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dc.contributor.authorWurster, James
dc.contributor.authorBate, Matthew R
dc.contributor.authorPrice, Daniel J
dc.contributor.authorBonnell, Ian A
dc.date.accessioned2022-04-21T15:31:15Z
dc.date.available2022-04-21T15:31:15Z
dc.date.issued2022-03-01
dc.identifier277693287
dc.identifier631a312a-dcf3-4e0c-b436-cdaed1c8972a
dc.identifier000770033800020
dc.identifier85130423089
dc.identifier.citationWurster , J , Bate , M R , Price , D J & Bonnell , I A 2022 , ' On the origin of magnetic fields in stars II : the effect of numerical resolution ' , Monthly Notices of the Royal Astronomical Society , vol. 511 , no. 1 , pp. 746–764 . https://doi.org/10.1093/mnras/stac123en
dc.identifier.issn0035-8711
dc.identifier.otherJisc: 375997255a9b4f998a33a116eaf8d3bc
dc.identifier.otherORCID: /0000-0003-0688-5332/work/111975646
dc.identifier.urihttps://hdl.handle.net/10023/25226
dc.descriptionFunding: JW and MRB acknowledge support from the European Research Council under the European Community’s Seventh Framework Programme (FP7/2007-2013 grant agreement no. 339248). JW and IAB acknowledge support from the University of St Andrews.en
dc.description.abstractAre the kG-strength magnetic fields observed in young stars a fossil field left over from their formation or are they generated by a dynamo? Our previous numerical study concluded that magnetic fields must originate by a dynamo process. Here, we continue that investigation by performing even higher numerical resolution calculations of the gravitational collapse of a 1 M⊙ rotating, magnetised molecular cloud core through the first and second collapse phases until stellar densities are reached. Each model includes Ohmic resistivity, ambipolar diffusion, and the Hall effect. We test six numerical resolutions, using between 105 and 3 × 107 particles to model the cloud. At all but the lowest resolutions, magnetic walls form in the outer parts of the first hydrostatic core, with the maximum magnetic field strength located within the wall rather than at the centre of the core. At high resolution, this magnetic wall is disrupted by the Hall effect, producing a magnetic field with a spiral-shaped distribution of intensity. As the second collapse occurs, this field is dragged inward and grows in strength, with the maximum field strength increasing with resolution. As the second core forms, the maximum field strength exceeds 1 kG in our highest resolution simulations, and the stellar core field strength exceeds this threshold at the highest resolution. Our resolution study suggests that kG-strength magnetic fields may be implanted in low-mass stars during their formation, and may persist over long timescales given that the diffusion timescale for the magnetic field exceeds the age of the Universe.
dc.format.extent19
dc.format.extent4768079
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Societyen
dc.subjectMagnetic fieldsen
dc.subjectMHDen
dc.subjectMethods: numericalsen
dc.subjectStars: formationen
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subjectNDASen
dc.subjectMCCen
dc.subject.lccQBen
dc.subject.lccQCen
dc.titleOn the origin of magnetic fields in stars II : the effect of numerical resolutionen
dc.typeJournal articleen
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.contributor.institutionUniversity of St Andrews. Sir James Mackenzie Institute for Early Diagnosisen
dc.identifier.doi10.1093/mnras/stac123
dc.description.statusPeer revieweden
dc.identifier.urlhttps://arxiv.org/abs/2201.07253en


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