REVIEW 3 major objections 7 minor 69 references
Heartbeat Stars Recognition Based on Recurrent Neural Networks: Method and Validation
T0 review · 3 major / 7 minor · reviewed 2026-08-15 · deepseek-v4-flash
Pith's one-line read Heartbeat stars can be found automatically by feeding the first 100 orbital harmonics of a light curve into a small recurrent network, which predicts eccentricity and works on real survey data at 86% accuracy.
desk verdict A genuinely cheap and novel harmonic-feature RNN for eccentricity regression, but the '86% accuracy' is a regression consistency score on known positives, not a detection rate, and the discovery claim rests on an unvalidated eclipse-count step. 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 the normalized orbital-harmonic feature vector: after locating the orbital frequency, the first 100 harmonic amplitudes extracted by FNPEAKS are divided by their Euclidean norm, so each light curve becomes a 100-number sequence. This vector is what the recurrent network sees, and it matters because it compresses a roughly 30,000-point light curve into a small ordered set, discards the orbital period and absolute flux scale, and lets a two-layer GRU or LSTM rather than a deep network predict eccentricity. The orbital-frequency finder is a second piece of machinery, since the network cannot be applied to real data until the harmonic grid is known; it works by testing which integer multiple of the strongest peak has the most harmonic matches, or, for pulsating systems, by finding the most common spacing between adjacent Fourier peaks.
What would settle it
Run the two trained networks on all 173 Kepler heartbeat stars listed in the Kirk et al. catalog and compare every predicted eccentricity with the published value; if significantly fewer than 86% of predictions land within 0.15, the claimed synthetic-to-real generalization would fail.
Extended reading notes
Core claim
The paper's central claim is that the morphology of a heartbeat-star light curve is encoded, for classification purposes, in the amplitudes of the first 100 orbital harmonics of its Fourier spectrum, and that a recurrent network reading only those amplitudes can recover the orbital eccentricity. The authors construct 52,000 synthetic light curves with ELLC by randomizing eccentricity, inclination, argument of periastron, mass ratio, surface brightness ratio, and radii, plus 2,000 zero-eccentricity close binaries to teach the network what is not a heartbeat star. They define a harmonic as a Fourier peak with signal-to-noise at least 4 that lies within 0.05 of an integer multiple of the orbital frequency, normalize the amplitude vector by its Euclidean norm, and train two-layer GRU and LSTM networks to output eccentricity. On held-out synthetic data the test accuracy is 95%; on real heartbeat stars from OGLE, Kepler, and TESS the networks agree with literature eccentricities to within 0.15 in 86% of cases; and within the Kirk et al. eclipsing-binary catalog the method finds four new heartbeat stars (KIC 4940438, 6794131, 7601633, 9243795), with KIC 6794131's model-fitted eccentricity of 0.179 close to the predicted 0.171.
Load-bearing premise
The load-bearing premise is that 52,000 synthetic ELLC light curves, generated with Gaussian noise but without tidally excited oscillations, are representative enough of real survey light curves that a network trained only on them will recognize real heartbeat stars.
Editorial extensions
If this is right
- Survey archives can be pre-filtered automatically: reducing each light curve to 100 harmonic amplitudes lets a two-layer recurrent network rank large numbers of candidates by predicted eccentricity before any human inspection.
- The same networks recognize eccentric binaries as well as heartbeat stars, and the two classes can be roughly separated by counting eclipses in the phase-folded light curve, so one pipeline can serve both searches.
- Because the orbital frequency is computed automatically, the method does not need a known period to extract features, allowing application to any periodic variable whose orbital harmonics are resolved.
- Visual inspection effort drops from hundreds of thousands of objects to a few hundred candidates, as demonstrated by finding about 1,200 high-eccentricity candidates and then four new heartbeat stars inside the Kirk et al. catalog.
Reading between the lines
- The reported 86% is an agreement rate with published eccentricities on known heartbeat stars, not a completeness or purity measurement against a labeled background; a realistic survey deployment would need a false-positive estimate on non-heartbeat stars.
- If the harmonic envelope is the main carrier of information, a natural test is whether a single interpretable statistic, such as the slope of harmonic amplitude versus harmonic number, correlates with eccentricity; if it does, the recurrent network could be distilled into a simpler explainable detector.
