Publication:
Evolution of star formation in the UKIDSS Ultra Deep Survey Field - II. Star formation as a function of stellar mass between z = 1.46 and 0.63

dc.contributor.authorAlyssa B. Drakeen_US
dc.contributor.authorChris Simpsonen_US
dc.contributor.authorIvan K. Baldryen_US
dc.contributor.authorPhil A. Jamesen_US
dc.contributor.authorChris A. Collinsen_US
dc.contributor.authorMasami Ouchien_US
dc.contributor.authorSuraphong Yumaen_US
dc.contributor.authorJames S. Dunlopen_US
dc.contributor.authorDaniel J.B. Smithen_US
dc.contributor.otherLiverpool John Moores Universityen_US
dc.contributor.otherUniversite Claude Bernard Lyon 1en_US
dc.contributor.otherUniversity of Tokyoen_US
dc.contributor.otherMahidol Universityen_US
dc.contributor.otherUniversity of Edinburgh, Institute for Astronomyen_US
dc.contributor.otherUniversity of Hertfordshireen_US
dc.date.accessioned2018-11-23T10:04:23Z
dc.date.available2018-11-23T10:04:23Z
dc.date.issued2015-01-01en_US
dc.description.abstract© 2015 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society. We present new results on the evolution of the cosmic star formation rate as a function of stellar mass in the Subaru/XMM-Newton Deep Survey-Ultra Deep Survey field. We make use of narrow-band-selected emission line galaxies in four redshift slices between z = 1.46 and 0.63, and compute stellar masses by fitting a series of templates to recreate each galaxy's star formation history. We determine mass-binned luminosity functions in each redshift slice, and derive the star formation rate density (ρSFR) as a function of mass using the [O III] or [O II] emission lines. We calculate dust extinction and metallicity as a function of stellar mass, and investigate the effect of these corrections on the shape of the overall ρSFR(M). We find that both these corrections are crucial for determining the shape of the ρSFR(M), and its evolution with redshift. The fully corrected ρSFR(M) is a relatively flat distribution, with the normalization moving towards lower values of ρSFR with increasing cosmic time/decreasing redshift, and requiring star formation to be truncated across all masses studied here. The peak of ρSFR(M) is found in the 1010.5 < M⊙ < 1011.0 mass bin at z = 1.46. In the lower redshift slices, the location of the peak is less certain; however, low-mass galaxies in the range 107.0 < M⊙ < 108.0 play an important part in the overall ρSFR(M) out to at least z ~ 1.2.en_US
dc.identifier.citationMonthly Notices of the Royal Astronomical Society. Vol.454, No.2 (2015), 2015-2025en_US
dc.identifier.doi10.1093/mnras/stv2027en_US
dc.identifier.issn13652966en_US
dc.identifier.issn00358711en_US
dc.identifier.other2-s2.0-84963559841en_US
dc.identifier.urihttps://repository.li.mahidol.ac.th/handle/20.500.14594/35892
dc.rightsMahidol Universityen_US
dc.rights.holderSCOPUSen_US
dc.source.urihttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84963559841&origin=inwarden_US
dc.subjectEarth and Planetary Sciencesen_US
dc.titleEvolution of star formation in the UKIDSS Ultra Deep Survey Field - II. Star formation as a function of stellar mass between z = 1.46 and 0.63en_US
dc.typeArticleen_US
dspace.entity.typePublication
mu.datasource.scopushttps://www.scopus.com/inward/record.uri?partnerID=HzOxMe3b&scp=84963559841&origin=inwarden_US

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