REVIEW 3 major objections 7 minor 1 cited by
Beyond Traditional Diagnostics: Identifying Active Galactic Nuclei with Spectral Energy Distribution Fitting in DESI Data
T0 review · 3 major / 7 minor · reviewed 2026-08-07 · deepseek-v4-flash
Pith's one-line read SED fitting of DESI galaxies recovers ~70% of line-selected AGN and 86-87% of WISE-selected AGN when all four WISE bands have good signal.
desk verdict Careful, useful DESI EDR calibration of SED-based AGN selection—but the headline completeness/contamination numbers are in-sample and need out-of-sample validation before they become survey predictions. read the letter →
The pith
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
The reading
What carries the argument
The load-bearing object is AGNFRAC, the fraction of the total infrared luminosity contributed by the AGN component in a CIGALE SED fit, combined with the infrared-quality flag FLAGINFRARED. The fits use optical (g, r, z) and WISE (W1-W4) photometry with the default grid of Fritz et al. (2006) AGN templates, Bruzual & Charlot (2003) stellar populations, and fixed solar metallicity, and the selection rule is simply AGNFRAC≥0.1 plus FLAGINFRARED=4. The machinery works by separating galaxies whose mid-infrared light is dominated by dust heated by the accretion disk from those whose infrared output comes from star formation; when the WISE bands are noisy or absent this separation collapses.
What would settle it
Take a sample of galaxies with deep Chandra or XMM coverage but no SED-based preselection, run the exact CIGALE grid described here, and compare the recovery rate of X-ray-confirmed AGN at AGNFRAC≥0.1 with the recovery rate of X-ray-quiet star-forming galaxies; if the two rates are not clearly separated, the threshold is not tracing nuclear activity.
Extended reading notes
Core claim
The central claim is that the CIGALE-derived AGN fraction (AGNFRAC), the fraction of infrared luminosity contributed by the AGN template, is a valid AGN indicator—but only when it is paired with reliable mid-infrared photometry. Using AGNFRAC≥0.1 together with FLAGINFRARED=4 (all four WISE bands with SNR≥3), the SED method matches about 70% of BPT-AGN and broad-line AGN and 86-87% of WISE-selected AGN, while star-forming contamination drops to about 15%. Without high-quality WISE data the AGN fraction distributions of star-forming and AGN galaxies become nearly indistinguishable (ROC AUC falls to ~0.57), so the method's power is contingent on the mid-infrared coverage. The paper also finds that roughly half of SED-AGN candidates are not caught by BPT, WISE, X-ray, or radio diagnostics; expanding the diagnostic set leaves only about 16% as SED-only, most of them old, passive galaxies whose optical light hides a mid-infrared excess suggestive of weak or fading nuclear activity.
Load-bearing premise
Every SED-AGN label is just the threshold AGNFRAC≥0.1, and that number comes from one specific model grid with Fritz et al. (2006) AGN templates at fixed solar metallicity, so the reported recovery and contamination rates are only as trustworthy as that grid.
Editorial extensions
If this is right
- Surveys that have photometry but limited spectroscopy can use AGNFRAC≥0.1 with full WISE coverage as a practical AGN selector.
- Relaxing the quality cut to FLAGINFRARED≥3 keeps the same median AGN fractions and yields a larger but less restrictive sample.
- The method substantially overlaps with, but does not replace, traditional diagnostics: it recovers ~50% of X-ray AGN and ~40% of radio AGN, so it should be combined with other tracers for a complete census.
- The SED-only AGN population, dominated by massive passive galaxies with high D4000 and red UVJ colors, is a plausible reservoir of weak or fading nuclear activity that other methods miss.
- Without high-SNR WISE photometry in all four bands, AGNFRAC is essentially non-discriminative, so applying the threshold blindly to photometry-poor samples would fail.
Reading between the lines
- If the SED-only candidates are confirmed as true AGN, this method would roughly double the AGN census at z≤0.5 relative to optical emission-line selection alone.
- The same pipeline could be applied to DESI DR1's much larger footprint, or to photometric-redshift samples where no spectra exist at all, extending AGN searches to fainter and more distant galaxies.
- The strong template dependence shown in Appendix C suggests that running a two-template ensemble (Fritz and SKIRTOR) or leaving metallicity free would let surveys explicitly trade completeness against star-forming contamination.
- Deep X-ray follow-up of the LINER-classified SED-AGN candidates would decide between true accretion and photoionization by old stellar populations, which is the main open question for the SED-only population.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper tests SED-based AGN identification using CIGALE optical-to-MIR SED fits of 510,938 DESI Early Data Release galaxies at z≤0.5 with reliable redshifts and good photometric/SED quality. The authors define SED-AGN by AGNFRAC≥0.1 combined with FLAGINFRARED=4 (SNR≥3 in all four WISE bands) and compare against BPT diagrams (three variants), WHAN, broad-Hα (BL-AGN), WISE color, X-ray, and radio selections. They report that the SED method recovers approximately 70% of BPT-AGN and BL-AGN and 86-87% of WISE-AGN, with 15% contamination from star-forming galaxies when good MIR data are available, whereas without high-SNR WISE photometry the AGN and star-forming populations are nearly indistinguishable. About half of the SED-AGN sample is not selected by the main classical diagnostics; after adding finer diagnostics (LINER, composite, retired, X-ray, radio), this 'SED-AGN Only' fraction drops to about 16%, with these objects being predominantly massive, passive, red-sequence galaxies. The paper advocates SED fitting as a complementary multi-wavelength AGN-selection tool for large surveys.
