Recognition: no theorem link
Seasonal Insolation Variability on Early Venus: Implications for Energy Budget
Pith reviewed 2026-05-13 00:55 UTC · model grok-4.3
The pith
Early Venus could experience large shifts in sunlight by latitude and season, yet the total energy received over each orbit changed only modestly, making atmospheric opacity the main control on surface temperature.
A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.
Core claim
Early Venus could experience substantial redistribution of insolation across latitude and orbital phase, but orbit-averaged incident flux varies only modestly across the explored parameter space, leaving atmospheric opacity as the dominant control on surface temperature. Insolation variations therefore act mainly as modulators rather than primary drivers of climate state, with their expression governed by the competition between forcing and radiative adjustment timescales.
What carries the argument
Latitude-orbital phase maps of incident solar flux translated through 0-D and 1-D energy-balance models that include a radiative relaxation timescale calibrated to modern Venus.
If this is right
- Insolation variations act mainly as modulators rather than primary drivers of climate state.
- The competition between forcing variability and radiative adjustment timescales determines how orbital changes express themselves at the surface.
- The insolation maps and response diagnostics supply boundary conditions for future three-dimensional climate simulations of early Venus.
- Regimes exist in which temperate surface conditions may have been sustained despite the explored dynamical states.
Where Pith is reading between the lines
- Reconstructing Venus's climate history should prioritize evolution of atmospheric composition over precise reconstruction of past rotation rate or eccentricity.
- The same mapping and timescale approach could be applied to early Earth to locate the divergence point where insolation stability gave way to different temperature controls.
- Many thick-atmosphere rocky planets may exhibit similar insolation stability, narrowing the orbital conditions that can alone trigger major climate shifts.
- If the modest average-flux result holds, searches for past habitable conditions on Venus should focus on windows when opacity was lower rather than on specific orbital configurations.
Load-bearing premise
The idealized 0-D and 1-D energy-balance models, including the radiative relaxation timescale tuned to modern Venus, correctly capture how the atmosphere would respond to different rotation, obliquity, eccentricity, and fainter solar input on early Venus.
What would settle it
A three-dimensional climate simulation driven by the paper's insolation maps that finds surface temperature changes more strongly with the tested orbital parameters than with adjustments to atmospheric opacity would contradict the claim that opacity dominates.
Figures
read the original abstract
Venus and Earth are similar in bulk properties yet followed dramatically different climatic trajectories. Reconstructing Venus's climate evolution requires understanding how rotation, obliquity, eccentricity, and solar luminosity shaped incident energy and the atmospheric response. Here we present latitude-orbital phase maps of incident solar flux for Venus at the present epoch and at an age of 0.5 Gyr, when the Sun was fainter and Venus may have occupied a different dynamical state. We explore slow- and fast-rotator regimes, moderate obliquity (10deg), and elevated eccentricity (e=0.15-0.30), motivated by dynamical studies of plausible limits. To translate flux maps into climate-relevant quantities, we apply an idealized atmospheric energy-balance framework with global (0-D) and latitude-dependent (1-D) formulations calibrated to modern Venus. This framework defines a radiative relaxation timescale that links forcing variability to thermal response. The resulting diagnostics connect orbital forcing to surface energy balance and assess seasonal and orbital variability relative to Venus's extreme greenhouse state. Our results show that early Venus could experience substantial redistribution of insolation across latitude and orbital phase, but orbit-averaged incident flux varies only modestly across the explored parameter space, leaving atmospheric opacity as the dominant control on surface temperature. Insolation variations therefore act mainly as modulators rather than primary drivers of climate state, with their expression governed by the competition between forcing and radiative adjustment timescales. The insolation maps and response diagnostics provide boundary conditions for future 3-D climate simulations of early Venus, including regimes in which temperate surface conditions may have been sustained.
Editorial analysis
A structured set of objections, weighed in public.
Referee Report
Summary. The paper computes latitude-orbital phase maps of incident solar flux on Venus for the present epoch and at 0.5 Gyr (fainter Sun, possible different rotation/obliquity/eccentricity). It applies idealized 0-D and 1-D atmospheric energy-balance models, calibrated to modern Venus via a single radiative relaxation timescale, to translate these maps into thermal-response diagnostics. The central claim is that orbit-averaged incident flux varies only modestly across the explored parameter space, so that atmospheric opacity remains the dominant control on surface temperature while insolation variations act primarily as modulators whose expression depends on the competition between forcing and radiative-adjustment timescales. The maps and diagnostics are offered as boundary conditions for future 3-D simulations.
