REVIEW 2 major objections 5 minor 54 references
XShooter redshifts for 58 lenses and 57 sources show no measurement bias, so the source-z distribution can calibrate large imaging surveys.
Reviewed by Pith at T0; open to challenge. T0 means a machine referee read the full paper against a public rubric. the ladder, T0–T4 →
T0 review · grok-4.5
2026-07-10 05:17 UTC pith:XLUED2U6
load-bearing objection Solid southern XShooter redshift catalog for DESI Legacy lenses; the “no bias / representative zs” claim is only qualitatively supported by color–magnitude plots and should be treated as provisional. the 2 major comments →
XShooter DESI Lens Program: Sample characterization
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Spectroscopic redshifts for 58 lenses and 57 sources drawn from neural-network-selected DESI Legacy Survey lenses show no color- or magnitude-dependent bias relative to the parent observed sample; the resulting source redshift distribution (median zs = 1.54) can therefore be used as a representative calibrator for large imaging-survey analyses.
What carries the argument
Quality-flagged XShooter redshifts (Qz = 1–4) extracted from continuum absorption (lenses) and emission lines (sources), combined with a direct comparison of g−r / r−z colors and z-band magnitudes between successful measurements and the full observed set.
Load-bearing premise
That matching color and magnitude distributions between systems with good redshifts and the full observed sample is enough to prove the spectroscopic success rate is uniform across the true source-redshift range.
What would settle it
A larger, deeper spectroscopic campaign of the same parent catalog that recovers redshifts for a substantial fraction of the currently failed or low-Qz sources and finds a systematically different redshift distribution would falsify the claim of representativeness.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper reports VLT/XShooter spectroscopy of 67 grade-A strong-lens candidates from the DESI Legacy Imaging Surveys (Huang et al. 2021; Storfer et al. 2024) at Dec < −20°. Redshifts are measured for 58 lenses and 57 sources (45 systems with both), with quality flags Qz = 1–4 based on continuum and emission-line features. The sample yields a source redshift range 0.28 < zs < 4.34 (median zs = 1.54) and a lens distribution mostly at z < 1. The authors also note two sources with outflow signatures and seven with rotating disks. On the basis of magnitude and g−r / r−z color comparisons (Figs. 3–4) between systems with successful redshifts (Qz > 2) and the observed sample, they conclude that no particular bias is associated with the redshift measurement operation, so the measured source-z distribution is likely representative of the true parent distribution and can be used to calibrate analyses in large imaging surveys.
Significance. A homogeneous spectroscopic characterization of a southern DESI Legacy Survey lens sample is a useful community resource, especially given the forthcoming Euclid and LSST strong-lens catalogues. The 82 % / 85 % success rates, the tabulated redshifts with quality flags (Table 2), and the extensive per-system 1D/2D spectral figures constitute a concrete, reusable data product. The identification of outflows and rotating disks adds modest astrophysical interest. The central claim that the measured source-z histogram can be treated as representative for survey calibration is of clear practical value if it holds, but it currently rests on an incomplete empirical test.
major comments (2)
- The central claim (Abstract; end of §3; §4) that the measured source redshift distribution is “likely representative of the true one” is supported only by the visual similarity of g−r / r−z colors and magnitudes between systems with Qz > 2 and the observed sample (Figs. 3–4). Color–magnitude similarity does not constrain whether the spectroscopic success function S(z) is flat across 0.28 < zs < 4.34. Emission-line detectability (the dominant Qz = 4 channel) depends on which lines fall into the NIR arm, sky-line density, and continuum S/N—all of which vary strongly with redshift. The paper never constructs a selection function, nor does it compare successful versus failed subsets in any redshift-sensitive observable beyond broadband colors. Without such a test (or an explicit caveat that the histogram is an observed, not completeness-corrected, distribution), the claim that the sample “ca
- §3 and Table 2 report 33 % of lens redshifts with Qz < 2 and several source redshifts with Qz = 1–2 (single-line or continuum-only). The text does not state whether the histograms in Fig. 2 or the “representative” claim include only Qz ≥ 3 systems or the full set. Because low-Qz redshifts are more susceptible to line misidentification and sky residuals (explicitly noted for several systems in the appendix figures), the paper should either restrict the science sample to a well-defined quality cut or quantify how the distribution changes when low-Qz objects are excluded.
minor comments (5)
- Storfer et al. is cited as 2022 in the Abstract and as 2024 in the body and references; the year should be made consistent.
- Table 1 lists program IDs and OB counts but does not give the total on-source exposure or the fraction of grade-A nights; a one-line summary would help readers assess data quality.
- Several appendix figure captions (e.g., DESI-024.5133-21.9299, DESI-033.8095-29.1570) discuss alternative line identifications or photometric-redshift tensions; these caveats should be cross-referenced in Table 2 or the main text so that users of the catalogue are aware of them.
