REVIEW 4 major objections 5 minor 55 references
Classifying Quasar Types Without a Spectrum
T0 review · 4 major / 5 minor · reviewed 2026-08-16 · deepseek-v4-flash
Pith's one-line read The shape of a quasar's brightness-variability curve carries enough information to separate Type 1 from Type 2 quasars without a spectrum, with 99% and 87% recovery in this sample.
desk verdict A genuinely new photometric Type 1/Type 2 quasar classifier with public code, but the headline 99/87% recovery rates are in-sample and confounded by different light curve quality between the two classes. 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 central object is the Slepian Wavelet Variance curve, a scale-by-scale estimate of a light curve's variance built from Slepian wavelets, which are data-adaptive bandpass filters derived from prolate spheroidal wave functions. Its key property is that it works on irregularly sampled time series, which is what ground-based surveys produce. The classification machinery then treats each curve as a point in a high-dimensional space: curves are interpolated to 50 spline points, standardized by subtracting their median, compared with absolute Pearson correlation distances, and clustered with agglomerative hierarchical clustering using complete linkage. A final slope criterion between the first and last spline points, with a threshold at $-0.225$, assigns the ambiguous cluster to Type 1 or Type 2 behavior.
What would settle it
Run the identical clustering on spectroscopically confirmed Type 1 and Type 2 quasars whose ZTF light curves are matched for number of observations, baseline, and sky region; if the recovery rates collapse toward chance, the variance-curve difference is an artifact of sampling density rather than quasar type.
Extended reading notes
Core claim
The paper's central discovery is that Type 1 and Type 2 quasars have distinct Slepian Wavelet Variance signatures in ZTF light curves: Type 1 curves typically fall to a minimum near about 10 days in the rest frame and then rise again at longer timescales, while Type 2 curves decline nearly monotonically, with most power at the shortest scales. The authors show that agglomerative hierarchical clustering of the variance curves, using absolute Pearson distances and complete linkage, groups most quasars correctly, and that a single slope cut at $-0.225$ cleanly separates the remaining mixed cluster. The final two-cluster split recovers 513 of 516 Type 1 quasars (99%) and 207 of 238 Type 2 quasars (87%). The few objects that land on the wrong side of the split show variability behavior opposite to their spectroscopic type, and the authors interpret these as candidates for changing-look or spectroscopically atypical quasars rather than as failures of the method.
Load-bearing premise
The separation between Type 1 and Type 2 variance curves reflects the quasars' intrinsic variability, not the far richer light-curve sampling and different sky coverage of the Type 1 sample.
Editorial extensions
If this is right
- If the result generalizes, quasar Type 1/Type 2 labels can be assigned or pre-screened from variability alone, reserving spectroscopy for confirmation and for the small fraction of ambiguous objects.
- The method is model-independent: unlike structure functions or the Damped Random Walk, it does not assume a shape for the power spectrum, so it can be applied to any survey light curve with sufficient sampling.
- The variance-curve minimum near $2^3$-$2^4$ days in Type 1 quasars can serve as an observable diagnostic for the transition between inner-disk reprocessing and outer-disk thermal variability.
- The 1% of Type 1 and 13% of Type 2 quasars with opposite variability signatures form a self-selected sample of candidate changing-look or misclassified AGNs for targeted follow-up.
- With LSST's long light curves, the same decomposition should probe longer timescales and sharpen the physical interpretation.
Reading between the lines
- Because the Type 1 sample required at least 1500 good observations and the Type 2 sample only 300, and because the two samples occupy different sky regions with different baseline distributions, the cleanest test of the paper's claim is a matched-sample rerun: identical cadence, baseline, and sky coverage for both spectral types.
- The bimodal slope distribution with a clean break at $-0.225$ suggests that a single scalar summary of the variance curve may carry most of the classification signal; an independent test would compare clustering against a simple slope-only threshold applied to a fresh sample.
- The misclassified objects' spectra predate the ZTF light curves, so their apparent 'wrong' variability is consistent with spectral-type evolution over roughly a decade; monitoring those 34 objects now could catch a changing-look transition in progress.
