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dc.contributor.authorWurster, JH
dc.contributor.authorBate, MR
dc.contributor.authorPrice, DJ
dc.date.accessioned2018-02-01T08:40:16Z
dc.date.issued2018-01-05
dc.description.abstractWe present results from radiation non-ideal magnetohydrodynamics (MHD) calculations that follow the collapse of rotating, magnetized, molecular cloud cores to stellar densities. These are the first such calculations to include all three non-ideal effects: ambipolar diffusion, Ohmic resistivity, and the Hall effect. We employ an ionization model in which cosmic ray ionization dominates at low temperatures and thermal ionization takes over at high temperatures. We explore the effects of varying the cosmic ray ionization rate from ζcr = 10−10 to 10−16 s−1. Models with ionization rates ≳10−12 s−1 produce results that are indistinguishable from ideal MHD. Decreasing the cosmic ray ionization rate extends the lifetime of the first hydrostatic core up to a factor of 2, but the lifetimes are still substantially shorter than those obtained without magnetic fields. Outflows from the first hydrostatic core phase are launched in all models, but the outflows become broader and slower as the ionization rate is reduced. The outflow morphology following stellar core formation is complex and strongly dependent on the cosmic ray ionization rate. Calculations with high ionization rates quickly produce a fast (≈14 km s−1) bipolar outflow that is distinct from the first core outflow, but with the lowest ionization rate, a slower (≈3−4 km s−1) conical outflow develops gradually and seamlessly merges into the first core outflow.en_GB
dc.description.sponsorshipJW and MRB acknowledge support from the European Research Council under the European Commission's Seventh Framework Programme (FP7/2007- 2013 grant agreement no. 339248). DJP and JW were funded by Australian Research Council grants FT130100034 andDP130102078. The calculations for this paper were performed on the University of Exeter Supercomputer, a DiRAC Facility jointly funded by STFC, the Large Facilities Capital Fund of BIS, and the University of Exeter. We used splash (Price 2007) for the column density figures.en_GB
dc.identifier.citationVol. 475, Iss. 2, pp. 1859 - 1880en_GB
dc.identifier.doi10.1093/mnras/stx3339
dc.identifier.urihttp://hdl.handle.net/10871/31265
dc.language.isoenen_GB
dc.publisherOxford University Pressen_GB
dc.relation.urlhttps://doi.org/10.24378/exe.264en_GB
dc.rights© 2018 The Author(s) Published by Oxford University Press on behalf of the Royal Astronomical Societyen_GB
dc.subjectmagnetic fieldsen_GB
dc.subjectMHDen_GB
dc.subjectradiative transferen_GB
dc.subjectmethods: numericalen_GB
dc.subjectstars: formationen_GB
dc.subjectstars: windsen_GB
dc.subjectoutflowsen_GB
dc.titleThe collapse of a molecular cloud core to stellar densities using radiation non-ideal magnetohydrodynamics (article)en_GB
dc.typeArticleen_GB
dc.date.available2018-02-01T08:40:16Z
dc.identifier.issn0035-8711
dc.descriptionThis is the final version of the article. Available from Oxford University Press via the DOI in this record.en_GB
dc.descriptionThe dataset associated with this article is located in ORE at: https://doi.org/10.24378/exe.264en_GB
dc.identifier.journalMonthly Notices of the Royal Astronomical Societyen_GB


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