REVIEW 2 major objections 5 minor 1 cited by
Searching for GEMS: TOI-5916 b & TOI-6158 b are two Saturn-density planets orbiting M2 dwarfs
T0 review · 2 major / 5 minor · reviewed 2026-08-04 · deepseek-v4-flash
Pith's one-line read The paper confirms two Saturn-density giant exoplanets orbiting M2 dwarf stars and reports a bias-corrected trend toward closer orbits among M-dwarf giant planets.
desk verdict Two new GEMS confirmations, one clean and one whose Saturn-density label rests on a grazing transit and unconstrained dilution; the population trend is suggestive but not yet tested. 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 argument rests on a joint Bayesian fit of transit light curves and radial velocities for each system, which simultaneously constrains the orbital parameters, planetary radius, and mass. For one target, the fit includes per-observation dilution terms to correct for unresolved background stars; the grazing geometry of that transit makes the dilution difficult to pin down. The population comparison uses a weighted empirical cumulative distribution, with each system weighted by the inverse of its geometric transit probability, to correct for the observational bias favoring close-in transiting planets.
What would settle it
A high-cadence, full-transit observation of TOI-6158 b with a space-based or large ground-based telescope would measure the transit shape and impact parameter precisely, determining whether the inferred dilution correction is correct; if the resulting radius moved outside the 8–15 Earth-radius GEMS range, the density classification would fail.
Extended reading notes
Core claim
The central discovery is that TOI-5916 b and TOI-6158 b are Saturn-density giant exoplanets orbiting M2 dwarf stars in short-period orbits. Their radii and masses place them squarely within the GEMS population, and both have measured densities consistent with Saturn's. The paper also reports a preliminary trend, which survives a geometric transit-bias correction, in which giant planets around M dwarfs sit systematically closer to their hosts than giant planets around FGK stars, and finds no evidence that these planets are inflated by stellar irradiation. Taken together, the two confirmations strengthen the claim that warm giant planets at Saturn-like densities form through a mechanism that o
Load-bearing premise
The density of TOI-6158 b hinges on an unconstrained dilution correction for a grazing transit; if the true dilution lies significantly outside the fitted range, the planet could shift from Saturn-density toward water-density, although the planet's existence would remain intact.
Editorial extensions
If this is right
- If the two planets are confirmed as claimed, the known transiting GEMS population grows to 35 objects, a sample size that allows more statistically meaningful tests of formation scenarios.
- Both planets having Saturn-like densities adds to the clustering of GEMS between 0.5 and 1 g/cm^3, strengthening the empirical claim that this density range is characteristic of the population.
- The bias-corrected orbital-distance trend, if real, implies that giant planets around M dwarfs migrate inward more effectively or experience stronger tidal effects than those around FGK stars.
- The lack of radius inflation with insolation, if it persists, rules out strong stellar heating as a dominant driver of the observed radii for these planets.
- These two systems become additional targets for atmospheric characterization with next-generation space telescopes.
Reading between the lines
- A testable extension is to measure the atmospheric carbon-to-oxygen ratio of these two planets: values near solar would favor core accretion, whereas super-solar values would favor gravitational instability.
- If the close-orbit trend is confirmed with more systems, planet–planet scattering followed by tidal circularization predicts an eccentricity distribution that declines with age; archival radial velocities could search for that signature.
- The grazing transit of TOI-6158 b offers a rare opportunity to constrain the dilution directly with a high-cadence observation of the fully covered transit, which would sharpen the density measurement and test whether the Saturn-density classification survives.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. This paper reports the confirmation of two transiting giant planets around M2 dwarfs, TOI-5916 b and TOI-6158 b, discovered by TESS and followed up with ground-based photometry (RBO and Swope) and HPF radial velocities. Joint modeling of the transit light curves and RVs yields orbital parameters, masses (219±28 M⊕ and 135+19−18 M⊕), radii (11.8+0.52−0.51 R⊕ and 10.4+2.70−1.11 R⊕), and densities (0.73+0.14−0.13 and 0.66+0.41−0.23 g cm⁻³). The authors interpret both planets as Saturn-density GEMS and use them to support population-level trends, including a close-in orbital period distribution for GEMS relative to FGK giants. The existence claims rest on coherent phase-folded RV signals and multiple transit datasets, and high-resolution imaging rules out bright stellar companions.
