GAMA/H-ATLAS : the local dust mass function and cosmic density as a function of galaxy type : a benchmark for models of galaxy evolution

We present the dust mass function (DMF) of 15 750 galaxies with redshift z < 0.1, drawn from the overlapping area of the GAMA and H-ATLAS surveys. The DMF is derived using the density corrected V-max method, where we estimate V-max using: (i) the normal photometric selection limit (pV(max)) and (...

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Hauptverfasser: Beeston, RA, Wright, AH, Maddox, S, Gomez, HL, Dunne, L, Driver, SP, Robotham, A, Clark, CJR, Vinsen, K, Takeuchi, TT, Popping, G, Bourne, N, Bremer, MN, Phillipps, S, Moffett, AJ, Baes, Maarten, Bland-Hawthorn, J, Brough, S, De Vis, P, Eales, SA, Holwerda, BW, Loveday, J, Liske, J, Smith, MWL, Smith, DJB, Valiante, E, Vlahakis, C, Wang, L
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creator Beeston, RA
Wright, AH
Maddox, S
Gomez, HL
Dunne, L
Driver, SP
Robotham, A
Clark, CJR
Vinsen, K
Takeuchi, TT
Popping, G
Bourne, N
Bremer, MN
Phillipps, S
Moffett, AJ
Baes, Maarten
Bland-Hawthorn, J
Brough, S
De Vis, P
Eales, SA
Holwerda, BW
Loveday, J
Liske, J
Smith, MWL
Smith, DJB
Valiante, E
Vlahakis, C
Wang, L
description We present the dust mass function (DMF) of 15 750 galaxies with redshift z < 0.1, drawn from the overlapping area of the GAMA and H-ATLAS surveys. The DMF is derived using the density corrected V-max method, where we estimate V-max using: (i) the normal photometric selection limit (pV(max)) and (ii) a bivariate brightness distribution (BBD) technique, which accounts for two selection effects. We fit the data with a Schechter function, and find M* = (4.65 +/- 0.18) x 10(7) h(70)(2) M-circle dot, alpha = (-1.22 +/- 0.01), phi* = (6.26 +/- 0.28) x 10(-3) h(70)(3) Mpc(-3) dex(-1) . The resulting dust mass density parameter integrated down to 10(4) M-circle dot is Omega(d) = (1.11 +/- 0.02) x 10(-6) which implies the mass fraction of baryons in dust is f(mb) = (2.40 +/- 0.04) x 10(-5); cosmic variance adds an extra 7-17 per cent uncertainty to the quoted statistical errors. Our measurements have fewer galaxies with high dust mass than predicted by semi-analytic models. This is because the models include too much dust in high stellar mass galaxies. Conversely, our measurements find more galaxies with high dust mass than predicted by hydrodynamical cosmological simulations. This is likely to be from the long time-scales for grain growth assumed in the models. We calculate DMFs split by galaxy type and find dust mass densities of Omega(d) = (0.88 +/- 0.03) x 10(-6) and Omega(d) = (0.060 +/- 0.005) x 10(-6) for late types and early types, respectively. Comparing to the equivalent galaxy stellar mass functions (GSMF) we find that the DMF for late types is well matched by the GSMF scaled by (8.07 +/- 0.35) x 10(-4).
