REVIEW 4 major objections 4 minor 63 references
Identifying Compton-thick AGNs with Machine learning algorithm in Chandra Deep Field-South
T0 review · 4 major / 4 minor · reviewed 2026-08-07 · deepseek-v4-flash
Pith's one-line read A Random Forest classifier trained on 210 secure AGNs identifies 67 Compton-thick AGNs in the Chandra Deep Field-South, 64 of them new, raising the field's CT fraction from about 11% to about 20%.
desk verdict Useful candidate list, but the central 'identification' claim is an extrapolation that isn't validated; reframe and it's a solid contribution. 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 a Random Forest ensemble, an algorithm that averages many decision trees whose node splits use Gini impurity. Its four inputs are quantities that track X-ray absorption: hardness ratio, redshift, rest-frame 6 µm luminosity, and the ratio of 6 µm to 2–10 keV luminosity. The last is the dominant discriminator, contributing 58% of the feature-importance score, with 6 µm luminosity at 22%, hardness ratio at 15%, and redshift at 5%. The purity-selection step is a separate mechanism: the classifier's output probability for secure non-CT-AGNs is fit to a Beta distribution, and the 99.7% right-tail critical value, 0.664, is chosen as the threshold for accepting a candidate as a 'pure' CT-AGN. That threshold is what converts a 90%-accurate classifier into a conservative candidate list meant to contain almost no false positives.
What would settle it
Take the 67 flagged sources and measure their column densities directly from stacked Chandra spectra or NuSTAR observations; if most have $N_{\mathrm{H}} < 1.5 \times 10^{24}\,\mathrm{cm}^{-2}$, the central claim of 64 new Compton-thick AGNs collapses.
Extended reading notes
Core claim
The paper's central claim is that a large population of Compton-thick AGNs hides among low-luminosity, low-count AGNs in the deepest Chandra field, and that a machine-learning classifier can pull them out. A Random Forest trained on 210 AGNs with secure classifications (62 CT, 148 non-CT) using four inputs—hardness ratio, redshift, 6 µm luminosity, and the 6 µm-to-2–10 keV luminosity ratio—reaches 90% accuracy, 80% precision, and 89% recall on a held-out test set. Applied to 254 AGNs whose classifications are insecure, and filtered with a high-purity probability threshold of 0.664 (the 99.7% right-tail critical value of a Beta distribution fit to the non-CT probabilities), the model identifies 67 CT-AGNs, three of them already known and 64 new. The paper then counts 146 CT-AGNs among the 728 AGNs in CDFS, a fraction of about 20%, and reports that CT-AGN host galaxies have higher star formation rates than non-CT-AGN hosts (median log SFR 1.19 versus 0.95; KS p-value $5.2 \times 10^{-3}$), while stellar mass distributions are statistically indistinguishable.
Load-bearing premise
The one untested load-bearing premise is that the decision boundary learned from bright, securely classified AGNs transfers unchanged to the 254 faint, low-count AGNs, even though the paper does not validate the classifier on that application sample.
Editorial extensions
If this is right
- The CDFS CT-AGN census grows from 79 to 146 objects, raising the fraction from about 11% to about 20% of the 728 AGNs in the field.
- At least 64 previously unknown CT-AGNs lie among faint, low-luminosity sources, so surveys that treat low-count X-ray sources as unobscured or non-AGN will systematically miss a large obscured population.
- The mid-infrared-to-X-ray luminosity ratio is the strongest predictor, which means multiwavelength photometry can preselect CT-AGN candidates for expensive X-ray follow-up.
- The host galaxies of the CT-AGNs show higher star formation rates than non-CT-AGN hosts, in line with a picture where heavy obscuration accompanies active star formation.
Reading between the lines
- The paper's 0.664 threshold is deliberately conservative: 126 of the 254 faint AGNs have probability above 0.5, so on the model's own output the true hidden CT population may be larger than the 67 reported; this is my inference, not the paper's claim.
- Because the classifier leans on the MIR-to-X-ray ratio, the 67 identifications are effectively photometric obscuration indicators rather than direct column-density measurements; direct X-ray spectroscopy or NuSTAR observations of the candidates would be the clean confirmation.
- The same trained classifier could be applied to other deep fields, such as CDF-N or COSMOS, to test whether the CT-AGN deficit relative to CXB models is a general property of deep X-ray surveys.
