
Comparison of 13 CO line and far‐infrared continuum emission as a diagnostic of dust and molecular gas physical conditions – I. Motivation and modelling
Author(s) -
Wall W. F.
Publication year - 2007
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.1365-2966.2006.11293.x
Subject(s) - physics , astrophysics , molecular cloud , infrared , millimeter , line (geometry) , submillimeter array , interstellar medium , thermal , far infrared , interstellar cloud , cosmic dust , spectral line , astronomy , star formation , galaxy , meteorology , geometry , mathematics , stars
Determining temperatures in molecular clouds from ratios of CO rotational lines or from ratios of continuum emission in different wavelength bands suffers from reduced temperature sensitivity in the high‐temperature limit. In theory, the ratio of far‐infrared (FIR), submillimetre or millimetre continuum to that of a 13 CO (or C 18 O) rotational line can place reliable upper limits on the temperature of the dust and molecular gas. Consequently, FIR continuum data from the COBE /Diffuse Infrared Background Experiment (DIRBE) instrument and Nagoya 4‐m 13 CO J = 1 → 0 spectral line data were used to plot 240 μm/ 13 CO J = 1 → 0 intensity ratios against 140/240 μm dust colour temperatures, allowing us to constrain the multiparsec‐scale physical conditions in the Orion A and B molecular clouds. The best‐fitting models to the Orion clouds consist of two components: a component near the surface of the clouds that is heated primarily by a very large scale (i.e. ∼1 kpc) interstellar radiation field and a component deeper within the clouds. The former has a fixed temperature and the latter has a range of temperatures that vary from one sightline to another. The models require a dust–gas temperature difference of 0 ± 2 K and suggest that 40–50 per cent of the Orion clouds are in the form of dust and gas with temperatures between 3 and 10 K. The implications are discussed in detail in later papers and include stronger dust–gas thermal coupling and higher Galactic‐scale molecular gas temperatures than are usually accepted, and an improved explanation for the N (H 2 )/ I (CO) conversion factor. It is emphasized that these results are preliminary and require confirmation by independent observations and methods.