Significance. If the results hold, the paper adds two massive giant planets around M dwarfs to the small GEMS census, with RV masses and photometric radii. The multi-instrument approach (TESS, ground-based photometry, speckle and AO imaging, HPF RVs) and the careful stellar characterization are strengths. The main weakness is that the Saturn-density classification of TOI-6158 b rests on a grazing transit (b = 0.86+0.09−0.06) and per-sector TESS dilution terms that the authors themselves state they cannot constrain precisely. The planet's existence is not at risk—the RV signal is independent of dilution—but the density claim in the title and abstract is not as secure as presented.
major comments (2)
- [§5 and Table 4] The paper states in §5 that for TOI-6158 'the grazing geometry precludes us from giving a precise estimate on the dilution,' yet Table 4 reports per-sector dilution values D = 1.475+0.242−0.213 (sector 56), 1.311+0.220−0.199 (sector 82), and 1.270+0.214−0.181 (sector 83). Because the observed transit depth scales as (R_p/R_*)^2 / D, the fitted R_p = 10.4+2.70−1.11 R⊕ and hence ρ_p = 0.66+0.41−0.23 g cm⁻³ are conditioned on the fitted D posterior. The text explicitly allows D near unity; at D = 1, R_p would shrink by roughly 12% and ρ_p would rise to about 1 g cm⁻³, placing the planet near or above water density rather than in the Saturn-density envelope. Please add a robustness test with D fixed to plausible values (e.g., D = 1 and D = 1.5) and report the resulting ρ_p posterior. Without this test, the density classification for TOI-6158 b is model-dependent rather than robust.
- [Abstract and §6.2] The abstract's statement that 'Both planets have Saturn-like densities' and the §6.2 claim of an '~84% probability to be less dense than water' overstate the certainty for TOI-6158 b. The posterior for ρ₂ has a 68% credible interval from 0.43 to 1.07 g cm⁻³, so water density is within 1σ even under the fitted dilution; under the D = 1 scenario the density moves further above water. The title and abstract should be qualified, for example by saying TOI-5916 b has a Saturn-like density and TOI-6158 b is consistent with a low-density, Saturn-like composition within the current uncertainties.
minor comments (5)
- [Abstract vs §1] The abstract defines GEMS as 'Exoplanets Transiting M-dwarf Stars,' while §1 defines it as 'Giant Exoplanets around M-dwarfs.' Please use the definition consistently.
- [Figure 2 caption and Figures 4–5] Typographical errors: 'Similiar' in the Figure 2 caption, and 'Resdiual' in the y-axis labels of Figures 4 and 5. Should be 'Similar' and 'Residual.'
- [Table 3] The header 'Metalicity' should be 'Metallicity.'
- [References] The Hotnisky et al. (2025) reference appears twice with the same DOI; merge the duplicate.
- [§6.3 and §7] The semi-major axis trend is based on small samples (35 GEMS) and the §6.3 text properly calls it preliminary with large uncertainties on the weighted medians. The conclusion's wording 'GEMS appear to tend towards shorter, sub-four day periods' is still stronger than the analysis supports; consider adding 'preliminary' there as well.
Circularity Check
No significant circularity: planet masses/radii/densities are derived from independent photometry and RVs; population trends are contextual, not fitted inputs.
full rationale
The derivation chain for the central claim (confirmation and bulk parameters of TOI-5916 b and TOI-6158 b) is self-contained with respect to new data. The radii come from a joint fit (exoplanet/PyMC3) of TESS, RBO, and Swope light curves; masses come from HPF RVs (K = 164±20 m/s and 95±13 m/s); densities are then M_p/(4/3 π R_p^3), i.e., ratios of independently constrained fitted quantities, not inputs. No fitted dilution term is relabeled as a prediction: Table 4 reports D_TESS values and the text explicitly acknowledges that the grazing geometry limits dilution precision for TOI-6158 b. That is a model-parameter risk and a limitation the authors flag, not circularity. The 'Saturn-density' language is an interpretation of the derived ρ values against Saturn's density (0.687 g/cm^3), not a constraint imposed in the fit. The GEMS/population comparisons ('growing trend', closer orbits) use the NASA Exoplanet Archive plus two published systems (Hotnisky et al. 2025) and add the two new objects as additional points; they are not predictions generated by a model fitted to those same points. Self-citations (Kanodia et al. 2024a, 2025; Kanodia 2025) define the GEMS classification and prior population context, but the measured masses, radii, and densities do not reduce to those citations. No equation in the paper is identical by construction to its input, and no fitted parameter is renamed as a prediction. Hence no circular step.