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The DMF is derived using the density corrected V-max method, where we estimate V-max using: (i) the normal photometric selection limit (pV(max)) and (ii) a bivariate brightness distribution (BBD) technique, which accounts for two selection effects. We fit the data with a Schechter function, and find M* = (4.65 +/- 0.18) x 10(7) h(70)(2) M-circle dot, alpha = (-1.22 +/- 0.01), phi* = (6.26 +/- 0.28) x 10(-3) h(70)(3) Mpc(-3) dex(-1) . The resulting dust mass density parameter integrated down to 10(4) M-circle dot is Omega(d) = (1.11 +/- 0.02) x 10(-6) which implies the mass fraction of baryons in dust is f(mb) = (2.40 +/- 0.04) x 10(-5); cosmic variance adds an extra 7-17 per cent uncertainty to the quoted statistical errors. Our measurements have fewer galaxies with high dust mass than predicted by semi-analytic models. This is because the models include too much dust in high stellar mass galaxies. Conversely, our measurements find more galaxies with high dust mass than predicted by hydrodynamical cosmological simulations. This is likely to be from the long time-scales for grain growth assumed in the models. We calculate DMFs split by galaxy type and find dust mass densities of Omega(d) = (0.88 +/- 0.03) x 10(-6) and Omega(d) = (0.060 +/- 0.005) x 10(-6) for late types and early types, respectively. 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The DMF is derived using the density corrected V-max method, where we estimate V-max using: (i) the normal photometric selection limit (pV(max)) and (ii) a bivariate brightness distribution (BBD) technique, which accounts for two selection effects. We fit the data with a Schechter function, and find M* = (4.65 +/- 0.18) x 10(7) h(70)(2) M-circle dot, alpha = (-1.22 +/- 0.01), phi* = (6.26 +/- 0.28) x 10(-3) h(70)(3) Mpc(-3) dex(-1) . The resulting dust mass density parameter integrated down to 10(4) M-circle dot is Omega(d) = (1.11 +/- 0.02) x 10(-6) which implies the mass fraction of baryons in dust is f(mb) = (2.40 +/- 0.04) x 10(-5); cosmic variance adds an extra 7-17 per cent uncertainty to the quoted statistical errors. Our measurements have fewer galaxies with high dust mass than predicted by semi-analytic models. This is because the models include too much dust in high stellar mass galaxies. Conversely, our measurements find more galaxies with high dust mass than predicted by hydrodynamical cosmological simulations. This is likely to be from the long time-scales for grain growth assumed in the models. We calculate DMFs split by galaxy type and find dust mass densities of Omega(d) = (0.88 +/- 0.03) x 10(-6) and Omega(d) = (0.060 +/- 0.005) x 10(-6) for late types and early types, respectively. 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Wright, AH ; Maddox, S ; Gomez, HL ; Dunne, L ; Driver, SP ; Robotham, A ; Clark, CJR ; Vinsen, K ; Takeuchi, TT ; Popping, G ; Bourne, N ; Bremer, MN ; Phillipps, S ; Moffett, AJ ; Baes, Maarten ; Bland-Hawthorn, J ; Brough, S ; De Vis, P ; Eales, SA ; Holwerda, BW ; Loveday, J ; Liske, J ; Smith, MWL ; Smith, DJB ; Valiante, E ; Vlahakis, C ; Wang, L</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-ghent_librecat_oai_archive_ugent_be_86074193</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>ASSEMBLY GAMA</topic><topic>DATA RELEASE</topic><topic>dust</topic><topic>extinction</topic><topic>FORMATION HISTORY</topic><topic>galaxies: ISM</topic><topic>galaxies: luminosity function</topic><topic>galaxies: statistics</topic><topic>HERSCHEL-ATLAS</topic><topic>INFRARED-EMISSION</topic><topic>LOW-REDSHIFT</topic><topic>LUMINOSITY FUNCTION</topic><topic>mass function</topic><topic>Physics and Astronomy</topic><topic>SPECTRAL ENERGY-DISTRIBUTION</topic><topic>STAR-FORMING GALAXIES</topic><topic>SUBMILLIMETER LUMINOSITY</topic><topic>submillimetre: