Petrogenesis of ungrouped enstatite meteorite Zakłodzie: Fabric, texture, and nanostructure analysis for identification of mechanisms responsible for chondrite–achondrite transition

1,2Agata M. Krzesińska,3Richard Wirth,3,4Monika A. Kusiak
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13296]
1Centre for Earth Evolution and Dynamics, Department of Geosciences, University of Oslo, Oslo, Norway
2Department of Earth Sciences, Natural History Museum, Cromwell Road, SW7 5BD London, UK
3GeoForschungsZentrum Potsdam, Section 3.5 Surface Geochemistry, D‐14473 Potsdam, Germany
4Institute of Geological Sciences Polish Academy of Sciences, ING PAN, Twarda 51/55, PL‐00818 Warszawa, Poland
Published by arrangement with John Wiley & Sons

Zakłodzie is an enstatite meteorite of unknown petrogenesis. Chemically, it resembles enstatite chondrites, but displays an achondrite‐like texture. Here we report on fabric and texture analyses of Zakłodzie utilizing X‐ray computed tomography and scanning electron microscopy and combine it with a nanostructural study of striated pyroxene by transmission electron microscopy. With this approach we identify mechanisms that led to formation of the texture and address the petrogenesis of the rock. Zakłodzie experienced a shock event in its early evolution while located at some depth inside a warm parent body. Shock‐related strain inverted pyroxene to the observed mixture of intercalated orthorhombic and monoclinic polymorphs. The heat that dissipated after the peak shock was added to primary, radiogenic‐derived heat and led to a prolonged thermal event. This caused local, equilibrium‐based partial melting of plagioclase and metal‐sulfide. Partial melting was followed by two‐stage cooling. The first phase of annealing (above 500 °C) allowed for crystallization of plagioclase and for textural equilibration of metal and sulfides with silicates. Below 500 °C, cooling was faster and more heterogeneous at cm scale, allowing retention of keilite and quenching of K‐rich feldspathic glass in some parts. Our study indicates that Zakłodzie is neither an impact melt rock nor a primitive achondrite, as suggested in former studies. An impact melt origin is excluded because enstatite in Zakłodzie was never completely melted and partial melting occurred during equilibrium‐based postshock conditions. Texturally, the rock represents a transition of chondrite and achondrite and was formed when early impact heat was added to internal radiogenic heat.

Geology of the Morasko craters, Poznań, Poland—Small impact craters in unconsolidated sediments

1M. Szokaluk,1R. Jagodziński,1A. Muszyński,1W. Szczuciński
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13290]
1Institute of Geology, Adam Mickiewicz University in Poznań, Bogumiła Krygowskiego 12, 61‐680 Poznań, Poland
Published by arrangement with John Wiley & Sons

Confirmed small impact craters in unconsolidated deposits are rare on Earth, and only a few have been the subjects of detailed investigations. Consequently, our knowledge of indicators permitting unambiguous identification of such structures is limited. In this work, detailed geological mapping was performed in the area of the Morasko craters, of which the largest crater is of about 96 m diameter. These craters were formed in the mid‐Holocene (~5000 yr ago) in unconsolidated sediments of a glacial terminal moraine. Fragments of the impactor—an iron meteorite—have been found in the craters’ vicinity for many decades. Despite numerous studies of the meteorite, no detailed research concerning the geological structure around the craters and of the ejecta deposits has been undertaken. The new data, including evaluation of over 52 sediment cores and 260 shallow drillings, permit the identification of four main sediment types: Neogene clays, diamicton with Neogene clay clasts containing charcoal pieces, diamicton without clasts, and sand with locally preserved paleosoil and charcoal pieces. Based on sedimentological properties, the ejecta deposits are mainly identified as diamicton with Neogene clay clasts, described as lithic impact breccia, covering locally preserved pre‐impact soil. Moreover, crater sections characterized by inverse stratigraphy of sediments are identified as belonging to overturned flaps.

