J/A+A/643/A149      J-PLUS Lyα-emitting candidates        (Spinoso+, 2020)
J-PLUS: Unveiling the brightest-end of the Lyα luminosity function at
2.0 < z < 3.3 over 1000 deg2.
    Spinoso D., Orsi A., Lopez-Sanjuan C., Bonoli S., Viironen K.,
    Izquierdo-Villalba D., Sobral D., Gurung-Lopez S., Hernan-Caballero A.,
    Ederoclite A., Varela J., Overzier R., Miralda-Escude J., Muniesa D.J.,
    Vilchez J.M., Alcaniz J., Angulo R.E., Cenarro A.J., Cristobal-Hornillos D.,
    Dupke R.A., Hernandez-Monteagudo C., Marin-Franch A., Moles M., Sodre L.Jr,
    Vazquez-Ramio H.
    <Astron. Astrophys. 643, A149 (2020)>
    =2020A&A...643A.149S 2020A&A...643A.149S        (SIMBAD/NED BibCode)
ADC_Keywords: Galaxy catalogs ; Ultraviolet ; Equivalent widths
Keywords: galaxies: luminosity function, mass function -
          galaxies: high-redshift - quasars: emission lines -
          techniques: photometric - methods: observational - surveys
Abstract:
    We present the photometric determination of the bright-end of the
    Lyα luminosity function (at LLyα≳1043.5erg/s) within
    four redshifts windows (Δz<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 ∼1000deg2, with limiting magnitude ∼22.
    Theanalysis of high-z Lyα-emitting sources over such a wide area
    is unprecedented, and allows to select a total of ∼14500
    hyper-bright(LLyα>1043.3erg/s) Lyα-emitting
    candidates. We test our selection with two spectroscopic follow-up
    programs at the GTC telescope,which confirm as line-emitting sources
    ∼89% of the targets, with ∼64% being genuine z∼2.2 QSOs. We extend the
    2.2≲z≲3.3 Lyα luminosity function for the first time above
    LLyα∼1044erg/s and down to densities of ∼10-8Mpc-3. Our
    results unveil with high detail the Schechter exponential-decay of the
    brightest-end of the Lyα LF, complementing the power-law
    component of previous LF determinations at
    43.3≲Log10(LLyα/(erg/s))≲44. We measure
    {PHI}*=(3.33±0.19)x10-6, Log(L*)=44.65±0.65 and
    α=-1.35±0.84 as an average over the redshifts we probe. These
    values are significantly different than the typical Schechter
    parameters measured for the Lyα LF of high-z star-forming LAEs.
    This suggests that z>2 AGN/QSOs (likely dominant in our samples) are
    described by a structurally different LF than z>2 star-forming LAEs,
    namely with L*QSOs∼100 L*LAEs and {PHI}*QSOs∼10-3{PHI}*LAEs.
    Finally, our method identifies very efficiently as high-z
    line-emitters sources without previous spectroscopic confirmation,
    currently classified as stars (∼2000 objects in each redshift bin, on
    average). Assuming a large predominance of Lyα-emitting AGN/QSOs
    in our samples, this supports the scenario by which these are the most
    abundant class of z≳2 Lyα emitters at
    LLyα≳1043.3erg/s.
Description:
    These four lists contain sources selected as genuine Lyman-alpha
    emitting candidates by the methodology detailed in the paper. In
    brief, the J-PLUS narrow-bands J0395, J0410, J0430 and J0515 were used
    to detect photometric excesses of sources within the DR1 dual-mode
    (i.e. r-band selected) parent sample. This excess and its significance
    was estimated by using the method detailed in Vilella-Rojo et al.
    (2015A&A...580A..47V 2015A&A...580A..47V) and discussed in Logrono-Garcia et al.
    (2019A&A...622A.180L 2019A&A...622A.180L). Each of the four NBs were used to target
    Lyman-alpha emission, respectively at redshift z=2.2, z=2.4, z=2.5 and
    z=3.2. After the first selection based on the NB-excess significance
    of each source, the resulting lists of objects were cleaned from the
    presence of known interlopers, namely low-z galaxies, stars and
    AGN/QSOs outside the redshift intervals probed by the narrow-bands for
    Lyman-alpha emission. All the above steps are extensively detailed in
    the paper. The four lists presented here include only the genuine
    Lyα-emitting candidates used to compute the luminosity functions
    presented in the paper. These candidates are defined as the sources
    selected on the basis of their reliable NB excess, which do not
    present any identification as known low-z interlopers. We stress that
    genuine candidates include the Lyα-emitting QSOs belonging to
    the SDSS spectroscopic sample (Paris et al., 2018A&A...613A..51P 2018A&A...613A..51P, Cat.