- Injecting tidally excited oscillations into the synthetic training set is an obvious robustness upgrade; the paper shows the network tolerates their absence in training, which suggests including them could improve high-eccentricity cases where these oscillations are strong.
- The method's period independence suggests the same trained networks could be applied to future surveys with different cadences, provided the Fourier spectrum resolves the orbital harmonics; that extension is untested and would be a useful external validation.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper proposes a machine-learning method for recognizing heartbeat stars (HBSs). Light curves are first transformed into Fourier spectra, from which the amplitudes of the first 100 orbital harmonics are extracted and normalized into a 100-dimensional feature vector. Two recurrent neural networks (GRU and LSTM) are trained on 52,000 synthetic light curves generated with ELLC to regress orbital eccentricity. The trained networks are then applied to real HBSs from OGLE, Kepler, and TESS, and to a catalog of eclipsing binaries from Kirk et al. The authors report 95% accuracy on a synthetic test set, 86% 'accuracy prediction consistency' on real data, and the identification of four new HBS candidates, one of which is fitted with a K95+ model. The paper emphasizes that the harmonic-feature approach reduces computational cost and can be extended to other periodic variables.
Significance. If the claims hold, the work is a useful step toward automated HBS discovery: the features are physically motivated and compact, the training is entirely synthetic so there is no circularity in the labels, the code is public, and the method is tested on external real-data catalogs. The realistic significance is, however, lower than the abstract suggests, because the headline 86% figure is a regression-consistency fraction, not a detection accuracy, and the four new candidates are not independently confirmed. The central architecture is sound and reproducible, and the main gaps are quantifiable and fixable within the scope of the manuscript.
major comments (3)
- [Sect. 3.1, abstract, conclusions] The headline '86% accuracy' is not an HBS detection accuracy: it is the fraction of known HBSs and eccentric binaries whose predicted eccentricity lies within ±0.15 of the literature value. In addition, five Kepler HBSs with weak heartbeat signals were excluded from the test set. The abstract and summary currently call this 'average detection accuracy', which overstates what is demonstrated. Please relabel the metric (e.g., regression consistency within 0.15), report per-dataset sizes and per-dataset fractions, and add actual binary classification metrics (precision/recall/F1 for the e>0.1 threshold) on the labeled test sets, ideally with a sensitivity analysis to the excluded weak-signal systems.
- [Sect. 3.2] The discovery pipeline is not validated as a detector. The paragraph in Sect. 3.2 states that systems with no eclipses or one eclipse are classified as HBSs, but also that this strategy is 'not entirely rigorous'; it then converts roughly 900 candidates into four HBSs without reporting precision, recall, or false-positive rates on any labeled sample. A grazing-eclipsing eccentric binary can show a single eclipse and would be misclassified by this rule. Please run the full pipeline on a labeled subset of the Kirk catalog (known HBSs, known eccentric binaries, circular EBs) and report a confusion matrix. In addition, only KIC 6794131 receives a K95+ fit; the other three candidates need independent confirmation (e.g., model fits to all four, additional photometry or radial velocities) before the paper can claim they are 'newly identified HBSs'.
- [Sect. 2.1 vs Sect. 4] The training set contains no tidally excited oscillations, yet Sect. 4 asserts robustness to TEOs based on the aggregate real-data performance. This generalization claim is plausible but unquantified: TEOs add harmonic power at specific frequencies and can change the normalized harmonic vector. Please report the consistency metric separately for known TEO-bearing and non-TEO HBSs in Fig. 4, and/or test the trained networks on synthetic light curves with injected TEO-like harmonic amplitudes.
minor comments (7)
- [Abstract] The first sentence contains a grammar issue: 'Since the variety of their light curve morphologies' should be 'Because of the variety of their light curve morphologies' (or similar).
- [Sect. 2.4] There is a duplicated word in 'the orbital orbital frequency'; it should be 'orbital frequency'.
- [Sect. 2.2 and 2.3] The feature vector is defined in Eq. (2) as (a1,...,an), but the network uses the first 100 harmonics; please clarify how vectors with fewer detected harmonics are handled and whether zero-padding or truncation is applied.
- [Sect. 2.3 and 3.1] The 0.02 deviation threshold used to define training accuracy and the 0.15 tolerance used for real-data consistency should be stated explicitly as the metric definitions; currently the term 'accuracy' is used in both places without a formal definition.
