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Overcooled haloes at z ≥ 10: a route to form low-mass first stars
It has been shown by Shchekinov & Vasiliev2006 (SV06) that HD molecules can be an important cooling agent in high redshift z >10 haloes if they undergo mergers under specific conditions so suitable shocks are created. Here we build upon Prieto et al. (2012) who studied in detail the merger-ge...
Autores principales: | , , |
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Lenguaje: | eng |
Publicado: |
2013
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1093/mnras/stt2049 http://cds.cern.ch/record/1559883 |
_version_ | 1780930657982087168 |
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author | Prieto, Joaquin Jimenez, Raul Verde, Licia |
author_facet | Prieto, Joaquin Jimenez, Raul Verde, Licia |
author_sort | Prieto, Joaquin |
collection | CERN |
description | It has been shown by Shchekinov & Vasiliev2006 (SV06) that HD molecules can be an important cooling agent in high redshift z >10 haloes if they undergo mergers under specific conditions so suitable shocks are created. Here we build upon Prieto et al. (2012) who studied in detail the merger-generated shocks, and show that the conditions for HD cooling can be studied by combining these results with a suite of dark-matter only simulations. We have performed a number of dark matter only simulations from cosmological initial conditions inside boxes with sizes from 1 to 4 Mpc. We look for haloes with at least two progenitors of which at least one has mass M > M_cr (z), where M_cr (z) is the SV06 critical mass for HD over-cooling. We find that the fraction of over-cooled haloes with mass between M_cr (z) and 10^{0.2} M_cr (z), roughly below the atomic cooling limit, can be as high as ~ 0.6 at z ~ 10 depending on the merger mass ratio. This fraction decreases at higher redshift reaching a value ~0.2 at z ~ 15. For higher masses, i.e. above 10^{0.2} M_cr (z) up to 10^{0.6} M_cr (z), above the atomic cooling limit, this fraction rises to values ~ 0.8 until z ~ 12.5. As a consequence, a non negligible fraction of high redshift z > 10 mini-haloes can drop their gas temperature to the Cosmic Microwave Background temperature limit allowing the formation of low mass stars in primordial environments. |
id | cern-1559883 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2013 |
record_format | invenio |
spelling | cern-15598832023-03-14T17:46:05Zdoi:10.1093/mnras/stt2049http://cds.cern.ch/record/1559883engPrieto, JoaquinJimenez, RaulVerde, LiciaOvercooled haloes at z ≥ 10: a route to form low-mass first starsAstrophysics and AstronomyIt has been shown by Shchekinov & Vasiliev2006 (SV06) that HD molecules can be an important cooling agent in high redshift z >10 haloes if they undergo mergers under specific conditions so suitable shocks are created. Here we build upon Prieto et al. (2012) who studied in detail the merger-generated shocks, and show that the conditions for HD cooling can be studied by combining these results with a suite of dark-matter only simulations. We have performed a number of dark matter only simulations from cosmological initial conditions inside boxes with sizes from 1 to 4 Mpc. We look for haloes with at least two progenitors of which at least one has mass M > M_cr (z), where M_cr (z) is the SV06 critical mass for HD over-cooling. We find that the fraction of over-cooled haloes with mass between M_cr (z) and 10^{0.2} M_cr (z), roughly below the atomic cooling limit, can be as high as ~ 0.6 at z ~ 10 depending on the merger mass ratio. This fraction decreases at higher redshift reaching a value ~0.2 at z ~ 15. For higher masses, i.e. above 10^{0.2} M_cr (z) up to 10^{0.6} M_cr (z), above the atomic cooling limit, this fraction rises to values ~ 0.8 until z ~ 12.5. As a consequence, a non negligible fraction of high redshift z > 10 mini-haloes can drop their gas temperature to