- Fig. 2 caption and axis labels would benefit from explicit statement of the quality cut (if any) applied to the plotted redshifts.
- Minor typographical issues: “XSchooter” (p. 2), “HandK” for H and K lines, and occasional missing spaces around redshifts (e.g., z=0.295).
Circularity Check
Empirical sample characterization with no derivation that reduces to its inputs; only minor non-load-bearing self-citation of the parent imaging catalog.
specific steps
-
self citation load bearing
[§3, paragraph discussing Fig. 4; also Abstract and §4]
"Given that Huang et al. (2021) did not perform any selection on the sources, this suggests that our redshift distribution of the sources is likely representative of the true one."
Huang is a co-author; the claim that the parent catalog is free of source selection is taken from the collaboration’s own prior imaging paper. This is only a minor premise supporting representativeness and does not force the measured redshifts or the color–magnitude comparison by construction; the redshifts remain independent spectral measurements.
full rationale
The paper reports new VLT/XShooter redshifts for 58 lenses and 57 sources drawn from an imaging neural-network catalog (Huang et al. 2021; Storfer et al. 2024). Redshifts are identified from observed absorption/emission lines against laboratory wavelengths and graded by continuum/line quality (Qz); this is direct measurement, not a fitted model or self-definitional construction. The central claim that the measured source-z distribution is “likely representative” rests on two empirical comparisons internal to the observed sample: (i) success rate versus zAB magnitude (Fig. 3) and (ii) g−r / r−z color distributions of systems with Qz>2 versus the full observed set (Fig. 4), plus the statement that Huang et al. imposed no source selection. These checks do not reduce by construction to any fitted parameter or to a uniqueness theorem; they are falsifiable photometric comparisons. The only self-citation of note is the parent-sample reference (authors overlap), which is used solely to establish that the imaging search did not pre-select sources; it is not load-bearing for the redshift values themselves nor for the color–magnitude test. No ansatz is smuggled, no prediction is a re-labeled fit, and no uniqueness result is imported. The skeptic’s concern that color similarity does not fully constrain S(z) is a completeness/correctness issue, not circularity. Score 1 reflects only the minor, non-circular self-citation of the imaging papers.
Axiom & Free-Parameter Ledger
axioms (3)
- domain assumption Observed emission and absorption lines can be identified with rest-frame atomic transitions (e.g., [O II], Hα, Ca H&K) to assign spectroscopic redshifts.
- domain assumption Quality flags Qz=1–4 correctly rank continuum and emission-line reliability for subsequent statistical use.
- domain assumption The Huang et al. (2021) and Storfer et al. (2024) grade-A candidates form a parent sample whose source population is the target of the representativeness claim.
read the original abstract
Large imaging surveys in cosmology are detecting orders of magnitude more lens systems than known so far. This unprecedented dataset will lead to robust constraints on cosmology and galaxy evolution models. However, a preliminary careful characterization of the lens and source samples are mandatory. In this work, we report on a VLT/XShooter observation program of 67 lens systems to characterize their spectroscopic redshift distribution. These systems were previously detected on the Dark Energy Spectroscopic Instrument Legacy Imaging Surveys by Huang et al. 2021 and Storfer et al. 2022 with deep residual neural network. We manage to measure redshifts for 58 lenses and 57 sources. We also identify 2 sources with indication of outflow in the shape of the emission lines and 7 sources with rotating disks in $[OII]$ or $H\alpha$. We find no particular bias associated to the redshift measurement operation, meaning that our measured source redshift distribution is likely representative of the true one and can be used to calibrate analyses in large imaging surveys.
