Recognition: no theorem link
NASA's Pandora SmallSat Mission: Simulating the Impact of Stellar Photospheric Heterogeneity and Its Correction
Pith reviewed 2026-05-15 15:56 UTC · model grok-4.3
The pith
Simulations show NASA's Pandora mission recovers stellar temperatures to 30 K and reduces contamination to under 10 ppm for simple spot patterns using out-of-transit data.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Given accurate models, Bayesian retrievals of Pandora spectrophotometry recover photospheric temperatures with typical uncertainties of ≈30 K, with no significant bias. Models with two spectral components are strongly favored in 95 percent of cases. For simple spot distributions, contamination signals of 10^2-10^3 ppm are reduced to ≲10 ppm, well below Pandora's expected transmission spectroscopy precision of 30-100 ppm. For complex distributions geometric degeneracies leave residuals at the 10^3 ppm level that require additional constraints such as spot-crossing events.
What carries the argument
Bayesian retrievals of multi-component stellar spectra from simulated out-of-transit Pandora spectrophotometry that incorporate time-dependent activity, instrument response functions, and noise models.
If this is right
- Contamination of 100-1000 ppm drops to ≲10 ppm when spot distributions are simple.
- Two-component models are preferred once spot filling factors exceed a 0.3 percent detection threshold.
- Complex spot geometries leave 1000 ppm residuals that cannot be corrected from stellar data alone.
- The mission can flag targets where extra information such as spot crossings or joint stellar-planetary retrievals will be required.
Where Pith is reading between the lines
- Pandora data on stars with simple activity could be used to prioritize targets for transmission spectroscopy with other facilities.
- If real stellar heterogeneity is often more complex than the tested scenarios, many observations may still need multi-epoch or multi-instrument follow-up.
- Incorporating the transmission spectrum itself into the retrieval could reduce residuals even in degenerate cases.
- The same simulation approach could be applied to other planned small-satellite or ground-based stellar monitoring programs.
Load-bearing premise
The eight constructed stellar activity scenarios, assumed instrument responses, and noise models accurately represent real Pandora observations, and the retrieval models contain all relevant physics.
What would settle it
Compare retrieved temperatures and residual contamination levels from actual Pandora observations against independent constraints such as high-resolution spectroscopy or observed spot-crossing events during transits.
Figures
read the original abstract
Stellar photospheric heterogeneity is a dominant astrophysical systematic impacting exoplanet transmission spectroscopy. NASA's Pandora SmallSat Mission is designed to address this challenge through contemporaneous visible photometry and NIR spectroscopy of exoplanet host stars. Here we present an end-to-end simulation study quantifying Pandora's ability to infer stellar photospheric properties and correct stellar contamination using out-of-transit observations. We construct eight representative stellar activity scenarios and generate 160 simulated Pandora datasets, incorporating time-dependent stellar spectra, instrument response, and noise. Given accurate models, Bayesian retrievals of Pandora spectrophotometry recover photospheric temperatures with typical uncertainties of ${\approx}30$ K, with no significant bias. Models with two spectral components (i.e., quiescent photosphere and spots) are strongly favored in 95% of cases; one-component models are preferred when true spot filling factors fall below a detection threshold of ${\approx}0.3$%. We propagate the true and inferred stellar parameters to compute true, inferred, and residual contamination signals under physically motivated spot geometries. For simple spot distributions, contamination signals of $10^2{-}10^3$ ppm are reduced to ${\lesssim}10$ ppm, well below Pandora's expected transmission spectroscopy precision (30$-$100 ppm). For more complex spot distributions, geometric degeneracies limit deterministic corrections, leaving residual contamination at the $10^3$ ppm level that must be mitigated using additional constraints, such as spot-crossing events and joint stellar-planetary retrievals of transmission spectra. These results define regimes in which stellar contamination can be corrected from stellar observations alone and show how Pandora stellar observations can identify cases where additional information is required.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The manuscript presents an end-to-end simulation study of NASA's Pandora SmallSat mission, constructing eight stellar activity scenarios to generate 160 synthetic datasets that incorporate time-dependent spectra, instrument response, and noise. Bayesian retrievals on out-of-transit spectrophotometry are used to recover photospheric temperatures and spot parameters, which are then propagated to compute true, inferred, and residual stellar contamination signals in transmission spectroscopy under different spot geometries.
