J/A+A/700/A203      Missing FeII bump in faint JWST AGNs      (Trefoloni+, 2025)

The missing Fe II bump in faint JWST active galactic nuclei: Possible evidence of metal-poor broad-line regions at early cosmic times. Trefoloni B., Ji X., Maiolino R., D'Eugenio F., Uebler H., Scholtz J., Marconi A., Marconcini C., Mazzolari G. <Astron. Astrophys. 700, A203 (2025)> =2025A&A...700A.203T 2025A&A...700A.203T (SIMBAD/NED BibCode)
ADC_Keywords: Active gal. nuclei ; QSOs ; Spectroscopy ; Abundances Keywords: galaxies: active - galaxies: high-redshift - quasars: emission lines - quasars: general - quasars: supermassive black holes - galaxies: Seyfert Abstract: Recent JWST observations have revealed a large population of intermediate/low-luminosity active galactic nuclei (AGN) at early times with peculiar properties, different from local AGN or luminous quasars. To better understand the physical conditions in the broad-line regions (BLRs) of these early AGN, we used the optical FeII (4434-4684Å) and the broad Hbeta emission, and the ratio between their equivalent widths RFe, as a probe on a purposefully assembled sample. Specifically, we gathered a sample of 31 high redshift (=6.5) AGN, observed by JWST, with broad Hbeta detection both in the high and low luminosity regimes (respectively 14 faint AGN and 17 quasars), to investigate their optical FeII emission properties. In addition, we carefully selected control samples at lower z. We found that the population of faint AGN (log(LHb/(erg/s))≲44) exhibits a significantly lower FeII emission than their local counterparts having a mean (median) RFe<0.24 (0.12) versus RFe~=0.90 (0.79) in the control sample. At the same time, the quasars at the epoch of reionisation observed by JWST present a FeII emission profile that closely resembles that observed at z<3. We argue that the weakness of the FeII bump in the faint JWST AGN might be due to the reduced metallicity of their broad line region (≲0.5Z), while luminous quasars have already reached chemical maturity (∼Z{sun} or higher). Lastly, we highlight an intriguing similarity between the spectral properties of the high redshift population of faint AGN with those harboured in local metal poor dwarf galaxies. Description: We assembled a sample of high-redshift AGN observed by JWST spanning a wide range in terms of luminosity and black hole mass with the aim of characterising the strength of the RFe. To this end, we performed a detailed spectroscopic analysis and selected control subsamples at lower redshift to compare their properties and assess possible differences. We remark that our control samples are selected to match the JWST AGN in both Hbeta FWHM and luminosity, which are the direct emission line observables that best capture the black hole properties and accretion parameters. Additionally, we also included as a separate comparison sample three metal-poor dwarf galaxies hosting low-luminosity AGN as tentative super local counterparts. File Summary: -------------------------------------------------------------------------------- FileName Lrecl Records Explanations -------------------------------------------------------------------------------- ReadMe 80 . This file tablea1.dat 115 34 The broad lines spectral properties estimated from the spectral fits of our sample tableb1.dat 63 34 Luminosities, black hole mass and Eddington ratio -------------------------------------------------------------------------------- Byte-by-byte Description of file: tablea1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Name Name of the source 21- 29 F9.5 deg RAdeg Right ascension (J2000) 31- 39 F9.5 deg DEdeg Declination (J2000) 41 A1 --- Hbprofile [GL] Hbeta line profile, G=Gaussian, L=Lorentzian 43- 47 F5.2 [10-7W] logLHb Logarithm of the Hbeta luminosity 49- 52 F4.2 [10-7W] e_logLHb Uncertainty on the logarithm of the Hbeta luminosity 54- 57 F4.2 --- RFe Ratio of the optical FeII (4434-4684Å) and the broad Hbeta emission equivalent widths 59- 62 F4.2 --- e_RFe Uncertainty on the RFe 64- 67 I4 km/s FWHMHb FWHM of the Hbeta line 69- 72 I4 km/s e_FWHMHb Uncertainty on the FWHM of the Hbeta line 74- 77 F4.2 [0.1nm] logEWOIII ?=- Logarithm of the equivalent width of [OIII]5007 79- 82 F4.2 [0.1nm] e_logEWOIII ?=- Uncertainty on the logarithm of the equivalent width of [OIII]5007 84- 88 F5.2 --- O3Hb ?=- Ratio between [OIII]5007 and narrow Hbeta 90- 94 F5.2 --- e_O3Hb ?=- Uncertainty on the ratio between [OIII]5007 and narrow Hbeta 96-100 F5.2 --- O32 ?=- Ratio between [OIII]5007 and [OII]3728 102-105 F4.2 --- e_O32 ?=- Uncertainty on the ratio between [OIII]5007 and [OII]3728 107-110 F4.2 --- Oabund ?=- Oxygen abundance, 12+log(O/H) 112-115 F4.2 --- e_Oabund ?=- Uncertainty on the oxygen abundance -------------------------------------------------------------------------------- Byte-by-byte Description of file: tableb1.dat -------------------------------------------------------------------------------- Bytes Format Units Label Explanations -------------------------------------------------------------------------------- 1- 19 A19 --- Name Name of the source 21- 25 F5.2 [10-7W] logL5100 Logarithm of the 5100Å luminosity 27- 30 F4.2 [10-7W] e_logL5100 Uncertainty on the logarithm of the 5100Å luminosity 32- 36 F5.2 [10-7W] logLbol Logarithm of the bolometric luminosity 38- 41 F4.2 [10-7W] e_logLbol Uncertainty on the logarithm of the bolometric luminosity 43- 47 F5.2 Msun logMBH Logarithm of the black hole mass 49- 52 F4.2 Msun e_logMBH Uncertainty on the logarithm of the black hole mass 54- 58 F5.2 --- logEr Logarithm of the Eddington ratio 60- 63 F4.2 --- e_logEr Uncertainty on the logarithm of the Eddington ratio -------------------------------------------------------------------------------- Acknowledgements: Bartolomeo Trefoloni, bartolomeo.trefoloni(at)unifi.it
(End) Patricia Vannier [CDS] 28-Jul-2025
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