Searcharxiv⌕ Search

arXiv · 2610.33339

Exploring the UV Fe III Emission along the Quasar Main Sequence

Abstract

The diversity of Type I AGNs can be organized along the Quasar Main Sequence (MS), a powerful framework primarily driven by the accretion rate and defined in the optical plane by the FWHM of $\mathrm{Hβ}$ and the Fe II strength ($R_{\rm FeII}$). Previous studies suggested that the UV Fe III evolves along this MS. However, a systematic analysis is still missing. We aim to characterize the UV Fe III emission across the MS, assess its potential as a tracer, and investigate how its properties depend on the conditions of the emitting gas. We analyzed the UV iron emission in 69 low-$z$ $(z \lesssim 1)$ AGNs observed with the Hubble Space Telescope. We fitted the 1700-2200 Angstrom range and investigated the main correlations using principal component analysis. We complemented with $\tt{CLOUDY}$ photoionization simulations to explore the dependence of the iron emission on gas density, ionization parameter, metallicity, microturbulence, column density, and spectral energy distribution. We find a positive correlation between the strengths of the UV iron emission and the optical $\mathrm{R_{FeII}}$ parameter. With this, we define a UV MS diagram using the FWHM of $\mathrm{Al III\,\lambda1860}$ and the equivalent width of $\mathrm{Fe III}$ + $\mathrm{Fe II}$. $\tt{CLOUDY}$ simulations support this result, predicting stronger Fe III emission at high $\mathrm{R_{FeII}}$. Additionally, we found object-to-object variations in the $\mathrm{Fe III}$ multiplets. Our results indicate that UV Fe III emission and $\mathrm{Al III}\,λ1860$ can serve as proxies for optical Fe II and $\mathrm{Hβ}$, extending the Quasar MS into the UV domain. The variations in the Fe III multiplets demonstrate that a single template may not represent all quasars. Thus, characterizing the Fe III emission and its dependence on physical conditions is essential for improving the modeling of UV AGN spectra.

Explore related subjects

Keep this discovery

Explore connections, maps & timelines

BibTeXRIS

Diego Martínez Collipal, Mary Loli Martínez-Aldama, Ashwani Pandey, Paola Marziani, Swayamtrupta Panda, Marco Cárdenas. 2026-10-23. Exploring the UV Fe III Emission along the Quasar Main Sequence. https://arxiv.org/abs/2610.33339

Cite the original work for its findings. Save a collection to share your selection of sources.

KEEP EXPLORING

Related papers

JWST Spectroscopic Census of ALMA Faint Submillimeter Galaxies in the Hubble Ultra Deep Field

We present a JWST/NIRSpec rest-frame optical spectroscopic census of ALMA 1-mm continuum sources in the Hubble Ultra Deep Field (UDF) identified by the deep ALMA UDF and ASPECS programs. Our sample is composed of the ALMA flux-limited ($S_{1\,\mathrm{mm}}\gtrsim 0.1\,\mathrm{mJy}$) sources observed with medium-resolution NIRSpec spectroscopy from JADES and SMILES, 16 faint submillimeter galaxies (SMGs) at spectroscopic redshifts of $z\sim 1$-$4$. These SMGs show bright longer-wavelength optical lines (H$α$, [N II]$λ\lambda6548,6583$, and [S II]$λ\lambda6717,6731$) and faint shorter-wavelength optical lines (H$β$ and [O III]$λ\lambda4959,5007$) with a large nebular attenuation, $E(B-V)\sim0.3$-$1.8$. We test the SMGs using BPT diagnostics and Chandra X-ray fluxes, and find that most SMGs are classified as AGNs; the AGN fraction is $\sim80\%$ for the SMGs at $M_*>10^{10.5} M_\odot$. We find only one SMG ($<10\%$) with a broad Balmer line, indicating that the SMGs are predominantly obscured AGNs. With the optical lines, we estimate the metallicities of the SMGs to be moderately high, $\sim0.4$-$2 Z_\odot$, exceeding the model-predicted dust-growth critical metallicity ($\sim0.1$-$0.2Z_\odot$), which naturally explains the dusty nature of the SMGs. Interestingly, the SMGs fall in the mass-metallicity relation and the star-formation main sequence, showing no significant differences from other high-$z$ galaxies. Similarly, we find electron densities of $n_e\sim10^2$-$10^3\,\mathrm{cm}^{-3}$ for the SMGs that are comparable with other high-$z$ galaxies. Together with the high SMG fraction ($\sim 100\%$) at the massive end ($M_*>10^{10.5} M_\odot$), these results indicate that the SMGs are mostly not special, but typical massive star-forming galaxies at high redshift.