Significance. If the results hold, the work provides a quantitative benchmark for Pandora's ability to mitigate stellar heterogeneity—a dominant systematic in exoplanet transmission spectroscopy—showing that contamination can be reduced from 10^2-10^3 ppm to ≲10 ppm for simple spot distributions, below the mission's expected 30-100 ppm precision. The simulation framework with time-dependent spectra and explicit model-selection tests adds practical value for mission planning and data analysis strategies.
major comments (2)
- [Abstract and §4] Abstract and §4 (retrieval results): the reported temperature recovery to ≈30 K with no significant bias and contamination reduction to ≲10 ppm are conditioned on the retrieval model exactly matching the two-component (quiescent + spots) generative model used to create the data; no simulations are shown for misspecification cases such as faculae (+300-500 K) or vertical temperature gradients, which would bias the posteriors on T_phot and the derived residual contamination even if instrument noise is matched.
- [§3.2] §3.2 (model selection): the finding that two-component models are strongly favored in 95% of cases and that one-component models are preferred only below a 0.3% filling-factor threshold is derived under perfect model match; this threshold and the reported detection performance may shift if the true stellar spectrum includes unmodeled components, undermining the claim that Pandora observations alone can identify when additional constraints are required.
minor comments (2)
- [Figure 5] Figure 5 (contamination propagation): the caption and text should explicitly state the assumed spot latitudes and longitudes used for the 'simple' versus 'complex' geometries, as these directly affect the reported residual levels of 10^3 ppm.
- [§2.3] §2.3 (noise model): the description of the noise model could include a brief statement on whether correlated noise (e.g., from instrument systematics) is included, to clarify the realism of the 30-100 ppm precision benchmark.
Simulated Author's Rebuttal
We thank the referee for their constructive comments, which correctly identify key assumptions in our simulation framework. We address each point below and have made partial revisions to clarify the scope and limitations of the results without overclaiming generality.
read point-by-point responses
-
Referee: [Abstract and §4] Abstract and §4 (retrieval results): the reported temperature recovery to ≈30 K with no significant bias and contamination reduction to ≲10 ppm are conditioned on the retrieval model exactly matching the two-component (quiescent + spots) generative model used to create the data; no simulations are shown for misspecification cases such as faculae (+300-500 K) or vertical temperature gradients, which would bias the posteriors on T_phot and the derived residual contamination even if instrument noise is matched.
Authors: We agree that the reported temperature recovery (~30 K, unbiased) and contamination reduction (to ≲10 ppm for simple spots) assume exact model match between retrieval and generative models. Our study is scoped to the two-component case as a baseline for Pandora's performance when this model is appropriate, which is common for many active stars. We did not run misspecification tests (faculae or gradients) as they fall outside the current simulation suite. The manuscript already highlights that complex geometries leave ~1000 ppm residuals, indicating limits. We will add explicit caveats in the abstract and §4 noting that results are conditioned on model correctness and that misspecification could introduce biases, recommending future work on such cases. revision: partial
-
Referee: [§3.2] §3.2 (model selection): the finding that two-component models are strongly favored in 95% of cases and that one-component models are preferred only below a 0.3% filling-factor threshold is derived under perfect model match; this threshold and the reported detection performance may shift if the true stellar spectrum includes unmodeled components, undermining the claim that Pandora observations alone can identify when additional constraints are required.
Authors: The model selection results (two-component favored in 95% of cases; one-component below ~0.3% filling factor) are derived under perfect model match. We acknowledge that unmodeled components could shift the Bayes factor thresholds and detection performance. Our claim is limited to showing that Pandora data can distinguish models and flag cases needing extra constraints when the two-component assumption holds. We will revise §3.2 to explicitly state this assumption and note that real applications may require cross-validation with other data. revision: partial
Circularity Check
No circularity: forward-modeling with known ground truth provides external benchmark
full rationale
The paper constructs eight stellar activity scenarios, generates 160 synthetic Pandora datasets with known inputs (time-dependent spectra, instrument response, noise), then performs Bayesian retrievals and compares recovered photospheric temperatures and contamination signals directly to those injected ground-truth values. This is a standard validation test against external benchmarks rather than any reduction by construction. No self-definitional steps, fitted inputs renamed as predictions, or load-bearing self-citations appear in the abstract or described chain. The central claims (≈30 K recovery with no bias, contamination reduced to ≲10 ppm for simple spots) are conditioned on model match but remain falsifiable against the known inputs, qualifying as self-contained simulation work.
