¹Zaicong Wang et al. (>10)
Geochimica et Cosmochimica Acta (in Press) Link to Article [https://doi.org/10.1016/j.gca.2024.03.029]
¹State Key Laboratory of Geological Processes and Mineral Resources, School of Earth Sciences, China University of Geosciences, Wuhan 430074, China
Copyright Elsevier

The Moon’s mare volcanism predominantly occurs within the Procellarum KREEP Terrane (PKT), which is widely thought to be associated with KREEP components within the lunar interior. The Chang’e-5 (CE-5) mission sampled a young (2 Ga) mare basalt Em4/P58 unit of northern Oceanus Procellarum. The geochemistry of the CE-5 mare basalt enables assessment of mantle source compositions which are essential to understand the thermo-chemical mechanism for prolonged volcanism during secular cooling of the Moon. Geochemical compositions of the CE-5 bulk soil, breccias, and basalt clasts from various depths within the drill core consistently display high concentrations of incompatible trace elements (ITE: ∼ 0.3 × high-K KREEP; ∼ 5 μg/g Th) with KREEP-like inter-element ratios, for example for La/Sm, Nb/Ta, and Zr/Y. Exotic impact ejecta, extensive magma differentiation (<70 % fractional crystallization) and significant assimilation of KREEP materials during magma transit and eruption cannot account for the ITE contents and ratios or radiogenic isotope compositions (e.g., εNdinitial of + 8 to + 9 and εHfinitial of + 40 to + 46) of the CE-5 basalts; instead, partial melting of their mantle source played a dominant role. The Chang’e-5 basalt is a chemically evolved low-Ti mare basalt (Mg# of ∼ 34) with enriched KREEP-like ITE compositions but high long-term time-integrated Sm/Nd and Lu/Hf ratio, which represents a hitherto unsampled type of mare basalt. It formed by melting of an augite-rich mantle source (late-stage magma ocean cumulates containing > 30–60 % augite, and little or no ilmenite), with a small amount of late-stage interstitial melt that resembles KREEP (∼1–1.5 modal %, equivalent to 0.2–0.3 μg/g Th). The voluminous mare basalts making up the Em4/P58 unit (>1500 km3) provide compelling evidence for large-scale, ITE enriched young mare magmatism within Oceanus Procellarum. In combination with remote sensing data and with the unique Th-rich Apollo 12 basalt fragment 12032,366–18 (impact ejecta likely from Oceanus Procellarum), this implies that significant portions of the FeO- and Th-rich mare regions of the western PKT may also have formed in a similar way.

¹Takazo Shibuya,^2,3Yasuhito Sekine,⁴Sakiko Kikuchi,^5,6,2Hiroyuki Kurokawa,³Keisuke Fukushi,⁷Tomoki Nakamura,⁸Sei-ichiro Watanabe
Geochimica et Cosmochimica Acta (in Press) Open Access Link to Article [https://doi.org/10.1016/j.gca.2024.03.022]
¹Super-cutting-edge Grand and Advanced Research (SUGAR) Program, Institute for Extra-cutting-edge Science and Technology Avant-garde Research (X-star), Japan Agency for Marine-Earth Science and Technology (JAMSTEC), Yokosuka 237-0061, Japan
²Earth-Life Science Institute (ELSI), Tokyo Institute of Technology, Meguro, Tokyo 152-8550, Japan
³Institute of Nature and Environmental Technology, Kanazawa University, Kakuma, Kanazawa 920-1192, Japan
⁴Kochi Institute for Core Sample Research, Institute for Extra-cutting-edge Science and Technology Avant-garde Research (X-star), Japan Agency for Marine-Earth Science and Technology (JAMSTEC), Nankoku, Kochi 783-8502, Japan
⁵Department of Earth Science and Astronomy, Graduate School of Arts and Sciences, The University of Tokyo, Tokyo 153-8902, Japan
⁶Department of Earth and Planetary Science, Graduate School of Science, The University of Tokyo, Tokyo 113-0033, Japan
⁷Department of Earth Sciences, Tohoku University, Sendai 980-8578, Japan
⁸Department of Earth and Environmental Sciences, Nagoya University, Nagoya 464-8601, Japan
Copyright Elsevier