Abundance and composition of kaolinite on Mars: Information from NIR spectra of rocks from acid-alteration environments, Riotinto, SE Spain

1Javier Cuadros,1Christian Mavris,2Joseph R.Michalski,3Jose Miguel Nieto,4Janice L.Bishop,5Saverio Fiore
Icarus (in Press) Link to Article [https://doi.org/10.1016/j.icarus.2019.04.027]
1Department of Earth Sciences, Natural History Museum, Cromwell Road, London SW7 5BD, UK
2Department of Earth Sciences, Laboratory for Space Research, University of Hong Kong, Pokfulam Road, Hong Kong, China
3Department of Earth Sciences, University of Huelva, 21071 Huelva, Spain
4SETI Institute, Mountain View, CA 94043, USA
5Institute of Methodologies for Environmental Analysis, CNR, Department of Geoenvironmental and Earth Sciences, University of Bari, Via Orabona 4, 70125 Bari, Italy
Copyright Elsevier

Investigation of Earth analogs and their environments is crucial for the full interpretation of geologic outcrops and processes on Mars. Phyllosilicates are important indicators of aqueous processes and their characterization is a significant piece of the geologic puzzle of Mars. They are chiefly investigated with Near-Infrared (NIR) spectroscopy from orbit. While these studies have revolutionized our understanding of aqueous processes on Mars, they are challenged by the chemical and structural complexity of phyllosilicates, non-linear response to mineral abundance, low penetration of infrared radiation in the target rocks, and spectral modifications caused by rock texture. Phyllosilicate-bearing samples from four locations in the Iberian Pyrite Belt (El Villar, Calañas, Quebrantahuesos, and Tharsis) were investigated using NIR, XRD and thermogravimetry in order to document the effects of acidic alteration under multiple environments and inform orbital detections on Mars. The samples are comprised of chlorite, illite, kaolinite, alunite, jarosite, goethite and interstratified chlorite-vermiculite and kaolinite-smectite. Kaolinite dominates the spectral signature relative to other phyllosilicates from abundances as low as 7 wt%. Only alunite and jarosite display spectral intensities similar to kaolinite. NIR spectra of bulk rock and <2 μm size fractions are very similar, indicating that spectra are dominated by the smaller particles. The octahedral Al-Fe-Mg composition of illite and kaolinite determine the positions of their OH combination band (~2.21 μm), commonly used for phyllosilicate characterization. The range of wavelength variation is narrower for kaolinite-dominated spectra, 2.205–2.216 μm, but wider than the spectral resolution of the orbital probe CRISM (~0.007 μm). Thus, in favorable conditions CRISM spectra can identify variations of kaolinite octahedral composition, a valuable tool to investigate kaolinite origin. A survey of kaolinite-bearing spectra from Mars (Leighton Crater, Mawrth Vallis and Nili Fossae regions) showed that most OH combination bands are within 2.205–2.212 μm. One spectrum displayed this band at 2.215–2.219 μm, and is a good candidate for kaolinite with significant Fe/Mg-substitution.

Best practices for the use of meteorite names in publications

1,2Philip R. Heck et al. (>10)
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13291]
1Robert A. Pritzker Center for Meteoritics and Polar Studies, Field Museum of Natural History, 1400 S Lake Shore Dr, Chicago, Illinois, 60605 USA
2Chicago Center for Cosmochemistry & Department of the Geophysical Sciences, University of Chicago, Chicago, Illinois, USA
Published by arrangement with John Wiley & Sons

This document contains suggestions for best practices by authors who refer to meteorites in publications. It can also be taken as a guide for publishers in establishing guidelines for authors. The following best practices are recommended in addition to acknowledging the loaning institution or loaning individual (unless required otherwise). The main motivations are to: help ensure that research on meteorites is reproducible, prevent confusion in the literature, and enhance tracking of specimens and related data.