Significance. If the reported quantitative results hold, the paper provides a useful reference for photometry-driven AGN selection in current and upcoming large surveys (DESI, Euclid, LSST), and its demonstration that AGNFRAC from optical-MIR fits is only usable when high-SNR WISE photometry is present is an important practical caution. The paper is unusually transparent: the full CIGALE parameter grid is published (Table A.1), the sensitivity of the classification to model choices is quantified (Table C.1 and Fig. D.1), the VAC and the data behind the figures are public, and the authors explicitly flag the limitations of the AGNFRAC uncertainties, the weakness of the [NeIII] detection, and the debated nature of LINERs. The qualitative claims—MIR photometry is essential and SED-AGN overlaps substantially with classical AGN samples, including an independent X-ray check that recovers about half of X-ray AGN—are well supported by the distribution shifts, ROC curves, and stacked spectra. The main quantitative claims (70%, 86-87%, 15%) are, however, in-sample and model-grid-specific, so their predictive value is the part of the paper that needs the most scrutiny.
major comments (3)
- [§4.1, Appendix D, Table 2] The headline recovery and contamination rates (≈70% for BPT-AGN and BL-AGN, 86% for WISE-AGN, 15% for BPT-SF in Table 2) are in-sample estimates: the AGNFRAC≥0.1 threshold is selected by ROC analysis (Appendix D, Fig. D.1) on the same FLAGINFRARED=4 sample that serves as the denominator for those rates, and Appendix D does not specify which classes define the positive and negative sets in the ROC analysis. Because the operating point is chosen from the same data used to quote the performance, the reported completeness and purity are self-assessments rather than predictions. Please provide an out-of-sample evaluation (for example, a training/test split of the ROC analysis, or a validation on the DESI DR1 VAC) or explicitly rephrase the headline numbers as the calibration performance of a threshold tuned on the same sample.
- [§3.3, §4.2, Table 2, Abstract] The 86-87% recovery of WISE-AGN is not an independent test, because the same WISE photometry (W1-W4) enters both the CIGALE fits that produce AGNFRAC and the Hviding et al. (2022) color criterion that defines WISE-AGN. The text notes this at §3.3, but the Abstract and §5 still headline the 87% figure. The genuinely independent high-energy checks give lower recovery (≈45-50% for X-ray AGN and ≈40% for radio AGN, §4.3), so the abstract and conclusions should either report the range of recovery across all benchmarks or explicitly label the WISE-AGN number as a partly circular consistency check.
- [§2.2, Table A.1, Appendix C, Table C.1] The quoted rates are specific to the default CIGALE grid and the chosen operating point. Table A.1 samples AGNFRAC at 0, 0.01, 0.1, 0.3, ..., so the '≥0.1' cut is nearly equivalent to 'any non-zero AGN contribution in the fit,' and small photometric or prior changes can move sources across the boundary. Table C.1 shows that switching to SKIRTOR AGN templates raises WISE-AGN recovery to ≈97% while increasing star-forming contamination to ≈27%, and that adopting a Charlot & Fall dust attenuation law reduces BPT-AGN recovery to ≈55%. The abstract should state that the 70%/86%/15% figures are for the default Fritz (2006) grid and that the model-induced spread is of order 10 percentage points.
minor comments (7)
- [§4.2 and §5] The '62%' star-forming contamination is not consistently defined: in §4.2 it is quoted for the BPT-SF sample as a whole, while the Fig. 5 caption and the fifth summary bullet attribute it to the case with limited WISE coverage. The Abstract's 'from 62% to 15%' therefore compares different samples; please give the FLAGINFRARED-stratified values explicitly.
- [§3.5] The BPT-AGN reference class includes composite sources from the [NII]-BPT in the definition of §3.5; because composites are not secure AGN, the '~70% recovery of BPT-AGN' mixes pure AGN with composites. Please quantify how the recovery changes when only the pure-AGN (non-composite) part of the [NII]-BPT is used.
- [Table 4, §4.4] The very low median SFR of SED-AGN Only galaxies (log SFR ≈ −2.23) and the 'passive' conclusion are derived from the same CIGALE fits that define AGNFRAC; an independent estimate (e.g., from FastSpecFit line luminosities or D4000 alone) would strengthen this claim.
- [Abstract] The phrase '~70% of narrow/broad-line AGN' is imprecise: Table 2 gives 69.3% for BPT-AGN and 70.1% for BL-AGN; please name the two reference samples explicitly.