- The reported star-formation enhancement could partly reflect selection effects between the bright training set and the faint application set; a control sample matched in redshift, stellar mass, and X-ray luminosity would isolate the physical signal.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper trains a Random Forest classifier on 210 securely classified AGNs in the Chandra Deep Field-South using four features (redshift, hardness ratio, 6 micron luminosity, and the MIR-to-X-ray luminosity ratio), reports a test-set accuracy of 90% and an OOB score of 0.87, and then applies the classifier to 254 low-luminosity AGNs with insecure classifications. Setting a probability threshold of 0.664 chosen from a Beta-distribution fit to the secure sample, the authors classify 67 sources as pure CT-AGNs, three of them previously known, and claim 64 newly identified CT-AGNs. They further use the resulting sample to argue that the CT-AGN fraction in CDFS rises to about 20% and that CT-AGN host galaxies have higher star formation rates than non-CT-AGN hosts.
Significance. If the 64 new classifications were validated, this would be a valuable demonstration of a machine-learning approach to recovering a missing obscured-AGN population in deep X-ray surveys, with implications for the cosmic X-ray background and host-galaxy evolution. The paper uses public CDFS data, states its feature definitions clearly, and provides a machine-readable catalog with probabilistic classifications, which is a useful community resource. However, the central identification claim currently rests on an unvalidated extrapolation of a classifier from bright, securely classified sources to faint, low-count sources, and no independent X-ray spectral confirmation is provided for any of the new candidates. The significance of the result therefore depends critically on whether that validation gap can be closed.
major comments (4)
- [Section 4.2 and Section 5.2] The central claim that 67 sources, 64 of them new, are 'successfully identified' as CT-AGNs is not supported by the evidence presented. The probability threshold of 0.664 is calibrated in Section 4.1 on the 210-source secure sample, and the reported 90% accuracy and OOB=0.87 are measured only on that same secure distribution. The 254 low-luminosity AGNs are, by construction in Section 2.4, the sources that fail all secure-classification criteria, so they are systematically fainter and noisier. No X-ray spectral fitting, NuSTAR observation, or any other independent diagnostic is presented for the 67 flagged sources, and no false-positive rate is estimated for this application sample. The phrase 'successfully identified' should be replaced by 'identified as candidates' unless the authors provide spectral confirmation for at least a subsample or otherwise validate the decision boundary on independent known CT-AGNs drawn from the low-luminosity regime.
- [Section 5.2] The reported total of 146 CT-AGNs double-counts the three previously known sources that appear among the 67 ML-selected objects. Since the authors state that '67 pure CT-AGNs... includes three already known CT-AGNs', the number of unique CT-AGNs is 79 + 67 - 3 = 143, corresponding to 143/728 = 19.6%, not 146/728 = 20.0%. Similarly, within the 464-source sample, the 62 known CT-AGNs plus 67 ML identifications with three overlapping sources give 126 unique CT-AGNs, which is 27.2%, not 27.8% as reported. These arithmetic discrepancies should be corrected, as they affect the paper's main quantitative conclusion about the CT-AGN fraction.
- [Section 4.2 versus Table 1] There is a direct inconsistency between the text and the catalog table. Section 4.2 states that XID 68, 414, and 575 'have been identified as CT-AGN, with NH > 10^24 cm-2', yet Table 1 lists XID 68 with Class-trad = 'non-CT-AGN' and Quality = 'Insecure'. If these sources were indeed known CT-AGNs, they should have satisfied criterion (2) in Section 2.4 and been included in the secure training sample rather than the low-luminosity application sample. This contradiction affects the count of 64 previously unknown CT-AGNs and must be resolved.
- [Section 5.3] The host-galaxy comparison uses the 67 ML-classified sources as CT-AGNs without independent confirmation. The reported KS-test result for SFR (p = 5.209e-3) therefore measures the separation between samples defined by the classifier, not by a verified physical classification. Because the dominant feature is the MIR-to-X-ray luminosity ratio (58% importance, Figure 5), and this ratio may correlate with star formation indicators through the 6 micron luminosity or SED decomposition, a classifier bias could produce the claimed SFR difference even if the true CT-AGN fraction among the candidates is lower. The authors should either confirm the labels for a subset or explicitly frame Section 5.3 as a comparison of ML-selected candidates conditional on the model.
minor comments (4)
- [Abstract and Section 6] The summary states that the algorithm 'successfully identified 67 new CT-AGNs', but Section 4.2 reports 67 total CT-AGNs including three previously known ones, with 64 new; the wording should be made consistent throughout.