Lunar soil hydration constrained by exospheric water liberated by meteoroid impacts

1,2M. Benna,3D. M. Hurley,1T. J. Stubbs,1P. R. Mahaffy,4R. C. Elphic
Nature Geoscience  (in Press) Link to Article [https://doi.org/10.1038/s41561-019-0345-3]
1NASA Goddard Space Flight Center, Greenbelt, MD, USA
2CSST, University of Maryland, Baltimore County, Baltimore, MD, USA
3The Johns Hopkins University Applied Physics Laboratory, Laurel, MD, USA
4NASA Ames Research Center, Moffett Field, CA, USA

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On the formation of diaplectic glass: Shock and thermal experiments with plagioclase of different chemical compositions

1,2Jörg Fritz,3,4Vera Assis Fernandes,3Ansgar Greshake,5Andreas Holzwarth,6Ute Böttger
Meteoritics & Planetary Science (in Press) Link to Article [https://doi.org/10.1111/maps.13289]
1Saalbau Weltraum Projekt, Liebigstraße 6, 64646 Heppenheim, Germany
2Zentrum für Rieskrater und Impaktforschung Nördlingen (ZERIN), Vordere Gerbergasse 3, 86720 Nördlingen, Germany
3Museum für Naturkunde, Leibniz Institut für Biodiversität und Evolutionsforschung, Invalidenstraße 43, 10115 Berlin, Germany
4School of Earth and Environmental Science, University of Manchester, Oxford Road, Manchester, M13 9PL UK
5Ernst Mach Institut für Kurzzeitdynamik, Fraunhofer Institut, Am Klingenberg 1, 79588 Efringen‐Kirchen, Germany
6Institut für Optische Sensoren Systeme, Deutsches Zentrum für Luft und Raumfahrt (DLR), Rutherfordstr. 2, 12489 Berlin, Germany
Published by arrangement with John Wiley & Sons

This contribution addresses the role of chemical composition, pressure, temperature, and time during the shock transformation of plagioclase into diaplectic glass—i.e., maskelynite. Plagioclase of An50‐57 and An94 was recovered as almost fully isotropic maskelynite from room temperature shock experiments at 28 and 24 GPa. The refractive index (RI) decreased to values of a quenched mineral glass for An50‐57 plagioclase shocked to 45 GPa and shows a maximum in An94 plagioclase shocked to 41.5 GPa. The An94 plagioclase experiments can serve as shock thermobarometer for lunar highland rocks and howardite, eucrite, and diogenite meteorites. Shock experiments at 28, 32, 36, and 45 GPa and initial temperatures of 77 and 293 K on plagioclase (An50‐57) produced materials with identical optical and Raman spectroscopic properties. In the low temperature (<540 K) region, the formation of maskelynite is entirely controlled by shock pressure. The RI of maskelynite decreased in heating experiments of 5 min at temperatures of >770 K, thus, providing a conservative upper limit for the postshock temperature history of the rock. Although shock recovery experiments and static pressure experiments differ by nine orders of magnitude in typical time scale (microseconds versus hours), the amorphization of plagioclase occurs at similar pressure and temperature conditions with both methods. The experimental shock calibration of plagioclase can, together with other minerals, be used as shock thermobarometer for naturally shocked rocks.

Modeling of surface spectra with and without dust from Martian infrared data: new aspects

1,4Zalewska, N.E.,2Mroczkowska-Szerszeń, M.,3Fritz, J.,4, Błęcka, M.
Aircraft Engineering and Aerospace Technology 91, 333-345 Link to Article [DOI: 10.1108/AEAT-01-2018-0051]
1Institute of Aviation, Warsaw, Poland
2Department of Geology and Geochemistry, Oil and Gas Institute, National Research Institute, Krakow, Poland
3Saalbau Weltraum Projekt, Heppenheim, Germany
4Department of Planetology, Space Research Center PAS, Warsaw, Poland

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Evaluating the influence of meteorite impact events on global potassium feldspar availability to the atmosphere since 600 ma

1,2Coldwell, B.C.,1,2,3,4,5Pankhurst, M.J.
Journal of the Geological Society 176, 209-224 Link to Article [DOI: 10.1144/jgs2018-084]
1Instituto Tecnológico y de Energías Renovables (ITER), Granadilla de Abona, Santa Cruz de Tenerife 38600, Spain
2Instituto Volcanológico de Canarias (INVOLCAN), Calle Álvaro Martín Díaz 1, San Cristóbal de La Laguna, Santa Cruz de Tenerife 38320, Spain
3School of Materials, University of Manchester, Manchester, M13 9PJ, United Kingdom
4Research Complex at Harwell, Harwell Campus, Didcot, OX11 0FA, United Kingdom
5School of Earth and Environment, University of Leeds, Leeds, LS2 9JT, United Kingdom

