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arxiv: 2404.03001 · v4 · pith:ARJOAJYVnew · submitted 2024-04-03 · 🌌 astro-ph.CO

DESI 2024 IV: Baryon Acoustic Oscillations from the Lyman Alpha Forest

DESI Collaboration: A. G. Adame , J. Aguilar , S. Ahlen , S. Alam , D. M. Alexander , M. Alvarez , O. Alves , A. Anand
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U. Andrade E. Armengaud S. Avila A. Aviles H. Awan S. Bailey C. Baltay A. Bault J. Bautista J. Behera S. BenZvi F. Beutler D. Bianchi C. Blake R. Blum S. Brieden A. Brodzeller D. Brooks E. Buckley-Geer E. Burtin R. Calderon R. Canning A. Carnero Rosell R. Cereskaite J. L. Cervantes-Cota S. Chabanier E. Chaussidon J. Chaves-Montero S. Chen X. Chen T. Claybaugh S. Cole A. Cuceu T. M. Davis K. Dawson R. de la Cruz A. de la Macorra A. de Mattia N. Deiosso A. Dey B. Dey J. Ding Z. Ding P. Doel J. Edelstein S. Eftekharzadeh D. J. Eisenstein A. Elliott P. Fagrelius K. Fanning S. Ferraro J. Ereza N. Findlay B. Flaugher A. Font-Ribera D. Forero-S\'anchez J. E. Forero-Romero C. Garcia-Quintero E. Gazta\~naga H. Gil-Mar\'in S. Gontcho A Gontcho A. X. Gonzalez-Morales V. Gonzalez-Perez C. Gordon D. Green D. Gruen R. Gsponer G. Gutierrez J. Guy B. Hadzhiyska C. Hahn M. M. S Hanif H. K. Herrera-Alcantar K. Honscheid C. Howlett D. Huterer V. Ir\v{s}i\v{c} M. Ishak S. Juneau N. G. Kara\c{c}ayli R. Kehoe S. Kent D. Kirkby A. Kremin A. Krolewski Y. Lai T.-W. Lan M. Landriau D. Lang J. Lasker J.M. Le Goff L. Le Guillou A. Leauthaud M. E. Levi T. S. Li E. Linder K. Lodha C. Magneville M. Manera D. Margala P. Martini M. Maus P. McDonald L. Medina-Varela A. Meisner J. Mena-Fern\'andez R. Miquel J. Moon S. Moore J. Moustakas E. Mueller A. Mu\~noz-Guti\'errez A. D. Myers S. Nadathur L. Napolitano R. Neveux J. A. Newman N. M. Nguyen J. Nie G. Niz H. E. Noriega N. Padmanabhan E. Paillas N. Palanque-Delabrouille J. Pan S. Penmetsa W. J. Percival M. M. Pieri M. Pinon C. Poppett A. Porredon F. Prada A. P\'erez-Fern\'andez I. P\'erez-R\`afols D. Rabinowitz A. Raichoor C. Ram\'irez-P\'erez S. Ramirez-Solano M. Rashkovetskyi C. Ravoux M. Rezaie J. Rich A. Rocher C. Rockosi N.A. Roe A. Rosado-Marin A. J. Ross G. Rossi R. Ruggeri V. Ruhlmann-Kleider L. Samushia E. Sanchez C. Saulder E. F. Schlafly D. Schlegel M. Schubnell H. Seo R. Sharples J. Silber F. Sinigaglia A. Slosar A. Smith D. Sprayberry T. Tan G. Tarl\'e S. Trusov R. Vaisakh D. Valcin F. Valdes M. Vargas-Maga\~na L. Verde M. Walther B. Wang M. S. Wang B. A. Weaver N. Weaverdyck R. H. Wechsler D. H. Weinberg M. White J. Yu Y. Yu S. Yuan C. Y\`eche E. A. Zaborowski P. Zarrouk H. Zhang C. Zhao R. Zhao R. Zhou H. Zou
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Pith reviewed 2026-05-19 07:25 UTC · model grok-4.3

classification 🌌 astro-ph.CO
keywords baryon acoustic oscillationslyman-alpha forestquasar spectracosmological distanceshigh-redshift expansionsound horizoncorrelation functions
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The pith

BAO in the Lyman-alpha forest of quasars yields a 2% measurement of the expansion rate at redshift 2.33.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

This paper presents a measurement of baryon acoustic oscillations drawn from the Lyman-alpha absorption in spectra of high-redshift quasars. Analysis of correlations among more than 420,000 forest spectra and 700,000 quasars extracts the characteristic oscillation scale at an effective redshift of 2.33. The result gives the Hubble expansion rate and transverse comoving distance at that epoch, each scaled to a reference sound horizon value, with quoted precisions of 2 percent and 2.4 percent. A sympathetic reader cares because the measurement adds an early-time anchor to the expansion history that can be combined with lower-redshift data to test models of cosmic evolution.

