dc.creator |
Arcila-Osejo, Liz Maria |
|
dc.creator |
Sawicki, Marcin, 1969- |
|
dc.creator |
Arnouts, Stephane |
|
dc.creator |
Golob, Anneya |
|
dc.creator |
Moutard, Thibaud |
|
dc.creator |
Sorba, Robert |
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dc.date.accessioned |
2022-04-26T13:08:03Z |
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dc.date.available |
2022-04-26T13:08:03Z |
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dc.date.issued |
2019-04-29 |
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dc.identifier.issn |
1365-2966 |
|
dc.identifier.issn |
0035-8711 |
|
dc.identifier.uri |
http://library2.smu.ca/xmlui/handle/01/30875 |
|
dc.description |
Accepted version |
en_CA |
dc.description.abstract |
We introduce the largest to date survey of massive quiescent galaxies at redshift ζ ∼ 1.6. With these data, which cover 27.6 deg<sup>2</sup>, we can find significant numbers of very rare objects such as ultra-massive quiescent galaxies that populate the extreme massive end of the galaxy mass function, or dense environments that are likely to become present-day massive galaxy clusters. In this paper, the first in a series, we apply our gζ<em>K</em><sub>s</sub> adaptation of the <em>B</em>ζ<em>K</em></span> technique to select our ζ ∼ 1.6 galaxy catalogue and then study the quiescent galaxy stellar mass function with good statistics over <em>M</em>⋆ ∼ 10<sup>10.2_</sup>10<sup>11.7</sup> M<sub>⊙</sub> – a factor of 30 in mass – including 60 ultra-massive ζ ∼ 1.6 quiescent galaxies with <em>M</em><sub>⋆</sub> > 10<sup>11.5</sup> M<sub>⊙</sub>. We find that the stellar mass function of quiescent galaxies at ζ ∼ 1.6 is well represented by the Schechter function over this large mass range. This suggests that the mass-quenching mechanism observed at lower redshifts must have already been well established by this epoch, and that it is likely due to a single physical mechanism over a wide range of mass. This close adherence to the Schechter shape also suggests that neither merging nor gravitational lensing significantly affects the observed quenched population. Finally, comparing measurements of <strong>M<sup>∗</sup> </strong>parameters for quiescent and star-forming populations (ours and from the literature), we find hints of an offset (<strong><em>M</em><sup>∗</sup><sub>SF</sub>><em>M</em></strong><sub><strong>∗PE</strong></sub>), which could suggest that the efficiency of the quenching process evolves with time. |
en_CA |
dc.description.provenance |
Submitted by Sherry Briere (sherry.briere@smu.ca) on 2022-04-26T13:08:03Z
No. of bitstreams: 1
Sawicki_M_article_2019_a.pdf: 1667959 bytes, checksum: 0fad65fcef7a6b1165a8b7f1b83e4620 (MD5) |
en |
dc.description.provenance |
Made available in DSpace on 2022-04-26T13:08:03Z (GMT). No. of bitstreams: 1
Sawicki_M_article_2019_a.pdf: 1667959 bytes, checksum: 0fad65fcef7a6b1165a8b7f1b83e4620 (MD5)
Previous issue date: 2019-07 |
en |
dc.language.iso |
en_CA |
en_CA |
dc.publisher |
Oxford University Press |
en_CA |
dc.publisher |
Royal Astronomical Society |
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dc.relation.uri |
https://arxiv.org/pdf/1904.11654.pdf |
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dc.rights |
This article has been accepted for publication in Monthly Notices of the Royal Astronomical Society © 2019 The Authors. Published by Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved. |
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dc.subject.lcsh |
Galaxies -- Formation |
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dc.subject.lcsh |
Stars -- Initial mass function |
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dc.title |
LARgE Survey – I. Dead monsters: the massive end of the passive galaxy stellar mass function at cosmic noon |
en_CA |
dc.type |
Text |
en_CA |
dcterms.bibliographicCitation |
Monthly Notices of the Royal Astronomical Society 486(4), 4880-4893. (2019) |
en_CA |