- [Throughout] There are several typographical errors, including 'Institude' in the author affiliations and 'expections' in Section 5.2; these should be corrected.
- [Table 1] The table notes state that missing count errors correspond to 90% confidence upper limits, but the rows in the printed excerpt do not distinguish upper limits from actual measured values in a visually transparent way; a consistent notation such as arrows or '<' would improve usability.
- [Section 3.2] The KS-test is described as checking that the training and test sets come from the same distribution, but the paper does not report the actual p-values; giving them in a table or in the text would strengthen the reproducibility of the split.
Circularity Check
No circularity: the 67-source identification is an out-of-sample model prediction; the unsupported step is distribution extrapolation, not equivalence.
full rationale
The derivation chain is not circular. The Random Forest is trained on 210 securely classified AGNs and evaluated on a held-out 30% test split, giving an accuracy of 0.90; the 0.664 threshold is fixed from the Beta-fitted probability distribution of non-CT sources in that labeled secure sample, before being applied to the 254 low-luminosity AGNs. The 67 flagged sources are therefore out-of-sample predictions, not re-statements of the training labels or of the threshold-fitting data. The dominant feature, log(L6um/L2-10keV), is a known CT-AGN diagnostic, but using it as an input feature does not make the model output identical to that input; the secure labels come from X-ray spectral column densities and prior catalogs. Citations to the authors' own Guo et al. (2020, 2021) work supply SED luminosities and some secure classifications, but these are external published measurements used as inputs, not conclusions imported to force the result. The main weakness, unvalidated extrapolation from bright, high-count sources to faint, low-count sources, is a generalization and calibration risk rather than a circularity. A separate bookkeeping issue is that the total of 146 CT-AGNs double-counts the three known sources contained in the 67, but this is an arithmetic error, not circular reasoning.
Assumptions & free parameters
free parameters (2)
- Probability threshold for CT-AGN classification =
0.664
- Random Forest hyperparameters =
n_estimators=25, max_depth=6, min_samples_leaf=6, min_samples_split=5, max_leaf_nodes=8
assumptions (5)
- domain assumption The 210 secure classifications used for training are correct.
- domain assumption The training sample is representative of the application sample.
- domain assumption The MIR-to-X-ray luminosity ratio is a valid proxy for Compton-thick absorption.
- domain assumption Classifier probabilities follow a Beta distribution.
- standard math Random Forest is a valid classifier for this task.
Cite this review
Pith. "Pith review of Identifying Compton-thick AGNs with Machine learning algorithm in Chandra Deep Field-South." pith.science (2026). https://pith.science/paper/6KRCCBTZ
@misc{pith2026250521105,
author = {Pith},
title = {Pith review of: Identifying Compton-thick AGNs with Machine learning algorithm in Chandra Deep Field-South},
year = {2026},
howpublished = {\url{https://pith.science/paper/6KRCCBTZ}},
note = {Machine review of arXiv:2505.21105}
}
abstract
Compton-thick active galactic nuclei (CT-AGNs), which are defined by column density $\mathrm{N_H} \geqslant 1.5 \times 10^{24} \ \mathrm{cm}^{-2}$, emit feeble X-ray radiation, even undetectable by X-ray instruments. Despite this, the X-ray emissions from CT-AGNs are believed to be a substantial contributor to the cosmic X-ray background (CXB). According to synthesis models of AGNs, CT-AGNs are expected to make up a significant fraction of the AGN population, likely around 30% or more. However, only $\sim$11% of AGNs have been identified as CT-AGNs in the Chandra Deep Field-South (CDFS). To identify hitherto unknown CT-AGNs in the field, we used a Random Forest algorithm for identifying them. First, we build a secure classified subset of 210 AGNs to train and evaluate our algorithm. Our algorithm achieved an accuracy rate of 90% on the test set after training. Then, we applied our algorithm to an additional subset of 254 AGNs, successfully identifying 67 CT-AGNs within this group. This result significantly increased the fraction of CT-AGNs in the CDFS, which is closer to the theoretical predictions of the CXB. Finally, we compared the properties of host galaxies between CT-AGNs and non-CT-AGNs and found that the host galaxies of CT-AGNs exhibit higher levels of star formation activity.
