Stardust Interstellar Preliminary Examination VIII: Identification of crystalline material in two interstellar candidates

Gainsforth et al. (>>10)*

*Find the extensive, full author and affiliation list on the publishers website.

Using synchrotron-based X-ray diffraction measurements, we identified crystalline material in two particles of extraterrestrial origin extracted from the Stardust Interstellar Dust Collector. The first particle, I1047,1,34 (Hylabrook), consisted of a mosaiced olivine grain approximately 1 µm in size with internal strain fields up to 0.3%. The unit cell dimensions were a = 4.85 ± 0.08 Å, b  =  10.34 ± 0.16 Å, c  =  6.08 ± 0.13 Å (2σ). The second particle, I1043,1,30 (Orion), contained an olivine grain ≈ 2 µm in length and >500 nm in width. It was polycrystalline with both mosaiced domains varying over ≈ 20º and additional unoriented domains, and contained internal strain fields < 1%. The unit cell dimensions of the olivine were a = 4.76 ± 0.05 Å, b  =  10.23 ± 0.10 Å, c  =  5.99 ± 0.06 Å (2σ), which limited the olivine to a forsteritic composition  >Fo65 (2σ). Orion also contained abundant spinel nanocrystals of unknown composition, but unit cell dimension a  = 8.06 ± 0.08 Å (2σ). Two additional crystalline phases were present and remained unidentified. An amorphous component appeared to be present in both these particles based on STXM and XRF results reported elsewhere.

Reference
Gainsforth et al. (in press) Stardust Interstellar Preliminary Examination VIII: Identification of crystalline material in two interstellar candidates. Meteoritics & Planetary Science
[doi:10.1111/maps.12148]
Published by arrangement with John Wiley & Sons

(The article is temporarily unavailable on the MAPS website.)

Stardust Interstellar Preliminary Examination III: Infrared spectroscopic analysis of interstellar dust candidates

Bechtel et al. (>>10)*

*Find the extensive, full author and affiliation list on the publishers website.

Under the auspices of the Stardust Interstellar Preliminary Examination, picokeystones extracted from the Stardust Interstellar Dust Collector were examined with synchrotron Fourier transform infrared (FTIR) microscopy to establish whether they contained extraterrestrial organic material. The picokeystones were found to be contaminated with varying concentrations and speciation of organics in the native aerogel, which hindered the search for organics in the interstellar dust candidates. Furthermore, examination of the picokeystones prior to and post X-ray microprobe analyses yielded evidence of beam damage in the form of organic deposition or modification, particularly with hard X-ray synchrotron X-ray fluorescence. From these results, it is clear that considerable care must be taken to interpret any organics that might be in interstellar dust particles. For the interstellar candidates examined thus far, however, there is no clear evidence of extraterrestrial organics associated with the track and/or terminal particles. However, we detected organic matter associated with the terminal particle in Track 37, likely a secondary impact from the Al-deck of the sample return capsule, demonstrating the ability of synchrotron FTIR to detect organic matter in small particles within picokeystones from the Stardust interstellar dust collector.

Reference
Bechtel et al. (in press) Stardust Interstellar Preliminary Examination III: Infrared spectroscopic analysis of interstellar dust candidates. Meteoritics & Planetary Science
[doi:10.1111/maps.12125]
Published by arrangement with John Wiley & Sons

(The article is temporarily unavailable on the MAPS website.)

Stardust Interstellar Preliminary Examination XI: Identification and elemental analysis of impact craters on Al foils from the Stardust Interstellar Dust Collector

Stroud et al. (>>10)*

*Find the extensive, full author and affiliation list on the publishers website.