We currently do not have a copyright agreement with this publisher and cannot display the abstract here

Photoluminescence and Cathodoluminescence of the Solid Cometary Substance

1Simonia, I.,2,3Gucsik, A.
Open Astronomy (Baltic Astronomy) 28, 1-12 Link to Article [DOI: 10.1515/astro-2019-0003]
1School of Natural Sciences and Engineering, Ilia State University, Cholokashvili str., 3/5, Tbilisi, 0162, Georgia
2Department of Geology, University of Johannesburg, Johannesburg, South Africa
3Department of Nonlinear and Laser Optics, Wigner Research Institute for Physics, Hungarian Academy of Sciences, Budapest, Hungary

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Using cosmogenic Lithium, Beryllium and Boron to determine the surface ages of icy objects in the outer solar system

1M.M.Hedman
Icarus (in Press) Link to Article [https://doi.org/10.1016/j.icarus.2019.04.014]
1Physics Department, University of Idaho, 875 Perimeter Drive, MS 0903, Moscow, ID 83844-0903, United States of America
Copyright Elsevier

Given current uncertainties in the cratering rates and geological histories of icy objects in the outer solar system, it is worth considering how the ages of icy surfaces could be constrained with measurements from future landed missions. A promising approach would be to determine cosmic-ray exposure ages of surface deposits by measuring the amounts of cosmogenic Lithium, Beryllium and Boron at various depths within a few meters of the surface. Preliminary calculations show that ice that has been exposed to cosmic radiation for one billion years should contain these cosmogenic nuclei at concentrations of a few parts per trillion, so any future experiment that might attempt to perform this sort of measurement will need to meet stringent sensitivity requirements.
The icy worlds of the outer solar system exhibit a complex array of geological structures that reflect diverse geological histories, but there is still a great deal of uncertainty regarding when various surface features formed. Absolute ages of geological formations on icy bodies have traditionally been estimated based on the observed crater densities for particular surface units. Different models of the impactor flux yield different age estimates, but in general these calculations indicate that the most heavily cratered icy surfaces are comparable in age to the Solar System (Di Sisto and Zanardi, 2016; Kirchoff et al., 2018; Kirchoff and Schenk, 2010; Zahnle et al., 2003). However, recent studies of the dynamical history of Saturn’s satellites suggest that many of that planet’s heavily-crateredmid-sized moons may be substantially less than a billion years old (Asphaug and Reufer, 2013; Ćuk et al., 2016). At the moment, it is not clear how to reconcile these dynamical arguments with the moons’ cratering records, which highlights how little direct information we have about the ages of solid surfaces in the outer solar system.
Even if future analyses of the currently-available data are able to settle the debates regarding the ages of heavily cratered worlds, there are several objects in the outer solar system that have complex geological histories extending up to the present day, including Europa, Enceladus, Titan, Triton and Pluto (Brown et al., 2010; Pappalardo et al., 2009; Schenk et al., 2018; Schenk and Zahnle, 2007; Spencer et al., 2009; Stern et al., 2015). For these objects, a key unanswered question is how long they have been active and how long fresh material can be exposed on their surfaces before it is buried or recycled. This question is not only relevant for efforts to understand the geological history of these bodies, it also determines how long ago materials on the surface were in contact with liquid water reservoirs, which has implications for efforts to assess their habitability. It is therefore worth considering what types of future experiments could help constrain the age of icy surfaces.
The most direct way to measure the absolute age of any solid material is with in-situ measurements of unstable isotopes and/or their daughter products. These sorts of radiometric dates have been obtained from laboratory measurements of both meteorites and lunar samples, and have yielded many important insights into the formation and history of solid bodies in the inner Solar System (Davis et al., 2003; Stöffler and Ryder, 2001). Furthermore, the Mars Science Laboratory recently measured the first radiometric age on another planet, demonstrating that such measurements can be performed by space missions (Farley et al., 2014). There has also been a great deal of recent interest in a mission that would land on Europa and conduct extremely sensitive measurements of surface composition in order to ascertain whether life could exist beneath that world’s surface (Hand et al., 2017). Hence it is worth examining whether a lander on an icy world could perform experiments that would yield information about the age of its surface deposits.