ISM</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Beeston, RA</creatorcontrib><creatorcontrib>Wright, AH</creatorcontrib><creatorcontrib>Maddox, S</creatorcontrib><creatorcontrib>Gomez, HL</creatorcontrib><creatorcontrib>Dunne, L</creatorcontrib><creatorcontrib>Driver, SP</creatorcontrib><creatorcontrib>Robotham, A</creatorcontrib><creatorcontrib>Clark, CJR</creatorcontrib><creatorcontrib>Vinsen, K</creatorcontrib><creatorcontrib>Takeuchi, TT</creatorcontrib><creatorcontrib>Popping, G</creatorcontrib><creatorcontrib>Bourne, N</creatorcontrib><creatorcontrib>Bremer, MN</creatorcontrib><creatorcontrib>Phillipps, S</creatorcontrib><creatorcontrib>Moffett, AJ</creatorcontrib><creatorcontrib>Baes, Maarten</creatorcontrib><creatorcontrib>Bland-Hawthorn, J</creatorcontrib><creatorcontrib>Brough, S</creatorcontrib><creatorcontrib>De Vis, P</creatorcontrib><creatorcontrib>Eales, SA</creatorcontrib><creatorcontrib>Holwerda, BW</creatorcontrib><creatorcontrib>Loveday, J</creatorcontrib><creatorcontrib>Liske, J</creatorcontrib><creatorcontrib>Smith, MWL</creatorcontrib><creatorcontrib>Smith, DJB</creatorcontrib><creatorcontrib>Valiante, E</creatorcontrib><creatorcontrib>Vlahakis, C</creatorcontrib><creatorcontrib>Wang, L</creatorcontrib><collection>Ghent University Academic Bibliography</collection></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Beeston, RA</au><au>Wright, AH</au><au>Maddox, S</au><au>Gomez, HL</au><au>Dunne, L</au><au>Driver, SP</au><au>Robotham, A</au><au>Clark, CJR</au><au>Vinsen, K</au><au>Takeuchi, TT</au><au>Popping, G</au><au>Bourne, N</au><au>Bremer, MN</au><au>Phillipps, S</au><au>Moffett, AJ</au><au>Baes, Maarten</au><au>Bland-Hawthorn, J</au><au>Brough, S</au><au>De Vis, P</au><au>Eales, SA</au><au>Holwerda, BW</au><au>Loveday, J</au><au>Liske, J</au><au>Smith, MWL</au><au>Smith, DJB</au><au>Valiante, E</au><au>Vlahakis, C</au><au>Wang, L</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>GAMA/H-ATLAS : the local dust mass function and cosmic density as a function of galaxy type : a benchmark for models of galaxy evolution</atitle><date>2018</date><risdate>2018</risdate><issn>0035-8711</issn><issn>1365-2966</issn><abstract>We present the dust mass function (DMF) of 15 750 galaxies with redshift z &lt; 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The DMF is derived using the density corrected V-max method, where we estimate V-max using: (i) the normal photometric selection limit (pV(max)) and (ii) a bivariate brightness distribution (BBD) technique, which accounts for two selection effects. We fit the data with a Schechter function, and find M* = (4.65 +/- 0.18) x 10(7) h(70)(2) M-circle dot, alpha = (-1.22 +/- 0.01), phi* = (6.26 +/- 0.28) x 10(-3) h(70)(3) Mpc(-3) dex(-1) . The resulting dust mass density parameter integrated down to 10(4) M-circle dot is Omega(d) = (1.11 +/- 0.02) x 10(-6) which implies the mass fraction of baryons in dust is f(mb) = (2.40 +/- 0.04) x 10(-5); cosmic variance adds an extra 7-17 per cent uncertainty to the quoted statistical errors. Our measurements have fewer galaxies with high dust mass than predicted by semi-analytic models. This is because the models include too much dust in high stellar mass galaxies. Conversely, our measurements find more galaxies with high dust mass than predicted by hydrodynamical cosmological simulations. This is likely to be from the long time-scales for grain growth assumed in the models. We calculate DMFs split by galaxy type and find dust mass densities of Omega(d) = (0.88 +/- 0.03) x 10(-6) and Omega(d) = (0.060 +/- 0.005) x 10(-6) for late types and early types, respectively. Comparing to the equivalent galaxy stellar mass functions (GSMF) we find that the DMF for late types is well matched by the GSMF scaled by (8.07 +/- 0.35) x 10(-4).</abstract><oa>free_for_read</oa></addata></record>
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source Oxford Journals Open Access Collection; Ghent University Academic Bibliography
subjects ASSEMBLY GAMA
DATA RELEASE
dust
extinction
FORMATION HISTORY
galaxies: ISM
galaxies: luminosity function
galaxies: statistics
HERSCHEL-ATLAS
INFRARED-EMISSION
LOW-REDSHIFT
LUMINOSITY FUNCTION
mass function
Physics and Astronomy
SPECTRAL ENERGY-DISTRIBUTION
STAR-FORMING GALAXIES
SUBMILLIMETER LUMINOSITY
submillimetre: ISM
title GAMA/H-ATLAS : the local dust mass function and cosmic density as a function of galaxy type : a benchmark for models of galaxy evolution
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