- [Sect. 2.3] The claim that 100 input units were chosen after 'extensive testing' would be more convincing with a small figure showing accuracy versus the number of harmonics used.
- [Sect. 3.1] The sentence 'we suggest classifying them as either type' for systems with both two eclipses and heartbeat signals is ambiguous; please specify the intended classification convention.
- [Title] The title contains an unusual space in 'V alidation'; this appears to be a formatting artifact and should be corrected.
Circularity Check
No circularity: synthetic-trained RNN is validated against external catalogs; self-citations are motivational, not load-bearing.
full rationale
The derivation chain is not circular. Section 2.1 creates 52,000 synthetic light curves with ELLC using randomly drawn parameters (ecc up to 0.9, incl 20–90 deg, etc.); the supervised target is the known eccentricity used to generate each model, so the network is fitted to forward-model labels rather than to the real catalogs it later tests against. Section 2.3's 95% accuracy is an in-distribution check on held-out synthetic curves, not a claim that the synthetic set defines the real answer. The 86% figure in Section 3.1 is explicitly a comparison between predicted eccentricity and published eccentricities from the OGLE, Kepler, and TESS catalogs; those external references are not inputs to training, and the paper states that OGLE orbital frequencies were adopted from the literature because the automatic period pipeline failed there. Section 3.2's four new HBS candidates are selected by an e>0.1 threshold plus visual and eclipse-count inspection; KIC 6794131 is additionally fitted with a K95+ model using the authors' own earlier methodology, but the fit is used as an after-the-fact validation, not as the training target. The only self-referential element is the motivational use of the authors' Li et al. 2024d harmonic analysis and the relaxed harmonic-matching threshold quoted from Eq. (1); these are methodological antecedents, not uniqueness theorems or fitted labels, and the central eccentricity-regression claim rests on independent external catalogs. Limitations exist—synthetic training omits TEOs, the eclipse-count classification is explicitly called 'not entirely rigorous', and only one of four candidates is model-fitted—but these are completeness and validation caveats, not circular reasoning. Hence no circular step can be exhibited.
Assumptions & free parameters
free parameters (5)
- Number of harmonic features =
100
- Eccentricity classification threshold =
0.1
- S/N threshold for harmonic detection =
4.0
- Harmonic matching tolerance =
0.05
- Real-data consistency tolerance =
0.15
assumptions (3)
- domain assumption ELLC model accurately simulates HBS light curves in the explored parameter space.
- domain assumption Heartbeat star light curves are fully characterized by their orbital Fourier harmonics.
- domain assumption The orbital frequency can be recovered automatically from the Fourier spectra.
Cite this review
Pith. "Pith review of Heartbeat Stars Recognition Based on Recurrent Neural Networks: Method and Validation." pith.science (2026). https://pith.science/paper/TRPC56IE
@misc{pith2026250504067,
author = {Pith},
title = {Pith review of: Heartbeat Stars Recognition Based on Recurrent Neural Networks: Method and Validation},
year = {2026},
howpublished = {\url{https://pith.science/paper/TRPC56IE}},
note = {Machine review of arXiv:2505.04067}
}
abstract
Since the variety of their light curve morphologies, the vast majority of the known heartbeat stars (HBSs) have been discovered by manual inspection. Machine learning, which has already been successfully applied to the classification of variable stars based on light curves, offers another possibility for the automatic detection of HBSs. We propose a novel feature extraction approach for HBSs. First, the orbital frequencies are calculated automatically according to the Fourier spectra of the light curves. Then, the amplitudes of the first 100 harmonics are extracted. Finally, these harmonics are normalized as feature vectors of the light curve. A training data set of synthetic light curves is constructed using ELLC, and their features are fed into recurrent neural networks (RNNs) for supervised learning, with the expected output being the eccentricity of these light curves. The performance of the RNNs is evaluated using a test data set of synthetic light curves, achieving 95$\%$ accuracy. When applied to known HBSs from the OGLE, Kepler, and TESS surveys, the networks achieve an average accuracy of 86$\%$. This method successfully identifies four new HBSs within the eclipsing binary catalog of Kirk et al. The use of orbital harmonics as features for HBSs proves to be a practical approach that significantly reduces the computational cost of neural networks. RNNs show excellent performance in recognizing this type of time series data. This method not only allows efficient identification of HBSs but can also be extended to recognize other types of periodic variable stars.
