Unique achondrite Northwest Africa 11042: Exploring the melting and breakup of the L chondrite parent body

1,2Zoltán Váci,1,2Carl B. Agee,3Munir Humayun,1,2Karen Ziegler,2Yemane Asmerom,2Victor Polyak,4Henner Busemann,4Daniela Krietsch,5Matthew Heizler,6Matthew E. Sanborn,6Qing‐Zhu Yin
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13456]
1Institute of Meteoritics, University of New Mexico, Albuquerque, New Mexico, 87131 USA
2Department of Earth and Planetary Sciences, University of New Mexico, Albuquerque, New Mexico, 87131 USA
3National High Magnetic Field Laboratory, Department of Earth Ocean & Atmospheric Science, Florida State University, Tallahassee, Florida, 32310 USA
4Institute of Geochemistry and Petrology, ETH Zürich, 8092 Zurich, Switzerland
5New Mexico Bureau of Geology, New Mexico Institute of Mining and Technology, Socorro, New Mexico, 87801 USA
6Department of Earth and Planetary Sciences, University of California, Davis, Davis, California, 95616 USA
Published by arrangement with John Wiley & Sons

Northwest Africa (NWA) 11042 is a heavily shocked achondrite with medium‐grained cumulate textures. Its olivine and pyroxene compositions, oxygen isotopic composition, and chromium isotopic composition are consistent with L chondrites. Sm‐Nd dating of its primary phases shows a crystallization age of 4100 ± 160 Ma. Ar‐Ar dating of its shocked mineral maskelynite reveals an age of 484.0 ± 1.5 Ma. This age coincides roughly with the breakup event of the L chondrite parent body evident in the shock ages of many L chondrites and the terrestrial record of fossil L chondritic chromite. NWA 11042 shows large depletions in siderophile elements (<0.01×CI) suggestive of a complex igneous history involving extraction of a Fe‐Ni‐S liquid on the L chondrite parent body. Due to its relatively young crystallization age, the heat source for such an igneous process is most likely impact. Because its mineralogy, petrology, and O isotopes are similar to the ungrouped achondrite NWA 4284 (this work), the two meteorites are likely paired and derived from the same parent body.

In situ analysis of platinum group elements in equilibrated ordinary chondrite kamacite and taenite

1Cosette M. Gilmour,1Christopher D. K. Herd
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13436]
1Department of Earth and Atmospheric Sciences, University of Alberta, 1‐26 Earth Sciences Building, Edmonton, AB, T6G 2E3 Canada
Published by arrangement with John Wiley & Sons

Platinum group element (PGE) concentrations have been determined in situ in ordinary chondrite kamacite and taenite grains via laser ablation inductively coupled plasma mass spectrometry (LA‐ICP‐MS). Results demonstrate that PGE concentrations in ordinary chondrite metal (kamacite and taenite) are similar among the three ordinary chondrite groups, in contrast to previous bulk metal studies in which PGE concentrations vary in the order H < L < LL. PGE concentrations are higher in taenite than kamacite, consistent with preferential PGE partitioning into taenite. PGE concentrations vary between and within metal grains, although average concentrations in kamacite broadly agree with results from bulk studies. The variability of PGE concentrations in metal decreases with increasing petrologic type; however, variability is still evident in most type six ordinary chondrites, suggesting that equilibration of PGEs does not occur between metal grains, but rather within individual metal grains via self‐diffusion during metamorphism. The constant average PGE concentrations within metal grains across different ordinary chondrite groups are consistent with the formation of metal via nebular condensation prior to the accretion of ordinary chondrite parent bodies. Post‐condensation effects, including heating during chondrule‐formation events, may have affected some element ratios, but have not significantly affected average metal PGE concentrations.

