REVIEW 3 major objections 6 minor 1 cited by
LEO-Vetter: Fully Automated Flux- and Pixel-Level Vetting of TESS Planet Candidates to Support Occurrence Rates
T0 review · 3 major / 6 minor · reviewed 2026-08-15 · deepseek-v4-flash
Pith's one-line read LEO-Vetter claims that a fully automated, publicly available pipeline can vet TESS planet candidates with 91% completeness and 97% reliability against false alarms, reducing about 20,000 detections to 172 candidates.
desk verdict A genuinely useful, publicly shipped TESS vetter whose headline completeness/reliability numbers are in-sample fitted values; the tool deserves peer review, and the numbers need a held-out check. 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 engine is a suite of decision metrics computed for each transit-like detection and compared against pass-fail thresholds: signal-to-noise ratio, transit model fits, a sine-wave variability test, transit duration and asymmetry checks, depth mean-to-median consistency, per-transit signal-to-noise consistency, uniqueness tests on the folded light curve, individual transit vetting, and a pixel-level difference-image centroid analysis. The thresholds were set by an optimization routine that varies false-alarm-test thresholds to minimize $\sqrt{(1-C)^2 + (1-R_{\rm FA})^2}$, using injected transits to measure completeness and orbit-scrambled light curves to estimate false-alarm reliability. This metric-plus-threshold design is what lets the pipeline be fully automated and uniform.
What would settle it
Apply LEO-Vetter with the published thresholds to an independent set of TESS light curves with known confirmed planets and known false positives, for example a different sector range or the 2-minute SPOC data, and compare the automated labels against the confirmed disposition. If the recovered fraction of confirmed planets is clearly below 91% or the false-alarm contamination of the candidate list clearly exceeds 3%, the reported completeness and reliability would be overstated.
Extended reading notes
Core claim
The paper claims that LEO-Vetter, a fully automated vetting pipeline for TESS transit signals, can replace the manual inspection currently used to build planet candidate catalogs without sacrificing the uniformity needed for demographic studies. On a test set of roughly 200,000 M dwarf light curves, it classifies 91.00% of injected transiting planets as planet candidates, rejects 99.91% of scrambled-light-curve false alarms, and reduces about 20,000 observed transit-like detections to 172 uniformly vetted candidates. The pipeline combines flux-level tests of transit shape, depth consistency, uniqueness, and signal-to-noise with a pixel-level centroid-offset test that flags signals coming from nearby stars. The authors conclude that this makes statistically grounded TESS occurrence-rate calculations possible because users can characterize both vetting completeness and false-alarm reliability from simulated data.
Load-bearing premise
The performance numbers rest on the assumption that transits injected into real light curves and false alarms made by scrambling orbit and sector order faithfully represent the real planets and noise/systematic signals a user will encounter.
Editorial extensions
If this is right
- Users can turn their own TESS transit-like detections into a vetted planet candidate catalog without manual review, using the published thresholds as a starting point.
- The injected and scrambled data products supplied with the pipeline let users measure vetting completeness and false-alarm reliability for their own sample, which is required input for occurrence-rate calculations.
- The same thresholds applied to a 300,000-star FGK dwarf sample give comparable completeness (90.86%) and reliability (88.19% overall, 98.64% at signal-to-noise above 12), suggesting the M-dwarf tuning transfers to other dwarf populations.
- Known TOIs that failed flux-level vetting recovered cleanly when 2-minute SPOC light curves were substituted for the longer-cadence FFI data, indicating performance improves with shorter cadence.
Reading between the lines
- Because the pass-fail thresholds were optimized on the very injected and scrambled datasets used to measure performance, an independent test on a separate sector set or on 2-minute cadence data would be the natural check of whether 91% and 97% generalize to new observations.
- The same architecture could be applied to other transit surveys with different bandpasses and cadence mixes; the limb-darkening assumptions and pixel-level code currently tied to TESS would need to be generalized first.
- If the pipeline's completeness depends strongly on cadence, users analyzing only Prime Mission 30-minute data should re-derive thresholds rather than reuse the published ones, since the paper itself reports a Prime Mission completeness of 69.88%.
