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Three-body recombination of hydrogen during primordial star formation
D. R. Flower 1★ and G. J. Harris 2
  1 Physics Department, The University of Durham, Durham DH1 3LE   2 Department of Physics & Astronomy, University College London, London WC1E 6BT
Correspondence to   E-mail: david.flower@durham.ac.uk
Copyright 2007 The Authors. Journal compilation © 2007 RAS
KEYWORDS
molecular processes • stars: formation • cosmology: miscellaneous

ABSTRACT

Abstract
          1 INTRODUCTION
          2 MODEL
          3 THREE-BODY RECOMBINATION OF HYDROGEN AND COLLISIONAL DISSOCIATION OF H2
          4 RESULTSREFERENCES

We consider the formation and destruction of H2 and HD during the gravitational contraction of condensations of the primordial gas, which led to the formation of the first generation of stars (Population III stars). The determination of the populations of the bound rovibrational levels of molecular hydrogen is considered in detail. Initially, the rates per unit volume at which these levels are populated and depopulated are not in equilibrium. As the density increases, equilibrium between the rates of population and depopulation is established first, and then the levels gradually thermalize (i.e. their populations tend towards a Boltzmann distribution at the kinetic temperature of the gas), with the lowest energy levels thermalizing first. Ultimately, both the bound and the continuum states thermalize (i.e. attain a Saha distribution), but this process is not complete until densities  nH≈ 1013 cm−3  are reached. Using the principle of microscopic reversibility, we derive an expression for the rate coefficient for three-body recombination of hydrogen which is found to differ significantly from the much used expression of Jacobs et al.


Accepted 2007 February 15. Received 2007 February 15; in original form 2007 January 23

DIGITAL OBJECT IDENTIFIER (DOI)
10.1111/j.1365-2966.2007.11632.x About DOI

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