Characterizing organic particle impacts on inert metal surfaces: Foundations for capturing organic molecules during hypervelocity transits of Enceladus plumes

1,2J. S. New,1,3R. A. Mathies,2M. C. Price,2M. J. Cole,1,3M. Golozar,2V. Spathis,2M. J. Burchell,1A. L. Butterworth
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13448]
1Space Sciences Laboratory, University of California, Berkeley, 7 Gauss Way, Berkeley, California, 94720 USA
2School of Physical Sciences, University of Kent, Canterbury, Kent, CT2 7NH UK
3Department of Chemistry, University of California, Berkeley, California, 94720 USA
Published by arrangement with John Wiley & Sons

The presence and accessibility of a sub‐ice‐surface saline ocean at Enceladus, together with geothermal activity and a rocky core, make it a compelling location to conduct further, in‐depth, astrobiological investigations to probe for organic molecules indicative of extraterrestrial life. Cryovolcanic plumes in the south polar region of Enceladus enable the use of remote in situ sampling and analysis techniques. However, efficient plume sampling and the transportation of captured organic materials to an organic analyzer present unique challenges for an Enceladus mission. A systematic study, accelerating organic ice‐particle simulants into soft inert metal targets at velocities ranging 0.5–3.0 km s−1, was carried out using a light gas gun to explore the efficacy of a plume capture instrument. Capture efficiency varied for different metal targets as a function of impact velocity and particle size. Importantly, organic chemical compounds remained chemically intact in particles captured at speeds up to ~2 km s−1. Calibration plots relating the velocity, crater, and particle diameter were established to facilitate future ice‐particle impact experiments where the size of individual ice particles is unknown.

Phoebe’s carbon isotope composition as evidence for self-shielding in the solar nebula

1,2,3Marc Neveu,4Christopher H.House,2,3,5Scott T.Wieman
Icarus (in Press) Link to Article [https://doi.org/10.1016/j.icarus.2020.113714]
1Department of Astronomy, University of Maryland, 4296 Stadium Dr., College Park, MD 20742, USA
2Planetary Environments Laboratory, NASA Goddard Space Flight Center, 8800 Greenbelt Rd., Greenbelt, MD 20770, USA
3Center for Research in Space Science and Technology, NASA Goddard Space Flight Center, 8800 Greenbelt Rd., Greenbelt, MD 20770, USA
4Department of Geosciences, Pennsylvania State University, 503 Deike Building, University Park, PA 16802, USA
5Center for Space Sciences and Technology, University of Maryland, Baltimore County, 1000 Hilltop Cir., Baltimore, MD 21250, USA
Copyright Elsevier

Clark et al. [Clark, R.N., Brown, R.H., Cruikshank, D.P., Swayze, G.A., 2019. Icarus, 321, 791–802] reported an extremely low value of the 12C/13C ratio in CO2 ice on Phoebe, a likely captured moon of Saturn. Unless Phoebe did not form in the solar system, we interpret this value as indication that Phoebe accreted surface carbon from a region of the protosolar nebula where 13C was enriched due to self-shielding of 12CO from photodissociation. This could imply that Phoebe is also enriched in 17,18O relative to most solar system objects sampled to date. Phoebe and other objects that may have sampled these 13C-rich regions, such as Pallas or Triton, may provide the opportunity to directly measure isotopic fractionations in endmembers of the self-shielded solar nebula.

Sr-Nd-Pb isotope systematics of Australasian tektites: Implications for the nature and composition of target materials and possible volatile loss of Pb

1Lukáš Ackerman,1Karel Žák,1Roman Skála,1Jan Rejšek,1Šárka Křížová,2Josh Wimpenny,3Tomáš Magna
Geochimica et Cosmochimica Acta (in Press) Link to Article [https://doi.org/10.1016/j.gca.2020.02.025]
1Institute of Geology of the Czech Academy of Sciences, Rozvojová 269, CZ-165 00 Praha 6, Czech Republic
2Lawrence Livermore National Laboratory, Livermore, CA 94550, USA
3Czech Geological Survey, Klárov 3, CZ-118 21 Praha 1, Czech Republic
Copyright Elsevier