Significance. If the extrapolation of the modern-Venus-calibrated EBM holds, the work supplies concrete, reproducible insolation boundary conditions and a clear separation between orbital forcing and greenhouse control that can guide 3-D GCM studies of early Venus. The modest variation in orbit-averaged flux is a useful quantitative result that narrows the plausible range of insolation-driven climate states.
major comments (2)
- [Methods (energy-balance framework)] Methods (energy-balance framework and radiative relaxation timescale): The single radiative relaxation timescale τ_rad is tuned to reproduce modern-Venus thermal inertia and then applied unchanged to the early-Venus case (lower solar constant, altered rotation/obliquity/eccentricity). Because the temperature equation is written as dT/dt = (F − σT⁴)/τ_rad, any dependence of τ_rad on equilibrium temperature, heat capacity, or opacity (all altered by the ~5–10 % fainter Sun) directly affects whether seasonal/orbital flux redistribution is damped or amplified. No derivation or sensitivity test of τ_rad under the early-Venus parameter set is provided, so the claim that “insolation variations act mainly as modulators” rests on an unverified extrapolation.
- [Results (orbit-averaged flux)] Results (orbit-averaged flux claim): The statement that orbit-averaged incident flux “varies only modestly across the explored parameter space” is load-bearing for the conclusion that atmospheric opacity dominates. The manuscript should report the actual range of orbit-averaged values (with uncertainties) for each combination of rotation regime, obliquity, and eccentricity so that readers can judge whether the variation is modest relative to the greenhouse forcing.
minor comments (2)
- [Abstract / Introduction] The abstract and introduction should explicitly state the numerical values adopted for the modern-Venus calibration of τ_rad and the solar constant at 0.5 Gyr so that the forward projection is reproducible.
- [Figures] Figure captions for the insolation maps should indicate the exact orbital phases and latitude grid used, and whether the maps are normalized to the modern solar constant or to the early-Sun value.
Simulated Author's Rebuttal
We thank the referee for their insightful comments, which highlight key limitations in our idealized energy-balance approach and the need for quantitative detail on orbit-averaged fluxes. We address each major comment below and will revise the manuscript accordingly to improve clarity and robustness.
read point-by-point responses
-
Referee: [Methods (energy-balance framework)] Methods (energy-balance framework and radiative relaxation timescale): The single radiative relaxation timescale τ_rad is tuned to reproduce modern-Venus thermal inertia and then applied unchanged to the early-Venus case (lower solar constant, altered rotation/obliquity/eccentricity). Because the temperature equation is written as dT/dt = (F − σT⁴)/τ_rad, any dependence of τ_rad on equilibrium temperature, heat capacity, or opacity (all altered by the ~5–10 % fainter Sun) directly affects whether seasonal/orbital flux redistribution is damped or amplified. No derivation or sensitivity test of τ_rad under the early-Venus parameter set is provided, so the claim that “insolation variations act mainly as modulators” rests on an unverified extrapolation.
Authors: We acknowledge this is a valid concern regarding the extrapolation. Our 0-D/1-D framework is intentionally simplified, with τ_rad calibrated as an effective constant to modern Venus thermal inertia to capture the competition between forcing and adjustment timescales. No first-principles derivation or sensitivity tests for early-Venus parameters were included in the submitted manuscript. In revision, we will add a new subsection performing sensitivity tests on τ_rad (varying it by factors of 0.5–2.0) to show impacts on seasonal damping, and we will explicitly discuss the constant-τ_rad assumption as a limitation of the idealized model when applied to altered solar constant and dynamics. This will better qualify our modulator conclusion. revision: yes
-
Referee: [Results (orbit-averaged flux)] Results (orbit-averaged flux claim): The statement that orbit-averaged incident flux “varies only modestly across the explored parameter space” is load-bearing for the conclusion that atmospheric opacity dominates. The manuscript should report the actual range of orbit-averaged values (with uncertainties) for each combination of rotation regime, obliquity, and eccentricity so that readers can judge whether the variation is modest relative to the greenhouse forcing.