Parent bodies of carbonaceous chondrites that initially contained metallic iron potentially exert strong reduction power during aqueous alteration to generate molecular hydrogen in excess of hydrogen solubility in water-rich fluids. The surplus hydrogen escapes from the system, which is subsequently supplied to overlying regions in planetesimals. Based on this concept, we conducted chemical equilibrium modeling of the aqueous alteration and simulated gaseous H2 migration within the icy planetesimal that has a melted mantle and an icy shell during the early stages of radiogenic heating. In the chemical equilibrium modeling, we simulated the aqueous alteration of chondritic rocks at 0–350 °C and a water/rock mass ratio of 0.2–10 with initial CO2 contents of 0–10 mol% in the fluid. The results showed that the mineral assemblage and solution composition change with the temperature, water/rock mass ratio, and initial fluid composition. The reproduced mineral paragenesis and abundance well explain those of carbonaceous chondrites. Furthermore, it was revealed that the initial H2 fugacity of the system influences not only the stability of minerals and solution compositions, but also the preservation potential of organic molecules. Indeed, within these parameter spaces, the modeling results account for the organic/inorganic carbon-rich alterations reported for the Tagish Lake meteorite, Ceres, and Ryugu. Simulations of gaseous H2 migration in a planetesimal revealed that gaseous H2 in the deep interior can be transported to the interface with an icy shell even if the permeability is low. Moreover, it is highly possible that an H2-rich layer would have been widely formed just below the icy shell. Therefore, it is expected that H2-rich regions beneath the ice layer in planetesimals have substantial potential for the synthesis and preservation of organic molecules. These results imply that the alteration of carbonaceous chondrite parent bodies and C-complex asteroids is characterized by not only the type of parent bodies (e.g., formation age and distance from the Sun) but also the locations within their parent bodies.

^1,2Kong, Seongyoung,¹Singh, Prashant,^1,2Sarkar, Arka,^1,2Viswanathan, Gayatri,³Kolen’ko, Yury V.,²Mudryk, Yaroslav,^2,4Johnson, Duane D.,^1,2Kovnir, Kirill
Chemistry of Materials 36, 1665-1677 Link to Article [DOI 10.1021/acs.chemmater.3c03003]
¹Department of Chemistry, Iowa State University, Ames, 50011, IA, United States
²Ames National Laboratory, U.S. Department of Energy, Ames, 50011, IA, United States
³Nanochemistry Research Group, International Iberian Nanotechnology Laboratory, Braga, 4715-330, Portugal
⁴Department of Materials Science & Engineering, Iowa State University, Ames, 50011, IA, United States

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^1,2,3He, Ye et al. (>10)
Aerospace 11, 114 Open Access Link to Article [DOI 10.3390/aerospace11020114]
¹Institute of Geology and Geophysics, Chinese Academy of Sciences, Beijing, 100029, China
²Institutes of Earth Science, Chinese Academy of Sciences, Beijing, 100029, China
³College of Earth and Planetary Sciences, University of Chinese Academy of Sciences, Beijing, 100049, China

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^1,2Masahiko Sato,^3,4Kosuke Kurosawa,²Sunao Hasegawa,⁵Futoshi Takahashi
Journal of Geophysical Research (Planets)(in Press) Open Access Link to Article [https://doi.org/10.1029/2023JE007864]
¹Department of Earth and Planetary Science, The University of Tokyo, Tokyo, Japan
²Institute of Space and Astronautical Science, Japan Aerospace Exploration Agency, Sagamihara, Japan
³Department of Human Environmental Science, Kobe University, Kobe, Japan
⁴Planetary Exploration Research Center, Chiba Institute of Technology, Narashino, Japan
⁵Department of Earth and Planetary Sciences, Kyushu University, Fukuoka, Japan
Published by arrangement with John Wiley & Sons

Knowledge of the shock remanent magnetization (SRM) property is crucial for interpreting the spatial change in a magnetic anomaly observed over an impact crater. This study conducted two series of impact-induced SRM acquisition experiments by varying the applied field intensity (0–400 μT) and impact conditions. Systematic remanence measurements of cube-shaped subsamples cut from shocked basalt containing single-domain titanomagnetite were conducted to investigate the effects of changes in pressure and temperature on the SRM acquisition. The peak pressure and temperature distributions in the shocked samples were estimated using shock-physics modeling. SRM intensity was proportional to the applied field intensity of up to 400 μT. SRM intensity data for peak pressure and temperature of up to 8.0 GPa and 530 K, respectively, clearly show that it increases with increasing pressure and decreases with increasing temperature. The SRM has unblocking temperature components up to a Curie temperature of 510 K, and it easily demagnetizes with alternating field demagnetization. The observed SRM properties can be explained by the pressure-induced microcoercivity reduction and temperature-induced modification of the blocking curve. Although the remanence acquisition efficiency of the SRM is significantly lower than that of the thermoremanent magnetization (TRM), the magnetic anomaly originating from the SRM distribution in a broader region may show a contribution comparable to that of the impact-induced TRM distribution in a narrow region.

¹Evgeny Smirnov
Icarus (in Press) Link to Article [https://doi.org/10.1016/j.icarus.2024.116058]
¹Evgeny SmirnovBelgrade Astronomical Observatory, Volgina 7, 11060, Belgrade, Serbia
Copyright Elsevier

This study explores how well various machine learning classifiers can identify mean-motion resonances in the main belt using supervised learning. The most popular classifiers are assessed: k-Nearest Neighbours, Decision Tree, Gradient Boosting, AdaBoost, Random Forest, and Naïve Bayes. In contrast to previous studies that often relied on default ML configurations, this research conducts a detailed investigation, fine-tuning, and testing of each classifier across various parameters. The results show that simpler models, especially k-Nearest Neighbours and Decision Tree, perform better than more complex ones, particularly in terms of
scores. The paper provides guides on selecting features, parameters, and training set sizes for optimal classifier performance and outlines a method for developing effective machine-learning models for asteroid classification.