The Stardust Interstellar Preliminary Examination team analyzed thirteen Al foils from the NASA Stardust interstellar collector tray in order to locate candidate interstellar dust (ISD) grain impacts. Scanning electron microscope (SEM) images reveal that the foils possess abundant impact crater and crater-like features. Elemental analyses of the crater features, with Auger electron spectroscopy, SEM-based energy dispersive X-ray (EDX) spectroscopy, and scanning transmission electron microscope-based EDX spectroscopy, demonstrate that the majority are either the result of impacting debris fragments from the spacecraft solar panels, or intrinsic defects in the foil. The elemental analyses also reveal that four craters contain residues of a definite extraterrestrial origin, either as interplanetary dust particles or ISD particles. These four craters are designated level 2 interstellar candidates, based on the crater shapes indicative of hypervelocity impacts and the residue compositions inconsistent with spacecraft debris.

Reference
Stround et al. (in press) Stardust Interstellar Preliminary Examination XI: Identification and elemental analysis of impact craters on Al foils from the Stardust Interstellar Dust Collector. Meteoritics & Planetary Science
[doi:10.1111/maps.12136]
Published by arrangement with John Wiley & Sons

(The article is temporarily unavailable on the MAPS website.)

Evolution of the angrite parent body: Implications of metamorphic coronas in NWA 3164

Bashar Baghdadi1,*, Gaston Godard2, Albert Jambon1

1UPMC Paris 6, Institut des Sciences de la Terre Paris, Paris Cedex 05, France
2Institut de Physique du Globe de Paris, Sorbonne Paris Cité, Univ. Paris-Diderot, Paris Cedex 05, France

Northwest Africa 3164 is a coarse-grained angrite that shows reaction coronas, a unique character among achondrites. Olivine (Fo57; 1.2 wt% CaO), fassaitic clinopyroxene, anorthite, and spinel account for 46–47, 28–29, 8–13, and 4–8 vol%, respectively; kamacite is an accessory phase. The spinel grains in contact with clinopyroxene are bounded by discontinuous 20 μm thick coronas of anorthite and olivine, indicating the reaction Cpx + Spl → Ol + An (R1). In addition, irregular coronas of clinopyroxene and spinel developed around the primary anorthite in contact with primary olivine, during the reaction Ol + An → Cpx + Spl (R2). R2 also generated clinopyroxene and spinel films between the secondary olivine and anorthite coronas produced during R1, implying that R1 preceded R2. Both are metamorphic reactions that developed in the solid state. Finally, the coronas are cross cut by μm-thick veinlets due to a late shock. A mass-balance study shows that R2 is almost the reverse of R1. The P–T metamorphic evolution of the rock, modeled by calculating a P–T isochemical diagram, indicates an equilibrium T of 940 ± 120 °C at P < 0.9 GPa for the initial assemblage, followed by an increase of T up to approximately 1000–1200 °C during reaction R1 and a subsequent cooling during R2. Several causes are envisaged to account for this metamorphic evolution. Contact metamorphism due to a hot magmatic intrusion in the angrite parent body is favored, as similar metamorphic coronas are well known in metamorphic terrestrial rocks. In addition to differentiation and magmatism, there is now evidence for metamorphism in the angrite parent body, which would have been a large asteroid or a planetary-sized body.

Reference
Baghdadi B, Godard G and Jambon A (in press) Evolution of the angrite parent body: Implications of metamorphic coronas in NWA 3164. Meteoritics & Planetary Science
[doi:10.1111/maps.12202]
Published by arrangement with John Wiley & Sons

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Comparisons of fresh complex impact craters on Mercury and the Moon: Implications of controlling factors in impact excavation processes

Zhiyong Xiaoa,b,*, Robert G. Stromb, Clark R. Chapmanc, James W. Headd, Christian Klimczake, Lillian R. Ostrachf, Jörn Helbertg, Piero D’Inceccog

aPlanetary Science Institute, Faculty of Earth Sciences, China University of Geosciences (Wuhan), Wuhan, Hubei, 430074, China
bLunar and Planetary Laboratory, University of Arizona, Tucson, Arizona, 85719, USA
cDepartment of Space Studies, Southwest Research Institute, Boulder, Colorado, 80302, USA
dDepartment of Geological Sciences, Brown University, Providence, Rhode Island, 02912, USA
eDepartment of Terrestrial Magnetism, Carnegie Institution of Washington, Washington, D.C., 20015, USA
fSchool of Earth and Space Exploration, Arizona State University, Arizona, USA, 85281
gInstitute of Planetary Research, Deutsches Zentrum für Luft- und Raumfahrt, 12489 Berlin, Germany