The Australasian tektite (AAT) strewn field is the largest strewn field on the Earth with about ∼10–30% coverage, both land and ocean, but a clearly identified source impact crater is absent despite the young age of AAT of ca. 790 ka. A genetic link between the Australasian tektites and their unequivocal parental materials is therefore largely impossible to establish. Nevertheless, the nature of the parental materials and the extent of volatilization can be constrained using the splash form tektites, carrying the chemical signatures of high-temperature processes, and the layered (so-called Muong Nong-type) tektites, which are less chemically homogenized and exceptionally abundant in the AAT field. New high-precision Sr, Nd and Pb isotopic measurements were obtained for a chemically and petrographically well-characterized suite of AAT, which included the Muong Nong-type (MN-AAT) with precisely known field locations in Laos and splash forms (SF-AAT) from different parts of the strewn field. In addition, optically dark and light zones of the MN-AAT were also separately analyzed. Homogeneous εNd values from −11.8 to −11.2, combined with a narrow range of two-stage Nd model ages from 1.67 to 1.72 Ga for the entire AAT suite, point to a well-mixed source, in terms of REE, of the crustal segment from which the sedimentary material for tektites was ultimately derived. The Sr isotopic data largely overlap for SF-AAT and MN-AAT (87Sr/86Sr = 0.71636–0.72021) and indicate Paleozoic to Mesozoic sedimentary parentage. However, late Neogene to early Quaternary re-deposition and formation of a thick silt-sized sedimentary section with vertical stratification is required to comply with 10Be data. Lead isotope systematics documents at least three different components which can perhaps be represented by different mineral phases, such as feldspar, zircon, organic matter adsorbed on young sediments etc., sorted during fluvial transport and final deposition. In addition, the SF-AAT have systematically lower Pb contents than the MN-AAT, and generally show isotopically heavier Pb isotopic ratios. This is theoretically consistent with a preferential volatilization of lighter Pb isotopes during evaporation and considerably larger Pb loss from SF-AAT when compared to MN-AAT. Nevertheless, further experimental work would be necessary to unambiguously distinguish kinetic fractionation from source mixing.

Transjordanite, Ni2P, a new terrestrial and meteoritic phosphide, and natural solid solutions barringerite-transjordanite (hexagonal Fe2P–Ni2P)

1,2Sergey N. Britvin,1Michail N. Murashko,3Yevgeny Vapnik,1Yury S. Polekhovsky,1,2Sergey V. Krivovichev,1Maria G. Krzhizhanovskaya,1Oleg S. Vereshchagin,1,4Vladimir V. Shilovskikh,1Natalia S. Vlasenko
American Mineralogist 105, 428 – 436 Link to Article [https://doi.org/10.2138/am-2020-7275]
1St. Petersburg State University, Universitetskaya Nab. 7/9, 199034 St. Petersburg, Russia
2Kola Science Center, Russian Academy of Sciences, Fersman Str. 14, 184200 Apatity, Russia
3Department of Geological and Environmental Sciences, Ben-Gurion University of the Negev, P.O.B. 653, Beer-Sheva 84105, Israel
4Institute of Mineralogy, Urals Branch of Russian Academy of Science, Miass 456317, Russia
Copyright: The Mineralogical Society of America

This paper is a first detailed report of natural hexagonal solid solutions along the join Fe2P–Ni2P. Transjordanite, Ni2P, a Ni-dominant counterpart of barringerite (a low-pressure polymorph of Fe2P), is a new mineral. It was discovered in the pyrometamorphic phosphide assemblages of the Hatrurim Formation (the Dead Sea area, Southern Levant) and was named for the occurrence on the Transjordan Plateau, West Jordan. Later on, the mineral was confirmed in the Cambria meteorite (iron ungrouped, fine octahedrite), and it likely occurs in CM2 carbonaceous chondrites (Mighei group). Under reflected light, transjordanite is white with a beige tint. It is non-pleochroic and weakly anisotropic. Reflectance values for four COM recommended wavelengths are [Rmax/Rmin, % (λ, nm)]: 45.1/44.2 (470), 49.9/48.5 (546), 52.1/50.3 (589), 54.3/52.1 (650). Transjordanite is hexagonal, space group P62m; unit-cell parameters for the holotype specimen, (Ni1.72Fe0.27)1.99P1.02, are: a = 5.8897(3), c = 3.3547(2) Å, V = 100.78(1) Å3, Z = 3. Dcalc = 7.30 g/cm3. The crystal structure of holotype transjordanite was solved and refined to R1 = 0.013 based on 190 independent observed [I > 2σ(I)] reflections. The crystal structure represents a framework composed of two types of infinite rods propagated along the c-axis: (1) edge-sharing tetrahedra [M(1)P4] and (2) edge-sharing [M(2)P5] square pyramids. Determination of unit-cell parameters for 12 members of the Fe2P–Ni2P solid-solution series demonstrates that substitution of Ni for Fe in transjordanite and vice versa in barringerite does not obey Vegard’s law, indicative of preferential incorporation of minor substituent into M(1) position. Terrestrial transjordanite may contain up to 3 wt% Mo, whereas meteoritic mineral bears up to 0.2 wt% S.