- [Footnote 7] 'FLAGNFRARED=4' is a typo for 'FLAGINFRARED=4'.
- [Fig. D.1] The ROC figure is dense; a short caption describing the default setting and each variant label (e.g., 'Z' = variable metallicity, 'AGN model' = SKIRTOR) would greatly improve readability.
- [§2.2 and Appendix C] The 'representative sample of ~50,000 galaxies' used for the model-dependence tests is described only by reference to Siudek et al. (2024); two sentences on its construction here would aid reproducibility.
Circularity Check
Headline recovery and contamination rates are in-sample: the AGNFRAC>=0.1 cut is ROC-tuned on the same FLAGINFRARED=4 labels later used to report 70%/86%/15%.
-
fitted input called prediction
[Sect. 4.1, Appendix D (Fig. D.1), and Table 2]
"Taking into account the strong correlation between AGNFRAC and the availability of WISE photometry with SNR>=3 (see also Sect. 4.2), we recommend applying a selection criterion of AGNFRAC>=0.1 combined with FLAGINFRARED=4 to define AGN based on SED fitting (SED-AGN). This threshold is motivated both by the observed peak in AGNFRAC distributions for spectroscopically confirmed AGN classes (see Fig. 4) and by its optimal diagnostic performance in the ROC analysis (see Appendix D). ... Table 2."
The ROC analysis in Appendix D is computed on the same FLAGINFRARED=4 sample used in Table 2, using the same BPT-AGN, BL-AGN, WISE-AGN, and BPT-SF labels. The threshold AGNFRAC>=0.1 is selected to optimize separation between those labels, and Table 2 then reports recovery/contamination percentages at that optimized cut for those same labels. Thus the headline values (70% BL-AGN, 69% BPT-AGN, 86% WISE-AGN, 15% BPT-SF contamination) are in-sample ROC operating points rather than independent predictions, with no held-out sample or cross-validation. The underlying CIGALE AGNFRAC is not label-trained, so this is a validation-loop circularity rather than full definitional equivalence.
full rationale
The SED fitting itself is not label-trained: CIGALE fits optical-MIR photometry against a fixed physical model grid, and BPT-AGN, BL-AGN, X-ray, and radio classifications rely on data that are not inputs to the fit, giving genuine independent support. The circular component is narrower: the decision threshold AGNFRAC>=0.1 is chosen via ROC analysis on the same FLAGINFRARED=4 sample and the same BPT/WISE/BL labels that are later used to quote recovery and contamination rates, so those rates are in-sample operating characteristics rather than out-of-sample predictions. In addition, the WISE-AGN benchmark shares the WISE photometry that constrains AGNFRAC, so the 86% WISE recovery is partly an internal consistency check; the paper acknowledges this in Sect. 3.3 but still presents it as validation. No load-bearing self-citation chain or imported uniqueness theorem is present, and Appendix C honestly quantifies model dependence (e.g., switching to SKIRTOR changes WISE recovery from 86% to 97% and contamination from 15% to 27%). Overall there is partial circularity in the headline validation loop, with independent content in the BPT, BL-AGN, X-ray, and radio comparisons.
Assumptions & free parameters
free parameters (2)
- AGNFRAC threshold =
0.1
- FLAGINFRARED cut =
=4 (all four WISE bands with SNR>=3)
assumptions (4)
- domain assumption The CIGALE model library with Fritz et al. (2006) AGN templates, Bruzual & Charlot (2003) stellar populations, Chabrier IMF, Calzetti attenuation, and Draine dust emission yields AGNFRAC values that trace true AGN contribution.
- domain assumption The reference diagnostics (BPT, WHAN, WISE, X-ray, radio) at their adopted thresholds are treated as ground truth for AGN, and galaxies not selected by them are treated as non-AGN for completeness calculations.
- domain assumption Parent sample selection cuts (ZWARN = 0 or 4, COADD_FIBERSTATUS = 0, z<=0.5, LOGM != 0, CHI2<=17) do not bias the AGN comparison.
- ad hoc to paper AGNFRAC uncertainties from CIGALE are unreliable in the faint or low-infrared regime and can be excluded from the classification.