Assumptions & free parameters
free parameters (5)
- Per-sector TESS dilution D =
TOI-5916: 1.045+0.083−0.074, 1.033+0.074−0.066; TOI-6158: 1.475+0.242−0.213, 1.311+0.220−0.199, 1.270+0.214−0.181
- HPF RV jitter =
19+20−13 m/s (TOI-5916); 32±12 m/s (TOI-6158)
- Per-dataset photometric jitter =
≈25–48 ppm (Table 4, 8 values)
- Quadratic limb-darkening coefficients =
not tabulated individually
- Orbital and transit parameters (P, T0, Rp/R*, a/R*, i, e, ω, K) =
Table 4: e.g., P=2.36712341 d and 3.04468990 d; Rp/R*=0.2213 and 0.2017; K=164±20 and 95±13 m/s
assumptions (6)
- domain assumption The TESS-Gaia Light Curve (TGLC) PSF modeling correctly removes contamination and dilution from neighboring stars.
- ad hoc to paper The anomalous background transit in TOI-5916 Sector 55 is not from the target and excising ±0.2 day does not remove real transit signal.
- domain assumption Stellar masses/radii from EXOFASTv2 SED + MIST isochrones, with HPF-SpecMatch priors, are accurate.
- domain assumption The HPF RV reduction (SERVAL, barycorrpy) provides a stable wavelength solution and no significant unseen companion dilutes the signal.
- domain assumption The NASA Exoplanet Archive sample plus two additions is representative enough for the GEMS vs FGK comparison; the transit probability formula (Eq. 2) and Horvitz-Thompson weighting correct the main geometric bias.
- domain assumption A quadratic limb-darkening law and the Kipping parameterization adequately model stellar intensity profiles for both transits.
Cite this review
Pith. "Pith review of Searching for GEMS: TOI-5916 b & TOI-6158 b are two Saturn-density planets orbiting M2 dwarfs." pith.science (2026). https://pith.science/paper/BIIJT4IP
@misc{pith2026251011798,
author = {Pith},
title = {Pith review of: Searching for GEMS: TOI-5916 b & TOI-6158 b are two Saturn-density planets orbiting M2 dwarfs},
year = {2026},
howpublished = {\url{https://pith.science/paper/BIIJT4IP}},
note = {Machine review of arXiv:2510.11798}
}
abstract
We confirm the planetary nature of (1) TOI-5916 b and (2) TOI-6158 b, two Exoplanets Transiting M-dwarf Stars (GEMS), both discovered by the Transiting Exoplanet Survey Satellite (TESS). Both systems were confirmed with ground-based photometry (Red Buttes Observatory and Swope, respectively) and radial velocity data from the Habitable-zone Planet Finder. Their radii are $R_{1}=11.8^{+0.52}_{-0.51}\text{ }R_{\oplus}$ and $R_{2}=10.4^{+2.70}_{-1.11}\text{ }R_{\oplus}$ and masses are $M_{1}=219\pm28\text{ }M_{\oplus}$ and $M_{2}=135^{+19}_{-18}\text{ }M_{\oplus}$. Both planets have Saturn-like densities ($\rho_{1} = 0.73^{+0.14}_{-0.13}\,\text{g cm}^{-3}$, $\rho_{2} = 0.66^{+0.41}_{-0.23}\,\text{g cm}^{-3}$), which appears to be a growing trend among GEMS systems and, more generally, warm Jupiters. In confirming both of these exoplanets, we add to the growing evidence for a population of Saturn-density planets among the GEMS systems. We also find evidence for a preliminary trend in which GEMS exhibit systematically closer orbits compared to FGK giants.
