2504.20299v1
The Cosmic Evolution of CIV Absorbers at $1.4<z<4.5$: Insights from $100,000$ Systems in DESI Quasars
First listed 2025-04-28 | Last updated 2025-09-04
Abstract
We present the largest catalog to date of triply ionized carbon (CIV) absorbers detected in quasar spectra from the Dark Energy Spectroscopic Instrument. Using an automated matched-kernel convolution method with adaptive signal-to-noise thresholds, we identify $101,487$ CIV systems in the redshift range $1.4 < z < 4.5$ from $300,637$ quasar spectra. Completeness is estimated via Monte Carlo simulations and catalog is $50\%$ complete at $\mathrm{EW}_{\mathrm{CIV}} \geq 0.4$ Angstroms. The differential equivalent width frequency distribution declines exponentially and shows weak redshift evolution. The absorber incidence per unit comoving path increases by a factor of $2-5$ from $z \approx 4.5$ to $z \approx 1.4$, with stronger redshift evolution for strong systems. Using column densities derived from the apparent optical depth method, we constrain the cosmic mass density of CIV, $Ω_{\mathrm{CIV}}$, which increases by a factor of $\sim 3.8$ from $(0.82 \pm 0.05) \times 10^{-8}$ at $z \approx 4.5$ to $(3.16 \pm 0.2) \times 10^{-8}$ at $z \approx 1.4$. From $Ω_{\rm CIV}$, we estimate a lower limit on intergalactic medium metallicity $\log(Z_{\rm IGM}/Z_{\odot}) \gtrsim -3.25$ at $z \sim 2.3$, with a smooth decline at higher redshifts. These trends trace the cosmic star formation history and HeII photoheating rate, suggesting a link between CIV enrichment, star formation, and UV background over $\sim 3$ Gyr. The catalog also provides a critical resource for future studies connecting circumgalactic metals to galaxy evolution, especially near cosmic noon.
Short digest
From 300,637 DESI quasar spectra, the team assembles the largest C IV absorber catalog to date—101,487 systems across 1.4<z<4.5—via an automated matched‑kernel finder with adaptive S/N thresholds. After Monte Carlo completeness corrections (50% complete at EW_CIV ≥ 0.4 Å), the EW frequency distribution declines exponentially with weak redshift evolution, while the incidence per comoving path rises by a factor of 2–5 toward z≈1.4, most strongly for the strongest systems. Apparent‑optical‑depth column densities yield Ω_CIV increasing by ~3.8×, from (0.82±0.05)×10^-8 at z≈4.5 to (3.16±0.2)×10^-8 at z≈1.4. Interpreting Ω_CIV as enrichment, they infer a lower limit log(Z_IGM/Z⊙) ≳ −3.25 at z≈2.3, tracking cosmic SFR and He II photoheating and providing a foundation to link CGM metals to galaxy growth near cosmic noon.
Key figures to inspect
- Figure 1: Use the S/N–redshift map (with percentile contours) to gauge selection and completeness versus z; note the Lyα‑forest repeat‑observation bump and how it modulates C IV detectability.
- Figure 2: Inspect the example spectrum to see continuum placement and the double‑Gaussian fit to the λ1548/1550 pair; the flat residuals validate normalization and the matched‑kernel detection on real DESI data.
- Figure 3: Compare DR1 vs DR2 absorber redshift histograms to see how DR2 extends path length and shifts the mean z, informing incidence and Ω_CIV leverage.
- Figure 4: Track how completeness‑corrected EW distributions remove the spurious turnover near 0.4 Å, check doublet‑ratio saturation trends, and read off AOD‑based N_CIV versus redshift (mean and scatter) that underpin Ω_CIV.
Discussion
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