Cite this review
Pith. "Pith review of Beyond Traditional Diagnostics: Identifying Active Galactic Nuclei with Spectral Energy Distribution Fitting in DESI Data." pith.science (2026). https://pith.science/paper/HP7S7BB4
@misc{pith2026250609143,
author = {Pith},
title = {Pith review of: Beyond Traditional Diagnostics: Identifying Active Galactic Nuclei with Spectral Energy Distribution Fitting in DESI Data},
year = {2026},
howpublished = {\url{https://pith.science/paper/HP7S7BB4}},
note = {Machine review of arXiv:2506.09143}
}
abstract
Active galactic nuclei (AGN) are typically identified through their distinctive X-ray or radio emissions, mid-infrared (MIR) colors, or emission lines. However, each method captures different subsets of AGN due to signal-to-noise (SNR) limitations, redshift coverage, and extinction effects, underscoring the necessity for a multi-wavelength approach for comprehensive AGN samples. This study explores the effectiveness of spectral energy distribution (SED) fitting as a robust method for AGN identification. Using {\tt CIGALE} optical-MIR SED fits on DESI Early Data Release galaxies, we compare SED-based AGN selection ({\tt AGNFRAC} $\geq0.1$) with traditional methods including BPT diagrams, WISE colors, X-ray, and radio diagnostics. SED fitting identifies $\sim 70\%$ of narrow/broad-line AGN and 87\% of WISE-selected AGN. Incorporating high SNR WISE photometry reduces star-forming galaxy contamination from 62\% to 15\%. Initially, $\sim50\%$ of SED-AGN candidates are undetected by standard methods, but additional diagnostics classify $\sim85\%$ of these sources, revealing LINERs and retired galaxies potentially representing evolved systems with weak AGN activity. Further spectroscopic and multi-wavelength analysis will be essential to determine the true AGN nature of these sources. SED fitting provides complementary AGN identification, unifying multi-wavelength AGN selections. This approach enables more complete -- albeit with some contamination -- AGN samples essential for upcoming large-scale surveys where spectroscopic diagnostics may be limited.
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Reference graph
Works this paper leans on
-
[1]
J., Salim , S., Boquien , M., et al
Agostino , C. J., Salim , S., Boquien , M., et al. 2023, , 526, 4455
2023
-
[2]
F., Argudo-Fern \'a ndez , M., et al
Almeida , A., Anderson , S. F., Argudo-Fern \'a ndez , M., et al. 2023, , 267, 44
2023
-
[3]
2024, arXiv e-prints, arXiv:2405.19288
Anand , A., Guy , J., Bailey , S., et al. 2024, arXiv e-prints, arXiv:2405.19288
arXiv 2024
-
[4]
J., Stern , D., Kochanek , C
Assef , R. J., Stern , D., Kochanek , C. S., et al. 2013, , 772, 26
2013
-
[5]
A., Phillips , M
Baldwin , J. A., Phillips , M. M., & Terlevich , R. 1981, , 93, 5
1981
-
[6]
2024, , 685, A141
Barchiesi , L., Vignali , C., Pozzi , F., et al. 2024, , 685, A141
2024
-
[7]
2025, , 694, A127
Bernal , S., S \'a nchez-S \'a ez , P., Ar \'e valo , P., et al. 2025, , 694, A127
2025
-
[8]
2013, , 551, A100
Berta , S., Lutz , D., Santini , P., et al. 2013, , 551, A100
2013
Show all 149 references
-
[9]
N., Kondapally , R., Williams , W
Best , P. N., Kondapally , R., Williams , W. L., et al. 2023, , 523, 1729
2023
-
[10]
2024, [ [arXiv] 2406.11962 ]
Bichang'a , B., Kaviraj , S., Lazar , I., et al. 2024, [ [arXiv] 2406.11962 ]
2024 arXiv
-
[11]
2019, , 622, A103
Boquien , M., Burgarella , D., Roehlly , Y., et al. 2019, , 622, A103
2019
-
[12]
Bradley , A. P. 1997, Pattern Recognition, 30, 1145
1997
-
[13]
Brandt , W. N. & Alexander , D. M. 2015, , 23, 1
2015
-
[14]
2023, , 166, 66
Brodzeller , A., Dawson , K., Bailey , S., et al. 2023, , 166, 66
2023
-
[15]
& Charlot , S
Bruzual , G. & Charlot , S. 2003, , 344, 1000
2003
-
[16]
J., Liu , X., Shen , Y., et al