Authors: We agree that explicit numerical ranges are required to support the claim. The submitted manuscript states the variation is modest based on the flux maps but does not tabulate the orbit-averaged values for each parameter set. In the revision, we will insert a table in the results section reporting the orbit-averaged incident flux (W m⁻²) for present-day and 0.5 Gyr cases, across slow/fast rotators, 10° obliquity, and e = 0.15/0.30. We will also show the percentage range relative to the mean and compare it to the solar-constant change and greenhouse effects. Since the calculations are deterministic, we will note that reported values have no statistical uncertainties but represent exact model outputs for the explored configurations. revision: yes
Circularity Check
No significant circularity; derivation uses external calibration for forward application
full rationale
The paper computes insolation maps directly from orbital parameters, rotation state, obliquity, eccentricity, and solar luminosity evolution at 0.5 Gyr using standard astronomical relations. It then applies a 0-D/1-D energy-balance model whose radiative relaxation timescale is calibrated once to modern Venus observations as an external benchmark. The early-Venus results are obtained by feeding the new insolation maps into this fixed model; no parameter is fitted to early-Venus data, no output is renamed as a prediction of itself, and no self-citation chain or ansatz is invoked to force the conclusion that orbit-averaged flux varies only modestly while opacity dominates. The central claim follows from comparing the computed flux variability against the model's fixed response timescale and is therefore independent of the target result by construction.
Axiom & Free-Parameter Ledger
free parameters (2)
- radiative relaxation timescale
- energy-balance model calibration parameters
axioms (2)
- domain assumption The explored slow- and fast-rotator regimes, 10-degree obliquity, and eccentricity range 0.15-0.30 represent plausible limits for early Venus.
- domain assumption The idealized 0-D and 1-D energy-balance framework with radiative relaxation timescale sufficiently captures the link between orbital forcing and surface energy balance for early Venus.
Reference graph
Works this paper leans on
-
[1]
C., Barnes, R., Domagal-Goldman, S., et al
Armstrong, J. C., Barnes, R., Domagal-Goldman, S., et al. 2014, Astrobiology, 14, 277, doi: 10.1089/ast.2013.1129
-
[2]
2007, Icarus, 188, 1, doi: 10.1016/j.icarus.2006.11.022
Atobe, K., & Ida, S. 2007, Icarus, 188, 1, doi: 10.1016/j.icarus.2006.11.022
-
[3]
Hedman, M. M. 2016, Astrobiology, 16, 487, doi: 10.1089/ast.2015.1427
-
[4]
2013, Astrobiology, 13, 225, doi: 10.1089/ast.2012.0851
Barnes, R., Mullins, K., Goldblatt, C., et al. 2013, Astrobiology, 13, 225, doi: 10.1089/ast.2012.0851
-
[5]
Berger, A. L. 1978, Journal of the Atmospheric Sciences, 35, 2362, doi: 10.1175/1520-0469(1978)035⟨2362:LTVODI⟩2.0.CO;2
-
[6]
2021, PSJ, 2, 220, doi: 10.3847/PSJ/ac26c0
Cascioli, G., Hensley, S., De Marchi, F., et al. 2021, PSJ, 2, 220, doi: 10.3847/PSJ/ac26c0
-
[7]
Chambers, J. E. 2001, Icarus, 152, 205, doi: 10.1006/icar.2001.6639
-
[8]