The impact cratering process is usually divided into the coupling, excavation, and modification stages, where each stage is controlled by a combination of different factors. Although recognized as the main factors governing impact processes on airless bodies, the relative importance of gravity, target and projectile properties, and impact velocity in each stage is not well understood. We focus on the excavation stage to place better constraints on its controlling factors by comparing the morphology and scale of crater-exterior structures for similar-sized fresh complex craters on the Moon and Mercury. We find that the ratios of continuous ejecta deposits, continuous secondaries facies, and the largest secondary craters on the continuous secondaries facies between same-sized Mercurian and lunar craters are consistent with predictions from gravity-regime crater scaling laws. Our observations support that gravity is a major controlling factor on the excavation stage of the formation of complex impact craters on the Moon and Mercury. On the other hand, similar-sized craters with identical background terrains on Mercury have different spatial densities of secondaries on the continuous secondaries facies, suggesting that impactor velocity may also be important during the excavation stage as larger impactor velocity may also cause greater ejection velocities. Moreover, some craters on Mercury have more circular and less clustered secondaries on the continuous secondaries facies than other craters on Mercury or the Moon. This morphological difference appears not to have been caused by the larger surface gravity or the larger median impact velocity on Mercury. A possible interpretation is that at some places on Mercury, the target material might have unique properties causing larger ejection angles during the impact excavation stage. We conclude that gravity is the major controlling factor on the impact excavation stage of complex craters, impact velocity and target properties may also affect the excavation stage but their importance is to a less degree compared with gravity.

Reference
Xiao Z, Strom RG, Chapman CR, Head JW, Klimczak C, Ostrach LR, Helbert J, and D’Incecco P (in press) Comparisons of fresh complex impact craters on Mercury and the Moon: Implications of controlling factors in impact excavation processes. Icarus
[doi:10.1016/j.icarus.2013.10.002]
Copyright Elsevier

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Book Review: Meteoriten—Meteorites: Zeitzeugen der Entstehung des Sonnensystems/Witnesses of the origin of the solar system.

A. J. Timothy Jull

Department of Geosciences, University of Arizona, Tucson Arizona, USA

No abstract is available for this article.

Reference
Jull AJT (in press) Book Review: Meteoriten—Meteorites: Zeitzeugen der Entstehung des Sonnensystems/Witnesses of the origin of the solar system. Meteoritics & Planetary Science
[doi:10.1111/maps.12210]
Published by arrangement with John Wiley & Sons

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The Bulk Composition of Mars

G. Jeffrey Taylor

Hawaii Institute of Geophysics and Planetology, School of Ocean and Earth Science and Technology, University of Hawaii, Honolulu, HI 96822

An accurate assessment of the bulk chemical composition of Mars is fundamental to understanding planetary accretion, differentiation, mantle evolution, the nature of the igneous parent rocks that were altered to produce sediments on Mars, and the initial concentrations of volatiles such as H, Cl and S, important constituents of the Martian surface. This paper reviews the three main approaches that have been used to estimate the bulk chemical composition of Mars: geochemical/cosmochemical, isotopic, and geophysical. The standard model is one developed by H. Wänke and G. Dreibus in a series of papers, which is based on compositions of Martian meteorites. Since their groundbreaking work, substantial amounts of data have become available to allow a reassessment of the composition of Mars from elemental data, including tests of the basic assumptions in the geochemical models. The results adjust some of the concentrations in the Wänke-Dreibus model, but in general confirm its accuracy. Bulk silicate Mars has roughly uniform depletion of moderately volatile elements such as K (0.6 x CI), and strong depletion of highly volatile elements (e.g., Tl). The highly volatile elements are within uncertainties uniformly depleted at about 0.06 CI abundances. The highly volatile chalcophile elements are likewise roughly uniformly depleted, but with more scatter, with normalized abundances of 0.03 CI. Bulk planetary H2O is much higher than estimated previously: it appears to be slightly less than in Earth, but D/H is similar in Earth and Mars, indicating a common source of water-bearing material in the inner solar system. K/Th ranges from ~3000 to ~5000 among the terrestrial planets, a small range compared to CI chondrites (19,000). FeO varies throughout the inner solar system: ~3 wt% in Mercury, 8 wt % in Earth and Venus, and 18 wt % in Mars. These differences can be produced by varying oxidation conditions, hence do not suggest the terrestrial planets were formed from fundamentally different materials. The broad chemical similarities among the terrestrial planets indicate substantial mixing throughout the inner solar system during planet formation, as suggested by dynamical models

