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dc.contributor.authorDunlop, J. S.
dc.contributor.authorMcLure, R. J.
dc.contributor.authorBiggs, A. D.
dc.contributor.authorGeach, J. E.
dc.contributor.authorMichalowski, M. J.
dc.contributor.authorIvison, R. J.
dc.contributor.authorRujopakarn, W.
dc.contributor.authorKampen, E. van
dc.contributor.authorKirkpatrick, A.
dc.contributor.authorPope, A.
dc.contributor.authorScott, D.
dc.contributor.authorSwinbank, A. M.
dc.contributor.authorTargett, T. A.
dc.contributor.authorAretxaga, I.
dc.contributor.authorAustermann, J. E.
dc.contributor.authorBest, P. N.
dc.contributor.authorBruce, V. A.
dc.contributor.authorChapin, E. L.
dc.contributor.authorCharlot, S.
dc.contributor.authorCirasuolo, M.
dc.contributor.authorCoppin, K. E. K.
dc.contributor.authorEllis, R. S.
dc.contributor.authorFinkelstein, S. L.
dc.contributor.authorHayward, C. C.
dc.contributor.authorHughes, D. H.
dc.contributor.authorIbar, E.
dc.contributor.authorKhochfar, S.
dc.contributor.authorKoprowski, M. P.
dc.contributor.authorNarayanan, D.
dc.contributor.authorPapovich, C.
dc.contributor.authorPeacock, J. A.
dc.contributor.authorRobertson, B.
dc.contributor.authorVernstrom, T.
dc.contributor.authorWerf, P. P. van der
dc.contributor.authorWilson, G. W.
dc.contributor.authorYun, M.
dc.date.accessioned2017-04-03T15:21:20Z
dc.date.available2017-04-03T15:21:20Z
dc.date.issued2017-04-01
dc.identifier.citationDunlop , J S , McLure , R J , Biggs , A D , Geach , J E , Michalowski , M J , Ivison , R J , Rujopakarn , W , Kampen , E V , Kirkpatrick , A , Pope , A , Scott , D , Swinbank , A M , Targett , T A , Aretxaga , I , Austermann , J E , Best , P N , Bruce , V A , Chapin , E L , Charlot , S , Cirasuolo , M , Coppin , K E K , Ellis , R S , Finkelstein , S L , Hayward , C C , Hughes , D H , Ibar , E , Khochfar , S , Koprowski , M P , Narayanan , D , Papovich , C , Peacock , J A , Robertson , B , Vernstrom , T , Werf , P P V D , Wilson , G W & Yun , M 2017 , ' A deep ALMA image of the Hubble Ultra Deep Field ' , Monthly Notices of the Royal Astronomical Society , vol. 466 , no. 1 , pp. 861-883 . https://doi.org/10.1093/mnras/stw3088
dc.identifier.issn0035-8711
dc.identifier.otherPURE: 10389623
dc.identifier.otherPURE UUID: 73ff8e78-27d7-490d-9b4b-2c884c88192f
dc.identifier.otherArXiv: http://arxiv.org/abs/1606.00227v1
dc.identifier.otherScopus: 85013228290
dc.identifier.otherORCID: /0000-0002-0729-2988/work/30423042
dc.identifier.urihttp://hdl.handle.net/2299/17744
dc.descriptionThis article has been accepted for publication in Monthly Notices of the Royal Astronomical Society, © : 2016, J.S. Dunlop, et al, MNRAS (April 1, 2017) 466 (1): 861-883, first published online November 30, 2016, by Oxford University Press on behalf of MNRAS. The version of record is available on line at doi: 10.1093/mnras/stw3088
dc.description.abstractWe present the results of the first, deep ALMA imaging covering the full 4.5 sq arcmin of the Hubble Ultra Deep Field (HUDF) as previously imaged with WFC3/IR on HST. Using a mosaic of 45 pointings, we have obtained a homogeneous 1.3mm image of the HUDF, achieving an rms sensitivity of 35 microJy, at a resolution of 0.7 arcsec. From an initial list of ~50 >3.5sigma peaks, a rigorous analysis confirms 16 sources with flux densities S(1.3) > 120 microJy. All of these have secure galaxy counterparts with robust redshifts ( = 2.15), and 12 are also detected at 6GHz in new deep JVLA imaging. Due to the wealth of supporting data in this unique field, the physical properties of the ALMA sources are well constrained, including their stellar masses (M*) and UV+FIR star-formation rates (SFR). Our results show that stellar mass is the best predictor of SFR in the high-z Universe; indeed at z > 2 our ALMA sample contains 7 of the 9 galaxies in the HUDF with M* > 2 x 10^10 Msun and we detect only one galaxy at z > 3.5, reflecting the rapid drop-off of high-mass galaxies with increasing redshift. The detections, coupled with stacking, allow us to probe the redshift/mass distribution of the 1.3-mm background down to S(1.3) ~ 10 micro-Jy. We find strong evidence for a steep `main sequence' for star-forming galaxies at z ~ 2, with SFR \propto M* and a mean specific SFR = 2.2 /Gyr. Moreover, we find that ~85% of total star formation at z ~ 2 is enshrouded in dust, with ~65% of all star formation at this epoch occurring in high-mass galaxies (M* > 2 x 10^10 Msun), for which the average obscured:unobscured SF ratio is ~200. Finally, we combine our new ALMA results with the existing HST data to revisit the cosmic evolution of star-formation rate density; we find that this peaks at z ~ 2.5, and that the star-forming Universe transits from primarily unobscured to primarily obscured thereafter at z ~ 4.en
dc.language.isoeng
dc.relation.ispartofMonthly Notices of the Royal Astronomical Society
dc.subjectastro-ph.GA
dc.titleA deep ALMA image of the Hubble Ultra Deep Fielden
dc.contributor.institutionCentre for Astrophysics Research
dc.contributor.institutionSchool of Physics, Astronomy and Mathematics
dc.description.statusPeer reviewed
rioxxterms.versionVoR
rioxxterms.versionofrecordhttps://doi.org/10.1093/mnras/stw3088
rioxxterms.typeJournal Article/Review
herts.preservation.rarelyaccessedtrue


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