The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation

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The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation. / Ren, Keven; Trenti, Michele; Mason, Charlotte A.

I: Astrophysical Journal, Bind 878, Nr. 2, 114, 20.06.2019.

Publikation: Bidrag til tidsskriftTidsskriftartikelForskningfagfællebedømt

Harvard

Ren, K, Trenti, M & Mason, CA 2019, 'The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation', Astrophysical Journal, bind 878, nr. 2, 114. https://doi.org/10.3847/1538-4357/ab2117

APA

Ren, K., Trenti, M., & Mason, C. A. (2019). The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation. Astrophysical Journal, 878(2), [114]. https://doi.org/10.3847/1538-4357/ab2117

Vancouver

Ren K, Trenti M, Mason CA. The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation. Astrophysical Journal. 2019 jun. 20;878(2). 114. https://doi.org/10.3847/1538-4357/ab2117

Author

Ren, Keven ; Trenti, Michele ; Mason, Charlotte A. / The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation. I: Astrophysical Journal. 2019 ; Bind 878, Nr. 2.

Bibtex

@article{dc1496ae9fbd4cae8dc5a774b20f2017,
title = "The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation",
abstract = "The Ultraviolet Luminosity Function (UVLF) is a key observable for understanding galaxy formation from cosmic dawn. There has been considerable debate on whether Schechter-like LFs (characterized by an exponential dropoff at the bright end) that describe the LF in our local universe are also a sufficient description of the LF at high redshifts (z > 6). We model the UVLF over cosmic history with a semi-empirical framework and include a log-normal scatter, Sigma, in galaxy luminosities with a conditional luminosity function approach. We show that stochasticity induces a flattening or a feedback scale in the median galaxy luminosity versus halo mass relation, L-c(M-h), to account for the increase of bright objects placed in lower-mass halos. We observe a natural broadening in the bright-end exponential segment of the UVLF for z > 6 if processes that regulate star formation acts on the same mass scale as at z similar to 5, where the degree of broadening is enhanced for larger Sigma. Alternatively, if the brightend feedback is triggered at a near-constant luminosity threshold, the feedback threshold occurs at progressively lower halo masses with increasing redshift, due to galaxies being more luminous on average at a fixed halo mass from rapid halo assembly. Such feedback results in an LF shape with a bright-end closer to that of a Schechter function. We include predictions for the z > 8 UVLFs from future all-sky surveys such as WFIRST, which has the potential to both quantify the scatter and type of feedback, and provide insight behind the mechanisms that drive star formation in the early universe.",
keywords = "galaxies: formation, galaxies: high-redshift, galaxies: luminosity function, mass function, HIGH-REDSHIFT GALAXIES, STELLAR MASS, DEEP FIELD, TO 8, REIONIZATION, END",
author = "Keven Ren and Michele Trenti and Mason, {Charlotte A.}",
year = "2019",
month = jun,
day = "20",
doi = "10.3847/1538-4357/ab2117",
language = "English",
volume = "878",
journal = "Astrophysical Journal",
issn = "0067-0049",
publisher = "Institute of Physics Publishing, Inc",
number = "2",

}

RIS

TY - JOUR

T1 - The Brightest Galaxies at Cosmic Dawn from Scatter in the Galaxy Luminosity versus Halo Mass Relation

AU - Ren, Keven

AU - Trenti, Michele

AU - Mason, Charlotte A.

PY - 2019/6/20

Y1 - 2019/6/20

N2 - The Ultraviolet Luminosity Function (UVLF) is a key observable for understanding galaxy formation from cosmic dawn. There has been considerable debate on whether Schechter-like LFs (characterized by an exponential dropoff at the bright end) that describe the LF in our local universe are also a sufficient description of the LF at high redshifts (z > 6). We model the UVLF over cosmic history with a semi-empirical framework and include a log-normal scatter, Sigma, in galaxy luminosities with a conditional luminosity function approach. We show that stochasticity induces a flattening or a feedback scale in the median galaxy luminosity versus halo mass relation, L-c(M-h), to account for the increase of bright objects placed in lower-mass halos. We observe a natural broadening in the bright-end exponential segment of the UVLF for z > 6 if processes that regulate star formation acts on the same mass scale as at z similar to 5, where the degree of broadening is enhanced for larger Sigma. Alternatively, if the brightend feedback is triggered at a near-constant luminosity threshold, the feedback threshold occurs at progressively lower halo masses with increasing redshift, due to galaxies being more luminous on average at a fixed halo mass from rapid halo assembly. Such feedback results in an LF shape with a bright-end closer to that of a Schechter function. We include predictions for the z > 8 UVLFs from future all-sky surveys such as WFIRST, which has the potential to both quantify the scatter and type of feedback, and provide insight behind the mechanisms that drive star formation in the early universe.

AB - The Ultraviolet Luminosity Function (UVLF) is a key observable for understanding galaxy formation from cosmic dawn. There has been considerable debate on whether Schechter-like LFs (characterized by an exponential dropoff at the bright end) that describe the LF in our local universe are also a sufficient description of the LF at high redshifts (z > 6). We model the UVLF over cosmic history with a semi-empirical framework and include a log-normal scatter, Sigma, in galaxy luminosities with a conditional luminosity function approach. We show that stochasticity induces a flattening or a feedback scale in the median galaxy luminosity versus halo mass relation, L-c(M-h), to account for the increase of bright objects placed in lower-mass halos. We observe a natural broadening in the bright-end exponential segment of the UVLF for z > 6 if processes that regulate star formation acts on the same mass scale as at z similar to 5, where the degree of broadening is enhanced for larger Sigma. Alternatively, if the brightend feedback is triggered at a near-constant luminosity threshold, the feedback threshold occurs at progressively lower halo masses with increasing redshift, due to galaxies being more luminous on average at a fixed halo mass from rapid halo assembly. Such feedback results in an LF shape with a bright-end closer to that of a Schechter function. We include predictions for the z > 8 UVLFs from future all-sky surveys such as WFIRST, which has the potential to both quantify the scatter and type of feedback, and provide insight behind the mechanisms that drive star formation in the early universe.

KW - galaxies: formation

KW - galaxies: high-redshift

KW - galaxies: luminosity function, mass function

KW - HIGH-REDSHIFT GALAXIES

KW - STELLAR MASS

KW - DEEP FIELD

KW - TO 8

KW - REIONIZATION

KW - END

U2 - 10.3847/1538-4357/ab2117

DO - 10.3847/1538-4357/ab2117

M3 - Journal article

VL - 878

JO - Astrophysical Journal

JF - Astrophysical Journal

SN - 0067-0049

IS - 2

M1 - 114

ER -

ID: 344976078