Core claim

For a given value of the sound horizon rd, the expansion at z_eff=2.33 is measured with 2 percent precision as H(z_eff) = (239.2 ± 4.8) (147.09 Mpc / rd) km/s/Mpc. A 2.4 percent measurement of the transverse comoving distance is given as D_M(z_eff) = (5.84 ± 0.14) (rd/147.09 Mpc) Gpc. These values are obtained from the Lyman-alpha forest spectra and their cross-correlations with quasars through a blinded analysis that was validated on synthetic data before unblinding.

What carries the argument

The baryon acoustic oscillation peak position extracted from the two-point correlation functions of Lyman-alpha forest pixels and quasar positions.

If this is right

  • The high-redshift BAO scale can be combined with lower-redshift measurements to constrain cosmological parameters.
  • The 2 percent precision on H(z) at z_eff=2.33 supplies a direct constraint on the expansion rate around that epoch.
  • Consistency checks across data splits and alternative analysis choices support the stability of the extracted scale.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Repeating the measurement with future larger samples could test whether the BAO scale remains constant with redshift.
  • The result supplies an independent early-universe distance calibration that can be compared against other high-redshift probes.
  • Tension with expansion histories inferred from other methods at similar redshifts would point to unaccounted effects in the modeling.

Load-bearing premise

The blinded analysis pipeline and synthetic-data validation fully capture all relevant systematics in the real spectra and correlations.

What would settle it

A statistically significant mismatch between the reported BAO scale and the scale predicted by a cosmological model fitted to independent lower-redshift distance measurements after fixing the sound horizon.

read the original abstract

We present the measurement of Baryon Acoustic Oscillations (BAO) from the Lyman-$\alpha$ (Ly$\alpha$) forest of high-redshift quasars with the first-year dataset of the Dark Energy Spectroscopic Instrument (DESI). Our analysis uses over $420\,000$ Ly$\alpha$ forest spectra and their correlation with the spatial distribution of more than $700\,000$ quasars. An essential facet of this work is the development of a new analysis methodology on a blinded dataset. We conducted rigorous tests using synthetic data to ensure the reliability of our methodology and findings before unblinding. Additionally, we conducted multiple data splits to assess the consistency of the results and scrutinized various analysis approaches to confirm their robustness. For a given value of the sound horizon ($r_d$), we measure the expansion at $z_{\rm eff}=2.33$ with 2\% precision, $H(z_{\rm eff}) = (239.2 \pm 4.8) (147.09~{\rm Mpc} /r_d)$ km/s/Mpc. Similarly, we present a 2.4\% measurement of the transverse comoving distance to the same redshift, $D_M(z_{\rm eff}) = (5.84 \pm 0.14) (r_d/147.09~{\rm Mpc})$ Gpc. Together with other DESI BAO measurements at lower redshifts, these results are used in a companion paper to constrain cosmological parameters.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

0 major / 2 minor

Summary. The paper reports the first BAO measurements from the Lyman-alpha forest in DESI year-1 data, using >420,000 Lyα forest spectra and cross-correlations with >700,000 quasars. After a blinded analysis validated on synthetic data and checked via data splits and variant pipelines, it extracts H(z_eff=2.33) = (239.2 ± 4.8) (147.09 Mpc / r_d) km/s/Mpc (2% precision) and D_M(z_eff=2.33) = (5.84 ± 0.14) (r_d / 147.09 Mpc) Gpc (2.4% precision), to be combined with lower-redshift DESI BAO results in a companion paper.

Significance. If the quoted precisions hold, this supplies a high-redshift BAO anchor that tightens constraints on dark energy and curvature when combined with the rest of the DESI BAO program. The blinded pipeline, synthetic-data validation, and internal consistency tests are genuine strengths that support the central claim of an unbiased scale measurement.

minor comments (2)
  1. The abstract and §1 could more explicitly state the effective redshift definition and the precise weighting used to obtain z_eff=2.33 from the auto- and cross-correlation peaks.
  2. Figure captions for the correlation-function plots should include the exact fitting range and the number of mock realizations used to estimate the covariance.