Figures
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Reference graph
Works this paper leans on
-
[1]
L., Chen, X., Ciardi, D., et al
Akeson, R. L., Chen, X., Ciardi, D., et al. 2013, PASP, 125, 989, doi: 10.1086/672273
doi:10.1086/672273 2013
-
[2]
Boss, A. P. 2006, The Astrophysical Journal, 641, 1148, doi: 10.1086/500530
-
[3]
Boss, A. P., & Kanodia, S. 2023, ApJ, 956, 4, doi: 10.3847/1538-4357/acf373
-
[4]
M., Bayliss, D., & Van Eylen, V
Bryant, E. M., Bayliss, D., & Van Eylen, V. 2023, MNRAS, 521, 3663, doi: 10.1093/mnras/stad626
-
[5]
Bryant, E. M., Bayliss, D., Hartman, J. D., et al. 2024, MNRAS, 533, 3893, doi: 10.1093/mnras/stae2034
-
[6]
2021, A&A, 656, A72, doi: 10.1051/0004-6361/202140390 Ca˜ nas, C
Burn, R., Schlecker, M., Mordasini, C., et al. 2021, A&A, 656, A72, doi: 10.1051/0004-6361/202140390 Ca˜ nas, C. I., Stefansson, G., Kanodia, S., et al. 2020, AJ, 160, 147, doi: 10.3847/1538-3881/abac67 Ca˜ nas, C. I., Kanodia, S., Libby-Roberts, J., et al. 2023, AJ, 166, 30, doi: 10.3847/1538-3881/acdac7
-
[7]
Chambers, K. C., Magnier, E. A., Metcalfe, N., et al. 2016, arXiv e-prints, arXiv:1612.05560, doi: 10.48550/arXiv.1612.05560
-
[8]
2016, ApJ, 823, 102, doi: 10.3847/0004-637X/823/2/102
Choi, J., Dotter, A., Conroy, C., et al. 2016, ApJ, 823, 102, doi: 10.3847/0004-637X/823/2/102
Show all 57 references
-
[9]
A., Kielkopf, J
Collins, K. A., Kielkopf, J. F., Stassun, K. G., & Hessman, F. V. 2017, AJ, 153, 77, doi: 10.3847/1538-3881/153/2/77
2017 doi
-
[10]
M., Skrutskie, M
Cutri, R. M., Skrutskie, M. F., van Dyk, S., et al. 2003, VizieR Online Data Catalog: 2MASS All-Sky Catalog of Point Sources (Cutri+ 2003), VizieR On-line Data Catalog: II/246. Originally published in: University of Massachusetts and Infrared Processing and Analysis Center, (I...
2003
-
[11]
M., Wright, E
Cutri, R. M., Wright, E. L., Conrow, T., et al. 2021, VizieR Online Data Catalog: AllWISE Data Release (Cutri+ 2013), VizieR On-line Data Catalog: II/328. Originally published in: IPAC/Caltech (2013)
2021
-
[12]
2025, AJ, 169, 4, doi: 10.3847/1538-3881/ad8ec1
Dong, J., Chontos, A., Zhou, G., et al. 2025, AJ, 169, 4, doi: 10.3847/1538-3881/ad8ec1
2025 doi
-
[13]
2016, ApJS, 222, 8, doi: 10.3847/0067-0049/222/1/8
Dotter, A. 2016, ApJS, 222, 8, doi: 10.3847/0067-0049/222/1/8
2016 doi
-
[14]
D., Rodriguez, J
Eastman, J. D., Rodriguez, J. E., Agol, E., et al. 2019, arXiv e-prints, arXiv:1907.09480. https://arxiv.org/abs/1907.09480
2019 arXiv
-
[15]
Fitzpatrick, E. L. 1999, PASP, 111, 63, doi: 10.1086/316293
1999 doi
-
[16]
2017, The Astronomical Journal, 154, 220, doi: 10.3847/1538-3881/aa9332 Gaia Collaboration, Vallenari, A., Brown, A.G.A., Prusti, T., & et al
Foreman-Mackey, D., Agol, E., Ambikasaran, S., & Angus, R. 2017, The Astronomical Journal, 154, 220, doi: 10.3847/1538-3881/aa9332 Gaia Collaboration, Vallenari, A., Brown, A.G.A., Prusti, T., & et al. 2022, A&A, doi: 10.1051/0004-6361/202243940 Gaia Collaboration, Vallenari, ...