Heavy halogen geochemistry of martian shergottite meteorites and implications for the halogen composition of the depleted shergottite mantle source

1Patricia L. Clay,1Katherine H. Joy,1Brian O’Driscoll,1Henner Busemann,1Lorraine Ruzié-Hamilton,1Ray Burgess,1Jonathan Fellowes,2Bastian Joachim-Mrosko,1John Pernet-Fisher,3,4Stanislav Strekopytov, 5Christopher J. Ballentine
American Mineralogist 105, 289 – 306 Link to Article [https://doi.org/10.2138/am-2020-7237]
1Department of Earth and Environmental Sciences, University of Manchester, Manchester, M13 9PL, U.K.
2Institute of Mineralogy and Petrography, University of Innsbruck, Innrain 52f, A-6020 Innsbruck, Austria
3Imaging and Analysis Centre, Natural History Museum, Cromwell Road, London, SW7 5BD, U.K.
4National Measurement Laboratory, LGC Ltd, Queens Road, Teddington, TW11 0LY, U.K.
5Department of Earth Sciences, University of Oxford, South Parks Road, Oxford, OX1 3AN, U.K.
Copyright: The Mineralogical Society of America

Volatile elements (e.g., H, C, N) have a strong influence on the physical and chemical evolution of planets and are essential for the development of habitable conditions. Measurement of the volatile and incompatible heavy halogens, Cl, Br, and I, can provide insight into volatile distribution and transport processes, due to their hydrophilic nature. However, information on the bulk halogen composition of martian meteorites is limited, particularly for Br and I, largely due to the difficulty in measuring ppb-level Br and I abundances in small samples. In this study, we address this challenge by using the neutron irradiation noble gas mass spectrometry (NI-NGMS) method to measure the heavy halogen composition of five olivine-phyric shergottite meteorites, including the enriched (Larkman Nunatak LAR 06319 and LAR 12011) and depleted (LAR 12095, LAR 12240, and Tissint) compositional end-members. Distinct differences in the absolute abundances and halogen ratios exist between enriched (74 to136 ppm Cl, 1303 to 3061 ppb Br, and 4 to 1423 ppb I) and depleted (10 to 26 ppm Cl, 46 to 136 ppb Br, and 3 to 329 ppb I) samples. All halogen measurements are within the ranges previously reported for martian shergottite, nakhlite, and chassignite (SNC) meteorites. Enriched shergottites show variable and generally high Br and I absolute abundances. Halogen ratios (Br/Cl and I/Cl) are in proportions that exceed those of both carbonaceous chondrites and the martian surface. This may be linked to a volatile-rich martian mantle source, be related to shock processes or could represent a small degree of heavy halogen contamination (a feature of some Antarctic meteorites, for example). The differences observed in halogen abundances and ratios between enriched and depleted compositions, however, are consistent with previous suggestions of a heterogeneous distribution of volatiles in the martian mantle. Depleted shergottites have lower halogen abundances and Br and Cl in similar proportions to bulk silicate Earth and carbonaceous chondrites. Tissint in particular, as an uncontaminated fall, allows an estimate of the depleted shergottite mantle source composition to be made: 1.2 ppm Cl, 7.0 ppb Br, and 0.2 ppb I. The resultant bulk silicate Mars (BSM) estimate (22 ppm Cl, 74 ppb Br, and 6 ppb I), including the martian crust and depleted shergottite mantle, is similar to estimates of the bulk silicate earth (BSE) halogen composition.

The interior and the fusion crust in Sariçiçek howardite: Study using X-ray diffraction, magnetization measurements and Mössbauer spectroscopy

1Maksimova, A.A.,2Unsalan, O.,1Chukin, A.V.,3Karabanalov, M.S.,4Jenniskens, P.,5Felner, I.,1Semionkin, V.A.,1Oshtrakh, M.I.
Spectrochimica Acta – Part A: Molecular abd Biomolecular Spectroscopy 228, 117819 Link to Article [DOI: 10.1016/j.saa.2019.117819]
1Institute of Physics and Technology, Ural Federal University, Ekaterinburg, 620002, Russian Federation
2Faculty of Science, Department of Physics, Ege University, Bornova, Izmir 35100, Turkey
3Institute of Material Science and Metallurgy, Ural Federal University, Ekaterinburg, 620002, Russian Federation
4SETI Institute, Mountain View, CA 94043, United States
5Racah Institute of Physics, The Hebrew University, Jerusalem, 91904, Israel