Simulated Author's Rebuttal

0 responses · 0 unresolved

We thank the referee for their positive review, accurate summary of the analysis, and recommendation to accept the manuscript. We are pleased that the blinded pipeline, synthetic-data validation, and consistency tests were recognized as strengths supporting the reliability of the BAO measurement.

Circularity Check

0 steps flagged

No circularity: direct BAO scale extraction from observed Lyα correlations

full rationale

The paper reports direct measurements of the BAO feature position in the Lyman-alpha forest auto-correlation and quasar cross-correlation functions from DESI first-year data. The reported H(z_eff) and D_M(z_eff) values are obtained by fitting the BAO peak location in these observed correlation functions and expressing the result relative to an external sound horizon rd; the analysis pipeline is blinded and validated on synthetic data, but the central results are extracted from real spectra without reduction to fitted inputs or self-citation chains by construction. The derivation chain remains self-contained against external benchmarks.

Axiom & Free-Parameter Ledger

0 free parameters · 2 axioms · 0 invented entities

The central claim rests on standard cosmological assumptions about the BAO feature as a standard ruler and the fidelity of the correlation-function modeling; no new free parameters or invented entities are introduced.

axioms (2)
  • domain assumption The BAO scale functions as a standard ruler whose observed size directly encodes the expansion history and transverse distance.
    Invoked when converting the measured correlation scale into H(z) and D_M(z).
  • domain assumption The cross-correlation and auto-correlation modeling isolates the BAO feature without significant contamination from unmodeled systematics.
    Required for the blinded pipeline to yield cosmological measurements.

pith-pipeline@v0.9.0 · 6918 in / 1465 out tokens · 45339 ms · 2026-05-19T07:25:59.445168+00:00 · methodology

discussion (0)

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Forward citations

Cited by 18 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score.

  1. Cosmological analysis of the DESI DR1 Lyman alpha 1D power spectrum

    astro-ph.CO 2026-01 unverdicted novelty 7.0

    DESI DR1 Lyman-alpha data yields Δ²★=0.379±0.032 and n★=-2.309±0.019 at k★=0.009 km⁻¹s and z=3, sharpening N_eff, α_s, and β_s constraints by factors of 1.18-1.90 when combined with other probes.

  2. DESI DR2 Results II: Measurements of Baryon Acoustic Oscillations and Cosmological Constraints

    astro-ph.CO 2025-03 accept novelty 7.0

    DESI DR2 BAO data exhibits 2.3 sigma tension with CMB in Lambda-CDM but prefers evolving dark energy (w0 > -1, wa < 0) at 3.1 sigma with CMB and 2.8-4.2 sigma when including supernovae.

  3. DESI 2024 VI: Cosmological Constraints from the Measurements of Baryon Acoustic Oscillations

    astro-ph.CO 2024-04 accept novelty 7.0

    First-year DESI BAO data are consistent with flat LambdaCDM and, when combined with CMB, show a 2.5-3.9 sigma preference for evolving dark energy (w0 > -1, wa < 0) that strengthens with certain supernova datasets.

  4. New Isocurvature Constraints from JWST UV Luminosity Function

    astro-ph.CO 2026-05 unverdicted novelty 6.0

    First UVLF-based constraints on model-agnostic isocurvature power spectra for CDM, baryon, neutrino, and dark radiation modes yield consistent 95% credible envelopes over k ~ 0.5-10 Mpc^{-1}.

  5. $H_0$ Without the Sound Horizon (or Supernovae): A 2% Measurement in DESI DR1

    astro-ph.CO 2025-10 conditional novelty 6.0

    A heuristic power-spectrum rescaling applied to DESI DR1 BAO data plus CMB acoustic scale anchor yields H0 values of 69.2 to 70.3 km/s/Mpc at sub-2% precision across three independent late-time datasets.

  6. Probing the limits of cosmological information from the Lyman-$\alpha$ forest 2-point correlation functions

    astro-ph.CO 2025-09 unverdicted novelty 6.0

    Using idealized synthetic data, knowing the true continuum in Lyα forest auto- and cross-correlations reduces uncertainties on the AP parameter and Ω_m by ~10%, with extension to 240 h^{-1}Mpc scales adding up to ~15%...