Chandler, C. O., McDonald, I., & Kane, S. R. 2016, AJ, 151, 59, doi: 10.3847/0004-6256/151/3/59
-
[9]
Constantinou, T., Shorttle, O., & Rimmer, P. B. 2025, Nature Astronomy, 9, 189, doi: 10.1038/s41550-024-02414-5
-
[10]
Correia, A. C. M., & Laskar, J. 2003, Icarus, 163, 24, doi: 10.1016/S0019-1035(03)00043-5
-
[11]
Correia, A. C. M., Laskar, J., & de Surgy, O. N. 2003, Icarus, 163, 1, doi: 10.1016/S0019-1035(03)00042-3
-
[12]
2011, A&A, 531, A45, doi: 10.1051/0004-6361/201116606
Cottereau, L., Rambaux, N., Lebonnois, S., & Souchay, J. 2011, A&A, 531, A45, doi: 10.1051/0004-6361/201116606
-
[13]
Cowan, N. B., Voigt, A., & Abbot, D. S. 2012, ApJ, 757, 80, doi: 10.1088/0004-637X/757/1/80
-
[14]
Cronin, T. W., & Emanuel, K. A. 2013, Journal of Advances in Modeling Earth Systems, 5, 843, doi: 10.1002/jame.20049
-
[15]
Dobrovolskis, A. R. 2013, Icarus, 226, 760, doi: 10.1016/j.icarus.2013.06.026
-
[16]
Donahue, T. M., Hoffman, J. H., Hodges, R. R., & Watson, A. J. 1982, Science, 216, 630, doi: 10.1126/science.216.4546.630
-
[17]
2020, Journal of Climate, 33, 3921, doi: 10.1175/JCLI-D-19-0329.1
Rhines, A. 2020, Journal of Climate, 33, 3921, doi: 10.1175/JCLI-D-19-0329.1
-
[18]
Edson, A., Lee, S., Bannon, P., Kasting, J. F., & Pollard, D. 2011, Icarus, 212, 1, doi: 10.1016/j.icarus.2010.11.023
-
[19]
Garvin, J. B., Getty, S. A., Arney, G. N., et al. 2022, PSJ, 3, 117, doi: 10.3847/PSJ/ac63c2
-
[20]
2009, Earth and Planetary Science Letters, 286, 503, doi: 10.1016/j.epsl.2009.07.016
Gillmann, C., Chassefi` ere, E., & Lognonn´ e, P. 2009, Earth and Planetary Science Letters, 286, 503, doi: 10.1016/j.epsl.2009.07.016
-
[21]
Gillmann, C., Way, M. J., Avice, G., et al. 2022, SSRv, 218, 56, doi: 10.1007/s11214-022-00924-0
-
[22]
Gough, D. O. 1981, SoPh, 74, 21, doi: 10.1007/BF00151270
-
[23]
2019, ApJ, 881, 67, doi: 10.3847/1538-4357/ab2a06 —
Guendelman, I., & Kaspi, Y. 2019, ApJ, 881, 67, doi: 10.3847/1538-4357/ab2a06 —. 2020, ApJ, 901, 46, doi: 10.3847/1538-4357/abaef8 —. 2022, AGU Advances, 3, e2022A V000684, doi: 10.1029/2022A V000684
-
[24]
2013, Nature, 497, 607, doi: 10.1038/nature12163
Hamano, K., Abe, Y., & Genda, H. 2013, Nature, 497, 607, doi: 10.1038/nature12163
-
[25]
2016, Icarus, 272, 178, doi: 10.1016/j.icarus.2016.02.048
Haus, R., Kappel, D., Tellmann, S., et al. 2016, Icarus, 272, 178, doi: 10.1016/j.icarus.2016.02.048
-
[26]
L., Pietrinferni, A., Cassisi, S., et al
Hidalgo, S. L., Pietrinferni, A., Cassisi, S., et al. 2018, A pJ, 856, 125, doi: 10.3847/1538-4357/aab158
-
[27]
Hill, M. L., Bott, K., Dalba, P. A., et al. 2023, AJ, 165, 34, doi: 10.3847/1538-3881/aca1c0
-
[28]
Ingersoll, A. P. 1969, Journal of Atmospheric Sciences, 26, 1191, doi: 10.1175/1520-0469(1969)026⟨1191:TRGAHO⟩2.0.CO;2
-
[29]
Kane, S. R. 2021, Planetary Habitability (IOP Publishing), doi: 10.1088/2514-3433/ac2aa1 —. 2022, Nature Astronomy, 6, 420, doi: 10.1038/s41550-022-01626-x
-
[30]
Kane, S. R., & Byrne, P. K. 2024, Nature Astronomy, 8, 417, doi: 10.1038/s41550-024-02228-5
-
[31]
Kane, S. R., Ceja, A. Y., Way, M. J., & Quintana, E. V. 2018, ApJ, 869, 46, doi: 10.3847/1538-4357/aaec68 16 Stephen R. Kane
-
[32]