the Cosmic Microwave Background temperature limit allowing the formation of low mass stars in primordial environments.It has been shown by Shchekinov and Vasiliev (SV06) that HD molecules can be an important cooling agent in high redshift z ≥ 10 haloes if they undergo mergers under specific conditions so suitable shocks are created. Here, we build upon Prieto et al. who studied in detail the merger-generated shocks, and show that the conditions for HD cooling can be studied by combining these results with a suite of dark matter only simulations. We have performed a number of dark matter only simulations from cosmological initial conditions inside boxes with sizes from 1 to 4 Mpc. We look for haloes with at least two progenitors of which at least one has mass M ≥ M_cr(z), where M_cr(z) is the SV06 critical mass for HD overcooling. We find that the fraction of overcooled haloes with mass between M_cr(z) and 10^0.2M_cr(z), roughly below the atomic cooling limit, can be as high as ∼0.6 at z ≈ 10 depending on the merger mass ratio. This fraction decreases at higher redshift reaching a value ∼0.2 at z ≈ 15. For higher masses, i.e. above 10^0.2M_cr(z) up to 10^0.6M_cr(z), above the atomic cooling limit, this fraction rises to values ≳ 0.8 until z ≈ 12.5. As a consequence, a non-negligible fraction of high redshift z ≳ 10 mini-haloes can drop their gas temperature to the cosmic microwave background temperature limit allowing the formation of low-mass stars in primordial environments.It has been shown by Shchekinov & Vasiliev2006 (SV06) that HD molecules can be an important cooling agent in high redshift z >10 haloes if they undergo mergers under specific conditions so suitable shocks are created. Here we build upon Prieto et al. (2012) who studied in detail the merger-generated shocks, and show that the conditions for HD cooling can be studied by combining these results with a suite of dark-matter only simulations. We have performed a number of dark matter only simulations from cosmological initial conditions inside boxes with sizes from 1 to 4 Mpc. We look for haloes with at least two progenitors of which at least one has mass M > M_cr (z), where M_cr (z) is the SV06 critical mass for HD over-cooling. We find that the fraction of over-cooled haloes with mass between M_cr (z) and 10^{0.2} M_cr (z), roughly below the atomic cooling limit, can be as high as ~ 0.6 at z ~ 10 depending on the merger mass ratio. This fraction decreases at higher redshift reaching a value ~0.2 at z ~ 15. For higher masses, i.e. above 10^{0.2} M_cr (z) up to 10^{0.6} M_cr (z), above the atomic cooling limit, this fraction rises to values ~ 0.8 until z ~ 12.5. As a consequence, a non negligible fraction of high redshift z > 10 mini-haloes can drop their gas temperature to the Cosmic Microwave Background temperature limit allowing the formation of low mass stars in primordial environments.arXiv:1307.1295oai:cds.cern.ch:15598832013-07-04 |
spellingShingle | Astrophysics and Astronomy Prieto, Joaquin Jimenez, Raul Verde, Licia Overcooled haloes at z ≥ 10: a route to form low-mass first stars |
title | Overcooled haloes at z ≥ 10: a route to form low-mass first stars |
title_full | Overcooled haloes at z ≥ 10: a route to form low-mass first stars |
title_fullStr | Overcooled haloes at z ≥ 10: a route to form low-mass first stars |
title_full_unstemmed | Overcooled haloes at z ≥ 10: a route to form low-mass first stars |
title_short | Overcooled haloes at z ≥ 10: a route to form low-mass first stars |
title_sort | overcooled haloes at z ≥ 10: a route to form low-mass first stars |
topic | Astrophysics and Astronomy |
url | https://dx.doi.org/10.1093/mnras/stt2049 http://cds.cern.ch/record/1559883 |
work_keys_str_mv | AT prietojoaquin overcooledhaloesatz10aroutetoformlowmassfirststars AT jimenezraul overcooledhaloesatz10aroutetoformlowmassfirststars AT verdelicia overcooledhaloesatz10aroutetoformlowmassfirststars |