  7. DESI 2024 VII: Cosmological Constraints from the Full-Shape Modeling of Clustering Measurements

    astro-ph.CO 2024-11 accept novelty 6.0

    DESI DR1 full-shape clustering yields Ω_m = 0.2962 ± 0.0095 and σ_8 = 0.842 ± 0.034 in flat ΛCDM, tightening to H_0 = 68.40 ± 0.27 km/s/Mpc with CMB and DESY3, while favoring w_0 > -1, w_a < 0 and limiting neutrino ma...

  8. DESI 2024 V: Full-Shape Galaxy Clustering from Galaxies and Quasars

    astro-ph.CO 2024-11 accept novelty 6.0

    DESI DR1 full-shape galaxy clustering constrains Omega_m = 0.296 ± 0.010, H0 = 68.63 ± 0.79 km/s/Mpc, and sigma_8 = 0.841 ± 0.034, consistent with LambdaCDM and Planck.

  9. DESI and Gravitational Wave Constraints Challenge Quintessential {\alpha}-Attractor Inflation

    astro-ph.CO 2026-05 conditional novelty 5.0

    Alpha-attractor quintessential inflation models are disfavored by DESI observations and Delta Neff limits from gravitational waves, as they predict an inconsistent scalar spectral index when the gravitational-wave abu...

  10. Local primordial non-Gaussianity using cross-correlations of DESI tracers

    astro-ph.CO 2026-04 conditional novelty 5.0

    Cross-correlating LRG and QSO samples in DESI DR1 yields f_NL^loc = 2.1 with 68% uncertainties of +8.8 and -8.3, an incremental improvement over auto-correlations alone.

  11. Measuring neutrino mass in light of ACT DR6 and DESI DR2

    astro-ph.CO 2026-03 unverdicted novelty 5.0

    New ACT and DESI data yield model-dependent upper limits on sum of neutrino masses, with holographic dark energy giving the tightest bounds and a consistent preference for degenerate hierarchy.

  12. Reanalyzing DESI DR1: 2. Constraints on Dark Energy, Spatial Curvature, and Neutrino Masses

    astro-ph.CO 2025-11 unverdicted novelty 5.0

    Reanalysis of DESI full-shape clustering data tightens constraints on neutrino mass, spatial curvature, and dark energy equation-of-state parameters relative to BAO-only results.

  13. Combined tracer analysis for DESI 2024 BAO

    astro-ph.CO 2025-08 accept novelty 5.0

    Combining LRG and ELG tracers with bias weighting improves BAO constraints by 11% on alpha_iso and 7% on alpha_AP in DESI DR1 data for the 0.8<z<1.1 bin.

  14. Constraints on Neutrino Physics from DESI DR2 BAO and DR1 Full Shape

    astro-ph.CO 2025-03 conditional novelty 5.0

    DESI DR2 BAO and full-shape data plus CMB yield ∑m_ν < 0.0642 eV (95% CL) under ΛCDM, in 3σ tension with oscillation lower limits, relaxed to <0.163 eV in w0waCDM.

  15. From Large Telescopes to the MUltiplexed Survey Telescope (MUST)

    astro-ph.IM 2026-05 unverdicted novelty 4.0

    MUST is a new 6.5 m telescope designed to deliver simultaneous optical spectra for over 20,000 targets across a 5 deg² field, enabling the largest 3D spectroscopic map of the Universe with redshifts for more than 100 ...

  16. Primordial magnetic fields in the light of upcoming post-EoR Lyman-$\alpha$ and 21-cm observations

    astro-ph.CO 2026-04 unverdicted novelty 4.0

    Forecasts show DESI-like and SKA1-Mid observations could constrain primordial magnetic field amplitude and spectral index to roughly 10% precision via 21cm auto-spectrum and Lyα-21cm cross-spectrum.

  17. Extended Dark Energy analysis using DESI DR2 BAO measurements

    astro-ph.CO 2025-03 conditional novelty 4.0

    Extended analysis of DESI DR2 data confirms robust evidence for dynamical dark energy with phantom crossing preference, stable under parametric and non-parametric modeling.

  18. DESI DR2 Results I: Baryon Acoustic Oscillations from the Lyman Alpha Forest

    astro-ph.CO 2025-03 accept novelty 4.0

    DESI DR2 delivers 0.65% precision BAO measurements from the LyA forest at z_eff=2.33, with D_H/r_d = 8.632 ± 0.098 ± 0.026 and D_M/r_d = 38.99 ± 0.52 ± 0.12.

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