    VII/286), whose redshift is compatible to Lyα-emission in the
    wavelength ranges probed by each narrow-band. See paper for further
    details about the selection procedures.
File Summary:
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 FileName      Lrecl  Records   Explanations
--------------------------------------------------------------------------------
ReadMe            80        .   This file
cj0395.dat       128     2547   LAE candidates DR1, in narrow-band J0395
cj0410.dat       128     5556   LAE candidates DR1, in narrow-band J0410
cj0430.dat       128     4994   LAE candidates DR1, in narrow-band J0430
cj0515.dat       128     1467   LAE candidates DR1, in narrow-band J0515
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See also:
   http://archive.cefca.es/catalogues/jplus-dr1 : J-PLUS-DR1 Home Page
Byte-by-byte Description of file: cj0395.dat cj0410.dat cj0430.dat cj0515.dat
--------------------------------------------------------------------------------
   Bytes Format Units   Label      Explanations
--------------------------------------------------------------------------------
   1-  5  I5    ---     TileId     Identifier of the Tile image where the object
                                    was detected (TILE_ID)
   7- 11  I5    ---     Id         Number identifier assigned by Sextractor for
                                    the object in the image (NUMBER)
  13- 22  F10.6 deg     RAdeg      Right ascension (J2000) (ALPHA_J2000)
  24- 33  F10.6 deg     DEdeg      Declination (J2000) (DELTA_J2000)
  35- 46  E12.6 mW/m2   FLya       Photometric estimate of the integrated
                                    line-flux in Lyα, corrected for
                                    filter-width losses (LYA_FLUX)
  48- 59  E12.6 mW/m2 e_FLya       Error on FLya (LYAFLUXERR)
  61- 72  E12.6 10-7W   LLya       ? Lyα luminosity computed from the
                                    sources FLya and redshift (LYA_LUM)
  74- 85  E12.6 10-7W e_LLya       ? Error on LLya (LYALUMERR)
  87- 98  E12.6 0.1nm   EWLya      Lyα equivalent width  (LYA_EW) (1)
 100-107  F8.6  ---     z          Sources redshift assuming detection at the
                                    narrow-band central wavelength (Z) (2)
 109-118  F10.6 ---   e_z          ?=-1 Redshift error (Z_ERR) (3)
     120  I1    ---     SDSS-QSO   [0/1] Flag identifying the presence of
                                    SDSS QSOs counterparts (at any z)
                                    (SDSS_QSO) (4)
     122  I1    ---     SDSS-QSORz [0/1] Flag identifying the presence of
                                    SDSS QSOs counterparts (at the redshift
                                    sampled by the NB used to select the
                                    candidates) (SDSSRIGHTzQSO) (4)
     124  I1    ---     LQAC-QSO   [0/1] Flag identifying the presence of LQAC
                                    (Souchay et al., 2015, Cat. J/A+A/583/75)
                                    QSOs counterparts (at any z) (LQAC_QSO) (4)
     126  I1    ---     WISE-QSO   [0/1] Flag identifying the presence of
                                    counterparts in the allWISE catalog (Wright
                                     et al. 2010, Cat. II/328) (WISE_QSO) (5)
     128  I1    ---     XRAY       [0/1] Flag identifying the presence of X-ray
                                    counterparts in the 2RXS and XMMSLEW2
                                    catalogs (Salvato et al., 2018,
                                    Cat. J/MNRAS/473/4937) (XRAY_SOURCE) (4)
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Note (1): EW=FLya/NB_continuum, where NB_continuum is computed with the method
 of Vilella-Rojo et al. (2015A&A...580A..47V 2015A&A...580A..47V).
Note (2):  For objects with SDSS counterpart, 'z' is equal to the SDSS zspec
 (Paris et al., 2018A&A...613A..51P 2018A&A...613A..51P, Cat. VII/286).
Note (3): namely half of the narrow-band FWHM for sources without SDSS
 counterparts, otherwise e_z is the value given by SDSS (see Paris et al.,
 2018A&A...613A..51P 2018A&A...613A..51P, Cat. VII/286 for details).
Note (4): 0 if no counterparts.
Note (5): with WISE colors compatible with QSO color locus (namely W1-W2>0.5,
 see e.g. Chhetri et al., 2020MNRAS.494..923C 2020MNRAS.494..923C). 0 if no counterparts.
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Acknowledgements:
    Daniele Spinoso, dspinoso(at)cefca.es
(End)                                        Patricia Vannier [CDS]  15-Sep-2020