Signed reviews
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper presents LEO-Vetter, a fully automated Robovetter-inspired vetting pipeline for TESS transit candidates. The tool implements thirteen flux-level tests against noise/systematic false alarms, four flux-level tests against astrophysical false positives, and a pixel-level centroid offset test using difference images. As a demonstration, the authors apply LEO-Vetter to roughly 200,000 M-dwarf QLP light curves, obtain 18,424 observed TCEs plus 62,410 injected and 15,655 scrambled TCEs, and use a differential evolution optimizer to set pass-fail thresholds on the false-alarm tests. They report a completeness of 91.00% and a false-alarm reliability of 96.97% on these same data, and after pixel-level vetting they produce a uniformly vetted catalog of 172 planet candidates. They also apply the M-dwarf-tuned thresholds to 300,000 FGK dwarfs and report lower overall reliability (88.19%), which they interpret as demonstrating that the thresholds are applicable to FGK dwarfs. The paper claims that the vetter's characterized completeness and reliability make it suitable for TESS occurrence-rate calculations.
Significance. If the performance claims hold, LEO-Vetter would be a valuable public resource: it is the first fully automated TESS vetter that combines flux-level tests with pixel-level difference-image analysis, and it is designed specifically for uniform catalog production in support of demographic studies. The paper's strengths include the public release of the code on GitHub and Zenodo, the use of injection and scrambling experiments following the Kepler DR25 methodology, the large-scale M-dwarf demonstration producing a 172-candidate catalog, and the per-candidate false-positive probabilities, positional probabilities, and disposition scores. The central weakness is that the headline completeness and reliability numbers are in-sample estimates: thresholds were optimized on the same injected and scrambled TCE sets used to quote performance, and the FGK re-run in §8.2 shows that reliability is sensitive to the stellar sample. This load-bearing issue must be addressed before the occurrence-rate support claim is credible.
major comments (3)
- [§5.6 and §6.1] The headline performance figures are in-sample fitted values, not independent predictions. In §5.6 the differential evolution optimizer minimizes sqrt((1-C)^2 + (1-R_FA)^2) over the injected and scrambled TCE sets, and §6.1 then quotes C = 91.00%, E = 99.91%, and R_FA = 96.97% computed on those same sets. The paper reports no held-out split, cross-validation, or alternative test set for the M-dwarf pipeline. Because the optimizer can exploit noise in the specific simulated TCEs, the quoted completeness and reliability may be optimistic. The FGK re-run in §8.2 provides the natural out-of-sample test: applying the same thresholds to FGK dwarfs gives C = 90.86% but R_FA = 88.19% overall. This demonstrates that the 97% reliability is not robust across stellar populations and that the claim of applicability to FGKM dwarfs is only weakly supported. An unbiased evaluation (e.g., tuning on one half of the M-dwarf data and evaluating on the other half, or presenting the FGK result as the headline transferable reliability) is required before the paper can claim that LEO-Vetter produces catalogs with characterized completeness and reliability for occurrence rates.
- [§6.3 and §7] The reliability of the final 172-candidate catalog is not characterized. The 96.97% false-alarm reliability in §6.1 is computed after flux-level vetting only; the pixel-level centroid offset test then removes 153 of 325 flux-level candidates, yet no completeness or reliability estimate is provided for the pixel-level stage. The centroid threshold of Δθ < 15″ appears to be hand-set based on performance on known TOIs rather than validated with injected or simulated pixel-level tests, and the paper does not quantify how many true planets might be lost at this stage. Since the stated purpose of the tool is to support occurrence-rate calculations that require end-to-end reliability of the final catalog, the absence of a validated pixel-level performance estimate is a load-bearing gap.
- [§5.5] The cleaning of simulated TCEs introduces manual judgment into the benchmark sets used for the headline numbers. The authors removed 389 injected and 479 scrambled TCEs from light curves containing known TOIs, eclipsing binaries, or 'signals that we determined to be previously unknown planet candidates or eclipsing binaries manually identified while testing the vetter.' This manual pruning can bias both completeness and effectiveness in unpredictable directions and weakens the claim that C and R_FA are purely simulation-based quantities. The paper should justify that the removed TCEs are not systematically different from the retained ones, or present the performance metrics with and without this cleaning step.
minor comments (6)
- [Abstract and §6.1] The point estimates 91.00% and 96.97% are quoted without any uncertainty. Statistical uncertainties from the finite TCE samples are small, but systematic uncertainties from simulation fidelity and threshold tuning are not; a brief statement about the dominant uncertainty would help readers.