- If the technique transfers to LSST, it could turn variability-based subtype screening into a population-scale tool for finding obscured or changing AGNs, but that depends on the matched-sample test being clean.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper applies Slepian Wavelet Variance (SWV) to ZTF light curves of 516 MILLIQUAS Type 1 and 238 Type 2 quasars, computes rest-frame variance curves at dyadic timescales, and uses agglomerative hierarchical clustering with a slope threshold to group curves into two classes. The authors report 99% recovery of Type 1 and 87% recovery of Type 2 labels, inspect the misclassified objects as possible changing-look or discrepant quasars, and interpret the curve shapes in terms of short- and long-term variability regimes. The paper argues that SWV is model-independent and complementary to structure functions and the Damped Random Walk model.
Significance. If the classification result were validated out of sample, this would be a valuable, inexpensive way to separate quasar spectral types using photometry alone, with obvious application to large surveys such as LSST. The paper has real strengths: the code is public, the SWV methodology is described in detail, the authors are transparent about several known biases, and they inspect all 34 misclassified objects individually. The physical discussion of the variance-curve minimum as a possible transition between X-ray reprocessing and outer-disk thermal variability is interesting, though it is clearly interpretive. However, the load-bearing recovery numbers are computed on the same sample used to choose the slope threshold and the number of clusters, and the Type 1 and Type 2 samples differ substantially in data quality and sky coverage. The paper currently demonstrates an interesting association between variance-curve shape and spectral class, not a validated classifier.
major comments (4)
- [Section 5, Figs. 9-10] The slope threshold of -0.225 is chosen by inspecting the bimodal slope distribution of the same 754 objects whose recovery rates are then quoted, and the decision to truncate the dendrogram at 5 flat sub-clusters is also made on this sample. The reported 99% and 87% recovery rates are therefore training-set agreement, not predictive accuracy. Please add out-of-sample validation, such as k-fold or repeated holdout cross-validation, or an independent ZTF/MILLIQUAS test set, and report how sensitive the recovery rates are to the slope threshold.
- [Section 2, Figs. 3, 7, 11] The two classes are not drawn from comparable light-curve populations. Type 1 quasars are required to have at least 1500 good observations and are concentrated in one region of the ZTF footprint, while Type 2 quasars require at least 300 good observations and are spread over SDSS sky. Fig. 11 shows that their baseline distributions are not drawn from the same underlying distribution, and their redshift distributions also differ, with Type 2 quasars predominantly at z <= 0.9. Because SWV filters are data-dependent and the variance curve shape depends on cadence, noise floor, baseline, and rest-frame timescale coverage, the observed separation could reflect data quality rather than intrinsic quasar type. Please rerun the analysis with samples matched on n_goodobs, baseline, and sky footprint, or demonstrate that the classifier separates the classes within matched subsamples.
- [Section 6 and Fig. 4] The short-scale rise that distinguishes the Type 2 archetype is admitted to be partly due to photometric uncertainties, and the long-scale variance estimates at 2^8-2^10 days are admitted to be unstable and biased low. The classifier uses the full 50-point spline including these scales, so the reported separation may be amplified by known artifacts rather than intrinsic variability differences. Please quantify the effect by truncating the spline at unreliable scales and by adding simulated noise floors to archetypal curves, and report whether the 99% and 87% rates survive.
- [Section 5, Fig. 11] The sentence stating that the classification is 'not baseline-limited' addresses only the fact that all quasars have at least 1500 days of baseline and that the probed timescales fit within that baseline. It does not address the demonstrated difference in the baseline distributions or the difference in observing cadence between the two samples. This statement overstates what Fig. 11 establishes and should be revised to acknowledge the sampling confound.
minor comments (5)
- [Appendix A, condition 2] The normalization condition is written as the sum of squared filter coefficients equal to -2^{-j}/Delta; for real coefficients this cannot be satisfied, and the minus sign is presumably a typo. Please correct.
- [Section 5] The sentence 'This is a elegant reminder' should read 'This is an elegant reminder', and the conclusion contains a sentence fragment, 'With the help of agglomerative hierarchical clustering.'
- [Abstract and Conclusion] The statements that 99% of Type 1 quasars have a parabola shape and 87% of Type 2 quasars are monotonically decreasing should be explicitly framed as in-sample recovery rates for this sample, not as population-level statements.
- [Table 1 note] The note 'the few that have DESI DR1 spectra taken after 2018 are all confirm' is grammatically incomplete, and the claim that DESI spectra confirm the variability type would be much stronger if the number of such objects and the individual matches were specified.
- [Section 5] The term 'recovery rate' should be defined precisely in the text, since the clustering is unsupervised and the labels are only used for evaluation; as written, 'recovery' could be mistaken for the success rate of a deployed classifier.