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Extraterrestrial amino acids and L‐enantiomeric excesses in the CM2 carbonaceous chondrites Aguas Zarcas and Murchison

1Daniel P. Glavin,1Jamie E. Elsila,1,2Hannah L. McLain,1,2José C. Aponte,1Eric T. Parker,1Jason P. Dworkin,4Dolores H. Hill,3,4Harold C. Connolly Jr.,4Dante S. Lauretta
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13451]
1NASA Goddard Space Flight Center, Greenbelt, Maryland, 20771 USA
Catholic University of America, Washington, District of Columbia, 20064 USA
2Lunar and Planetary Laboratory, University of Arizona, Tucson, Arizona, 85721 USA
3Rowan University, Glassboro, New Jersey, 08028 USA
4Lunar and Planetary Laboratory, University of Arizona, Tucson, Arizona, 85721 USA
Published by arrangement with John Wiley & Sons

The abundances, distributions, enantiomeric ratios, and carbon isotopic compositions of amino acids in two fragments of the Aguas Zarcas CM2 type carbonaceous chondrite fall and a fragment of the CM2 Murchison meteorite were determined via liquid chromatography time‐of‐flight mass spectrometry and gas chromatography isotope ratio mass spectrometry. A suite of two‐ to six‐carbon aliphatic primary amino acids was identified in the Aguas Zarcas and Murchison meteorites with abundances ranging from ~0.1 to 158 nmol/g. The high relative abundances of α‐amino acids found in these meteorites are consistent with a Strecker‐cyanohydrin synthesis on these meteorite parent bodies. Amino acid enantiomeric and carbon isotopic measurements in both fragments of the Aguas Zarcas meteorites indicate that both samples experienced some terrestrial protein amino acid contamination after their fall to Earth. In contrast, similar measurements of alanine in Murchison revealed that this common protein amino acid was both racemic (D ≈ L) and heavily enriched in 13C, indicating no measurable terrestrial alanine contamination of this meteorite. Carbon isotope measurements of two rare non‐proteinogenic amino acids in the Aguas Zarcas and Murchison meteorites, α‐aminoisobutyric acid and D‐ and L‐isovaline, also fall well outside the typical terrestrial range, confirming they are extraterrestrial in origin. The detections of non‐terrestrial L‐isovaline excesses of ~10–15% in both the Aguas Zarcas and Murchison meteorites, and non‐terrestrial L‐glutamic acid excesses in Murchison of ~16–40% are consistent with preferential enrichment of circularly polarized light generated L‐amino acid excesses of conglomerate enantiopure crystals during parent body aqueous alteration and provide evidence of an early solar system formation bias toward L‐amino acids prior to the origin of life.

A thick crustal block revealed by reconstructions of early Mars highlands

1,2Sylvain Bouley,3James Tuttle Keane,4David Baratoux,5Benoit Langlais,6Isamu Matsuyama,1Francois Costard,7Roger Hewins,8Valerie Payré,7Violaine Sautter,1Antoine Séjourné,4Olivier Vanderhaeghe,2Brigitte Zanda

Nature Geoscience 13, 105-109 Link to Article [DOIhttps://doi.org/10.1038/s41561-019-0512-6]

1GEOPS – Géosciences Paris Sud, Univ. Paris-Sud, CNRS, Université Paris-Saclay, Orsay, France
2IMCCE – Observatoire de Paris, CNRS-UMR 8028, Paris, France
3California Institute of Technology, Pasadena, CA, USA
4Geosciences Environnement Toulouse, UMR 5563 CNRS, IRD & Université de Toulouse, Toulouse, France
5Laboratoire de Planétologie et Géodynamique, CNRS UMR 6112, Université de Nantes, Université d’Angers, Nantes, France
6Lunar and Planetary Laboratory, University of Arizona, Tucson, AZ, USA
7Institut de Minéralogie, de Physique des Matériaux, et de Cosmochimie (IMPMC) – Sorbonne Université- Muséum National d’Histoire Naturelle, UPMC Université Paris 06, UMR CNRS 7590, IRD UMR 206, Paris, France
8Department of Earth, Environmental and Planetary Sciences, Rice University, Houston, TX, USA

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