- [§3.8] There is a typo: 'A value if C_i ≈ 0' should read 'A value of C_i ≈ 0'.
- [§5.2] The definition of P_max as 'half the length of the longest continuous stretch of consecutive sectors' is confusing; it would be clearer to say 'half the length of the longest continuous observing stretch within a sector or across consecutive sectors.'
- [§6.1] The sentence 'LEO-Vetter successfully classified 91.00% of injected planets as PCs' should say 'of injected TCEs recovered by the BLS search,' to match the definition of completeness in Eq. (14).
- [§8.2] The conclusion that 'the thresholds optimized for M dwarfs are also applicable to FGK dwarfs' is too strong given that R_FA drops from 96.97% to 88.19%; the SNR > 12 reliability of 98.64% should be reported more prominently if the authors intend this as the applicable regime.
- [§7.3] The disposition scores are derived from metric standard deviations measured on the same injected dataset used for threshold optimization; the text should note that these scores are therefore not an independent validation of the vetter's reliability.
Circularity Check
Headline completeness/reliability numbers are computed on the same simulated TCE sets used to optimize the pass-fail thresholds, so the central performance claim is an in-sample fit rather than an independent prediction.
-
fitted input called prediction
[§5.6 "Tuning Pass-Fail Thresholds" and §6.1 "Flux-Level Vetting"]
"We ran an optimization routine by varying pass-fail thresholds and computing the resulting completeness and reliability values, with the goal of minimizing the function sqrt((1-C)^2 + (1-R_FA)^2). … Using the thresholds provided in §3 and §4, LEO-Vetter successfully classified 91.00% of injected planets as PCs, while rejecting 99.91% of simulated false alarms as FAs. … corresponding to an overall catalog reliability of 96.97% (i.e., a noise/systematic false alarm rate of 3.03%) following Eqn. 16."
The reported C = 91.00% and R_FA = 96.97% are measured on the same injected and scrambled TCE datasets that the differential evolution optimizer used to select the pass-fail thresholds in §5.6. Those two numbers are exactly the components of the minimized objective, so the headline performance is the optimization target evaluated on its own training set, not an independent validation. The optimizer can exploit noise in these specific simulated TCEs, and the paper reports no held-out split or cross-validation. The FGK re-run in §8.2 gives R_FA = 88.19% with the same thresholds, showing dataset sensitivity.
full rationale
The core circularity is in-sample performance evaluation: §5.6 tunes thresholds by minimizing sqrt((1-C)^2 + (1-R_FA)^2) on the injected and scrambled TCE sets, and §6.1 then quotes C = 91.00% and R_FA = 96.97% from those same sets. Because C and R_FA are the two terms of the optimized objective, the headline numbers reduce by construction to fitted values on the training data. The paper reports no held-out split or cross-validation for the M-dwarf set, and the FGK test in §8.2 shows that the M-dwarf-tuned thresholds yield a lower reliability (88.19%) on a different stellar sample, confirming that the quoted 97% is not a robust out-of-sample estimate. No significant self-citation load-bearing circularity is present: the cited Robovetter/KDR25 tests, Model-Shift, and TRICERATOPS are external tools or prior independent work, and the TOI recovery check provides partial independent support for completeness. But because the central performance claim used for occurrence-rate readiness is the fitted in-sample value, the circularity score is 6 rather than lower.
Assumptions & free parameters
free parameters (5)
- Optimized false alarm pass-fail thresholds =
See Table 1 and §3; e.g., SNR<6.2, CHI<7.8, Chases<0.78, MS1<0.2, MS2/3<0.8, SHP>0.6.
- Astrophysical false positive thresholds =
Rp>22 Re, V<1.5, OE>3, secondary MS4>0 etc., delta_theta<15 arcsec.
