J-PLUS: Unveiling the brightest end of the Lyα luminosity function at 2.0 < z < 3.3 over 1000 deg2

Hernández-Monteagudo, C.; Hernán-Caballero, A.; Varela, J.; Ederoclite, A.; Vílchez, J. M.; Sobral, D.; Cenarro, A. J.; Dupke, R. A.; Bonoli, S.; Cristóbal-Hornillos, D.; López-Sanjuan, C.; Marín-Franch, A.; Moles, M.; Overzier, R.; Angulo, R. E.; Alcaniz, J.; Orsi, A.; Gurung-López, S.; Spinoso, D.; Izquierdo-Villalba, D.; Miralda-Escudé, J.; Sodré, L., Jr.; Viironen, K.; Muniesa, D. J.; Vázquez-Ramió, H.

Spain, New Zealand, United Kingdom, United States, Brazil

Abstract

We present the photometric determination of the bright end of the Lyα luminosity function (LF; at LLyα ≳ 1043.3 erg s-1) within four redshift windows (Δ z < 0.16) in the interval 2.2​ ≲ ​z​ ≲ ​3.3. Our work is based on the Javalambre Photometric Local Universe Survey (J-PLUS) first data release, which provides multiple narrow-band measurements over ∼1000 deg2, with limiting magnitude r​ ∼ ​22. The analysis of high-z Lyα-emitting sources over such a wide area is unprecedented and allows us to select approximately 14 500 hyper-bright (LLyα > 1043.3 erg s-1) Lyα-emitting candidates. We test our selection with two spectroscopic programs at the GTC telescope, which confirm ∼89% of the targets as line-emitting sources, with ∼64% being genuine z​ ∼ ​2.2 quasars (QSOs). We extend the 2.2​ ≲ ​z​ ≲ ​3.3 Lyα LF for the first time above LLyα ∼ 1044 erg s-1 and down to densities of ∼10-8 Mpc-3. Our results unveil the Schechter exponential decay of the brightest-end of the Lyα LF in great detail, complementing the power-law component of previous determinations at 43.3 ≲ Log10(LLyα/erg s-1) ≲ 44. We measure Φ* = (3.33 ± 0.19)×10-6, Log(L*) = 44.65 ± 0.65, and α = -1.35 ± 0.84 as an average over the probed redshifts. These values are significantly different from the typical Schechter parameters measured for the Lyα LF of high-z star-forming Lyman-α emitters (LAEs). This implies that z​ > ​2 AGNs/QSOs (likely dominant in our samples) are described by a structurally different LF from that used to describe z​ > ​2 star-forming LAEs, namely LQSOs* ~ 100LLAEs* and ΦQSOs* ~ 10-3 ΦLAEs*, with the transition between the two LFs happening at LLyα ∼ 1043.5 erg s-1. This supports the scenario in which Lyα-emitting AGNs/QSOs are the most abundant class of z​ ≳ ​2 Lyα emitters at LLyα ≳ 1043.3 erg s-1. Finally, we suggest that a significant number of these z​ ≳ ​2 AGNs/QSOs (∼60% of our samples) are currently misclassified as stars based on their broad-band colours, but are identified for the first time as high-z line-emitters by our narrow-band-based selection.

Catalogs are available in electronic form both on the J-PLUS website at https://www.j-plus.es/ancillarydata/dr1_lya_emitting_candidates and at the CDS via anonymous ftp to http://cdsarc.u-strasbg.fr (ftp://130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/cat/J/A+A/643/A149

2020 Astronomy and Astrophysics
Gaia 27