Figures
Reference graph
Works this paper leans on
-
[1]
Abell , G. O., Corwin , Jr., H. G., & Olowin , R. P. 1989, , 70, 1
work page 1989
-
[2]
Adnan , S. M. R., Hasan , M. J., Al-Imtiaz , A., et al. 2025, , 699, A259
work page 2025
- [3]
- [4]
-
[5]
2010, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol
Bacon , R., Accardo , M., Adjali , L., et al. 2010, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol. 7735, Ground-based and Airborne Instrumentation for Astronomy III, ed. I. S. McLean , S. K. Ramsay , & H. Takami , 773508
work page 2010
-
[6]
E., Bocquet , S., Stalder , B., et al
Bleem , L. E., Bocquet , S., Stalder , B., et al. 2020, , 247, 25
work page 2020
-
[7]
E., Stalder , B., Brodwin , M., et al
Bleem , L. E., Stalder , B., Brodwin , M., et al. 2015 a , , 216, 20
work page 2015
-
[8]
E., Stalder , B., de Haan , T., et al
Bleem , L. E., Stalder , B., de Haan , T., et al. 2015 b , , 216, 27
work page 2015
-
[9]
CHEX-MATE Collaboration , Arnaud , M., Ettori , S., et al. 2021, , 650, A104
work page 2021
- [10]
-
[11]
Collaboration, D., Adame, A. G., Aguilar, J., et al. 2024, The Astronomical Journal, 168, 58
work page 2024
-
[12]
Despali , G., Heinze , F. M., Fassnacht , C. D., et al. 2025, , 699, A222
work page 2025
-
[13]
D \' az-S \'a nchez , A., Dannerbauer , H., Sulzenauer , N., Iglesias-Groth , S., & Rebolo , R. 2021, , 919, 48
work page 2021
-
[14]
Diehl , H. T., Buckley-Geer , E. J., Lindgren , K. A., et al. 2017, , 232, 15
work page 2017
- [15]
- [16]
-
[17]
Euclid Collaboration , Lines , N. E. P., Collett , T. E., et al. 2025 b , arXiv e-prints, arXiv:2503.15326
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[18]
Euclid Collaboration , Rojas , K., Collett , T. E., et al. 2025 c , arXiv e-prints, arXiv:2503.15325
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[19]
Euclid Collaboration , Walmsley , M., Holloway , P., et al. 2025 d , arXiv e-prints, arXiv:2503.15324
work page internal anchor Pith review Pith/arXiv arXiv 2025
- [20]
-
[21]
Hinton , S. R., Davis , T. M., Lidman , C., Glazebrook , K., & Lewis , G. F. 2016, Astronomy and Computing, 15, 61
work page 2016
-
[22]
Huang , X., Inchausti , J. C., Storfer , C. J., et al. 2025, arXiv e-prints, arXiv:2509.18089
- [23]
- [24]
- [25]
- [26]
-
[27]
Knowles , K., Cotton , W. D., Rudnick , L., et al. 2022, , 657, A56
work page 2022
-
[28]
Koulouridis , E., Clerc , N., Sadibekova , T., et al. 2021, , 652, A12
work page 2021
- [29]
-
[30]
Euclid Definition Study Report
Laureijs , R., Amiaux , J., Arduini , S., et al. 2011, ArXiv e-prints [ [arXiv] 1110.3193 ]
work page internal anchor Pith review Pith/arXiv arXiv 2011
-
[31]
Li , T., Collett , T. E., Acebron , A., et al. 2025, Breaking the mass sheet degeneracy in strong lensing time delay cosmology with a new sample of double source plane lenses. , HST Proposal. Cycle 33, ID. \#18097
work page 2025
-
[32]
Li , T., Collett , T. E., Krawczyk , C. M., & Enzi , W. 2024, , 527, 5311
work page 2024
-
[33]
DESI Strong Lens Foundry IV: Spectroscopic Confirmation of DESI Lens Candidates with VLT/MUSE
Lin , E., Toro Bertolla , I., Cikota , A., et al. 2025, arXiv e-prints, arXiv:2509.18078
work page internal anchor Pith review Pith/arXiv arXiv 2025
-
[34]
May , P. E. 2013, PhD thesis, University of Birmingham, UK
work page 2013
-
[35]
Mehrtens , N., Romer , A. K., Hilton , M., et al. 2012, , 423, 1024
work page 2012
- [36]
-
[37]
Meneghetti , M., Davoli , G., Bergamini , P., et al. 2020, Science, 369, 1347
work page 2020
-
[38]
Newman , A. B., Belli , S., Ellis , R. S., & Patel , S. G. 2018, , 862, 126
work page 2018
- [39]
- [40]
-
[41]
Richard , J., Claeyssens , A., Lagattuta , D., et al. 2021, , 646, A83
work page 2021
-
[42]
Rodney , S. A., Brammer , G. B., Pierel , J. D. R., et al. 2021, Nature Astronomy, 5, 1118
work page 2021
- [43]
- [44]
-
[45]
Sainz de Murieta , A., Collett , T. E., Magee , M. R., et al. 2024, , 535, 2523
work page 2024
-
[46]
J., Vernardos , G., Collett , T
Shajib , A. J., Vernardos , G., Collett , T. E., et al. 2024, , 220, 87
work page 2024
- [47]
- [48]
- [49]
-
[50]
Smithsonian Astrophysical Observatory . 2000, SAOImage DS9: A utility for displaying astronomical images in the X11 window environment , Astrophysics Source Code Library, record ascl:0003.002
work page 2000
- [51]
-
[52]
2026, arXiv e-prints, arXiv:2602.16077
Urcelay , F., Huang , X., Sheu , W., et al. 2026, arXiv e-prints, arXiv:2602.16077
-
[53]
F., Huang , X., & Hernandez , J
Urcelay , F., Jullo , E., Barrientos , L. F., Huang , X., & Hernandez , J. 2025, , 694, A35
work page 2025
- [54]
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.