- Detrending window =
0.5 days
- BLS search criteria and Pmax =
SNR>9, Ntr>=3, Pmax = half longest continuous stretch or 40 days.
- Centroid offset threshold =
delta_theta < 15 arcsec
assumptions (6)
- domain assumption Input light curves are already dilution-corrected, outlier-removed, and quality-flag cleaned before vetting.
- domain assumption Transits are strictly periodic with no significant TTVs.
- domain assumption Scrambled light curves reproduce realistic TESS false alarms.
- domain assumption Injected quadratic limb-darkened circular-orbit transits represent the real planet population.
- domain assumption The Pont et al. (2006) and Hartman & Bakos (2016) noise model accurately captures TESS correlated noise.
- domain assumption TESS PRF difference-image fitting locates the transit source well enough for the 15 arcsec cutoff.
Cite this review
Pith. "Pith review of LEO-Vetter: Fully Automated Flux- and Pixel-Level Vetting of TESS Planet Candidates to Support Occurrence Rates." pith.science (2026). https://pith.science/paper/OKS4ELHA
@misc{pith2026250910619,
author = {Pith},
title = {Pith review of: LEO-Vetter: Fully Automated Flux- and Pixel-Level Vetting of TESS Planet Candidates to Support Occurrence Rates},
year = {2026},
howpublished = {\url{https://pith.science/paper/OKS4ELHA}},
note = {Machine review of arXiv:2509.10619}
}
read the original abstract
The Transiting Exoplanet Survey Satellite (TESS) has identified several thousand planet candidates orbiting a wide variety of stars, and has provided an exciting opportunity for demographic studies. However, current TESS planet searches require significant manual inspection efforts to identify planets among the enormous number of detected transit-like signatures, which limits the scope of such searches. Demographic studies also require a detailed understanding of the relationship between observed and true exoplanet populations; a task for which current TESS planet catalogs are rendered unsuitable by the subjectivity of vetting by eye. We present LEO-Vetter, a publicly available and fully automated exoplanet vetting system designed after the Kepler Robovetter, which is capable of efficiently producing catalogs of promising planet candidates and making statistically robust TESS demographic studies possible. LEO-Vetter implements flux- and pixel-level tests against noise/systematic false positives and astrophysical false positives. The vetter achieves high completeness (91%) and high reliability against noise/systematic false alarms (97%) based on its performance on simulated data. We demonstrate the usefulness of the vetter by searching ~200,000 M dwarf light curves, and reducing ~20,000 transit-like detections down to 172 uniformly vetted planet candidates. LEO-Vetter facilitates analyses that would otherwise be impractical to perform on all possible signals due to time constraints or computational limitations. Users will be able to efficiently produce their own TESS planet catalog starting with transit-like detections, as well as have the framework needed to characterize their catalog's completeness and reliability for occurrence rates.
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Forward citations
Cited by 1 Pith paper
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COUNTESS I: A Uniformly Vetted Catalog of Known and New Transiting Exoplanets in the TESS Northern Continuous Viewing Zone
A multi-cadence TESS pipeline recovers 72% of known northern-CVZ TOIs and delivers 10 new planet candidates, including two statistically validated sub-Neptunes.
Reference graph
Works this paper leans on
-
[1]
, " * write output.state after.block = add.period write newline
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-
[2]
write newline
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-
[3]
thebibliography [1] 20pt to REFERENCES 6pt =0pt \@twocolumntrue 12pt -12pt 10pt plus 3pt =0pt =0pt =1pt plus 1pt =0pt =0pt -12pt =13pt plus 1pt =20pt =13pt plus 1pt \@M =10000 =-1.0em =0pt =0pt 0pt =0pt =1.0em @enumiv\@empty 10000 10000 `\.\@m \@noitemerr \@latex@warning Empty `thebibliography' environment \@ifnextchar \@reference \@latexerr Missing key o...
