Fig. 4

Steady-state abundances relative to total H nuclei for H2 and chemical species involved in its formation for dust-free single point models with G0 = 104, W = 5 × 10−7, TK = 1000 K, and nH ranging from105 to 2 × 1012 cm−3. An analytical expression of the steady state abundance of H2, assuming destruction by photodissociation and formation by H− only, is alsoplotted in black dotted line (see Appendix C). Boundaries defined in Fig. 3 are also indicated on the upper axis. It is important to note that because of the decrease of the electron fraction following recombination at high density, a three-body reaction takes over from the formation via H− (boundary ①) at a lower density than indicated in Fig. 3.
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