Axiom & Free-Parameter Ledger
free parameters (2)
- spot filling factor
- photospheric and spot temperatures
axioms (2)
- domain assumption Stellar spectra can be represented as linear combinations of quiescent photosphere and spot spectral components.
- domain assumption Instrument response and noise properties are known and correctly modeled in the simulations.
Reference graph
Works this paper leans on
-
[1]
Ahrer, E.-M., Stevenson, K. B., Mansfield, M., et al. 2023, Nature, 614, 653, doi: 10.1038/s41586-022-05590-4
-
[2]
2025, ApJL, 985, L10, doi: 10.3847/2041-8213/add010
Ahrer, E.-M., Radica, M., Piaulet-Ghorayeb, C., et al. 2025, ApJL, 985, L10, doi: 10.3847/2041-8213/add010
-
[3]
2023, ARA&A, 61, 329, doi: 10.1146/annurev-astro-052920-103508
Aigrain, S., & Foreman-Mackey, D. 2023, ARA&A, 61, 329, doi: 10.1146/annurev-astro-052920-103508
-
[4]
Alderson, L., Wakeford, H. R., Alam, M. K., et al. 2023, Nature, 614, 664, doi: 10.1038/s41586-022-05591-3
-
[5]
Allen, N. H., Espinoza, N., Boehm, V. A., et al. 2026, AJ, 171, 105, doi: 10.3847/1538-3881/ae28cb
-
[6]
M., Bonfils, X., Forveille, T., et al
Almenara, J. M., Bonfils, X., Forveille, T., et al. 2022, A&A, 667, L11, doi: 10.1051/0004-6361/202244791
-
[7]
Apai, D., Milster, T. D., Kim, D. W., et al. 2019, AJ, 158, 83, doi: 10.3847/1538-3881/ab2631 Astropy Collaboration, Robitaille, T. P., Tollerud, E. J., et al. 2013, A&A, 558, A33, doi: 10.1051/0004-6361/201322068 Astropy Collaboration, Price-Whelan, A. M., Sip˝ ocz, B. M., et al. 2018, AJ, 156, 123, doi: 10.3847/1538-3881/aabc4f Astropy Collaboration, Pr...
-
[8]
Barclay, T., Quintana, E. V., Col´ on, K., et al. 2025, arXiv e-prints, arXiv:2502.09730, doi: 10.48550/arXiv.2502.09730
-
[9]
Barnes, J. R., Jeffers, S. V., Haswell, C. A., et al. 2017, Monthly Notices of the Royal Astronomical Society, 471, 811, doi: 10.1093/mnras/stx1482
-
[10]
Barnes, J. R., Jeffers, S. V., Jones, H. R. A., et al. 2015, The Astrophysical Journal, 812, 42, doi: 10.1088/0004-637X/812/1/42
-
[11]
2013, ApJ, 778, 153, doi: 10.1088/0004-637X/778/2/153
Benneke, B., & Seager, S. 2013, ApJ, 778, 153, doi: 10.1088/0004-637X/778/2/153
-
[12]
Berardo, D., de Wit, J., & Rackham, B. V. 2024, ApJL, 961, L18, doi: 10.3847/2041-8213/ad1b5b
-
[13]
Berdyugina, S. V. 2005, Living Reviews in Solar Physics, 2, 8, doi: 10.12942/lrsp-2005-8
-
[14]
2021, The Exoplanet Characterization Toolkit (ExoCTK), 1.0.0 Zenodo, doi: 10.5281/zenodo.4556063
Bourque, M., Espinoza, N., Filippazzo, J., et al. 2021, The Exoplanet Characterization Toolkit (ExoCTK), 1.0.0 Zenodo, doi: 10.5281/zenodo.4556063
-
[15]
Bourque, M., Espinoza, N., Filippazzo, J., et al. 2022, ExoCTK: Exoplanet Characterization Tool Kit,, Astrophysics Source Code Library, record ascl:2207.012
work page 2022
-
[16]
The TESS All-Sky Rotation Survey: Periods for 1,046,317 Stars Within 500 pc