work page 2017
-
[4]
1974, IEEE Transactions on Automatic Control, 19, 10.1109/TAC.1974.1100705
Akaike , H. 1974, IEEE Transactions on Automatic Control, 19, 10.1109/TAC.1974.1100705
arXiv 1974
-
[5]
Boley , K. M., Wang , J., Zinn , J. C., et al. 2021, , 162, 85, 10.3847/1538-3881/ac0e2d
-
[6]
J., Koch , D., Basri , G., et al
Borucki , W. J., Koch , D., Basri , G., et al. 2010, Science, 327, 977, 10.1126/science.1185402
-
[7]
Bryson , S., Coughlin , J., Batalha , N. M., et al. 2020 a , , 159, 279, 10.3847/1538-3881/ab8a30
-
[8]
L., Kunimoto , M., & Mullally , S
Bryson , S., Coughlin , J. L., Kunimoto , M., & Mullally , S. E. 2020 b , , 160, 200, 10.3847/1538-3881/abb316
Show all 81 references
-
[9]
2025, Research Notes of the AAS, 9, 81, 10.3847/2515-5172/adcb3a
Bryson, S., & Kunimoto, M. 2025, Research Notes of the AAS, 9, 81, 10.3847/2515-5172/adcb3a
2025 doi
-
[10]
T., Jenkins , J
Bryson , S. T., Jenkins , J. M., Gilliland , R. L., et al. 2013, , 125, 889, 10.1086/671767
2013 doi
-
[11]
2019, TESS-ExoClass
Burke , C. 2019, TESS-ExoClass . https://github.com/christopherburke/TESS-ExoClass
2019
-
[12]
J., Levine , A., Fausnaugh , M., et al
Burke , C. J., Levine , A., Fausnaugh , M., et al. 2020, TESS-Point: High precision TESS pointing tool , Astrophysics Source Code Library, record ascl:2003.001
2020
-
[13]
B., Kuchner , M., et al
Cacciapuoti , L., Kostov , V. B., Kuchner , M., et al. 2022, , 513, 102, 10.1093/mnras/stac652
2022 doi
-
[14]
Catanzarite, J. H. 2015, NASA Ames Research Center
2015
-
[15]
L., Clarke , B
Christiansen , J. L., Clarke , B. D., Burke , C. J., et al. 2020, , 160, 159, 10.3847/1538-3881/abab0b
2020 doi
-
[16]
2017, , 600, A30, 10.1051/0004-6361/201629705
Claret , A. 2017, , 600, A30, 10.1051/0004-6361/201629705
2017 doi
-
[17]
Coughlin , J. L. 2017, Description of the TCERT Vetting Reports for Data Release 25 , Kepler Science Document KSCI-19105-002, id. 15. Edited by Natalie Batalha and Michael R. Haas
2017
-
[18]
L., Thompson , S
Coughlin , J. L., Thompson , S. E., Bryson , S. T., et al. 2014, , 147, 119, 10.1088/0004-6256/147/5/119
2014 doi
-
[19]
L., Mullally , F., Thompson , S
Coughlin , J. L., Mullally , F., Thompson , S. E., et al. 2016, , 224, 12, 10.3847/0067-0049/224/1/12
2016 doi
-
[20]
J., et al
Dattilo , A., Vanderburg , A., Shallue , C. J., et al. 2019, , 157, 169, 10.3847/1538-3881/ab0e12
2019 doi
-
[21]
I., & Johnson , J
Dawson , R. I., & Johnson , J. A. 2012, , 756, 122, 10.1088/0004-637X/756/2/122
2012 doi
-
[22]
2024, , 531, 1276, 10.1093/mnras/stae1152
Dholakia , S., Palethorpe , L., Venner , A., et al. 2024, , 531, 1276, 10.1093/mnras/stae1152
2024 doi
-
[23]
Dransfield , G., Timmermans , M., Triaud , A. H. M. J., et al. 2024, , 527, 35, 10.1093/mnras/stad1439
2024 doi
-
[24]
Eschen , Y. N. E., & Kunimoto , M. 2024, , 531, 5053, 10.1093/mnras/stae1496
2024 doi
-
[25]