Kane, S. R., & Gelino, D. M. 2012a, Astrobiology, 12, 940, doi: 10.1089/ast.2011.0798 —. 2012b, PASP, 124, 323, doi: 10.1086/665271
-
[33]
Kane, S. R., Kopparapu, R. K., & Domagal-Goldman, S. D. 2014, ApJL, 794, L5, doi: 10.1088/2041-8205/794/1/L5
-
[34]
Kane, S. R., & Torres, S. M. 2017, AJ, 154, 204, doi: 10.3847/1538-3881/aa8fce
-
[35]
R., Vervoort, P., Horner, J., & Pozuelos, F
Kane, S. R., Vervoort, P., Horner, J., & Pozuelos, F. J. 2020, PSJ, 1, 42, doi: 10.3847/PSJ/abae63
-
[36]
Kane, S. R., Hill, M. L., Kasting, J. F., et al. 2016, ApJ, 830, 1, doi: 10.3847/0004-637X/830/1/1
-
[37]
R., Arney, G., Crisp, D., et al
Kane, S. R., Arney, G., Crisp, D., et al. 2019, Journal of Geophysical Research (Planets), 124, 2015, doi: 10.1029/2019JE005939
-
[38]
Kasting, J. F. 1988, Icarus, 74, 472, doi: 10.1016/0019-1035(88)90116-9
-
[39]
Kasting, J. F., Whitmire, D. P., & Reynolds, R. T. 1993, Icarus, 101, 108, doi: 10.1006/icar.1993.1010
-
[40]
2023, Solar Energy, 249, 250, doi: 10.1016/j.solener.2022.11.022
Kopp, G. 2023, Solar Energy, 249, 250, doi: 10.1016/j.solener.2022.11.022
-
[41]
Kopp, G., & Lean, J. L. 2011, Geophys. Res. Lett., 38, L01706, doi: 10.1029/2010GL045777
-
[42]
Kopparapu, R. K., Ramirez, R. M., SchottelKotte, J., et al. 2014, ApJ, 787, L29, doi: 10.1088/2041-8205/787/2/L29
-
[43]
Kopparapu, R. K., Ramirez, R., Kasting, J. F., et al. 2013, ApJ, 765, 131, doi: 10.1088/0004-637X/765/2/131
-
[44]
Krissansen-Totton, J., Fortney, J. J., & Nimmo, F. 2021, PSJ, 2, 216, doi: 10.3847/PSJ/ac2580
-
[45]
2008, Icarus, 196, 1, doi: 10.1016/j.icarus.2008.02.017
Laskar, J. 2008, Icarus, 196, 1, doi: 10.1016/j.icarus.2008.02.017
-
[46]
2009, Nature, 459, 817, doi: 10.1038/nature08096
Laskar, J., & Gastineau, M. 2009, Nature, 459, 817, doi: 10.1038/nature08096
-
[47]
1993, Nature, 361, 615, doi: 10.1038/361615a0
Laskar, J., Joutel, F., & Robutel, P. 1993, Nature, 361, 615, doi: 10.1038/361615a0
-
[48]
1993, Nature, 361, 608, doi: 10.1038/361608a0
Laskar, J., & Robutel, P. 1993, Nature, 361, 608, doi: 10.1038/361608a0
-
[49]
2004, A&A, 428, 261, doi: 10.1051/0004-6361:20041335
Laskar, J., Robutel, P., Joutel, F., et al. 2004, A&A, 428, 261, doi: 10.1051/0004-6361:20041335
-
[50]
2010, Journal of Geophysical Research (Planets), 115, E06006, doi: 10.1029/2009JE003458
Lebonnois, S., Hourdin, F., Eymet, V., et al. 2010, Journal of Geophysical Research (Planets), 115, E06006, doi: 10.1029/2009JE003458
-
[51]
2016, Icarus, 278, 38, doi: 10.1016/j.icarus.2016.06.004
Lebonnois, S., Sugimoto, N., & Gilli, G. 2016, Icarus, 278, 38, doi: 10.1016/j.icarus.2016.06.004
-
[52]
S., Grassi, D., Mahieux, A., et al
Limaye, S. S., Grassi, D., Mahieux, A., et al. 2018, SSRv, 214, 102, doi: 10.1007/s11214-018-0525-2
-
[53]
Linsenmeier, M., Pascale, S., & Lucarini, V. 2015, Planet. Space Sci., 105, 43, doi: 10.1016/j.pss.2014.11.003
-
[54]
Margot, J.-L., Campbell, D. B., Giorgini, J. D., et al. 2021, Nature Astronomy, doi: 10.1038/s41550-021-01339-7
-
[55]
Miles, E. L., Ostberg, C., Kane, S. R., et al. 2025, AJ, 170, 29, doi: 10.3847/1538-3881/add71c
-
[56]
2024, Icarus, 422, 116245, doi: 10.1016/j.icarus.2024.116245 O’Brien, D