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Works this paper leans on
-
[1]
, " * write output.state after.block = add.period write newline
ENTRY address archivePrefix author booktitle chapter doi edition editor eprint howpublished institution journal key month number organization pages publisher school series title misctitle type volume year version url label extra.label sort.label short.list INTEGERS output.state before.all mid.sentence after.sentence after.block FUNCTION init.state.consts ...
-
[2]
write newline
" write newline "" before.all 'output.state := FUNCTION format.url url empty "" new.block "" url * "" * if FUNCTION format.eprint eprint empty "" archivePrefix empty "" archivePrefix "arXiv" = new.block " " eprint * " " * new.block " " eprint * " " * if if if FUNCTION format.doi doi empty "" " " doi * " " * if FUNCTION format.pid doi empty eprint empty ur...
-
[4]
2008, , 689, 666, 10.1086/592595
Ajello , M., Greiner , J., Sato , G., et al. 2008, , 689, 666, 10.1086/592595
doi:10.1086/592595 2008
-
[5]
Ananna , T. T., Treister , E., Urry , C. M., et al. 2019, , 871, 240, 10.3847/1538-4357/aafb77
-
[6]
1993, , 31, 473, 10.1146/annurev.aa.31.090193.002353
Antonucci , R. 1993, , 31, 473, 10.1146/annurev.aa.31.090193.002353
arXiv 1993
-
[7]
Astropy Collaboration , Robitaille , T. P., Tollerud , E. J., et al. 2013, , 558, A33, 10.1051/0004-6361/201322068
-
[8]
Astropy Collaboration , Price-Whelan , A. M., Sip o cz , B. M., et al. 2018, , 156, 123, 10.3847/1538-3881/aabc4f
-
[9]
Bower , R. G., Benson , A. J., Malbon , R., et al. 2006, , 370, 645, 10.1111/j.1365-2966.2006.10519.x
arXiv 2006
Show all 63 references
-
[10]
2001, Machine Learning, 45, 5, 10.1023/A:1010933404324
Breiman , L. 2001, Machine Learning, 45, 5, 10.1023/A:1010933404324
2001 doi
-
[11]
2015, , 802, 89, 10.1088/0004-637X/802/2/89
Buchner , J., Georgakakis , A., Nandra , K., et al. 2015, , 802, 89, 10.1088/0004-637X/802/2/89
2015 doi
-
[12]
2011, , 728, 58, 10.1088/0004-637X/728/1/58
Burlon , D., Ajello , M., Greiner , J., et al. 2011, , 728, 58, 10.1088/0004-637X/728/1/58
2011 doi
-
[13]
2006, , 446, 459, 10.1051/0004-6361:20053893
Cappi , M., Panessa , F., Bassani , L., et al. 2006, , 446, 459, 10.1051/0004-6361:20053893
2006 doi
-
[14]
L., & Walter , F
Carilli , C. L., & Walter , F. 2013, , 51, 105, 10.1146/annurev-astro-082812-140953
2013 doi
-
[15]
2004, Compton Thick AGN: the dark side of the X-ray background (Springer Netherlands), 245--272
Comastri, A. 2004, Compton Thick AGN: the dark side of the X-ray background (Springer Netherlands), 245--272
2004
-
[16]
2019, , 629, A133, 10.1051/0004-6361/201833799
Corral , A., Georgantopoulos , I., Akylas , A., & Ranalli , P. 2019, , 629, A133, 10.1051/0004-6361/201833799
2019 doi
-
[17]
N., et al
Ding , N., Luo , B., Brandt , W. N., et al. 2018, , 868, 88, 10.3847/1538-4357/aaea60
2018 doi
-
[18]
2000, , 539, L9, 10.1086/312838
Ferrarese , L., & Merritt , D. 2000, , 539, L9, 10.1086/312838
2000 doi
-
[19]
2010, , 519, A92, 10.1051/0004-6361/201014039