2022, , 666, A10, 10.1051/0004-6361/202243731
Esparza-Borges , E., Parviainen , H., Murgas , F., et al. 2022, , 666, A10, 10.1051/0004-6361/202243731
2022 doi
-
[26]
L., Plavchan , P., Bianco , S
Feliz , D. L., Plavchan , P., Bianco , S. N., et al. 2021, , 161, 247, 10.3847/1538-3881/abedb3
2021 doi
-
[27]
2021, Research Notes of the American Astronomical Society, 5, 91, 10.3847/2515-5172/abf56b
Fiscale , S., Ciaramella , A., Inno , L., et al. 2021, Research Notes of the American Astronomical Society, 5, 91, 10.3847/2515-5172/abf56b
2021 doi
-
[28]
D., Jensen , E
Giacalone , S., Dressing , C. D., Jensen , E. L. N., et al. 2021, , 161, 24, 10.3847/1538-3881/abc6af
2021 doi
-
[29]
J., MacDougall , M
Gilbert , G. J., MacDougall , M. G., & Petigura , E. A. 2022, , 164, 92, 10.3847/1538-3881/ac7f2f
2022 doi
-
[30]
Gregory , P. C. 2011, , 410, 94, 10.1111/j.1365-2966.2010.17428.x
2011
-
[31]
M., Seager , S., Huang , C
Guerrero , N. M., Seager , S., Huang , C. X., et al. 2021, , 254, 39, 10.3847/1538-4365/abefe1
2021 doi
-
[32]
R., Millman, K
Harris, C. R., Millman, K. J., van der Walt, S. J., et al. 2020, Nature, 585, 357, 10.1038/s41586-020-2649-2
2020 doi
-
[33]
D., & Bakos , G
Hartman , J. D., & Bakos , G. \'A . 2016, Astronomy and Computing, 17, 1, 10.1016/j.ascom.2016.05.006
2016 doi
-
[34]
D., Bayliss , D., Brahm , R., et al
Hartman , J. D., Bayliss , D., Brahm , R., et al. 2024, , 168, 202, 10.3847/1538-3881/ad6f07
2024 doi
-
[35]
Hastings , W. K. 1970, Biometrika, 57, 97, 10.1093/biomet/57.1.97
1970 doi
-
[36]
J., Mulders , G
Hippke , M., David , T. J., Mulders , G. D., & Heller , R. 2019, , 158, 143, 10.3847/1538-3881/ab3984
2019 doi
-
[37]
2022, cuvarbase: fast period finding utilities for GPUs , Astrophysics Source Code Library, record ascl:2210.030
Hoffman , J. 2022, cuvarbase: fast period finding utilities for GPUs , Astrophysics Source Code Library, record ascl:2210.030
2022
-
[38]
X., Vanderburg , A., P \'a l , A., et al
Huang , C. X., Vanderburg , A., P \'a l , A., et al. 2020, Research Notes of the American Astronomical Society, 4, 204, 10.3847/2515-5172/abca2e
2020 doi
-
[39]
2020, TESS Lightcurves From The MIT Quick-Look Pipeline ("QLP"), STScI/MAST, 10.17909/T9-R086-E880
Huang, Chelsea X. 2020, TESS Lightcurves From The MIT Quick-Look Pipeline ("QLP"), STScI/MAST, 10.17909/T9-R086-E880
2020 doi
-
[40]
Hunter, J. D. 2007, Computing in Science & Engineering, 9, 90, 10.1109/MCSE.2007.55
2007 doi
-
[41]
M., Chandrasekaran, H., McCauliff, S
Jenkins, J. M., Chandrasekaran, H., McCauliff, S. D., et al. 2010, in Software and Cyberinfrastructure for Astronomy, ed. N. M. Radziwill & A. Bridger, Vol. 7740, International Society for Optics and Photonics (SPIE), 77400D, 10.1117/12.856764
2010 doi
-
[43]
M., Twicken , J
Jenkins , J. M., Twicken , J. D., McCauliff , S., et al. 2016 b , in , Vol. 9913, Software and Cyberinfrastructure for Astronomy IV, 99133E, 10.1117/12.2233418