Burke , C. J., Liu , X., Shen , Y., et al. 2022, , 516, 2736
2022
-
[17]
J., Liu , Y., Ward , C
Burke , C. J., Liu , Y., Ward , C. A., et al. 2024, arXiv e-prints, arXiv:2402.06882
2024 arXiv
-
[18]
2011, , 728, 58
Burlon , D., Ajello , M., Greiner , J., et al. 2011, , 728, 58
2011
-
[19]
C., et al
Calzetti , D., Armus , L., Bohlin , R. C., et al. 2000, , 533, 682
2000
-
[20]
M., Satyapal , S., Abel , N
Cann , J. M., Satyapal , S., Abel , N. P., et al. 2019, , 870, L2
2019
-
[21]
2003, , 115, 763
Chabrier , G. 2003, , 115, 763
2003
-
[22]
& Fall , S
Charlot , S. & Fall , S. M. 2000, , 539, 718
2000
-
[23]
2023, , 944, 107
Chaussidon , E., Y \`e che , C., Palanque-Delabrouille , N., et al. 2023, , 944, 107
2023
-
[24]
2011, , 413, 1687
Cid Fernandes , R., Stasi \'n ska , G., Mateus , A., & Vale Asari , N. 2011, , 413, 1687
2011
-
[25]
S., et al
Cid Fernandes , R., Stasi \'n ska , G., Schlickmann , M. S., et al. 2010, , 403, 1036
2010
-
[26]
2015, , 576, A10
Ciesla , L., Charmandaris , V., Georgakakis , A., et al. 2015, , 576, A10
2015
-
[27]
2023, , 672, A191
Ciesla , L., G \'o mez-Guijarro , C., Buat , V., et al. 2023, , 672, A191
2023
-
[28]
M., Negus , J., Barrows , R
Comerford , J. M., Negus , J., Barrows , R. S., et al. 2022, , 927, 23
2022
-
[29]
J., Cotton , W
Condon , J. J., Cotton , W. D., Greisen , E. W., et al. 1998, , 115, 1693
1998
-
[30]
J., Singh , M., Adams , N., et al
Conselice , C. J., Singh , M., Adams , N., et al. 2023, , 525, 1353
2023
-
[31]
P., Werner , M., Akeson , R., et al
Crill , B. P., Werner , M., Akeson , R., et al. 2020, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol. 11443, Space Telescopes and Instrumentation 2020: Optical, Infrared, and Millimeter Wave, ed. M. Lystrup & M. D. Perrin , 114430I
2020
-
[32]
2024, arXiv e-prints, arXiv:2405.20385
Csizi , B., Tortorelli , L., Siudek , M., et al. 2024, arXiv e-prints, arXiv:2405.20385
2024 arXiv
-
[33]
A., Helou , G., Magdis , G
Dale , D. A., Helou , G., Magdis , G. E., et al. 2014, , 784, 83
2014
-
[34]
Das , S., Smith , D. J. B., Haskell , P., et al. 2024, , 531, 977
2024
-
[35]
2022, , 164, 207
DESI Collaboration , Abareshi , B., Aguilar , J., et al. 2022, , 164, 207
2022
-
[36]
G., et al
DESI Collaboration , Abdul-Karim , M., Adame , A. G., et al. 2025, arXiv e-prints, arXiv:2503.14745
2025 arXiv
-
[37]
G., Aguilar , J., et al
DESI Collaboration , Adame , A. G., Aguilar , J., et al. 2024 a , , 168, 58
2024
-
[38]
G., Aguilar , J., et al
DESI Collaboration , Adame , A. G., Aguilar , J., et al. 2024 b , , 167, 62
2024
-
[39]
G., Aguilar , J., et al
DESI Collaboration , Adame , A. G., Aguilar , J., et al. 2024 c , arXiv e-prints, arXiv:2411.12022
2024 arXiv
-
[40]
2016 a , arXiv e-prints, arXiv:1611.00036
DESI Collaboration , Aghamousa , A., Aguilar , J., et al. 2016 a , arXiv e-prints, arXiv:1611.00036
2016 arXiv
-
[41]
2016 b , arXiv e-prints, arXiv:1611.00037
DESI Collaboration , Aghamousa , A., Aguilar , J., et al. 2016 b , arXiv e-prints, arXiv:1611.00037
2016 arXiv
-
[42]
J., Lang , D., et al
Dey , A., Schlegel , D. J., Lang , D., et al. 2019, , 157, 168
2019
-
[43]
1978, , 63, 63
Dodorico , S., Benvenuti , P., & Sabbadin , F. 1978, , 63, 63
1978
-
[44]
2014, arXiv e-prints, arXiv:1412.4872
Dor \'e , O., Bock , J., Ashby , M., et al. 2014, arXiv e-prints, arXiv:1412.4872
2014 arXiv
-
[45]
T., Aniano , G., Krause , O., et al
Draine , B. T., Aniano , G., Krause , O., et al. 2014, , 780, 172
2014
-
[46]
2024, , 687, A76
Dubois , J., Siudek , M., Fraix-Burnet , D., & Moultaka , J. 2024, , 687, A76
2024
-
[47]
2025 a , , 697, A1
Euclid Collaboration , Mellier , Y., Abdurro'uf , et al. 2025 a , , 697, A1
2025
-
[48]
2025 b , arXiv e-prints, arXiv:2503.15312
Euclid Collaboration , Siudek , M., Huertas-Company , M., et al. 2025 b , arXiv e-prints, arXiv:2503.15312