Gilli , R., Vignali , C., Mignoli , M., et al. 2010, , 519, A92, 10.1051/0004-6361/201014039
2010 doi
-
[20]
2022, , 666, A17, 10.1051/0004-6361/202243708
Gilli , R., Norman , C., Calura , F., et al. 2022, , 666, A17, 10.1051/0004-6361/202243708
2022 doi
-
[21]
D., Alexander , D
Goulding , A. D., Alexander , D. M., Bauer , F. E., et al. 2012, , 755, 5, 10.1088/0004-637X/755/1/5
2012 doi
-
[22]
2020, , 492, 1887, 10.1093/mnras/stz3589
Guo , X., Gu , Q., Ding , N., Contini , E., & Chen , Y. 2020, , 492, 1887, 10.1093/mnras/stz3589
2020 doi
-
[23]
2021, , 908, 169, 10.3847/1538-4357/abd0f5
Guo , X., Gu , Q., Ding , N., Yu , X., & Chen , Y. 2021, , 908, 169, 10.3847/1538-4357/abd0f5
2021 doi
-
[24]
2023, , 135, 014102, 10.1088/1538-3873/acb294
Guo , X., Gu , Q., Xu , J., et al. 2023, , 135, 014102, 10.1088/1538-3873/acb294
2023 doi
-
[25]
1991, , 380, L51, 10.1086/186171
Haardt , F., & Maraschi , L. 1991, , 380, L51, 10.1086/186171
1991 doi
-
[26]
A., Craig , W
Harrison , F. A., Craig , W. W., Christensen , F. E., et al. 2013, , 770, 103, 10.1088/0004-637X/770/2/103
2013 doi
-
[27]
F., Hernquist , L., Cox , T
Hopkins , P. F., Hernquist , L., Cox , T. J., et al. 2006, , 163, 1, 10.1086/499298
2006 doi
-
[28]
Hunter , J. D. 2007, Computing in Science and Engineering, 9, 90, 10.1109/MCSE.2007.55
2007 doi
-
[29]
S., Miller , J
Kammoun , E. S., Miller , J. M., Zoghbi , A., et al. 2019, , 877, 102, 10.3847/1538-4357/ab1c5f
2019 doi
-
[30]
Karson, M., Chakravarti, I., Laha, R., & Roy, J. 1968, J. Am. Stat. Assoc., 63, 1047
1968
- [31]
-
[32]
D., Brightman , M., Nandra , K., et al
Kocevski , D. D., Brightman , M., Nandra , K., et al. 2015, , 814, 104, 10.1088/0004-637X/814/2/104
2015 doi
-
[33]
Kormendy , J., & Ho , L. C. 2013, , 51, 511, 10.1146/annurev-astro-082708-101811
2013 doi
-
[34]
M., Vignali , C., Lanzuisi , G., Gruppioni , C., & Pozzi , F
La Caria , M. M., Vignali , C., Lanzuisi , G., Gruppioni , C., & Pozzi , F. 2019, , 487, 1662, 10.1093/mnras/stz1381
2019 doi
-
[35]
M., Yaqoob , T., Boorman , P
LaMassa , S. M., Yaqoob , T., Boorman , P. G., et al. 2019, , 887, 173, 10.3847/1538-4357/ab552c
2019 doi
-
[36]
L., Chiaberge , M., Heckman , T., et al
Lambrides , E. L., Chiaberge , M., Heckman , T., et al. 2020, , 897, 160, 10.3847/1538-4357/ab919c
2020 doi
-
[37]
B., Gandhi , P., Alexander , D
Lansbury , G. B., Gandhi , P., Alexander , D. M., et al. 2015, , 809, 115, 10.1088/0004-637X/809/2/115
2015 doi
-
[38]
B., Alexander , D
Lansbury , G. B., Alexander , D. M., Aird , J., et al. 2017, , 846, 20, 10.3847/1538-4357/aa8176
2017 doi
-
[39]
2015 a , , 573, A137, 10.1051/0004-6361/201424924
Lanzuisi , G., Ranalli , P., Georgantopoulos , I., et al. 2015 a , , 573, A137, 10.1051/0004-6361/201424924
2015 doi
-
[40]
2015 b , , 578, A120, 10.1051/0004-6361/201526036
Lanzuisi , G., Perna , M., Delvecchio , I., et al. 2015 b , , 578, A120, 10.1051/0004-6361/201526036
2015 doi
-
[41]
2018, , 480, 2578, 10.1093/mnras/sty2025
Lanzuisi , G., Civano , F., Marchesi , S., et al. 2018, , 480, 2578, 10.1093/mnras/sty2025
