Resonances of the InSight Seismometer on Mars

Bulletin of the Seismological Society of America Seismological Society of America (SSA) 111:6 (2021) 2951-2963

Authors:

Kenneth Hurst, Lucile Fayon, Brigitte Knapmeyer-Endrun, Cedric Schmelzbach, Martin van Driel, Joan Ervin, Sharon Kedar, William T Pike, Simon Calcutt, Tristram Warren, Constantino Charalambous, Alexander Stott, Marco Bierwirth, Philippe Lognonne, Sebastien de Raucourt, Taoufik Gabsi, Tanguy Nebut, Oliver Robert, Sylvain Tillier, Savas Ceylan, Maren Böse, John Clinton, Domenico Giardini, Anna Horleston, Taichi Kawamura, Amir Khan, Guenole Orhand-Mainsant, John-Robert Scholz, Simon Stähler, Jennifer Stevanovic, William B Banerdt

Vertical distribution of aerosols and hazes over Jupiter's great red spot and its surroundings in 2016 from HST/WFC3 imaging

Journal of Geophysical Research: Planets American Geophysical Union 126:11 (2021) e2021JE006996

Authors:

Asier Anguiano‐Arteaga, Santiago Pérez‐Hoyos, Agustín Sánchez‐Lavega, José Francisco Sanz‐Requena, Patrick GJ Irwin

Abstract:

In this work, we have analyzed images provided by the Hubble Space Telescope's Wide Field Camera 3 (HST/WFC3) in December 2016, with a spectral coverage from the ultraviolet to the near infrared. We have obtained the spectral reflectivity of the GRS and its surroundings, with particular emphasis on selected, dynamically interesting regions. A spectral characterization of the GRS area is performed following two different procedures: (a) in terms of Altitude/Opacity and Color Indices (AOI and CI); (b) by means of automatic spectral classification. We used the NEMESIS radiative transfer suite to retrieve the main atmospheric parameters (e.g., particle vertical and size distributions, refractive indices) that are able to explain the observed spectral reflectivity. The optimal a priori model atmosphere used for the retrievals is obtained from a grid of about 12,000 different atmospheric models, and choosing the one that best fits South Tropical Zone (STrZ) spectra and its observed limb-darkening. We conclude that the spectral reflectivity of the GRS area is well reproduced with the following layout: (a) a stratospheric haze with its base near the 100 mbar level, with optical depths at 900 nm of the order of unity and particles with a size of 0.3 μm; (b) a more vertically extended tropospheric haze, with τ (900 nm) ∼10 down to 500 mbar and micron sized particles. Both haze layers show a stronger short wavelength absorption, and thus both act as chromophores. The altitude difference between clouds tops in the GRS and surrounding areas is ∼10 km.

Tracing the earliest stages of hydrothermal alteration on the CM chondrite parent body

Meteoritics and Planetary Science Wiley 56:9 (2021) 1708-1728

Authors:

AJ King, E Mason, HC Bates, PF Schofield, KL Donaldson Hanna, NE Bowles, SS Russell

Meridional variations on C2H2 in Jupiter's stratosphere from Juno UVS observations

Journal of Geophysical Research: Planets American Geophysical Union 126:8 (2021) e2021JE006928

Authors:

Rohini S Giles, Thomas K Greathouse, Vincent Hue, G Randall Gladstone, Henrik Melin, Leigh N Fletcher, Patrick GJ Irwin, Joshua A Kammer, Maarten H Versteeg, Bertrand Bonfond, Denis C Grodent, Scott J Bolton, Steven M Levin

Abstract:

The Ultraviolet Spectrograph (UVS) instrument on the Juno mission records far-ultraviolet reflected sunlight from Jupiter. These spectra are sensitive to the abundances of chemical species in the upper atmosphere and to the distribution of the stratospheric haze layer. We combine observations from the first 30 perijoves of the mission in order to study the meridional distribution of acetylene (C2H2) in Jupiter's stratosphere. We find that the abundance of C2H2 decreases toward the poles by a factor of 2–4, in agreement with previous analyses of mid-infrared spectra. This result is expected from insolation rates: near the equator, the UV solar flux is higher, allowing more C2H2 to be generated from the UV photolysis of CH4. The decrease in abundance toward the poles suggests that horizontal mixing rates are not rapid enough to homogenize the latitudinal distribution.

A stringent upper limit of 20 pptv for methane on Mars and constraints on its dispersion outside Gale crater

Astronomy and Astrophysics EDP Sciences 650 (2021) A140

Authors:

F Montmessin, Oi Korablev, A Trokhimovskiy, F Lefevre, Aa Fedorova, L Baggio, A Irbah, G Lacombe, Kevin S Olsen, As Braude, Da Belyaev, J Alday, F Forget, F Daerden, J Pla-Garcia, S Rafkin, CF Wilson, A Patrakeev, A Shakun, Jl Bertaux

Abstract:

Context. Reports on the detection of methane in the Martian atmosphere have motivated numerous studies aiming to confirm or explain its presence on a planet where it might imply a biogenic or more likely a geophysical origin.
Aims. Our intent is to complement and improve on the previously reported detection attempts by the Atmospheric Chemistry Suite (ACS) on board the ExoMars Trace Gas Orbiter (TGO). This latter study reported the results of a campaign that was a few months in length, and was significantly hindered by a dusty period that impaired detection performances.
Methods. We unveil 640 solar occultation measurements gathering 1.44 Martian years worth of data produced by the ACS.
Results. No methane was detected. Probing the clear northern summer season allowed us to reach 1σ upper limits of around 10 pptv (20 pptv at 2σ), with an annual mean of the smallest upper limits of 20 pptv. Upper limits are controlled by the amount of dust in the atmosphere, which impairs detection performance around the equator and during the southern spring and summer seasons. Observations performed near Gale crater yielded 1σ upper limits of up to four times less than the background values measured by the Curiosity rover during the corresponding seasons.
Conclusions. Reconciliation of the absence of methane in the TGO spectra with the positive detections by Curiosity is even more difficult in light of this annual survey performed by ACS. Stronger constraints are placed on the physical and chemical mechanism capable of explaining why the mean of the best overall upper limits of ACS is ten times below the smallest methane abundances measured by Curiosity.