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dc.contributor.authorWild, Vivienne
dc.contributor.authorAlmaini, Omar
dc.contributor.authorDunlop, Jim
dc.contributor.authorSimpson, Chris
dc.contributor.authorRowlands, Kate
dc.contributor.authorBowler, Rebecca
dc.contributor.authorMaltby, David
dc.contributor.authorMcLure, Ross
dc.date.accessioned2016-08-12T08:30:33Z
dc.date.available2016-08-12T08:30:33Z
dc.date.issued2016-11-21
dc.identifier.citationWild , V , Almaini , O , Dunlop , J , Simpson , C , Rowlands , K , Bowler , R , Maltby , D & McLure , R 2016 , ' The evolution of post-starburst galaxies from z=2 to 0.5 ' , Monthly Notices of the Royal Astronomical Society , vol. 463 , no. 1 , pp. 832-844 . https://doi.org/10.1093/mnras/stw1996en
dc.identifier.issn0035-8711
dc.identifier.otherPURE: 244954023
dc.identifier.otherPURE UUID: e942f628-76bc-4b1e-bbc1-caba766844af
dc.identifier.otherBibCode: 2016arXiv160800588W
dc.identifier.otherBibCode: 2016MNRAS.463..832W
dc.identifier.otherWOS: 000386464900068
dc.identifier.otherScopus: 84996583940
dc.identifier.urihttps://hdl.handle.net/10023/9291
dc.descriptionV. W. and K. R. acknowledge support of the European Research Council via the award of a starting grant (SEDMorph; P.I. V. Wild).en
dc.description.abstractWe present the evolution in the number density and stellar mass functions of photometrically selected post-starburst galaxies in the UKIDSS Ultra Deep Survey, with redshifts of 0.5 < z < 2 and stellar masses log (M/M⊙) >10. We find that this transitionary species of galaxy is rare at all redshifts, contributing ∼5 per cent of the total population at z ∼ 2, to <1 per cent by z ∼ 0.5. By comparing the mass functions of quiescent galaxies to post-starburst galaxies at three cosmic epochs, we show that rapid quenching of star formation can account for 100 per cent of quiescent galaxy formation, if the post-starburst spectral features are visible for ∼250 Myr. The flattening of the low-mass end of the quiescent galaxy stellar mass function seen at z ∼ 1 can be entirely explained by the addition of rapidly quenched galaxies. Only if a significant fraction of post-starburst galaxies have features that are visible for longer than 250 Myr, or they acquire new gas and return to the star-forming sequence, can there be significant growth of the red sequence from a slower quenching route. The shape of the mass function of these transitory post-starburst galaxies resembles that of quiescent galaxies at z ∼ 2, with a preferred stellar mass of log (M/M⊙) ∼10.6, but evolves steadily to resemble that of star-forming galaxies at z < 1. This leads us to propose a dual origin for post-starburst galaxies: (1) at z ≳ 2 they are exclusively massive galaxies that have formed the bulk of their stars during a rapid assembly period, followed by complete quenching of further star formation; (2) at z ≲ 1 they are caused by the rapid quenching of gas-rich star-forming galaxies, independent of stellar mass, possibly due to environment and/or gas-rich major mergers.
dc.format.extent13
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Societyen
dc.rightsCopyright 2016 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society. This work is made available online in accordance with the publisher’s policies. This is the author created, accepted version manuscript following peer review and may differ slightly from the final published version. The final published version of this work is available at https://dx.doi.org/10.1093/mnras/stw1996en
dc.subjectGalaxies: high-redshiften
dc.subjectGalaxies: luminosity function, mass functionen
dc.subjectGalaxies: formationen
dc.subjectGalaxies: evolutionen
dc.subjectGalaxies: stellar contenten
dc.subjectQB Astronomyen
dc.subjectQC Physicsen
dc.subjectNDASen
dc.subjectBDCen
dc.subject.lccQBen
dc.subject.lccQCen
dc.titleThe evolution of post-starburst galaxies from z=2 to 0.5en
dc.typeJournal articleen
dc.contributor.sponsorEuropean Research Councilen
dc.description.versionPreprinten
dc.description.versionPostprinten
dc.contributor.institutionUniversity of St Andrews. School of Physics and Astronomyen
dc.identifier.doihttps://doi.org/10.1093/mnras/stw1996
dc.description.statusPeer revieweden
dc.identifier.urlhttp://adsabs.harvard.edu/abs/2016arXiv160800588Wen
dc.identifier.grantnumberERC-2012-StG-20111012en


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