2016 doi
-
[44]
2023, , 523, 1182, 10.1093/mnras/stad1492
Kipping , D. 2023, , 523, 1182, 10.1093/mnras/stad1492
2023 doi
-
[45]
Kipping , D. M. 2016, , 455, 1680, 10.1093/mnras/stv2379
2016 doi
-
[46]
I., Witzke , V., et al
Kostogryz , N., Shapiro , A. I., Witzke , V., et al. 2023, Research Notes of the American Astronomical Society, 7, 39, 10.3847/2515-5172/acc180
2023 doi
-
[47]
B., Mullally , S
Kostov , V. B., Mullally , S. E., Quintana , E. V., et al. 2019, , 157, 124, 10.3847/1538-3881/ab0110
2019 doi
-
[48]
2002, , 391, 369, 10.1051/0004-6361:20020802
Kov \'a cs , G., Zucker , S., & Mazeh , T. 2002, , 391, 369, 10.1051/0004-6361:20020802
2002 doi
- [49]
-
[50]
2025, mkunimoto/LEO-vetter: v0.6.1, Zenodo, 10.5281/ZENODO.16945146
Kunimoto, M. 2025, mkunimoto/LEO-vetter: v0.6.1, Zenodo, 10.5281/ZENODO.16945146
2025 doi
-
[51]
2022 a , Research Notes of the American Astronomical Society, 6, 236, 10.3847/2515-5172/aca158
Kunimoto , M., Tey , E., Fong , W., et al. 2022 a , Research Notes of the American Astronomical Society, 6, 236, 10.3847/2515-5172/aca158
2022 doi
-
[52]
2022 b , , 259, 33, 10.3847/1538-4365/ac5688
Kunimoto , M., Daylan , T., Guerrero , N., et al. 2022 b , , 259, 33, 10.3847/1538-4365/ac5688
2022 doi
-
[53]
H., et al
Kuzuhara , M., Fukui , A., Livingston , J. H., et al. 2024, , 967, L21, 10.3847/2041-8213/ad3642
2024 doi
-
[54]
D., et al
Li , J., Tenenbaum , P., Twicken , J. D., et al. 2019, , 131, 024506, 10.1088/1538-3873/aaf44d
2019 doi
- [55]
-
[56]
J., Marcy , G
Lissauer , J. J., Marcy , G. W., Bryson , S. T., et al. 2014, , 784, 44, 10.1088/0004-637X/784/1/44
2014 doi
-
[57]
2002, , 580, L171, 10.1086/345520
Mandel , K., & Agol , E. 2002, , 580, L171, 10.1086/345520
2002 doi
-
[58]
D., Jenkins , J
McCauliff , S. D., Jenkins , J. M., Catanzarite , J., et al. 2015, , 806, 6, 10.1088/0004-637X/806/1/6
2015 doi
-
[59]
2010, in P roceedings of the 9th P ython in S cience C onference, ed
McKinney , W. 2010, in P roceedings of the 9th P ython in S cience C onference, ed. S t\'efan van der W alt & J arrod M illman, 56 -- 61, 10.25080/Majora-92bf1922-00a
2010 doi
-
[60]
W., Rosenbluth , M
Metropolis , N., Rosenbluth , A. W., Rosenbluth , M. N., Teller , A. H., & Teller , E. 1953, , 21, 1087, 10.1063/1.1699114
1953 doi
-
[61]
2020, , 498, 1726, 10.1093/mnras/staa2438
Montalto , M., Borsato , L., Granata , V., et al. 2020, , 498, 1726, 10.1093/mnras/staa2438
2020 doi
-
[62]
Morton , T. D. 2012, , 761, 6, 10.1088/0004-637X/761/1/6
2012 doi
-
[63]
2025, LMFIT: Non-Linear Least-Squares Minimization and Curve-Fitting for Python, 1.3.3, Zenodo, 10.5281/zenodo.15014437
Newville, M., Otten, R., Nelson, A., et al. 2025, LMFIT: Non-Linear Least-Squares Minimization and Curve-Fitting for Python, 1.3.3, Zenodo, 10.5281/zenodo.15014437
2025 doi
-
[64]
2025, Exoplanet Follow-up Observing Program Web Service, IPAC, 10.26134/ExoFOP5