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Works this paper leans on
-
[1]
2019, MNRAS, 482, 5078, doi: 10.1093/mnras/sty2836
Aguirre, C., Pichara, K., & Becker, I. 2019, MNRAS, 482, 5078, doi: 10.1093/mnras/sty2836
-
[2]
Armstrong, D. J., Kirk, J., Lam, K. W. F., et al. 2016, MNRAS, 456, 2260, doi: 10.1093/mnras/stv2836
-
[3]
Audenaert, J., Kuszlewicz, J. S., Handberg, R., et al. 2021, AJ, 162, 209, doi: 10.3847/1538-3881/ac166a
-
[4]
Barbara, N. H., Bedding, T. R., Fulcher, B. D., Murphy, S. J., & Van Reeth, T. 2022, MNRAS, 514, 2793, doi: 10.1093/mnras/stac1515
-
[5]
G., Hambleton, K., Vos, J., et al
Beck, P. G., Hambleton, K., Vos, J., et al. 2014, A&A, 564, A36, doi: 10.1051/0004-6361/201322477
-
[6]
2020, MNRAS, 493, 2981, doi: 10.1093/mnras/staa350
Becker, I., Pichara, K., Catelan, M., et al. 2020, MNRAS, 493, 2981, doi: 10.1093/mnras/staa350
-
[7]
2014, MNRAS, 443, 3068, doi: 10.1093/mnras/stu1379
Borkovits, T., Derekas, A., Fuller, J., et al. 2014, MNRAS, 443, 3068, doi: 10.1093/mnras/stu1379
-
[8]
Brogaard, K., Hansen, C. J., Miglio, A., et al. 2018, MNRAS, 476, 3729, doi: 10.1093/mnras/sty268 6 https://github.com/MinyuLi/HBSsNN
Show all 69 references
-
[9]
J., Fuller, J., Guo, Z., Lehman, H., & Hambleton, K
Cheng, S. J., Fuller, J., Guo, Z., Lehman, H., & Hambleton, K. 2020, ApJ, 903, 122, doi: 10.3847/1538-4357/abb46d
2020 doi
- [10]
-
[11]
J., & Feng, F
Cui, K., Armstrong, D. J., & Feng, F. 2024, ApJS, 274, 29, doi: 10.3847/1538-4365/ad62fd
2024 doi
-
[12]
Elizabethson, A., Serna, J., Garc´ ıa-Varela, A., Hern´ andez, J., & Cabrera-Garc´ ıa, J. F. 2023, AJ, 166, 189, doi: 10.3847/1538-3881/acf865
2023 doi
-
[13]
2017, MNRAS, 472, 1538, doi: 10.1093/mnras/stx2135
Fuller, J. 2017, MNRAS, 472, 1538, doi: 10.1093/mnras/stx2135
2017 doi
-
[14]
2017, MNRAS, 472, L25, doi: 10.1093/mnrasl/slx130
Thompson, S. 2017, MNRAS, 472, L25, doi: 10.1093/mnrasl/slx130
2017 doi
-
[15]
2025, ApJS, 276, 57, doi: 10.3847/1538-4365/ad9dd6
Gao, X., Chen, X., Wang, S., & Liu, J. 2025, ApJS, 276, 57, doi: 10.3847/1538-4365/ad9dd6
2025 doi
-
[16]
2016, ApJ, 832, 121, doi: 10.3847/0004-637X/832/2/121 10
Gaulme, P., McKeever, J., Jackiewicz, J., et al. 2016, ApJ, 832, 121, doi: 10.3847/0004-637X/832/2/121 10
2016 doi
-
[17]
2024, MNRAS, 528, 6997, doi: 10.1093/mnras/stae404
Guo, F., Lin, J., Wang, X., et al. 2024, MNRAS, 528, 6997, doi: 10.1093/mnras/stae404
2024 doi
-
[18]
2021, FrASS, 8, 67, doi: 10.3389/fspas.2021.663026
Guo, Z. 2021, FrASS, 8, 67, doi: 10.3389/fspas.2021.663026
2021
-
[19]
2019, ApJ, 885, 46, doi: 10.3847/1538-4357/ab41f6
Guo, Z., Fuller, J., Shporer, A., et al. 2019, ApJ, 885, 46, doi: 10.3847/1538-4357/ab41f6
2019 doi
-
[20]
R., & Fuller, J
Guo, Z., Gies, D. R., & Fuller, J. 2017, ApJ, 834, 59, doi: 10.3847/1538-4357/834/1/59
2017 doi
-
[21]
2020, ApJ, 888, 95, doi: 10.3847/1538-4357/ab58c2
