5000, or ?v 60
    km/sec
  • Sensitivity NEP 3.4 ? 10-15
    W/Hz1/2 (front end)
  • ?Trec(DSB) 150 K
  • Results
  • The map of Figure 3 contains only about 20 of
    our data
  • The NII line appears in emission over most of
    the region
  • The observed line emission largely follows the
    free-free radio contours (Retallack, 1983)
  • The line peaks at 0.51 K on the position of
    the Carina II radio continuum peak (G287.57-0.59,
    Figure 4)
  • The line velocity centroid well matches that of
    the radio recombination lines (Brooks, Storey,
    Whiteoak, 2001)

Acknowledgements This work was supported by NSF
grants OPP-0094605, OPP-0338149, and NASA grant
NNG05GK70H. We are indebted to the Cardiff group
under P. A. R. Ade for their excellent filters,
to the GSFC group (S.H. Moseley, D. J. Benford,
J. G. Staguhn) for their excellent bolometers,
and to J.W. Kooi who set up LOs for our
frequency calibration at the pole. We also thank
the many people who have contributed to the
success of SPIFI both at AST/RO and the JCMT
including, and especially C. M. Bradford, A. D.
Bolatto, J.A. Davidson, M. L. Savage
  • References
  • Bradford et al. Ap. Opt. 41, 2561 (2002)
  • Brooks, K.J. et al. AA, 412, 751 (2003)
  • Brooks, K.J., Storey, J.W.V., Whiteoak, J.B.
    MNRAS 327, 46 (2001)
  • Mizutani, Onaka, Shibai AA 382, 610 (2002)
  • Mizutani, Onaka, Shibai AA 423, 579 (2004)
  • Retallack, D.S. MNRAS 204, 669 (1983)
  • Stacey et al. ApJ 373, 423 (1991)
  • Stark, A.A. et al., PASP, 115, 567 (2001)
  • Wright, E.L. et al. ApJ 381, 200 (1991)
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