J/PASJ/70/S10       GOLDRUSH I. UV magnitudes                (Ono+, 2018)

Great Optically Luminous Dropout Research Using Subaru HSC (GOLDRUSH). I. UV luminosity functions at z∼4-7 derived with the half-million dropouts on the 100 deg2 sky. Ono Y., Ouchi M., Harikane Y., Toshikawa J., Rauch M., Yuma S., Sawicki M., Shibuya T., Shimasaku K., Oguri M., Willott C., Akhlaghi M., AkiyamaI M., Coupon J., Kashikawa N., Komiyama Y., Konno A., Lin L., Matsuoka Y., Miyazaki S., Nagao T., Nakajima K., SilvermaniJ., Tanaka M., Taniguchi Y., Wang S.-Y. <Publ. Astron. Soc. Jap., 70, S10 (2018)> =2018PASJ...70S..10O 2018PASJ...70S..10O (SIMBAD/NED BibCode)
ADC_Keywords: Galaxies, photometry ; Photometry, ultraviolet ; Redshifts Keywords: galaxies: formation - galaxies: evolution - galaxies: high-redshift Abstract: We study the UV luminosity functions (LFs) at z∼4, 5, 6, and 7 based on the deep large-area optical images taken by the Hyper Suprime-Cam (HSC) Subaru Strategic Program (SSP). On the 100 deg2 sky of the HSC SSP data available to date, we take enormous samples consisting of a total of 579565 dropout candidates at z∼4-7 by the standard color selection technique, 358 out of which are spectroscopically confirmed by our follow-up spectroscopy and other studies. We obtain UV LFs at z∼4-7 that span a very wide UV luminosity range of ∼0.002-100L*UV(-26<MUV←14mag) by combining LFs from our program and the ultra-deep Hubble Space Telescope legacy surveys. We derive three parameters of the best-fit Schechter function, Φ*, MUV, and α, of the UV LFs in the magnitude range where the active galactic nucleus (AGN) contribution is negligible, and find that and Φ* decrease from z∼4 to 7 with no significant evolution of MUV. Because our HSC SSP data bridge the LFs of galaxies and AGNs with great statistical accuracy, we carefully investigate the bright end of the galaxy UV LFs that are estimated by the subtraction of the AGN contribution either aided by spectroscopy or the best-fit AGN UV LFs. We find that the bright end of the galaxy UV LFs cannot be explained by the Schechter function fits at >2σ significance, and require either double power-law functions or modified Schechter functions that consider a magnification bias due to gravitational lensing. Description: In this study, we use early data products of the HSC SSP that were obtained in 2014-2016 (Aihara et al., 2018PASJ...70S...8A 2018PASJ...70S...8A). Specifically, we use the internal data release of S16A, where additional data taken in 2016 January-April have been merged with the version of Public Data Release 1. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file table4.dat 84 358 Spectroscopically identified galaxies and AGNs in our dropout samples -------------------------------------------------------------------------------- Byte-by-byte Description of file: table4.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 8 A8 --- Type [Galaxies AGNs] Type 10- 12 A3 --- --- [HSC] 14- 27 A14 --- HSC HSC designation (JHHMMSS+DDMMSS) 29- 30 I2 h RAh Right ascension (J2000.0) 32- 33 I2 min RAm Right ascension (J2000.0) 35- 39 F5.2 s RAs Right ascension (J2000.0) 41 A1 --- DE- Declination sign (J2000.0) 42- 43 I2 deg DEd Declination (J2000.0) 45- 46 I2 arcmin DEm Declination (J2000.0) 48- 52 F5.2 arcsec DEs Declination (J2000.0) 54- 58 F5.3 --- zsp Spectroscopic redshift 60- 63 F4.1 mag UVmag Apparent UV magnitude 65- 69 F5.1 mag UVMAG Absolute UV magnitude 71 I1 --- Sample [1/4] Sample (1) 73 I1 --- Flag [1/2] Galaxy/AGN flag (1 = galaxy; 2 = AGN) 75- 84 A10 --- r_zsp Reference for spectroscopic redshift (2) -------------------------------------------------------------------------------- Note (1): The dropout sample in which the source is selected, as follows: 1 = g-dropout 2 = r-dropout 3 = i-dropout 4 = z-dropout Note (2): References as follows: S08 = Saito et al. (2008ApJ...675.1076S 2008ApJ...675.1076S) O08 = Ouchi et al. (2008, Cat. J/ApJS/176/301) W10 = Willott et al. (2010AJ....140..546W 2010AJ....140..546W) C12 = Curtis-Lake et al. (2012MNRAS.422.1425C 2012MNRAS.422.1425C) Mas12 = Masters et al. (2012, Cat. J/ApJ/755/169) M12 = Mallery et al. (2012, Cat. J/ApJ/760/128) W13 = Willott et al. (2013AJ....145....4W 2013AJ....145....4W) L13 = Le Fevre et al. (2013A&A...559A..14L 2013A&A...559A..14L) K15 = Kashikawa et al. (2015ApJ...798...28K 2015ApJ...798...28K) Kr15 = Kriek et al. (2015ApJS..218...15K 2015ApJS..218...15K) W16 = Wang et al. (2016, Cat. J/ApJ/819/24) T16 = Toshikawa et al. (2016, Cat. J/ApJ/826/114) Mo16 = Momcheva et al. (2016ApJS..225...27M 2016ApJS..225...27M) M16 = Matsuoka et al. (2016ApJ...828...26M 2016ApJ...828...26M) P17 = Paris et al. (2017A&A...597A..79P 2017A&A...597A..79P, Cat. VII/279) T17 = Tasca et al. (2017, Cat. J/A+A/600/A110) Y17 = Yang et al. (2017AJ....153..184Y 2017AJ....153..184Y) Mas17 = Masters et al. (2017, Cat. J/ApJ/841/111) M17 = Matsuoka et al. (2018PASJ...70S..35M 2018PASJ...70S..35M) S17 = Shibuya et al. (2018PASJ,,,70S..15S) H17 = R. Higuchi et al. (in preparation) -------------------------------------------------------------------------------- History: From electronic version of the journal
(End) Patricia Vannier [CDS] 11-Feb-2019
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