Guo, Z., Shporer, A., Hambleton, K., & Isaacson, H. 2020, ApJ, 888, 95, doi: 10.3847/1538-4357/ab58c2
2020 doi
-
[22]
W., Prˇ sa, A., et al
Hambleton, K., Kurtz, D. W., Prˇ sa, A., et al. 2016, MNRAS, 463, 1199, doi: 10.1093/mnras/stw1970
2016 doi
-
[23]
2018, MNRAS, 473, 5165, doi: 10.1093/mnras/stx2673
Hambleton, K., Fuller, J., Thompson, S., et al. 2018, MNRAS, 473, 5165, doi: 10.1093/mnras/stx2673
2018 doi
-
[24]
M., Kurtz, D
Hambleton, K. M., Kurtz, D. W., Prˇ sa, A., et al. 2013, MNRAS, 434, 925, doi: 10.1093/mnras/stt886
2013 doi
-
[25]
2015, arXiv e-prints, arXiv:1502.01852, doi: 10.48550/arXiv.1502.01852 He lminiak, K
He, K., Zhang, X., Ren, S., & Sun, J. 2015, arXiv e-prints, arXiv:1502.01852, doi: 10.48550/arXiv.1502.01852 He lminiak, K. G., Ukita, N., Kambe, E., et al. 2016, MNRAS, 461, 2896, doi: 10.1093/mnras/stw1514
-
[26]
A., Tat, K., & Thorp, R
Hinners, T. A., Tat, K., & Thorp, R. 2018, AJ, 156, 7, doi: 10.3847/1538-3881/aac16d
2018 doi
-
[27]
1997, Neural Computation, 9, 1735, doi: 10.1162/neco.1997.9.8.1735
Hochreiter, S., & Schmidhuber, J. 1997, Neural Computation, 9, 1735, doi: 10.1162/neco.1997.9.8.1735
1997 doi
-
[28]
2018a, MNRAS, 476, 3233, doi: 10.1093/mnras/sty483
Hon, M., Stello, D., & Yu, J. 2018a, MNRAS, 476, 3233, doi: 10.1093/mnras/sty483
-
[29]
Hon, M., Stello, D., & Zinn, J. C. 2018b, ApJ, 859, 64, doi: 10.3847/1538-4357/aabfdb
-
[30]
Jamal, S., & Bloom, J. S. 2020, ApJS, 250, 30, doi: 10.3847/1538-4365/aba8ff
2020 doi
-
[31]
S., Strader, J., et al
Jayasinghe, T., Kochanek, C. S., Strader, J., et al. 2021, MNRAS, 506, 4083, doi: 10.1093/mnras/stab1920
2021 doi
-
[32]
B., Caballero-Nieves, S
Johnston, K. B., Caballero-Nieves, S. M., Petit, V., Peter, A. M., & Haber, R. 2020, MNRAS, 491, 3805, doi: 10.1093/mnras/stz3165
2020 doi
-
[33]
2016, Aj, 151, 68, doi: 10.3847/0004-6256/151/3/68
Kirk, B., Conroy, K., Prˇ sa, A., et al. 2016, Aj, 151, 68, doi: 10.3847/0004-6256/151/3/68
2016 doi
-
[34]
2015a, PASA, 32, e023, doi: 10.1017/pasa.2015.23
Kjurkchieva, D., & Vasileva, D. 2015a, PASA, 32, e023, doi: 10.1017/pasa.2015.23
2015 doi
- [35]
-
[36]
2016, NewA, 48, 30, doi: 10.1016/j.newast.2016.04.004
Kjurkchieva, D., & Vasileva, D. 2016, NewA, 48, 30, doi: 10.1016/j.newast.2016.04.004
2016 doi
-
[37]
2016a, Ap&SS, 361, 132, doi: 10.1007/s10509-016-2722-3
Kjurkchieva, D., Vasileva, D., & Dimitrov, D. 2016a, Ap&SS, 361, 132, doi: 10.1007/s10509-016-2722-3
-
[38]
2016b, AJ, 152, 189, doi: 10.3847/0004-6256/152/6/189
Kjurkchieva, D., Vasileva, D., & Dimitrov, D. 2016b, AJ, 152, 189, doi: 10.3847/0004-6256/152/6/189
-
[39]
2024, A&A, 685, A145, doi: 10.1051/0004-6361/202349075 Ko laczek-Szyma´ nski, P
Koenigsberger, G., & Estrella-Trujillo, D. 2024, A&A, 685, A145, doi: 10.1051/0004-6361/202349075 Ko laczek-Szyma´ nski, P. A., Lojko, P., Pigulski, A., R´ o˙ za´ nski, T., & Mo´ zdzierski, D. 2024, A&A, 686, A199, doi: 10.1051/0004-6361/202348104 Ko laczek-Szyma´ nski, P. A.,...