The fact that the surfaces of icy bodies are composed primarily of water ice makes many of the commonly-used radiometric dating systems problematic. Even allowing for the possibility that the water ice on various worlds could have substantial amounts of methane, ammonia, and various organic compounds, the elemental composition of their surfaces would still be dominated by the light elements Hydrogen, Carbon, Nitrogen and Oxygen. The longest-lived unstable isotope of these elements is 14C, which has ahalf-life of about 5700 years (http://www.nndc.bnl.gov/nudat2). While this isotope has been extensively used to date events from the Quaternary period here on Earth (http://intchron.org), and has even been proposed as a way to probe carbon transport processes on Titan (Lorenz et al., 2002), its half-life is far too short to probe the geological history of surfaces that are millions or billions of years old. Indeed, most commonly-used techniques for radiometrically dating rocks involve nuclei with half-lives of order 1 billion years, such as 40K, 87Rb and various isotopes of Uranium. While elements with such long-lived unstable isotopes like Potassium could be present near the surfaces of some icy worlds, a dating technique that relies on such contaminants would require more detailed information about the surface composition of these bodies than we currently have.
In the absence of long-lived isotopes, the most promising way to date ancient icy surfaces is with cosmic-ray exposure ages. The basic idea behind these dates is that any exposed surface is constantly being bombarded with high-energy cosmic rays that cause nuclear reactions within the material. The concentration of the resulting cosmogenic nuclei near the surface therefore increases over time and can provide information about the age of the surface deposit. Such cosmic-ray exposure ages have been used to date various surface deposits on both the Earth and the Moon, and to determine when meteorites broke free from their parent asteroids (Dunai, 2010; Eugster, 2003; Herzog and Caffee, 2014).
Of course, cosmic-ray exposure ages do depend on the assumed flux of cosmic rays, which can vary over time. Indeed, records of cosmogenic nuclei like 14C and 10Be in terrestrial ice cores show that the cosmic ray flux here on Earth has varied byroughly a factor of two on timescales of hundreds to thousands of years (Steinhilber et al., 2012). Fortunately, these variations appear to average out over the longer timescales relevant for dating astronomical bodies. For example, analyses of the cosmic-ray exposure ages from stony meteorites (which range between 1 and 100 million years) indicate that the average cosmic ray flux has varied by less than about 10% over the past 10 million years (Wieler et al., 2013). Exposure ages of iron meteorites extend back 1–2 billion years and can potentially constrain the cosmic ray flux on even longer timescales. However, the interpretation of these data is still uncertain, with some recent analyses suggesting the flux has varied by less than 50%, while others argue for factor of 3 flux variations over timescales of 500 million years (Alexeev, 2016; Alexeev, 2017; Ammon et al., 2009; Wieler et al., 2013). Such long-term flux variations would certainly need to be better constrained before cosmic-ray exposureages could provide accurate geological histories for icy moons. However, even if the long-term variations were as large as a factor of 3 over 500 million years, cosmic-ray exposure ages could still be used to determine if the heavily-cratered icy surfaces in the Saturn system are comparable to the age of the solar system or just a few hundred million years old.
Nuclear reactions induced by high-energy cosmic rays usually generate nuclei with atomic numbers comparable to or less than that of the original nuclei. This again means that only elements with low atomic numbers are likely to be available. Among these, isotopes of Hydrogen, Carbon, Nitrogen and Oxygen are probably not viable because these elements should be common native constituents of the ice, and so distinguishing any cosmogenic material will be extremely challenging. On the other hand, any Helium generated by cosmic rays should diffuse through ice on geological timescales, so this material will probably escape the surface. This leaves Lithium, Beryllium and Boron as the most promising elements for cosmic-ray exposure dating of icy surfaces. These elements are all found at very low concentrations in chondrites, Earth’s crust and ocean water (see Table 1), and they are all chemically reactive species that can be retained in-situ for geological timescales (Indeed, cosmogenic Beryllium in terrestrial ice cores have been used to trace variations in the cosmic ray flux into Earth’s atmosphere over the past 10, 000 years, e.g. (Steinhilber et al., 2012)).