Circularity Check
Slope threshold is selected in-sample and recovery rates are computed on the same 754 objects, making the headline 99%/87% performance a training-set description rather than an independent prediction.
-
fitted input called prediction
[Section 5, Figs. 9-10 (slope criterion and recovery rates)]
"the slope between the first and last points of the splines show a clear bimodality without overlap at the value −0.225 (see Fig. 9). Therefore, for the objects in Cluster 2, if a variance curve has an average slope below −0.225, we label it as a Type 2 and we keep it in Cluster 2. Otherwise, if the average slope value is above −0.225, we label it as a Type 1 and we move it to Cluster 1. ... We now obtain 544 quasars in Cluster 1 and 210 quasars in Cluster 2, with 513/516 Type 1 correctly recovered (99%) and 207/238 Type 2 correctly recovered (87%)."
The classification rule is not fully out-of-sample: the −0.225 slope cutoff is chosen by inspecting the slope distribution of the same 524 objects in Cluster 2 that are then relabeled and counted. The reported 99%/87% recovery rates are computed on the same 754 objects used to select this cutoff, so they quantify in-sample separation after a data-dependent threshold has been placed at the observed gap between the two types. No independent test set or cross-validation is presented, so the headline recovery rates are a training-set description rather than an independent prediction; the high rates are partly built into choosing the threshold on this exact sample.
full rationale
The variance curves themselves are computed from ZTF photometry and are not defined in terms of the MILLIQUAS spectral labels, so there is no self-definitional circularity: Type 1/Type 2 labels enter only as the external reference for evaluating the clustering. The agglomerative hierarchical clustering is unsupervised, and the self-citations to Graham et al. (2014) and Mondal & Percival (2012) are methodological provenance rather than load-bearing support for the specific Type 1 versus Type 2 claim, which is tested against an external spectroscopic catalogue. The one partially circular element is the slope criterion: the −0.225 threshold is selected after inspecting the slope distribution of the same sample whose recovery rates are then reported, so the 99%/87% figures are in-sample performance, not validated predictive accuracy. The additional concerns about differing n_goodobs thresholds and sky/baseline distributions are real threats to external validity, but they are confounds rather than circularity by construction. Overall, the central derivation is not equivalent to its inputs, but the headline performance metric is inflated by being measured on the training sample, warranting a partial circularity score of 4 rather than 0.
Assumptions & free parameters
free parameters (3)
- Slope threshold for Cluster 2 separation =
-0.225
- Number of flat clusters =
5
- Minimum good observations thresholds =
1500 (Type 1), 300 (Type 2)
assumptions (3)
- domain assumption Observation times are a realization of a stationary point process, and the sampling intervals are a portion of a stationary sequence of positive random variables.
- standard math The dyadic scale structure partitions the total variance cleanly across scales.
- domain assumption Rest-frame timescales are correctly computed from MILLIQUAS spectroscopic redshifts.
Cite this review
Pith. "Pith review of Classifying Quasar Types Without a Spectrum." pith.science (2026). https://pith.science/paper/T7W5LJPV
@misc{pith2026260811916,
author = {Pith},
title = {Pith review of: Classifying Quasar Types Without a Spectrum},
year = {2026},
howpublished = {\url{https://pith.science/paper/T7W5LJPV}},
note = {Machine review of arXiv:2608.11916}
}
read the original abstract
Distinguishing between Type 1 and Type 2 quasars is important because it helps us understand accretion regimes, black hole mass scaling, disk instabilities and feedback processes in active galaxies. Although spectroscopy provides robust classification, it does not scale well with the millions of quasars observed in modern surveys, as it requires substantial time and resources to acquire a good spectrum. On the photometry side, quasar light curves are always irregularly sampled and affected by the specifics of photometric surveys, making them difficult to analyze. In this work, we show that we can use irregularly sampled light curves from the Zwicky Transient Facility to classify quasar types without a spectrum, using Slepian Wavelet Variance. This technique allows us to decompose the variance of light curves into multiple timescales. We use agglomerative hierarchical clustering to classify 516 Type 1 and 238 Type 2 quasars from the MILLIQUAS catalogue, solely based on their wavelet variance curves. We obtain a recovery rate of 99% for Type 1 and 87% for Type 2 quasars, and the few misclassified quasars show the opposite variability behaviour to their spectral type. In contrast to structure functions and the Damped Random Walk model, Slepian Wavelet Variance offers a complementary, model-independent view of variability across short and long timescales.
