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Issue A&A
Volume 389, Number 2, July II 2002
Page(s) 393 - 404
Section Extragalactic astronomy
DOI 10.1051/0004-6361:20020646



A&A 389, 393-404 (2002)
DOI: 10.1051/0004-6361:20020646

Two-phase equilibrium and molecular hydrogen formation in damped Lyman-alpha systems

H. Liszt

National Radio Astronomy Observatory, 520 Edgemont Road, Charlottesville, VA 22903-2475, USA

(Received 20 March 2002 / Accepted 29 April 2002 )

Abstract
Molecular hydrogen is quite underabundant in damped Lyman- $\alpha$ systems at high redshift, when compared to the interstellar medium near the Sun. This has been interpreted as implying that the gas in damped Lyman- $\alpha$ systems is warm like the nearby neutral intercloud medium, rather than cool, as in the clouds which give rise to most H I absorption in the Milky Way. Other lines of evidence suggest that the gas in damped Lyman- $\alpha$ systems - in whole or part - is actually cool; spectroscopy of neutral and ionized carbon, discussed here, shows that the damped Lyman- $\alpha$ systems observed at lower redshift z < 2.3 are largely cool, while those seen at z > 2.8 are warm (though not devoid of ${\rm H}_2$). To interpret the observations of carbon and hydrogen we constructed detailed numerical models of ${\rm H}_2$ formation under the conditions of two-phase thermal equilibrium, like those which account for conditions near the Sun, but with varying metallicity, dust-gas ratio, etc. We find that the low metallicity of damped Lyman- $\alpha$ systems is enough to suppress ${\rm H}_2$ formation by many orders of magnitude even in cool diffuse clouds, as long as the ambient optical/uv radiation field is not too small. For very low metallicity and under the most diffuse conditions, ${\rm H}_2$ formation will be dominated by slow gas-phase processes not involving grains, and a minimum molecular fraction in the range 10-8-10-7 is expected.


Key words: quasars: absorption lines -- ISM: molecules

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