J/A+A/672/A186  Ionizing photons in UV-faint z∼3-7 galaxies (Prieto-Lyon+, 2023)

The production of ionizing photons in UV-faint z ∼ 3-7 galaxies. Prieto-Lyon G., Strait V., Mason C.A., Brammer G., Caminha G.B., Mercurio A., Acebron A., Bergamini P., Grillo C., Rosati P., Vanzella E., Castellano M., Merlin E., Paris D., Boyett K., Calabro A., Morishita T., Mascia S., Pentericci L., Roberts-Borsani G., Roy N., Treu T., Vulcani B. <Astron. Astrophys. 672, A186 (2023)> =2023A&A...672A.186P 2023A&A...672A.186P (SIMBAD/NED BibCode)
ADC_Keywords: Galaxies ; Ultraviolet ; Redshifts ; Equivalent widths Keywords: quasars: emission lines - galaxies: high-redshift - galaxies: evolution Abstract: The demographics of the production and escape of ionizing photons from UV-faint early galaxies is a key unknown in discovering the primary drivers of reionization. With the advent of JWST it is finally possible to observe the rest-frame optical nebular emission from individual sub-L* z>3 galaxies to measure the production of ionizing photons, χion. Here we study a sample of 370 z∼3-7 galaxies spanning -23<MUV←15.5 (median MUV~-18) with deep multi-band HST and JWST/NIRCam photometry covering the rest-UV to optical from the GLASS and UNCOVER JWST surveys. Our sample includes 102 galaxies with Lyman-alpha emission detected in MUSE spectroscopy. We use H-alpha fluxes inferred from NIRCam photometry to estimate the production rate of ionizing photons which do not escape these galaxies χion(1-fesc). We find median log10χion(1-fesc)=25.33±0.47, with a broad intrinsic scatter 0.42dex, implying a broad range of galaxy properties and ages in our UV-faint sample. Galaxies detected with Lyman-alpha have ∼0.1dex higher χion(1-fesc), which is explained by their higher H-alpha EW distribution, implying younger ages, higher sSFR and thus more O/B stars. We find significant trends of increasing χion(1-fesc) with increasing H-alpha EW, decreasing UV luminosity, and decreasing UV slope, implying the production of ionizing photons is enhanced in young, low metallicity galaxies. We find no significant evidence for sources with very high ionizing escape fraction (fesc>0.5) in our sample, based on their photometric properties, even amongst the Lyman-alpha selected galaxies. This work demonstrates that considering the full distribution of χion across galaxy properties is important for assessing the primary drivers of reionization. Description: We have inferred the hydrogen ionizing photon production rate, modulo the escape fraction, in the largest sample of individual sub-L* z>3 galaxies to date, spanning -23≲MUV≲-15.5 with a median MUV=-18.1, thanks to deep JWST/NIRCam imaging. catalog.dat contains all data needed to reproduce the seven figures showed in the publication. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file catalog.dat 512 370 All data needed to reproduce the seven figures showed in the publication -------------------------------------------------------------------------------- Byte-by-byte Description of file: catalog.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 5 A5 --- ID GLASS sources start with G, UNCOVER start with U 7- 24 F18.16 deg RAdeg Right ascension (J2000) 26- 44 F19.15 deg DEdeg Declination (J2000) 46- 51 A6 --- GalType Galaxy type, Lyman Alpha Emitter or non Lyman Alpha Emitter 53- 70 F18.16 --- z Redshift taken from Lyman Alpha if LAE or from EAZY if nonLAE 72- 90 F19.16 --- mu Magnification 92-112 F21.18 --- e_mu ?=- Magnification error 114-132 F19.15 mag MUV UV magnitude measured at 1500Å (AB) 134-153 F20.18 mag e_MUV UV magnitude measured at 1500Å error (AB) 155-174 F20.17 --- beta UV slope 176-195 F20.18 --- e_beta UV slope error 197-218 E22.16 10+7Hz/J Xion ?=- (1-fesc)χion (in Hz/erg unit) 220-241 E22.16 10+7Hz/J e_Xion ?=- (1-fesc)χion error (in Hz/erg unit) 243-265 E23.16 mW/m2 FHa ?=- Flux Hα (in erg/cm2/s unit) 267-288 E22.16 mW/m2 e_FHa ?=- Flux Hα error (in erg/cm2/s unit) 290-311 F22.16 0.1nm EWHa ?=- Hα equivalent width 313-332 F20.14 0.1nm e_EWHa []?=- Hα equivalent width error 334-355 E22.16 10mW/m2/nm ContHa ?=- Continuum flux density taken for EWHa (in erg/cm2/s/Å unit) 357-378 E22.16 10mW/m2/nm e_ContHa ?=- Continuum flux density taken for EWHa error (in erg/cm2/s/Å unit) 380-402 E23.16 mW/m2 FOIIIHb ?=- Flux OIII+Hb (in erg/cm2/s unit) 404-425 E22.16 mW/m2 e_FOIIIHb ?=- Flux OIII+Hb error (in erg/cm2/s unit) 427-446 F20.15 0.1nm EWOIIIHb ?=- Equivalent width OIII+Hβ 448-466 F19.14 0.1nm e_EWOIIIHb []?=- Equivalent width OIII+Hβ error 468-489 E22.16 10mW/m2/nm ContOIIIHb ?=- Continuum flux density taken for EWOIII+Hb (in erg/cm2/s/Å unit) 491-512 E22.16 10mW/m2/nm e_ContOIIIHb ?=- Continuum flux density taken for EWOIII+Hb error (in erg/cm2/s/Å unit) -------------------------------------------------------------------------------- Acknowledgements: Gonzalo Prieto-Lyon, gonzalo.prieto(at)nbi.ku.dk
(End) Patricia Vannier [CDS] 14-Apr-2023
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