¹Clara Maurel,¹Jérôme Gattacceca
Proceedings of the National Academy of Science of America (PNAS) 121, e2312802121 Link to Article [https://doi.org/10.1073/pnas.23128021]
¹CNRS, Aix Marseille Université, IRD, INRAE, Centre de Recherche et d’Enseignement des Géosciences de l’Environnement (CEREGE), Aix-en-Provence 13545, France

Magnetic fields in protoplanetary disks are thought to play a prominent role in the formation of planetary bodies. Acting upon turbulence and angular momentum transport, they may influence the motion of solids and accretion onto the central star. By searching for the record of the solar nebula field preserved in meteorites, we aim to characterize the strength of a disk field with a spatial and temporal resolution far superior to observations of extrasolar disks. Here, we present a rock magnetic and paleomagnetic study of the andesite meteorite Erg Chech 002 (EC002). This meteorite contains submicron iron grains, expected to be very reliable magnetic recorders, and carries a stable, high-coercivity magnetization. After ruling out potential sources of magnetic contamination, we show that EC002 most likely carries an ancient thermoremanent magnetization acquired upon cooling on its parent body. Using the U-corrected Pb-Pb age of the meteorite’s pyroxene as a proxy for the timing of magnetization acquisition, we estimate that EC002 recorded a field of 60 ± 18 µT at a distance of ~2 to 3 astronomical units, 2.0 ± 0.3 My after the formation of calcium-aluminum-rich inclusions. This record can only be explained if EC002 was magnetized by the field prevalent in the solar nebula. This makes EC002’s record, particularly well resolved in time and space, one of the two earliest records of the solar nebula field. Such a field intensity is consistent with stellar accretion rates observed in extrasolar protoplanetary disks.

^1,2,3Fan Liu,^3,4,5,6,7,8Yuan-Sen Ting,^3,4David Yong,^9,10Bertram Bitsch,^1,3Amanda Karakas,²Michael T. Murphy,^11,12Meridith Joyce,¹³Aaron Dotter,^14,15Fei Dai
Nature 627, 501-504 Link to Article [DOI https://doi.org/10.1038/s41586-024-07091-y]
¹School of Physics and Astronomy, Monash University, Clayton, Victoria, Australia
²Centre for Astrophysics and Supercomputing, Swinburne University of Technology, Hawthorn, Victoria, Australia
³ARC Centre for All Sky Astrophysics in 3D (ASTRO-3D), Canberra, Australian Capital Territory, Australia
⁴Research School of Astronomy and Astrophysics, Australian National University, Weston, Australian Capital Territory, Australia
⁵School of Computing, Australian National University, Acton, Australian Capital Territory, Australia
⁶Department of Astronomy, The Ohio State University, Columbus, OH, USA
⁷Center for Cosmology and AstroParticle Physics (CCAPP), The Ohio State University, Columbus, OH, USA
⁸Observatories of the Carnegie Institution of Washington, Pasadena, CA, USA
⁹Max-Planck-Institut für Astronomie, Heidelberg, Germany
¹⁰Department of Physics, University College Cork, Cork, Ireland
¹¹HUN-REN Research Centre for Astronomy and Earth Sciences, Konkoly Observatory, Budapest, Hungary
¹²CSFK, MTA Centre of Excellence, Budapest, Hungary
¹³Department of Physics and Astronomy, Dartmouth College, Hanover, NH, USA
¹⁴Division of Geological and Planetary Sciences, California Institute of Technology, Pasadena, CA, USA
¹⁵Department of Astronomy, California Institute of Technology, Pasadena, CA, USA

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^1,2Qadri S.B.,²Goswami R.,²Imler G.,²Qadri S.N.
Materialia 33, 102035 Link to Article [DOI 10.1016/j.mtla.2024.102035]
¹Retired Emeritus, US Naval Research Laboratory, Washington, 20375, DC, United States
²Materials Science and Technology Division, US Naval Research Laboratory, Washington, 20375, DC, United States

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¹Agrosì, Giovanna, ²Manzari, Paola,¹Mele, Daniela,¹Tempesta, Gioacchino, ¹Rizzo, Floriana,³Catelani, Tiziano,⁴Bindi, Luca
Communications Earth and Environment 5, 67 Open Access Link to Article [DOI 10.1038/s43247-024-01233-w]
¹Dipartimento di Scienze della Terra e Geoambientali, Università degli Studi di Bari Aldo Moro, Via Orabona 4, Bari, I-70125, Italy
²Agenzia Spaziale Italiana, Centro Spaziale di Matera, Matera, Terlecchia, I-75100, Italy
³Centro Servizi MEMA, Università di Firenze, Via Capponi 3r, Florence, I-50121, Italy
⁴Dipartimento di Scienze della Terra, Università di Firenze, Via La Pira 4, Florence, I-50121, Italy

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