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Works this paper leans on
-
[1]
Abbott, T. M. C., Adam´ ow, M., Aguena, M., et al. 2021, ApJS, 255, 20, doi: 10.3847/1538-4365/ac00b3
-
[2]
F., Argudo-Fern´ andez, M., et al
Almeida, A., Anderson, S. F., Argudo-Fern´ andez, M., et al. 2023, ApJS, 267, 44, doi: 10.3847/1538-4365/acda98
-
[3]
Antonucci, R. 1993, ARA&A, 31, 473, doi: 10.1146/annurev.aa.31.090193.002353 Ar´ evalo, P., Churazov, E., Lira, P., et al. 2024, A&A, 684, A133, doi: 10.1051/0004-6361/202347080 18H ´elias et al. Figure 13.The 3 MILLIQUAS Type 1 exhibiting Type 2 variability, out of 516 objects. Blue light curves are in theg-band, red light curves are in ther-band. Respec...
arXiv 1993
-
[4]
Baldwin, J. A., Phillips, M. M., & Terlevich, R. 1981, PASP, 93, 5, doi: 10.1086/130766
doi:10.1086/130766 1981
-
[5]
2019, ARA&A, 57, 467, doi: 10.1146/annurev-astro-081817-051948
Blandford, R., Meier, D., & Readhead, A. 2019, ARA&A, 57, 467, doi: 10.1146/annurev-astro-081817-051948
-
[6]
J., Shen, Y., Blaes, O., et al
Burke, C. J., Shen, Y., Blaes, O., et al. 2021, Science, 373, 789, doi: 10.1126/science.abg9933
-
[7]
2018, ApJ, 855, 117, doi: 10.3847/1538-4357/aab091
Cai, Z.-Y., Wang, J.-X., Zhu, F.-F., et al. 2018, ApJ, 855, 117, doi: 10.3847/1538-4357/aab091
-
[8]
2019, Nature Astronomy, 3, 251, doi: 10.1038/s41550-018-0659-x
Chelouche, D., Pozo Nu˜ nez, F., & Kaspi, S. 2019, Nature Astronomy, 3, 251, doi: 10.1038/s41550-018-0659-x
Show all 55 references
-
[9]
1964, Physics Today, 17, 21, doi: 10.1063/1.3051610
Chiu, H.-Y. 1964, Physics Today, 17, 21, doi: 10.1063/1.3051610
1964 doi
-
[10]
2011, ApJL, 727, L24, doi: 10.1088/2041-8205/727/1/L24
Dexter, J., & Agol, E. 2011, ApJL, 727, L24, doi: 10.1088/2041-8205/727/1/L24
2011 doi
-
[11]
W., & Rix, H.-W
El-Badry, K., Hogg, D. W., & Rix, H.-W. 2026, PASP, 138, 024102, doi: 10.1088/1538-3873/ae3f56 Classifying Quasar Types Without a Spectrum19 Figure 14.The 31 MILLIQUAS Type 2 exhibiting Type 1 variability, out of 238 objects. Blue light curves are in theg-band, red light curve...