2025 arXiv
-
[49]
2025 c , arXiv e-prints, arXiv:2503.15321
Euclid Collaboration , Stevens , G., Fotopoulou , S., et al. 2025 c , arXiv e-prints, arXiv:2503.15321
2025
-
[50]
N., Evans , J
Evans , I. N., Evans , J. D., Mart \' nez-Galarza , J. R., et al. 2024, arXiv e-prints, arXiv:2407.10799
2024 arXiv
-
[51]
N., Primini , F
Evans , I. N., Primini , F. A., Glotfelty , K. J., et al. 2010, , 189, 37
2010
-
[52]
A., Alexander , D
Fawcett , V. A., Alexander , D. M., Brodzeller , A., et al. 2023, , 525, 5575
2023
-
[53]
2006, , 366, 767
Fritz , J., Franceschini , A., & Hatziminaoglou , E. 2006, , 366, 767
2006
-
[54]
2010, Reviews of Modern Physics, 82, 3121
Genzel , R., Eisenhauer , F., & Gillessen , S. 2010, Reviews of Modern Physics, 82, 3121
2010
-
[55]
M., Salim , S., Weinberg , N
Ghez , A. M., Salim , S., Weinberg , N. N., et al. 2008, , 689, 1044
2008
-
[56]
2007, , 463, 79
Gilli , R., Comastri , A., & Hasinger , G. 2007, , 463, 79
2007
-
[57]
2010, , 519, A92
Gilli , R., Vignali , C., Mignoli , M., et al. 2010, , 519, A92
2010
-
[58]
A., Heckman , T
Groves , B. A., Heckman , T. M., & Kauffmann , G. 2006, , 371, 1559
2006
-
[59]
2025, , 981, L8
Guo , W.-J., Pan , Z., Siudek , M., et al. 2025, , 981, L8
2025
-
[60]
A., et al
Guo , W.-J., Zou , H., Fawcett , V. A., et al. 2024 a , , 270, 26
2024
-
[61]
L., et al
Guo , W.-J., Zou , H., Greenwell , C. L., et al. 2024 b , arXiv e-prints, arXiv:2408.00402
2024 arXiv
-
[62]
2023, , 165, 144
Guy , J., Bailey , S., Kremin , A., et al. 2023, , 165, 144
2023
-
[63]
J., Ruiz-Macias , O., et al
Hahn , C., Wilson , M. J., Ruiz-Macias , O., et al. 2023, , 165, 253
2023
-
[64]
N., Reines , A
Hainline , K. N., Reines , A. E., Greene , J. E., & Stern , D. 2016, , 832, 119
2016
-
[65]
Harrison , C. M. & Ramos Almeida , C. 2024, Galaxies, 12, 17
2024
-
[66]
Heckman , T. M. 1980, , 87, 152
1980
-
[67]
Heckman , T. M. & Best , P. N. 2014, , 52, 589
2014
-
[68]
J., White , R
Helfand , D. J., White , R. L., & Becker , R. H. 2015, , 801, 26
2015
-
[69]
2018, , 481, 1774
Herpich , F., Stasi \'n ska , G., Mateus , A., Vale Asari , N., & Cid Fernandes , R. 2018, , 481, 1774
2018
-
[70]
& Lanusse , F
Huertas-Company , M. & Lanusse , F. 2023, , 40, e001
2023
-
[71]
E., Hainline , K
Hviding , R. E., Hainline , K. N., Rieke , M., et al. 2022, , 163, 224
2022
-
[72]
M., Tyson , J
Ivezi \'c , Z ., Kahn , S. M., Tyson , J. A., et al. 2019, , 873, 111
2019
-
[73]
I., Noeske , K
Izotov , Y. I., Noeske , K. G., Guseva , N. G., et al. 2004, , 415, L27
2004
-
[74]
H., Cohen , M., Masci , F., et al
Jarrett , T. H., Cohen , M., Masci , F., et al. 2011, , 735, 112
2011
-
[75]
& Yan , R
Ji , X. & Yan , R. 2020, , 499, 5749
2020
-
[76]
M., & Salim , S
Juneau , S., Dickinson , M., Alexander , D. M., & Salim , S. 2011, , 736, 104
2011
-
[77]
2013, , 764, 176
Juneau , S., Dickinson , M., Bournaud , F., et al. 2013, , 764, 176
2013
-
[78]
M., Tremonti , C., et al
Kauffmann , G., Heckman , T. M., Tremonti , C., et al. 2003, , 346, 1055
2003
-
[79]
J., Groves , B., Kauffmann , G., & Heckman , T
Kewley , L. J., Groves , B., Kauffmann , G., & Heckman , T. 2006, , 372, 961
2006
-
[80]
J., Heisler , C
Kewley , L. J., Heisler , C. A., Dopita , M. A., & Lumsden , S. 2001, , 132, 37
2001
-
[81]
M., Dunkley , J., et al
Komatsu , E., Smith , K. M., Dunkley , J., et al. 2011, , 192, 18
2011
-
[82]
& Ho , L
Kormendy , J. & Ho , L. C. 2013, , 51, 511
2013
-
[83]
E., Sajina , A., et al
Lacy , M., Ridgway , S. E., Sajina , A., et al. 2015, , 802, 102
2015
-
[84]
J., Sajina , A., et al
Lacy , M., Storrie-Lombardi , L. J., Sajina , A., et al. 2004, , 154, 166
2004
-
[85]
W., & Mykytyn , D
Lang , D., Hogg , D. W., & Mykytyn , D. 2016, The Tractor: Probabilistic astronomical source detection and measurement , Astrophysics Source Code Library, record ascl:1604.008