NExScI. 2025, Exoplanet Follow-up Observing Program Web Service, IPAC, 10.26134/ExoFOP5
2025 doi
-
[65]
2022, , 91, 101693, 10.1016/j.newast.2021.101693
Ofman , L., Averbuch , A., Shliselberg , A., et al. 2022, , 91, 101693, 10.1016/j.newast.2021.101693
2022
-
[66]
P., Ansdell , M., Ioannou , Y., et al
Osborn , H. P., Ansdell , M., Ioannou , Y., et al. 2020, , 633, A53, 10.1051/0004-6361/201935345
2020 doi
-
[67]
2006, , 373, 231, 10.1111/j.1365-2966.2006.11012.x
Pont , F., Zucker , S., & Queloz , D. 2006, , 373, 231, 10.1111/j.1365-2966.2006.11012.x
2006
-
[68]
E., et al
Prsa , A., Kochoska , A., Conroy , K. E., et al. 2022, VizieR Online Data Catalog: TESS Eclipsing Binary stars. I. Sectors 1-26 (Prsa+, 2022) , VizieR On-line Data Catalog: J/ApJS/258/16. Originally published in: 2022ApJS..258...16P, 10.26093/cds/vizier.22580016
2022 doi
-
[69]
2021, , 502, 2845, 10.1093/mnras/stab203
Rao , S., Mahabal , A., Rao , N., & Raghavendra , C. 2021, , 502, 2845, 10.1093/mnras/stab203
2021 doi
-
[70]
R., Winn , J
Ricker , G. R., Winn , J. N., Vanderspek , R., et al. 2015, Journal of Astronomical Telescopes, Instruments, and Systems, 1, 014003, 10.1117/1.JATIS.1.1.014003
2015 doi
-
[71]
2016, Kepler: Kepler Transit Model Codebase Release
Rowe , J. 2016, Kepler: Kepler Transit Model Codebase Release. , 1.0, Zenodo, 10.5281/zenodo.60297
2016 doi
-
[72]
F., Coughlin , J
Rowe , J. F., Coughlin , J. L., Antoci , V., et al. 2015, , 217, 16, 10.1088/0067-0049/217/1/16
2015 doi
-
[73]
J., & Vanderburg , A
Shallue , C. J., & Vanderburg , A. 2018, , 155, 94, 10.3847/1538-3881/aa9e09
2018 doi
-
[74]
G., Oelkers , R
Stassun , K. G., Oelkers , R. J., Paegert , M., et al. 2019, , 158, 138, 10.3847/1538-3881/ab3467
2019 doi
-
[75]
Team, T. P. D. 2020, pandas-dev/pandas: Pandas, latest, Zenodo, 10.5281/zenodo.3509134
2020 doi
-
[76]
2023, , 165, 95, 10.3847/1538-3881/acad85
Tey , E., Moldovan , D., Kunimoto , M., et al. 2023, , 165, 95, 10.3847/1538-3881/acad85
2023 doi
-
[77]
E., Coughlin , J
Thompson , S. E., Coughlin , J. L., Hoffman , K., et al. 2018, , 235, 38, 10.3847/1538-4365/aab4f9
2018 doi
-
[78]
Valizadegan , H., Martinho , M. J. S., Wilkens , L. S., et al. 2022, , 926, 120, 10.3847/1538-4357/ac4399
2022 doi
-
[79]
E., et al
Virtanen, P., Gommers, R., Oliphant, T. E., et al. 2020, Nature Methods, 17, 261, 10.1038/s41592-019-0686-2
2020 doi
-
[80]
2019, , 158, 25, 10.3847/1538-3881/ab21d6
Yu , L., Vanderburg , A., Huang , C., et al. 2019, , 158, 25, 10.3847/1538-3881/ab21d6
2019 doi
-
[81]
K., Christiansen , J
Zink , J. K., Christiansen , J. L., & Hansen , B. M. S. 2019, , 483, 4479, 10.1093/mnras/sty3463
2019 doi
-
[82]
K., Hardegree-Ullman , K
Zink , J. K., Hardegree-Ullman , K. K., Christiansen , J. L., et al. 2020, , 159, 154, 10.3847/1538-3881/ab7448
2020 doi
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