2026 doi
-
[12]
S., Landau, S., Leese, M., & Stahl, D
Everitt, B. S., Landau, S., Leese, M., & Stahl, D. 2001, Cluster Analysis (Wiley Series in Probability and Statistics) Faucher-Gigu` ere, C.-A., & Quataert, E. 2012, MNRAS, 425, 605, doi: 10.1111/j.1365-2966.2012.21512.x
2001
-
[13]
M., Peterson, B
Fausnaugh, M. M., Peterson, B. M., Starkey, D. A., Horne, K., & AGN Storm Collaboration. 2017, Frontiers in Astronomy and Space Sciences, 4, 55, doi: 10.3389/fspas.2017.00055
2017
-
[14]
Flesch, E. W. 2015, PASA, 32, e010, doi: 10.1017/pasa.2015.10
2015 doi
-
[15]
Flesch, E. W. 2023, The Open Journal of Astrophysics, 6, doi: 10.21105/astro.2308.01505
2023 arXiv
-
[16]
Frank, J., King, A., & Raine, D. J. 2002, Accretion Power in Astrophysics: Third Edition
2002
-
[17]
J., Djorgovski, S
Graham, M. J., Djorgovski, S. G., Drake, A. J., et al. 2014, MNRAS, 439, 703, doi: 10.1093/mnras/stt2499
2014 doi
-
[18]
2025, A&A, 693, A319, doi: 10.1051/0004-6361/202450562
Kankkunen, S., Tornikoski, M., & Hovatta, T. 2025, A&A, 693, A319, doi: 10.1051/0004-6361/202450562
2025 doi
-
[19]
P., Vogeley, M
Kasliwal, V. P., Vogeley, M. S., & Richards, G. T. 2015, MNRAS, 451, 4328, doi: 10.1093/mnras/stv1230
2015 doi
-
[20]
C., Bechtold, J., & Siemiginowska, A
Kelly, B. C., Bechtold, J., & Siemiginowska, A. 2009, ApJ, 698, 895, doi: 10.1088/0004-637X/698/1/895
2009 doi
-
[21]
C., Becker, A
Kelly, B. C., Becker, A. C., Sobolewska, M., Siemiginowska, A., & Uttley, P. 2014, ApJ, 788, 33, doi: 10.1088/0004-637X/788/1/33 Koz lowski, S. 2016, ApJ, 826, 118, doi: 10.3847/0004-637X/826/2/118
2014 doi
-
[22]
A., & Bian, F
Lai, S., Wolf, C., Onken, C. A., & Bian, F. 2023, MNRAS, 521, 3682, doi: 10.1093/mnras/stad651 L´ opez-Navas, E., Ar´ evalo, P., Bernal, S., et al. 2023, MNRAS, 518, 1531, doi: 10.1093/mnras/stac3174
2023 doi
-
[23]
1969, Nature, 223, 690, doi: 10.1038/223690a0
Lynden-Bell, D. 1969, Nature, 223, 690, doi: 10.1038/223690a0
1969 doi
-
[24]
Lyubarskii, Y. E. 1997, MNRAS, 292, 679, doi: 10.1093/mnras/292.3.679
1997 doi
-
[25]
L., Ivezi´ c,ˇZ., Kochanek, C
MacLeod, C. L., Ivezi´ c,ˇZ., Kochanek, C. S., et al. 2010, ApJ, 721, 1014, doi: 10.1088/0004-637X/721/2/1014
2010 doi
-
[26]
Malmquist, K. G. 1922, Meddelanden fran Lunds Astronomiska Observatorium Serie I, 100, 1
1922
-
[27]
Malmquist, K. G. 1925, Meddelanden fran Lunds Astronomiska Observatorium Serie I, 106, 1 Mart´ ınez Collipal, D., & Panda, S. 2026, Research Notes of the American Astronomical Society, 10, 97, doi: 10.3847/2515-5172/ae6648
1925 doi
-
[28]
J., Laher, R
Masci, F. J., Laher, R. R., Rusholme, B., et al. 2019, PASP, 131, 018003, doi: 10.1088/1538-3873/aae8ac
2019 doi
- [29]
-
[30]
McQuitty, L. L. 1960, Educational and Psychological Measurement, 20, 55, doi: 10.1177/001316446002000106
1960 doi
-
[31]
Mondal, D., & Percival, D. B. 2012, in Statistical Challenges in Modern Astronomy V, ed. E. D. Feigelson & G. J. Babu, Vol. 902, 403–418, doi: 10.1007/978-1-4614-3520-4 38
2012 doi
-
[32]
S., Richards, G
Moreno, J., Vogeley, M. S., Richards, G. T., & Yu, W. 2019, PASP, 131, 063001, doi: 10.1088/1538-3873/ab1597
2019 doi
-
[33]
2011, ApJL, 743, L12, doi: 10.1088/2041-8205/743/1/L12
Gandhi, P. 2011, ApJL, 743, L12, doi: 10.1088/2041-8205/743/1/L12
2011 doi
-
[34]