2016
-
[86]
D., Alexander , D
Lehmer , B. D., Alexander , D. M., Bauer , F. E., et al. 2010, , 724, 559
2010
-
[87]
D., et al
Leitherer , C., Schaerer , D., Goldader , J. D., et al. 1999, , 123, 3
1999
-
[88]
2013, arXiv e-prints, arXiv:1308.0847
Levi , M., Bebek , C., Beers , T., et al. 2013, arXiv e-prints, arXiv:1308.0847
2013 arXiv
-
[89]
M., et al
Mainzer , A., Bauer , J., Cutri , R. M., et al. 2014, , 792, 30
2014
-
[90]
2020, The Messenger, 180, 24
Maiolino , R., Cirasuolo , M., Afonso , J., et al. 2020, The Messenger, 180, 24
2020
-
[91]
2018, , 620, A50
Ma ek , K., Buat , V., Roehlly , Y., et al. 2018, , 620, A50
2018
-
[92]
2005, , 362, 799
Maraston , C. 2005, , 362, 799
2005
-
[93]
W., Banerji , M., Maiolino , R., & Bowler , R
Marshall , A., Auger-Williams , M. W., Banerji , M., Maiolino , R., & Bowler , R. 2022, , 515, 5617
2022
-
[94]
2024, arXiv e-prints, arXiv:2402.00109
Mazzolari , G., Gilli , R., Brusa , M., et al. 2024, arXiv e-prints, arXiv:2402.00109
2024 arXiv
-
[95]
M., Lang , D., Schlafly , E
Meisner , A. M., Lang , D., Schlafly , E. F., & Schlegel , D. J. 2021, Research Notes of the American Astronomical Society, 5, 168
2021
-
[96]
2021, Nature Reviews Physics, 3, 712
Melchior , P., Joseph , R., Sanchez , J., MacCrann , N., & Gruen , D. 2021, Nature Reviews Physics, 3, 712
2021
-
[97]
A., Banerji , M., et al
Merloni , A., Alexander , D. A., Banerji , M., et al. 2019, The Messenger, 175, 42
2019
-
[98]
2024, , 682, A34
Merloni , A., Lamer , G., Liu , T., et al. 2024, , 682, A34
2024
-
[99]
2018, , 478, 2576
Mezcua , M., Civano , F., Marchesi , S., et al. 2018, , 478, 2576
2018
-
[100]
& Dom \' nguez S \'a nchez , H
Mezcua , M. & Dom \' nguez S \'a nchez , H. 2024, , 528, 5252
2024
-
[101]
2024, , 966, L30
Mezcua , M., Pacucci , F., Suh , H., Siudek , M., & Natarajan , P. 2024, , 966, L30
2024
-
[102]
2023, , 943, L5
Mezcua , M., Siudek , M., Suh , H., et al. 2023, , 943, L5
2023
-
[103]
2019, , 488, 685
Mezcua , M., Suh , H., & Civano , F. 2019, , 488, 685
2019
-
[104]
N., Doel , P., Gutierrez , G., et al
Miller , T. N., Doel , P., Gutierrez , G., et al. 2023, arXiv e-prints, arXiv:2306.06310
2023 arXiv
-
[105]
2021 a , , 653, A70
Mountrichas , G., Buat , V., Georgantopoulos , I., et al. 2021 a , , 653, A70
2021
-
[106]
2021 b , , 646, A29
Mountrichas , G., Buat , V., Yang , G., et al. 2021 b , , 646, A29
2021
-
[107]
2023, FastSpecFit: Fast spectral synthesis and emission-line fitting of DESI spectra , Astrophysics Source Code Library, record ascl:2308.005
Moustakas , J., Scholte , D., Dey , B., & Khederlarian , A. 2023, FastSpecFit: Fast spectral synthesis and emission-line fitting of DESI spectra , Astrophysics Source Code Library, record ascl:2308.005
2023
-
[108]
M., S \'a nchez , F
Negus , J., Comerford , J. M., S \'a nchez , F. M., et al. 2023, , 945, 127
2023
-
[109]
Oke , J. B. & Gunn , J. E. 1983, , 266, 713
1983
-
[110]
& Salim , S
Osborne , C. & Salim , S. 2024, , 962, 59
2024
-
[111]
2016, , 24, 13
Padovani , P. 2016, , 24, 13
2016
-
[112]
R., & Moustakas , J
Pai , A., Blanton , M. R., & Moustakas , J. 2024, arXiv e-prints, arXiv:2407.05508
2024 arXiv
-
[113]
S., Kannappan , S
Polimera , M. S., Kannappan , S. J., Richardson , C. T., et al. 2022, , 931, 44
2022
-
[114]
2024, , 168, 245
Poppett , C., Tyas , L., Aguilar , J., et al. 2024, , 168, 245
2024
-
[115]
M., Robotham , A
Prathap , J., Hopkins , A. M., Robotham , A. S. G., et al. 2024, arXiv e-prints, arXiv:2402.11817
2024
-
[116]
2025, , 982, 10
Pucha , R., Juneau , S., Dey , A., et al. 2025, , 982, 10
2025
-
[117]
A., et al
Raichoor , A., Moustakas , J., Newman , J. A., et al. 2023, , 165, 126
2023
-
[118]
A., Dopita , M
