期刊
ASTROPHYSICAL JOURNAL
卷 569, 期 1, 页码 157-183出版社
IOP PUBLISHING LTD
DOI: 10.1086/339287
关键词
galaxies : evolution; galaxies : ISM; stars : formation
We investigate the relationship between H I H-2, and the star formation rate (SFR) using azimuthally averaged data for seven CO-bright spiral galaxies. Contrary to some earlier studies based on global fluxes, we find that Sigma(SFR) exhibits a much stronger correlation with Sigma(H2) than with Sigma(H) (I), as Sigma(H) (I) saturates at a value of 10 M. pc(-2) or even declines for large Sigma(SFR). Hence, the good correlation between Sigma(SFR) and the total (H I+H-2) gas surface density Sigma(gas) is driven by the molecular component in these galaxies, with the observed relation between Sigma(SFR) and Sigma(H2) following a Schmidt-type law of index n(mol) approximate to 0.8 if a uniform extinction correction is applied or n(mol) approximate to 1.4 for a radially varying correction dependent on gas density. The corresponding Schmidt law indices for Sigma(gas) versus Sigma(SFR) are 1.1 and 1.7 for the two extinction models, in rough agreement with previous studies of the disk-averaged star formation law. An alternative to the Schmidt law, in which the gas depletion timescale is proportional to the orbital timescale, is also consistent with the data if radially varying extinction corrections are applied. We find no clear evidence for a link between the gravitational instability parameter for the gas disk (Q(g)) and the SFR, and we suggest that Q(g) be considered a measure of the gas fraction. This implies that for a state of marginal gravitational stability to exist in galaxies with low gas fractions, it must be enforced by the stellar component. In regions where we have both H I and CO measurements, the ratio of H I to H-2 surface density scales with radius as roughly R-1.5, and we suggest that the balance between H I and H-2 is determined primarily by the midplane interstellar pressure. These results favor a law of star formation in quiescent disks in which the ambient pressure and metallicity control the formation of molecular clouds from H I with star formation then occurring at a roughly constant rate per unit H-2 mass.
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