Boyle, A. W., Bouma, L. G., & Mann, A. W. 2026, arXiv e-prints, arXiv:2603.05586, doi: 10.48550/arXiv.2603.05586
work page internal anchor Pith review Pith/arXiv arXiv doi:10.48550/arxiv.2603.05586 2026
-
[17]
2021, The Journal of Open Source Software, 6, 3001, doi: 10.21105/joss.03001 22Rackham et al
Buchner, J. 2021, The Journal of Open Source Software, 6, 3001, doi: 10.21105/joss.03001 22Rackham et al
-
[18]
Chakraborty, H., Almenara, J. M., Lendl, M., et al. 2025, A&A, 702, A100, doi: 10.1051/0004-6361/202555998
-
[19]
Green, G. M. 2015, ApJ, 812, 128, doi: 10.1088/0004-637X/812/2/128
-
[20]
Espinoza, N., & Perrin, M. D. 2026, in Handbook of Exoplanets (Springer International Publishing AG), 216, doi: 10.1007/978-3-319-30648-3 216-1
-
[21]
Espinoza, N., Rackham, B. V., Jord´ an, A., et al. 2019, MNRAS, 482, 2065, doi: 10.1093/mnras/sty2691
-
[22]
Espinoza, N., Allen, N. H., Glidden, A., et al. 2025, ApJL, 990, L52, doi: 10.3847/2041-8213/adf42e
-
[23]
D., Radica, M., Welbanks, L., et al
Feinstein, A. D., Radica, M., Welbanks, L., et al. 2023, Nature, 614, 670, doi: 10.1038/s41586-022-05674-1
-
[24]
Foote, T. O., Barclay, T., Hedges, C. L., et al. 2023, Journal of Astronomical Telescopes, Instruments, and Systems, 9, 047001, doi: 10.1117/1.JATIS.9.4.047001
-
[25]
2025, The Journal of Open Source Software, 10, 8305, doi: 10.21105/joss.08305
Garcia, L., Rackham, B., & Panwar, V. 2025, The Journal of Open Source Software, 10, 8305, doi: 10.21105/joss.08305
-
[26]
Garcia, L. J., Moran, S. E., Rackham, B. V., et al. 2022, A&A, 665, A19, doi: 10.1051/0004-6361/202142603
-
[27]
Nature 585(7825), 357–362 (2020) https://doi.org/ 10.1038/s41586-020-2649-2
Harris, C. R., Millman, K. J., van der Walt, S. J., et al. 2020, Nature, 585, 357, doi: 10.1038/s41586-020-2649-2
-
[28]
H., Barman, T., Baron, E., Aufdenberg, J
Hauschildt, P. H., Barman, T., Baron, E., Aufdenberg, J. P., & Schweitzer, A. 2025, A&A, 698, A47, doi: 10.1051/0004-6361/202554171
-
[29]
Hedges, C., Holcomb, R. J., Hord, B., et al. 2024, in Software and Cyberinfrastructure for Astronomy VIII, Vol. 13101 (SPIE), 182–190, doi: 10.1117/12.3020326
-
[30]
2014, ApJ, 783, 9, doi: 10.1088/0004-637X/783/1/9
Hirano, T., Sanchis-Ojeda, R., Takeda, Y., et al. 2014, ApJ, 783, 9, doi: 10.1088/0004-637X/783/1/9
-
[31]
Hunter, J. D. 2007, Computing in Science and Engineering, 9, 90, doi: 10.1109/MCSE.2007.55
-
[32]
O., Wende-von Berg, S., Dreizler, S., et al
Husser, T. O., Wende-von Berg, S., Dreizler, S., et al. 2013, A&A, 553, A6, doi: 10.1051/0004-6361/201219058
-
[33]
2024, Astronomy and Astrophysics, 687, A138, doi: 10.1051/0004-6361/202449541
Ilin, E., Poppenh¨ ager, K., Stelzer, B., & Dsouza, D. 2024, Astronomy and Astrophysics, 687, A138, doi: 10.1051/0004-6361/202449541
-
[34]
