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dc.contributor.authorErcolano, B.
dc.contributor.authorBonnell, I.~A.
dc.contributor.authorDale, James
dc.date.accessioned2017-07-12T16:32:35Z
dc.date.available2017-07-12T16:32:35Z
dc.date.issued2015-07-21
dc.identifier.citationErcolano , B , Bonnell , I A & Dale , J 2015 , ' Early evolution of embedded clusters ' , Monthly Notices of the Royal Astronomical Society , vol. 451 , no. 1 , pp. 987-1003 . https://doi.org/10.1093/mnras/stv913
dc.identifier.issn0035-8711
dc.identifier.otherPURE: 11150811
dc.identifier.otherPURE UUID: ab15eacc-2054-4f13-8b34-e264932ba993
dc.identifier.otherBibtex: urn:ae7f90ccd3275731371402c40272dcc7
dc.identifier.otherScopus: 84938258813
dc.identifier.otherORCID: /0000-0001-5252-5771/work/62751070
dc.identifier.urihttp://hdl.handle.net/2299/18897
dc.descriptionThis article has been accepted for publication in Monthly Notices of the Royal Astronomical Society. © 2015 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society.
dc.description.abstractWe examine the combined effects of winds and photoionizing radiation from O-type stars on embedded stellar clusters formed in model turbulent molecular clouds covering a range of masses and radii. We find that feedback is able to increase the quantities of dense gas present, but decreases the rate and efficiency of the conversion of gas to stars relative to control simulations in which feedback is absent. Star formation in these calculations often proceeds at a rate substantially slower than the freefall rate in the dense gas. This decoupling is due to the weakening of, and expulsion of gas from, the deepest parts of the clouds’ potential wells where most of the star formation occurs in the control simulations. This results in large fractions of the stellar populations in the feedback simulation becoming dissociated from dense gas. However, where star formation does occur in both control and feedback simulations, it does so in dense gas, so the correlation between star formation activity and dense gas is preserved. The overall dynamical effects of feedback on the clusters are minimal, with only small fraction of stars becoming unbound, despite large quantities of gas being expelled from some clouds. This owes to the settling of the stars into virialized and stellar-dominated configurations before the onset of feedback. By contrast, the effects of feedback on the observable properties of the clusters – their U-, B- and V-band magnitudes – are strong and sudden. The time-scales on which the clusters become visible and unobscured are short compared with the time-scales which the clouds are actually destroyed.en
dc.format.extent17
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Society
dc.subjectstars: formation, ISM: bubbles, H II regions
dc.titleEarly evolution of embedded clustersen
dc.contributor.institutionCentre for Astrophysics Research
dc.description.statusPeer reviewed
rioxxterms.versionVoR
rioxxterms.versionofrecordhttps://doi.org/10.1093/mnras/stv913
rioxxterms.typeJournal Article/Review
herts.preservation.rarelyaccessedtrue


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