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ISO observation of molecular hydrogen and fine‐structure lines in the photodissociation region IC 63
Author(s) -
Thi W.F.,
Van Dishoeck E. F.,
Bell T.,
Viti S.,
Black J.
Publication year - 2009
Publication title -
monthly notices of the royal astronomical society
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 2.058
H-Index - 383
eISSN - 1365-2966
pISSN - 0035-8711
DOI - 10.1111/j.1365-2966.2009.15501.x
Subject(s) - physics , photodissociation , infrared , spectrometer , ultraviolet , wavelength , astrophysics , spectral line , atomic physics , optics , astronomy , photochemistry , chemistry
We wish to constrain the main physical properties of the photodissociation region (PDR) IC 63. We present the results of a survey for the lowest pure‐rotational lines of H 2 with the Short Wavelength Spectrometer and for the major fine‐structure cooling lines of O  i at 63 and 145 μm and C  ii at 157.7 μm with the Long Wavelength Spectrometer on board the Infrared Space Observatory ( ISO ) in the high‐density PDR IC 63. The observations are compared with available photochemical models based on optical absorption and/or millimetre emission line data with and without enhanced H 2 formation rate on grain surfaces. The cloud density n H is constrained by the fine‐structure lines. The models include both collisional excitation and ultraviolet (UV) pumping of the H 2 ro‐vibrational levels. Molecular pure‐rotational lines up to S(5) are detected. The inferred column density of warm H 2 at 106 ± 11 K is (5.9 ± 1.8) +0.9 −0.7 × 10 21  cm −2 , while that of the hot component at 685 ± 68 K is (1.2 ± 0.4) × 10 19  cm −2 . Fine‐structure lines are also detected in the far‐infrared spectrum of IC 63. The fine‐structure lines constrain the density of the PDR to be (1–5) × 10 3  cm −3 . The impinging UV field on the PDR is enhanced by a factor of 10 3 compared to the mean interstellar field and is consistent with direct measurements in the UV. PDR models that include an enhanced H 2 formation at high dust temperature give higher H 2 intensities than models without enhancement. However, the predicted intensities are still lower than the observed intensities.

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