Iyer, A. R., & Line, M. R. 2020, ApJ, 889, 78, doi: 10.3847/1538-4357/ab612e JWST Transiting Exoplanet Community Early Release Science Team, Ahrer, E.-M., Alderson, L., et al. 2023, Nature, 614, 649, doi: 10.1038/s41586-022-05269-w
-
[35]
2025, arXiv e-prints, arXiv:2506.05392, doi: 10.48550/arXiv.2506.05392
Kipping, D., & Benneke, B. 2025, arXiv e-prints, arXiv:2506.05392, doi: 10.48550/arXiv.2506.05392
-
[36]
Kirk, J., Rackham, B. V., MacDonald, R. J., et al. 2021, AJ, 162, 34, doi: 10.3847/1538-3881/abfcd2
-
[37]
E., Schutte, M., Hebb, L., et al
Libby-Roberts, J. E., Schutte, M., Hebb, L., et al. 2023, AJ, 165, 249, doi: 10.3847/1538-3881/accc2f
-
[38]
2023, ApJL, 955, L22, doi: 10.3847/2041-8213/acf7c4
Lim, O., Benneke, B., Doyon, R., et al. 2023, ApJL, 955, L22, doi: 10.3847/2041-8213/acf7c4
-
[39]
May, E. M., MacDonald, R. J., Bennett, K. A., et al. 2023, ApJL, 959, L9, doi: 10.3847/2041-8213/ad054f
-
[40]
B., McQuillan, A., & Goldstein, E
Mazeh, T., Perets, H. B., McQuillan, A., & Goldstein, E. S. 2015, ApJ, 801, 3, doi: 10.1088/0004-637X/801/1/3
-
[41]
2010, in Proceedings of the 9th Python in Science Conference, ed
McKinney, W. 2010, in Proceedings of the 9th Python in Science Conference, ed. St´ efan van der Walt & Jarrod Millman, 56 – 61, doi: 10.25080/Majora-92bf1922-00a
-
[42]
2014, ApJS, 211, 24, doi: 10.1088/0067-0049/211/2/24
McQuillan, A., Mazeh, T., & Aigrain, S. 2014, ApJS, 211, 24, doi: 10.1088/0067-0049/211/2/24
-
[43]
Moran, S. E., Stevenson, K. B., Sing, D. K., et al. 2023, ApJL, 948, L11, doi: 10.3847/2041-8213/accb9c
-
[44]
2025, AJ, 170, 204, doi: 10.3847/1538-3881/ade2df
Mori, M., Fukui, A., Hirano, T., et al. 2025, AJ, 170, 204, doi: 10.3847/1538-3881/ade2df
-
[45]
Hawley, S. L. 2017, ApJ, 846, 99, doi: 10.3847/1538-4357/aa8555
-
[46]
Murray, C. A., Garcia, L., Rackham, B. V., et al. 2026, arXiv e-prints, arXiv:2603.15414. https://arxiv.org/abs/2603.15414
-
[47]
Narrett, I. S., Rackham, B. V., & de Wit, J. 2024, AJ, 167, 107, doi: 10.3847/1538-3881/ad1f6c
-
[48]
R., Irwin, J., Charbonneau, D., et al
Newton, E. R., Irwin, J., Charbonneau, D., et al. 2016, ApJ, 821, 93, doi: 10.3847/0004-637X/821/2/93
-
[49]
Niraula, P., Rackham, B. V., de Wit, J., et al. 2026, arXiv e-prints, arXiv:2603.24585, doi: 10.48550/arXiv.2603.24585
-
[50]
Norris, C. M., Beeck, B., Unruh, Y. C., et al. 2017, A&A, 605, A45, doi: 10.1051/0004-6361/201629879
-
[51]
Norris, C. M., Unruh, Y. C., Witzke, V., et al. 2023, MNRAS, 524, 1139, doi: 10.1093/mnras/stad1738
-
[52]
V., Madhusudhan, N., & Apai, D
Pinhas, A., Rackham, B. V., Madhusudhan, N., & Apai, D. 2018, MNRAS, 480, 5314, doi: 10.1093/mnras/sty2209
-
[53]
Quintana, E. V., Dotson, J. L., Col´ on, K. D., et al. 2024, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol. 13092, Space Telescopes and Instrumentation 2024: Optical, Infrared, and Millimeter Wave, ed. L. E. Coyle, S. Matsuura, & M. D. Perrin, 1309214, doi: 10.1117/12.3020633