Rich , J. A., Dopita , M. A., Kewley , L. J., & Rupke , D. S. N. 2010, , 721, 505
2010
-
[119]
C., Janowiecki , S., et al
Salim , S., Lee , J. C., Janowiecki , S., et al. 2016, , 227, 2
2016
-
[120]
Salpeter , E. E. 1955, , 121, 161
1955
-
[121]
C., Schawinski , K., et al
Sarzi , M., Shields , J. C., Schawinski , K., et al. 2010, , 402, 2187
2010
-
[122]
2007, , 382, 1415
Schawinski , K., Thomas , D., Sarzi , M., et al. 2007, , 382, 1415
2007
-
[123]
F., Kirkby , D., Schlegel , D
Schlafly , E. F., Kirkby , D., Schlegel , D. J., et al. 2023, , 166, 259
2023
-
[124]
W., Hardcastle , M
Shimwell , T. W., Hardcastle , M. J., Tasse , C., et al. 2022, , 659, A1
2022
-
[125]
2022, arXiv e-prints, arXiv:2211.11792
Siudek , M., Lisiecki , K., Mezcua , M., et al. 2022, arXiv e-prints, arXiv:2211.11792
2022 arXiv
-
[126]
2018 a , arXiv e-prints, arXiv:1805.09905
Siudek , M., Ma ek , K., Pollo , A., et al. 2018 a , arXiv e-prints, arXiv:1805.09905
2018 arXiv
-
[127]
2018 b , , 617, A70
Siudek , M., Ma ek , K., Pollo , A., et al. 2018 b , , 617, A70
2018
-
[128]
2017, , 597, A107
Siudek , M., Ma ek , K., Scodeggio , M., et al. 2017, , 597, A107
2017
-
[129]
2024, , 691, A308
Siudek , M., Pucha , R., Mezcua , M., et al. 2024, , 691, A308
2024
-
[130]
Stalevski , M., Fritz , J., Baes , M., Nakos , T., & Popovi \'c , L. C . 2012, , 420, 2756
2012
-
[131]
2016, , 458, 2288
Stalevski , M., Ricci , C., Ueda , Y., et al. 2016, , 458, 2288
2016
-
[132]
Stasi \'n ska , G., Cid Fernandes , R., Mateus , A., Sodr \'e , L., & Asari , N. V. 2006, , 371, 972
2006
-
[133]
J., Benford , D
Stern , D., Assef , R. J., Benford , D. J., et al. 2012, , 753, 30
2012
-
[134]
2005, , 631, 163
Stern , D., Eisenhardt , P., Gorjian , V., et al. 2005, , 631, 163
2005
-
[135]
2016, , 24, 10
Tadhunter , C. 2016, , 24, 10
2016
-
[136]
E., Robotham , A
Thorne , J. E., Robotham , A. S. G., Davies , L. J. M., et al. 2022, , 509, 4940
2022
-
[137]
J., & Tremonti , C
Trouille , L., Barger , A. J., & Tremonti , C. 2011, , 742, 46
2011
-
[138]
Truebenbach , A. E. & Darling , J. 2017, , 468, 196
2017
-
[139]
A., Coriat , M., Traulsen , I., et al
Webb , N. A., Coriat , M., Traulsen , I., et al. 2020, , 641, A136
2020
-
[140]
E., van Dokkum , P
Whitaker , K. E., van Dokkum , P. G., Brammer , G., & Franx , M. 2012, , 754, L29
2012
-
[141]
L., Eisenhardt , P
Wright , E. L., Eisenhardt , P. R. M., Mainzer , A. K., et al. 2010, , 140, 1868
2010
-
[142]
L., Greene , J
Wylezalek , D., Zakamska , N. L., Greene , J. E., et al. 2018, , 474, 1499
2018
-
[143]
2020, , 491, 740
Yang , G., Boquien , M., Buat , V., et al. 2020, , 491, 740
2020
-
[144]
I., Papovich , C., et al
Yang , G., Caputi , K. I., Papovich , C., et al. 2023, , 950, L5
2023
-
[145]
G., Adelman , J., Anderson , John E., J., et al
York , D. G., Adelman , J., Anderson , John E., J., et al. 2000, , 120, 1579
2000
-
[146]
A., et al
Zhou , R., Dey , B., Newman , J. A., et al. 2023, , 165, 58
2023
-
[147]
2017, , 129, 064101
Zou , H., Zhou , X., Fan , X., et al. 2017, , 129, 064101
2017
-
[148]
, " * write output.state after.block = add.period write newline
ENTRY address archiveprefix author booktitle chapter edition editor howpublished institution eprint journal key month note number organization pages publisher school series title type volume year label extra.label sort.label short.list INTEGERS output.state before.all mid.sent...
-
[149]
write newline
" write newline "" before.all 'output.state := FUNCTION n.dashify 't := "" t empty not t #1 #1 substring "-" = t #1 #2 substring "--" = not "--" * t #2 global.max substring 't := t #1 #1 substring "-" = "-" * t #2 global.max substring 't := while if t #1 #1 substring * t #2 gl...
Reviewed August 7, 2026 · model on record in the stance chip above.
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