astro-ph.GA↗

On the relation between magnetic field strength and gas density in the interstellar medium. II. Density uncertainties and diffuse gas constraints

The relationship between magnetic field strength and gas density is essential to understand the interstellar medium and star formation. Zeeman measurements in dense atomic and molecular gas phases have traditionally been used to directly probe magnetic field strengths in the Milky Way. This allowed derivation of a relationship between magnetic field strength $B$ and gas number density $n$. We recently generalized this relation as a two-part power-law with non-zero slopes and a transition density given as $B/B_0 \propto (n/n_0)^{α_1}$ for $n \le n_0$ and $(n/n_0)^{α_2}$ for $n > n_0$. Here, we extend our previous hierarchical Bayesian framework by incorporating a large body of pulsar observations that probe the diffuse interstellar medium and explicitly modelling density uncertainties through a log-density intrinsic scatter $R_n$ applied to all densities. We also account for magnetic field geometry and measurement uncertainties through a magnetic hyperparameter to estimate $B$. This results in a stronger constraint on the diffuse gas part of the $B$--$n$ relation. Our results confirm a non-zero exponent in the diffuse gas and a broad transition density with our best model and data set yielding maximum a posteriori results of $α_1 = 0.20^{+0.01}_{-0.03}$, $α_2 = 0.65^{+0.06}_{-0.07}$, $n_0 = 3330^{+270}_{-3220}\,\text{cm}^{-3}$, and $B_0 = 10.11^{+0.71}_{-5.97}\,μ\text{G}$.

astro-ph.GA↗

Where did all the Little Red Dots go? The abundance of LRD analogues among objects with broad lines at $z < 0.35$

One of the most puzzling discoveries since the launch of the James Webb Space Telescope is a numerous population of sources at high redshift nicknamed ``Little Red Dots'' (LRDs). Characterized by broad Balmer emission lines, compact morphologies and v-shaped spectral energy distributions (SEDs) in the rest-frame optical, the nature of LRDs remains elusive. A major challenge is the high redshift nature of LRDs, which makes observations very expensive and difficult. Finding local LRD analogues is a crucial step in unravelling the physical processes giving rise to LRDs, as cheaper observations with many facilities would become available. In this paper, we conduct a search for local LRD analogues by starting from an unbiased parent catalogue of all SDSS objects with broad H$α$ or H$β$ emission lines (both galaxies and quasars) at $0 < z < 0.35$, complemented by archival photometry and spectroscopy. We find that among broad-line objects, $19\%$ show a v-shaped SED. We then select objects whose SED is well described by a modified black body (MBB), and identify nine local LRD analogues. After accounting for selection limitations we get an abundance of $0.08\%$ of all objects with broad lines. Among only objects which match the typical continuum and emission line luminosities of LRDs, $5\%$ display a v-shape and $0.37\%$ display a MBB-like SED. We recover one previously-identified local LRD analogue (the so-called ``Egg''), validating our methodology. Among the other eight analogues, one (J0302$-$0101) shows all the hallmarks of an LRD despite being visibly embedded in the core of a galaxy; another object is ambiguous, and the remaining six may have alternative explanations for their peculiar SEDs. Our study highlights that LRDs are extremely rare at $z < 0.35$; we find very few objects with broad lines which have LRD-like SEDs, even without attempting to match the compactness of LRDs.

astro-ph.GA↗