Musseau, Y., Tobie, G., Dumoulin, C., et al. 2024, Icarus, 422, 116245, doi: 10.1016/j.icarus.2024.116245 O’Brien, D. P., Morbidelli, A., & Levison, H. F. 2006, Icarus, 184, 39, doi: 10.1016/j.icarus.2006.04.005
-
[57]
2019a, ApJ, 874, 1, doi: 10.3847/1538-4357/ab06cc —
Ohno, K., & Zhang, X. 2019a, ApJ, 874, 1, doi: 10.3847/1538-4357/ab06cc —. 2019b, ApJ, 874, 2, doi: 10.3847/1538-4357/ab06ca
-
[58]
Ostberg, C., & Kane, S. R. 2019, AJ, 158, 195, doi: 10.3847/1538-3881/ab44b0
-
[59]
Ostberg, C., Kane, S. R., Li, Z., et al. 2023, AJ, 165, 168, doi: 10.3847/1538-3881/acbfaf
-
[60]
2023, A&A, 674, A227, doi: 10.1051/0004-6361/202245790
Revol, A., Bolmont, E., Tobie, G., et al. 2023, A&A, 674, A227, doi: 10.1051/0004-6361/202245790
-
[61]
2022, SSRv, 218, 70, doi: 10.1007/s11214-022-00937-9
Rolf, T., Weller, M., G¨ ulcher, A., et al. 2022, SSRv, 218, 70, doi: 10.1007/s11214-022-00937-9
-
[62]
Rose, B. E. J., Cronin, T. W., & Bitz, C. M. 2017, ApJ, 846, 28, doi: 10.3847/1538-4357/aa8306
-
[63]
2023, SSRv, 219, 51, doi: 10.1007/s11214-023-00995-7
Salvador, A., Avice, G., Breuer, D., et al. 2023, SSRv, 219, 51, doi: 10.1007/s11214-023-00995-7
-
[64]
Showman, A. P., & Guillot, T. 2002, A&A, 385, 166, doi: 10.1051/0004-6361:20020101
-
[65]
Spiegel, D. S., Menou, K., & Scharf, C. A. 2009, ApJ, 691, 596, doi: 10.1088/0004-637X/691/1/596
-
[66]
Spiegel, D. S., Raymond, S. N., Dressing, C. D., Scharf, C. A., & Mitchell, J. L. 2010, ApJ, 721, 1308, doi: 10.1088/0004-637X/721/2/1308
-
[67]
2007, Journal of Geophysical Research (Atmospheres), 112, D09112, doi: 10.1029/2006JD007901
Takagi, M., & Matsuda, Y. 2007, Journal of Geophysical Research (Atmospheres), 112, D09112, doi: 10.1029/2006JD007901
-
[68]
Tomasko, M. G., Doose, L. R., Smith, P. H., & Odell, A. P. 1980, J. Geophys. Res., 85, 8167, doi: 10.1029/JA085iA13p08167
-
[69]
Trenberth, K. E., Fasullo, J. T., & Kiehl, J. 2009, Bulletin of the American Meteorological Society, 90, 311, doi: 10.1175/2008BAMS2634.1
-
[70]
2021, Nature, 598, 276, doi: 10.1038/s41586-021-03873-w
Turbet, M., Bolmont, E., Chaverot, G., et al. 2021, Nature, 598, 276, doi: 10.1038/s41586-021-03873-w
-
[71]
R., Kirtland Turner, S., & Gilmore, J
Vervoort, P., Horner, J., Kane, S. R., Kirtland Turner, S., & Gilmore, J. B. 2022, AJ, 164, 130, doi: 10.3847/1538-3881/ac87fd
-
[72]
Way, M. J., & Del Genio, A. D. 2020, Journal of Geophysical Research (Planets), 125, e06276, doi: 10.1029/2019JE006276
-
[73]
Way, M. J., Del Genio, A. D., Kiang, N. Y., et al. 2016, Geophys. Res. Lett., 43, 8376, doi: 10.1002/2016GL069790
-
[74]
J., Georgakarakos, N., & Clune, T
Way, M. J., Georgakarakos, N., & Clune, T. L. 2023, AJ, 166, 227, doi: 10.3847/1538-3881/ad0373 Seasonal Insolation V ariability on Early Venus 17
-
[75]
Way, M. J., Aleinov, I., Amundsen, D. S., et al. 2017, ApJS, 231, 12, doi: 10.3847/1538-4365/aa7a06
-
[76]
Widemann, T., Smrekar, S. E., Garvin, J. B., et al. 2023, SSRv, 219, 56, doi: 10.1007/s11214-023-00992-w
-
[77]
Williams, D. M., & Pollard, D. 2003, International Journal of Astrobiology, 2, 1, doi: 10.1017/S1473550403001356
-
[78]
Yang, J., Bou´ e, G., Fabrycky, D. C., & Abbot, D. S. 2014, ApJL, 787, L2, doi: 10.1088/2041-8205/787/1/L2
discussion (0)
Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.