2018 doi
-
[42]
2023, Experimental Astronomy, 56, 141, 10.1007/s10686-023-09896-7
Li , H., Walter , R., Produit , N., & Hubert , F. 2023, Experimental Astronomy, 56, 141, 10.1007/s10686-023-09896-7
2023 doi
-
[43]
2019, , 877, 5, 10.3847/1538-4357/ab184b
Li , J., Xue , Y., Sun , M., et al. 2019, , 877, 5, 10.3847/1538-4357/ab184b
2019 doi
-
[44]
Liang , E. P. T. 1979, , 234, 1105, 10.1086/157594
1979 doi
-
[45]
2017, , 232, 8, 10.3847/1538-4365/aa7847
Liu , T., Tozzi , P., Wang , J.-X., et al. 2017, , 232, 8, 10.3847/1538-4365/aa7847
2017 doi
-
[46]
N., Xue , Y
Luo , B., Brandt , W. N., Xue , Y. Q., et al. 2017, , 228, 2, 10.3847/1538-4365/228/1/2
2017 doi
-
[47]
1998, , 338, 781
Maiolino , R., Salvati , M., Bassani , L., et al. 1998, , 338, 781. astro-ph/9806055
1998 arXiv
-
[48]
2016, , 817, 34, 10.3847/0004-637X/817/1/34
Marchesi , S., Civano , F., Elvis , M., et al. 2016, , 817, 34, 10.3847/0004-637X/817/1/34
2016 doi
-
[49]
2022, , 935, 114, 10.3847/1538-4357/ac80be
Marchesi , S., Zhao , X., Torres-Alb \`a , N., et al. 2022, , 935, 114, 10.3847/1538-4357/ac80be
2022 doi
-
[50]
2018, , 235, 17, 10.3847/1538-4365/aaa83d
Masini , A., Civano , F., Comastri , A., et al. 2018, , 235, 17, 10.3847/1538-4365/aaa83d
2018 doi
-
[51]
2003, , 588, 696, 10.1086/374335
Moretti , A., Campana , S., Lazzati , D., & Tagliaferri , G. 2003, , 588, 696, 10.1086/374335
2003 doi
-
[52]
2015, , 53, 365, 10.1146/annurev-astro-082214-122302
Netzer , H. 2015, , 53, 365, 10.1146/annurev-astro-082214-122302
2015 doi
- [53]
-
[54]
2020, , 641, A6, 10.1051/0004-6361/201833910
Planck Collaboration , Aghanim , N., Akrami , Y., et al. 2020, , 641, A6, 10.1051/0004-6361/201833910
2020 doi
-
[55]
E., Treister , E., et al
Ricci , C., Bauer , F. E., Treister , E., et al. 2017, , 468, 1273, 10.1093/mnras/stx173
2017 doi
- [56]
-
[57]
2023, , 675, A65, 10.1051/0004-6361/202345980
Silver , R., Torres-Alb \`a , N., Zhao , X., et al. 2023, , 675, A65, 10.1051/0004-6361/202345980
2023 doi
-
[58]
2022, , 940, 148, 10.3847/1538-4357/ac9bf8
Silver , R., Torres-Alb\`a , N., Zhao , X., et al. 2022, , 940, 148, 10.3847/1538-4357/ac9bf8
2022 doi
-
[59]
2020, , 888, 8, 10.3847/1538-4357/ab5718
Toba , Y., Yamada , S., Ueda , Y., et al. 2020, , 888, 8, 10.3847/1538-4357/ab5718
2020 doi
-
[60]
2021, , 922, 252, 10.3847/1538-4357/ac1c73
Torres-Alb \`a , N., Marchesi , S., Zhao , X., et al. 2021, , 922, 252, 10.3847/1538-4357/ac1c73
2021 doi
-
[61]
Ueda , Y., Akiyama , M., Hasinger , G., Miyaji , T., & Watson , M. G. 2014, , 786, 104, 10.1088/0004-637X/786/2/104
2014 doi
- [62]
-
[63]
2022, , 941, 97, 10.3847/1538-4357/ac9c07
Vijarnwannaluk , B., Akiyama , M., Schramm , M., et al. 2022, , 941, 97, 10.3847/1538-4357/ac9c07
2022 doi
-
[64]
A., Fabian , A
Worsley , M. A., Fabian , A. C., Bauer , F. E., et al. 2005, , 357, 1281, 10.1111/j.1365-2966.2005.08731.x
2005
Reviewed August 7, 2026 · model on record in the stance chip above.
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