2024 doi
-
[40]
2022, A&A, 659, A47, doi: 10.1051/0004-6361/202142171 Ko laczek-Szyma´ nski, P
Ratajczak, M., & Udalski, A. 2022, A&A, 659, A47, doi: 10.1051/0004-6361/202142171 Ko laczek-Szyma´ nski, P. A., & R´ o˙ za´ nski, T. 2023, A&A, 671, A22, doi: 10.1051/0004-6361/202245226
2022 doi
-
[41]
O., & Quataert, E
Kumar, P., Ao, C. O., & Quataert, E. J. 1995, ApJ, 449, 294, doi: 10.1086/176055
1995 doi
-
[42]
2023, ApJS, 266, 28, doi: 10.3847/1538-4365/acca13
Li, M.-Y., Qian, S.-B., Zhu, L.-Y., et al. 2023, ApJS, 266, 28, doi: 10.3847/1538-4365/acca13
2023 doi
-
[43]
2024a, ApJ, 974, 278, doi: 10.3847/1538-4357/ad794c
Li, M.-Y., Qian, S.-B., Zhou, A.-Y., et al. 2024a, ApJ, 974, 278, doi: 10.3847/1538-4357/ad794c
-
[44]
2024b, MNRAS, 530, 586, doi: 10.1093/mnras/stae885
Li, M.-Y., Qian, S.-B., Zhu, L.-Y., et al. 2024b, MNRAS, 530, 586, doi: 10.1093/mnras/stae885
-
[45]
2024c, MNRAS, 534, 281, doi: 10.1093/mnras/stae2057
Li, M.-Y., Qian, S.-B., Zhou, A.-Y., et al. 2024c, MNRAS, 534, 281, doi: 10.1093/mnras/stae2057
-
[46]
2024d, ApJ, 962, 44, doi: 10.3847/1538-4357/ad18c1
Li, M.-Y., Qian, S.-B., Zhu, L.-Y., et al. 2024d, ApJ, 962, 44, doi: 10.3847/1538-4357/ad18c1
-
[47]
2025, PASJ, 77, 118, doi: 10.1093/pasj/psae103
Li, M.-Y., Qian, S.-B., Zhu, L.-Y., et al. 2025, PASJ, 77, 118, doi: 10.1093/pasj/psae103
2025 doi
-
[48]
2014, A&A, 563, A59, doi: 10.1051/0004-6361/201322871
Maceroni, C., Lehmann, H., da Silva, R., et al. 2014, A&A, 563, A59, doi: 10.1051/0004-6361/201322871
2014 doi
-
[49]
2023, Nature Astronomy, 7, 1218, doi: 10.1038/s41550-023-02036-3
MacLeod, M., & Loeb, A. 2023, Nature Astronomy, 7, 1218, doi: 10.1038/s41550-023-02036-3
2023 doi
- [50]
-
[51]
Z., Tramper, F., et al
Maravelias, G., Bonanos, A. Z., Tramper, F., et al. 2022, A&A, 666, A122, doi: 10.1051/0004-6361/202141397
2022 doi
-
[52]
Maxted, P. F. L. 2016, A&A, 591, A111, doi: 10.1051/0004-6361/201628579
2016 doi
-
[53]
2024, A&A, 691, A106, doi: 10.1051/0004-6361/202449995
Monsalves, N., Jaque Arancibia, M., Bayo, A., et al. 2024, A&A, 691, A106, doi: 10.1051/0004-6361/202449995
2024 doi
-
[54]
S., P´ erez, F., & van der Walt, S
Naul, B., Bloom, J. S., P´ erez, F., & van der Walt, S. 2018, Nature Astronomy, 2, 151, doi: 10.1038/s41550-017-0321-z O’Leary, R. M., & Burkart, J. 2014, MNRAS, 440, 3036, doi: 10.1093/mnras/stu335
2018 doi
-
[55]
