학술논문
J-PLUS: Unveiling the brightest end of the Lyα luminosity function at 2.0 < z < 3.3 over 1000 deg2 .
Document Type
Article
Author
Spinoso, D.; Orsi, A.; López-Sanjuan, C.; Bonoli, S.; Viironen, K.; Izquierdo-Villalba, D.; Sobral, D.; Gurung-López, S.; Hernán-Caballero, A.; Ederoclite, A.; Varela, J.; Overzier, R.; Miralda-Escudé, J.; Muniesa, D. J.; Vílchez, J. M.; Alcaniz, J. (NURSE); Angulo, R. E.; Cenarro, A. J.; Cristóbal-Hornillos, D.; Dupke, R. A.
Source
Subject
*STELLAR luminosity function
*LUMINOSITY
*GALACTIC redshift
*QUASARS
*REDSHIFT
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Language
ISSN
0004-6361
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* L QSOs * ~ 100 L LAEs * $ L^*_{\rm QSOs}\!\sim\!100\,L^*_{\rm LAEs} $ and ΦQSOs* ~ 10−3 ΦLAEs* Φ QSOs * ~ 10 − 3 Φ LAEs * $ \Phi^*_{\rm QSOs}\!\sim\!10^{-3}\,\Phi^*_{\rm LAEs} $ , 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. [ABSTRACT FROM AUTHOR]