-
[54]
2017, ApJ, 834, 151, doi: 10.3847/1538-4357/aa4f6c
Rackham, B., Espinoza, N., Apai, D., et al. 2017, ApJ, 834, 151, doi: 10.3847/1538-4357/aa4f6c
-
[55]
Rackham, B. V. 2023, speclib, 0.0-beta.0 Zenodo, doi: 10.5281/zenodo.7868050
-
[56]
Rackham, B. V. 2025, speclib: Tools for working with stellar spectral libraries,, Astrophysics Source Code Library, record ascl:2505.001
work page 2025
-
[57]
Rackham, B. V., Apai, D., & Giampapa, M. S. 2018, ApJ, 853, 122, doi: 10.3847/1538-4357/aaa08c Pandora Stellar Contamination Simulated Performance23
-
[58]
Rackham, B. V., Apai, D., & Giampapa, M. S. 2019, AJ, 157, 96, doi: 10.3847/1538-3881/aaf892
-
[59]
Rackham, B. V., & de Wit, J. 2024, AJ, 168, 82, doi: 10.3847/1538-3881/ad5833
-
[60]
V., Espinoza, N., Berdyugina, S
Rackham, B. V., Espinoza, N., Berdyugina, S. V., et al. 2023, RAS Techniques and Instruments, 2, 148, doi: 10.1093/rasti/rzad009
-
[61]
Rasmussen, C. E., & Williams, C. K. I. 2006, Gaussian Processes for Machine Learning (The MIT Press)
work page 2006
-
[62]
Rathcke, A. D., Buchhave, L. A., de Wit, J., et al. 2025, ApJL, 979, L19, doi: 10.3847/2041-8213/ada5c7
-
[63]
2026, AJ, 171, 263, doi: 10.3847/1538-3881/ae4d3c
Rotman, Y., McGill, P., Welbanks, L., et al. 2026, AJ, 171, 263, doi: 10.3847/1538-3881/ae4d3c
-
[64]
Rustamkulov, Z., Sing, D. K., Liu, R., & Wang, A. 2022, ApJL, 928, L7, doi: 10.3847/2041-8213/ac5b6f
-
[65]
Rustamkulov, Z., Sing, D. K., Mukherjee, S., et al. 2023, Nature, 614, 659, doi: 10.1038/s41586-022-05677-y
-
[66]
Sagynbayeva, S., Farr, W. M., Morris, B. M., & Luger, R. 2025, ApJ, 990, 32, doi: 10.3847/1538-4357/adf6be
-
[67]
Shapiro, A. I., Solanki, S. K., Krivova, N. A., et al. 2014, A&A, 569, A38, doi: 10.1051/0004-6361/201323086
-
[68]
Solanki, S. K. 2003, A&A Rv, 11, 153, doi: 10.1007/s00159-003-0018-4
-
[69]
W., Garc´ ıa-Mej´ ıa, J., et al
Tamburo, P., Yee, S. W., Garc´ ıa-Mej´ ıa, J., et al. 2025, AJ, 170, 200, doi: 10.3847/1538-3881/adf72f TRAPPIST-1 JWST Community Initiative, de Wit, J.,
-
[70]
2024, Nature Astronomy, 8, 810, doi: 10.1038/s41550-024-02298-5
Doyon, R., et al. 2024, Nature Astronomy, 8, 810, doi: 10.1038/s41550-024-02298-5
-
[71]
2008, Contemporary Physics, 49, 71, doi: 10.1080/00107510802066753
Trotta, R. 2008, Contemporary Physics, 49, 71, doi: 10.1080/00107510802066753
-
[72]
Virtanen, P., Gommers, R., Oliphant, T. E., et al. 2020, Nature Methods, 17, 261, doi: 10.1038/s41592-019-0686-2
-
[73]
Wakeford, H. R., Lewis, N. K., Fowler, J., et al. 2019, AJ, 157, 11, doi: 10.3847/1538-3881/aaf04d
-
[74]
Witzke, V., Shapiro, A. I., Kostogryz, N. M., et al. 2022, ApJL, 941, L35, doi: 10.3847/2041-8213/aca671
-
[75]
Zhang, Z., Zhou, Y., Rackham, B. V., & Apai, D. 2018, AJ, 156, 178, doi: 10.3847/1538-3881/aade4f
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.