P., Ansdell, M., Ioannou, Y., et al
Osborn, H. P., Ansdell, M., Ioannou, Y., et al. 2020, A&A, 633, A53, doi: 10.1051/0004-6361/201935345
2020 doi
-
[56]
2021a, MNRAS, 508, 3967, doi: 10.1093/mnras/stab2805
Ou, J.-W., Yu, C., Jiang, C., Yang, M., & Niu, H. 2021a, MNRAS, 508, 3967, doi: 10.1093/mnras/stab2805
-
[57]
2021b, ApJ, 922, 37, doi: 10.3847/1538-4357/ac22b0
Ou, J.-W., Yu, C., Yang, M., et al. 2021b, ApJ, 922, 37, doi: 10.3847/1538-4357/ac22b0
-
[58]
2021, AJ, 162, 67, doi: 10.3847/1538-3881/ac0824 11
Qu, H., Sako, M., M¨ oller, A., & Doux, C. 2021, AJ, 162, 67, doi: 10.3847/1538-3881/ac0824 11
2021 doi
-
[59]
L., Gaulme, P., McKeever, J., et al
Rawls, M. L., Gaulme, P., McKeever, J., et al. 2016, ApJ, 818, 108, doi: 10.3847/0004-637X/818/2/108 S´ anchez-S´ aez, P., Reyes, I., Valenzuela, C., et al. 2021, AJ, 161, 141, doi: 10.3847/1538-3881/abd5c1
2016 doi
-
[60]
2019, MNRAS, 483, 5534, doi: 10.1093/mnras/sty3146
Schanche, N., Collier Cameron, A., H´ ebrard, G., et al. 2019, MNRAS, 483, 5534, doi: 10.1093/mnras/sty3146
2019 doi
-
[61]
2016, ApJ, 829, 34, doi: 10.3847/0004-637X/829/1/34
Shporer, A., Fuller, J., Isaacson, H., et al. 2016, ApJ, 829, 34, doi: 10.3847/0004-637X/829/1/34
2016 doi
-
[62]
M., Schnittman, J., et al
Solanki, S., Cieplak, A. M., Schnittman, J., et al. 2025, ApJS, 276, 17, doi: 10.3847/1538-4365/ad8a62
2025 doi
-
[63]
E., Everett, M., Mullally, F., et al
Thompson, S. E., Everett, M., Mullally, F., et al. 2012, ApJ, 753, 86, doi: 10.1088/0004-637X/753/1/86
2012 doi
-
[64]
Tsang, B. T. H., & Schultz, W. C. 2019, ApJL, 877, L14, doi: 10.3847/2041-8213/ab212c Ula¸ s, B., Szklen´ ar, T., & Szab´ o, R. 2025, A&A, 695, A81, doi: 10.1051/0004-6361/202452020
2019 doi
-
[65]
2021, A&A, 652, A107, doi: 10.1051/0004-6361/202141068
Vida, K., B´ odi, A., Szklen´ ar, T., & Seli, B. 2021, A&A, 652, A107, doi: 10.1051/0004-6361/202141068
2021 doi
-
[66]
A., Ratajczak, M., & Koz lowski, S
Wrona, M., Ko laczek-Szyma´ nski, P. A., Ratajczak, M., & Koz lowski, S. 2022a, ApJ, 928, 135, doi: 10.3847/1538-4357/ac56e6
-
[67]
A., et al
Wrona, M., Ratajczak, M., Ko laczek-Szyma´ nski, P. A., et al. 2022b, ApJS, 259, 16, doi: 10.3847/1538-4365/ac4018
-
[68]
Zahn, J. P. 1975, A&A, 41, 329
1975
-
[69]
Zhang, K., & Bloom, J. S. 2021, MNRAS, 505, 515, doi: 10.1093/mnras/stab1248
2021 doi
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