2017 doi
-
[17]
2025, ApJS, 276, 47, doi: 10.3847/1538-4365/ad9c65
Mao, S. 2025, ApJS, 276, 47, doi: 10.3847/1538-4365/ad9c65
2025 doi
-
[18]
X., Wang, S., et al
Gan, T., Wang, S. X., Wang, S., et al. 2022, The Astronomical Journal, 165, 17, doi: 10.3847/1538-3881/ac9b12
2022 doi
-
[19]
P., Mather, J
Gardner, J. P., Mather, J. C., Clampin, M., et al. 2006, SSRv, 123, 485, doi: 10.1007/s11214-006-8315-7
2006 doi
-
[20]
2019, ApJ, 887, 93, doi: 10.3847/1538-4357/ab5362
Finkbeiner, D. 2019, ApJ, 887, 93, doi: 10.3847/1538-4357/ab5362
2019 doi
-
[21]
Han, T., & Brandt, T. D. 2023, The Astronomical Journal, 165, 71, doi: 10.3847/1538-3881/acaaa7
2023 doi
-
[22]
D., et al
Han, T., Robertson, P., Brandt, T. D., et al. 2025, ApJL, 988, L4, doi: 10.3847/2041-8213/ade794
2025 doi
-
[23]
2024, AJ, 167, 4, doi: 10.3847/1538-3881/ad09c2
Han, T., Robertson, P., Kanodia, S., et al. 2024, AJ, 167, 4, doi: 10.3847/1538-3881/ad09c2
2024 doi
-
[24]
J., Lee, H., MacQueen, P
Hill, G. J., Lee, H., MacQueen, P. J., et al. 2021, AJ, 162, 298, doi: 10.3847/1538-3881/ac2c02
2021 doi
-
[25]
G., & Thompson, D
Horvitz, D. G., & Thompson, D. J. 1952, Journal of the American Statistical Association, 47, 663, doi: 10.1080/01621459.1952.10483446
1952
-
[27]
2025, The Astronomical Journal, 170, 1, doi: 10.3847/1538-3881/add2ef
Hotnisky, A., Kanodia, S., Libby-Roberts, J., et al. 2025, The Astronomical Journal, 170, 1, doi: 10.3847/1538-3881/add2ef
2025 doi
-
[28]
Ciardi, D. R. 2011, AJ, 142, 19, doi: 10.1088/0004-6256/142/1/19
2011 doi
-
[29]
X., Vanderburg, A., P´ al, A., et al
Huang, C. X., Vanderburg, A., P´ al, A., et al. 2020, Research Notes of the American Astronomical Society, 4, 204, doi: 10.3847/2515-5172/abca2e
2020 doi
-
[30]
Ida, S., & Lin, D. N. C. 2005, ApJ, 626, 1045, doi: 10.1086/429953
2005 doi
-
[31]
2023, PASJ, 75, 713, doi: 10.1093/pasj/psad031
Kagetani, T., Narita, N., Kimura, T., et al. 2023, PASJ, 75, 713, doi: 10.1093/pasj/psad031
2023 doi
-
[32]
2025, ApJ, 978, 97, doi: 10.3847/1538-4357/ad9823
Kanodia, S. 2025, ApJ, 978, 97, doi: 10.3847/1538-4357/ad9823
2025 doi
-
[33]
2018, Research Notes of the American Astronomical Society, 2, 4, doi: 10.3847/2515-5172/aaa4b7
Kanodia, S., & Wright, J. 2018, Research Notes of the American Astronomical Society, 2, 4, doi: 10.3847/2515-5172/aaa4b7
2018 doi
-
[34]
W., et al
Kanodia, S., Mahadevan, S., Ramsey, L. W., et al. 2018, in Ground-based and Airborne Instrumentation for Astronomy VII, ed. C. J. Evans, L. Simard, & H. Takami, Vol. 10702, International Society for Optics and Photonics (SPIE), 107026Q, doi: 10.1117/12.2313491
2018 doi
-
[35]
I., Mahadevan, S., et al
Kanodia, S., Ca˜ nas, C. I., Mahadevan, S., et al. 2024a, AJ, 167, 161, doi: 10.3847/1538-3881/ad27cb 15
-
[36]
F., Ca˜ nas, C
Kanodia, S., Gupta, A. F., Ca˜ nas, C. I., et al. 2024b, AJ, 168, 235, doi: 10.3847/1538-3881/ad7796
- [37]
-
[38]
H., Ellis, T
Kasper, D. H., Ellis, T. G., Yeigh, R. R., et al. 2016, Publications of the Astronomical Society of the Pacific, 128, 105005, doi: 10.1088/1538-3873/128/968/105005
2016 doi
-
[39]
Kipping, D. M. 2013, MNRAS, 435, 2152, doi: 10.1093/mnras/stt1435
2013 doi
-
[40]
2022a, Research Notes of the American Astronomical Society, 6, 236, doi: 10.3847/2515-5172/aca158
Kunimoto, M., Tey, E., Fong, W., et al. 2022a, Research Notes of the American Astronomical Society, 6, 236, doi: 10.3847/2515-5172/aca158
-
[41]
2022b, ApJS, 259, 33, doi: 10.3847/1538-4365/ac5688
Kunimoto, M., Daylan, T., Guerrero, N., et al. 2022b, ApJS, 259, 33, doi: 10.3847/1538-4365/ac5688
-
[42]
Laughlin, G., Bodenheimer, P., & Adams, F. C. 2004, 612, L73, doi: 10.1086/424384
2004 doi
-
[43]
2012, in Ground-based and Airborne Instrumentation for Astronomy IV, ed
Mahadevan, S., Ramsey, L., Bender, C., et al. 2012, in Ground-based and Airborne Instrumentation for Astronomy IV, ed. I. S. McLean, S. K. Ramsay, & H. Takami, Vol. 8446, International Society for Optics and Photonics (SPIE), 84461S, doi: 10.1117/12.926102
2012 doi
-
[44]
W., Terrien, R., et al
Mahadevan, S., Ramsey, L. W., Terrien, R., et al. 2014, in Ground-based and Airborne Instrumentation for Astronomy V, ed. S. K. Ramsay, I. S. McLean, & H. Takami, Vol. 9147, International Society for Optics and Photonics (SPIE), 91471G, doi: 10.1117/12.2056417 NASA Exoplanet A...