2015, ARA&A, 53, 365, doi: 10.1146/annurev-astro-082214-122302
Netzer, H. 2015, ARA&A, 53, 365, doi: 10.1146/annurev-astro-082214-122302
2015 doi
-
[35]
2022, MNRAS, 509, 2637, doi: 10.1093/mnras/stab3133
Netzer, H. 2022, MNRAS, 509, 2637, doi: 10.1093/mnras/stab3133
2022 doi
-
[36]
Neustadt, J. M. M., & Kochanek, C. S. 2022, MNRAS, 513, 1046, doi: 10.1093/mnras/stac888
2022 doi
-
[37]
A., Bian, F., Fan, X., et al
Onken, C. A., Bian, F., Fan, X., et al. 2020, MNRAS, 496, 2309, doi: 10.1093/mnras/staa1635
2020 doi
-
[38]
M., Richards, G
Peters, C. M., Richards, G. T., Myers, A. D., et al. 2015, ApJ, 811, 95, doi: 10.1088/0004-637X/811/2/95
2015 doi
-
[39]
M., Foltz, C
Peterson, B. M., Foltz, C. B., Byard, P. L., & Wagner, R. M. 1982, ApJS, 49, 469, doi: 10.1086/190807 Pozo Nu˜ nez, F., Bruckmann, C., Deesamutara, S., et al. 2023, MNRAS, 522, 2002, doi: 10.1093/mnras/stad286
1982 doi
-
[40]
T., Myers, A
Richards, G. T., Myers, A. D., Peters, C. M., et al. 2015, ApJS, 219, 39, doi: 10.1088/0067-0049/219/2/39 S´ anchez-S´ aez, P., Lira, H., Mart´ ı, L., et al. 2021, AJ, 162, 206, doi: 10.3847/1538-3881/ac1426
2015 doi
-
[41]
L., Koo, D
Sarajedini, V. L., Koo, D. C., Klesman, A. J., et al. 2011, ApJ, 731, 97, doi: 10.1088/0004-637X/731/2/97 SDSS Collaboration, Adamane Pallathadka, G.,
2011 doi
- [42]
-
[43]
Shields, G. A. 1999, PASP, 111, 661, doi: 10.1086/316378
1999 doi
- [44]
-
[45]
H., Cordes, J
Simonetti, J. H., Cordes, J. M., & Spangler, S. R. 1984, ApJ, 284, 126, doi: 10.1086/162391
1984 doi
-
[46]
Slepian, D., & Pollak, H. O. 1961, The Bell System Technical Journal, 40, 43, doi: 10.1002/j.1538-7305.1961.tb03976.x
1961
-
[47]
Stalevski, M., Fritz, J., Baes, M., Nakos, T., & Popovi´ c, L. ˇC. 2012, MNRAS, 420, 2756, doi: 10.1111/j.1365-2966.2011.19775.x
2012
-
[48]
J., et al
Stern, D., McKernan, B., Graham, M. J., et al. 2018, ApJ, 864, 27, doi: 10.3847/1538-4357/aac726 Classifying Quasar Types Without a Spectrum21 Figure 14.(continued) 22H ´elias et al
2018 doi
-
[49]
Taylor, M. B. 2005, in Astronomical Society of the Pacific Conference Series, Vol. 347, Astronomical Data Analysis Software and Systems XIV, ed. P. Shopbell, M. Britton, & R. Ebert, 29
2005
-
[50]
Ulrich, M.-H., Maraschi, L., & Urry, C. M. 1997, ARA&A, 35, 445, doi: 10.1146/annurev.astro.35.1.445 Vanden Berk, D. E., Wilhite, B. C., Kron, R. G., et al. 2004, ApJ, 601, 692, doi: 10.1086/380563
1997 doi
-
[51]
S., & Uttley, P
Vaughan, S., Edelson, R., Warwick, R. S., & Uttley, P. 2003, MNRAS, 345, 1271, doi: 10.1046/j.1365-2966.2003.07042.x
2003
-
[52]
A., et al
Wolf, C., Lai, S., Onken, C. A., et al. 2024, Nature Astronomy, 8, 520, doi: 10.1038/s41550-024-02195-x
2024 doi
-
[53]
2008, Hierarchical Clustering, 31–62, doi: https://doi.org/10.1002/9780470382776.ch3
Xu, R., & Wunsch, D. 2008, Hierarchical Clustering, 31–62, doi: https://doi.org/10.1002/9780470382776.ch3
2008 doi
-
[54]
G., Adelman, J., Anderson, Jr., J
York, D. G., Adelman, J., Anderson, Jr., J. E., et al. 2000, AJ, 120, 1579, doi: 10.1086/301513
2000 doi
-
[55]
S., Koz lowski, S., & Udalski, A
Zu, Y., Kochanek, C. S., Koz lowski, S., & Udalski, A. 2013, ApJ, 765, 106, doi: 10.1088/0004-637X/765/2/106
2013 doi
Reviewed August 16, 2026 · model on record in the stance chip above.
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