The thermal and chemical evolution of star-forming clouds is studied for different gas metallicities, Z, using the model of Omukai, updated to include deuterium chemistry and the effects of cosmic microwave background (CMB) radiation. HD-line cooling dominates the thermal balance of clouds when Z~10-5 to 10-3 Zsolar and density ~105 cm-3. Early on, CMB radiation prevents the gas temperature from falling below TCMB, although this hardly alters the cloud thermal evolution in low-metallicity gas. From the derived temperature evolution, we assess cloud/core fragmentation as a function of metallicity from linear perturbation theory, which requires that the core elongation E≡(b-a)/a>ENL~1, where a (b) is the short (long) core axis length. The fragment mass is given by the thermal Jeans mass at E=ENL. Given these assumptions and the initial (Gaussian) distribution of E, we compute the fragment mass distribution as a function of metallicity. We find that (1) for Z=0, all fragments are very massive, <~103 Msolar, consistent with previous studies; (2) for Z>10-6 Zsolar a few clumps go through an additional high-density (>~1010 cm-3) fragmentation phase driven by dust cooling, leading to low-mass fragments; (3) the mass fraction in low-mass fragments is initially very small, but at Z~10-5 Zsolar it becomes dominant and continues to grow as Z is increased; (4) as a result of the two fragmentation modes, a bimodal mass distribution emerges in 0.01<Z/Zsolar<0.1 and (5) for >~0.1 Zsolar, the two peaks merge into a single-peaked mass function, which might be regarded as the precursor of the ordinary Salpeter-like initial mass function.
Thermal and Fragmentation Properties of Star-forming Clouds in Low-Metallicity Environments
FERRARA, ANDREA
2005
Abstract
The thermal and chemical evolution of star-forming clouds is studied for different gas metallicities, Z, using the model of Omukai, updated to include deuterium chemistry and the effects of cosmic microwave background (CMB) radiation. HD-line cooling dominates the thermal balance of clouds when Z~10-5 to 10-3 Zsolar and density ~105 cm-3. Early on, CMB radiation prevents the gas temperature from falling below TCMB, although this hardly alters the cloud thermal evolution in low-metallicity gas. From the derived temperature evolution, we assess cloud/core fragmentation as a function of metallicity from linear perturbation theory, which requires that the core elongation E≡(b-a)/a>ENL~1, where a (b) is the short (long) core axis length. The fragment mass is given by the thermal Jeans mass at E=ENL. Given these assumptions and the initial (Gaussian) distribution of E, we compute the fragment mass distribution as a function of metallicity. We find that (1) for Z=0, all fragments are very massive, <~103 Msolar, consistent with previous studies; (2) for Z>10-6 Zsolar a few clumps go through an additional high-density (>~1010 cm-3) fragmentation phase driven by dust cooling, leading to low-mass fragments; (3) the mass fraction in low-mass fragments is initially very small, but at Z~10-5 Zsolar it becomes dominant and continues to grow as Z is increased; (4) as a result of the two fragmentation modes, a bimodal mass distribution emerges in 0.01File | Dimensione | Formato | |
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