2014 doi
-
[45]
P., Bender, C
Ninan, J. P., Bender, C. F., Mahadevan, S., et al. 2018, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol. 10709, High Energy, Optical, and Infrared Detectors for Astronomy VIII, ed. A. D. Holland & J. Beletic, 107092U, doi: 10.1117/12.2312787
2018 doi
-
[46]
2020, MNRAS, 491, 4481, doi: 10.1093/mnras/stz3207
Osborn, A., & Bayliss, D. 2020, MNRAS, 491, 4481, doi: 10.1093/mnras/stz3207
2020 doi
-
[47]
2024, ApJ, 963, 122, doi: 10.3847/1538-4357/ad1bef
Pfalzner, S., & Dincer, F. 2024, ApJ, 963, 122, doi: 10.3847/1538-4357/ad1bef
2024 doi
-
[48]
W., Adams, M
Ramsey, L. W., Adams, M. T., III, T. G. B., et al. 1998, in Advanced Technology Optical/IR Telescopes VI, ed. L. M. Stepp, Vol. 3352, International Society for Optics and Photonics (SPIE), 34 – 42, doi: 10.1117/12.319287
1998 doi
-
[49]
A., & Ford, E
Rasio, F. A., & Ford, E. B. 1996, Science, 274, 954, doi: 10.1126/science.274.5289.954
1996 doi
-
[50]
R., Winn, J
Ricker, G. R., Winn, J. N., Vanderspek, R., et al. 2014, Journal of Astronomical Telescopes, Instruments, and Systems, 1, 014003, doi: 10.1117/1.JATIS.1.1.014003
2014 doi
- [51]
-
[52]
J., Howell, S
Scott, N. J., Howell, S. B., Horch, E. P., & Everett, M. E. 2018, PASP, 130, 054502, doi: 10.1088/1538-3873/aab484
2018 doi
-
[53]
2014, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol
Srinath, S., McGurk, R., Rockosi, C., et al. 2014, in Society of Photo-Optical Instrumentation Engineers (SPIE) Conference Series, Vol. 9148, Adaptive Optics Systems IV, ed. E. Marchetti, L. M. Close, & J.-P. Vran, 91482Z, doi: 10.1117/12.2055672
2014 doi
-
[54]
G., Oelkers, R
Stassun, K. G., Oelkers, R. J., Paegert, M., et al. 2019, AJ, 158, 138, doi: 10.3847/1538-3881/ab3467
2019 doi
-
[55]
2016, ApJ, 833, 175, doi: 10.3847/1538-4357/833/2/175 Stef´ ansson, G., Ca˜ nas, C., Wisniewski, J., et al
Stefansson, G., Hearty, F., Robertson, P., et al. 2016, ApJ, 833, 175, doi: 10.3847/1538-4357/833/2/175 Stef´ ansson, G., Ca˜ nas, C., Wisniewski, J., et al. 2020, AJ, 159, 100, doi: 10.3847/1538-3881/ab5f15 Stef´ ansson, G., Mahadevan, S., Miguel, Y., et al. 2023, Science, 38...
2016 doi
- [56]
-
[57]
W., Petigura, E
Yee, S. W., Petigura, E. A., & von Braun, K. 2017, ApJ, 836, 77, doi: 10.3847/1538-4357/836/1/77
2017 doi
-
[58]
J., et al
Zechmeister, M., Reiners, A., Amado, P. J., et al. 2018, A&A, 609, A12, doi: 10.1051/0004-6361/201731483 16
2018 doi
Reviewed August 4, 2026 · model on record in the stance chip above.
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