Reference
Taylor GJ (in press) The Bulk Composition of Mars. Chemie der Erde
[doi:10.1016/j.chemer.2013.09.006]
Copyright Elsevier

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Trace element geochemistry of CR chondrite metal

Emmanuel Jacquet1,2,*, Marine Paulhiac-Pison1,3, Olivier Alard4, Anton T. Kearsley5, Matthieu Gounelle1,6

1Laboratoire de Minéralogie et Cosmochimie du Muséum, CNRS & Muséum National d’Histoire Naturelle, Paris, France
2Canadian Institute for Theoretical Astrophysics, University of Toronto, Toronto, ON, Canada
3Ecole Normale Supérieure de Paris, Paris, France
4Géosciences Montpellier, Université de Montpellier II, Montpellier Cedex 5, France
5Impacts and Astromaterials Research Centre, Department of Mineralogy, The Natural History Museum, London, UK
6Institut Universitaire de France, Maison des Universités, Paris, France

We report trace element analyses by laser ablation inductively coupled plasma mass spectrometry (LA-ICP-MS) of metal grains from nine different CR chondrites, distinguishing grains from chondrule interior (“interior grains”), chondrule surficial shells (“margin grains”), and the matrix (“isolated grains”). Save for a few anomalous grains, Ni-normalized trace element patterns are similar for all three petrographic settings, with largely unfractionated refractory siderophile elements and depleted volatile Au, Cu, Ag, S. All three types of grains are interpreted to derive from a common precursor approximated by the least-melted, fine-grained objects in CR chondrites. This also excludes recondensation of metal vapor as the origin of the bulk of margin grains. The metal precursors were presumably formed by incomplete condensation, with evidence for high-temperature isolation of refractory platinum-group-element (PGE)-rich condensates before mixing with lower temperature PGE-depleted condensates. The rounded shape of the Ni-rich, interior grains shows that they were molten and that they equilibrated with silicates upon slow cooling (1–100 K h−1), largely by oxidation/evaporation of Fe, hence their high Pd content, for example. We propose that Ni-poorer, amoeboid margin grains, often included in the pyroxene-rich periphery common to type I chondrules, result from less intense processing of a rim accreted onto the chondrule subsequent to the melting event recorded by the interior grains. This means either that there were two separate heating events, which formed olivine/interior grains and pyroxene/margin grains, respectively, between which dust was accreted around the chondrule, or that there was a single high-temperature event, of which the chondrule margin records a late “quenching phase,” in which case dust accreted onto chondrules while they were molten. In the latter case, high dust concentrations in the chondrule-forming region (at least three orders of magnitude above minimum mass solar nebula models) are indicated.

Reference
Jacquet E, Paulhiac-Pison M, Alard O, Kearsley AT and Gounelle M (in press) Trace element geochemistry of CR chondrite metal. Meteoritics & Planetary Science
[doi:10.1111/maps.12212]
Published by arrangement with John Wiley & Sons

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Making giant planet cores: convergent migration and growth of planetary embryos in non-isothermal discs

A. Pierens1,2, C. Cossou1,2 and S. N. Raymond1,2

1Université de Bordeaux, Observatoire Aquitain des Sciences de l’Univers, BP 89 33271 Floirac Cedex, France
2Laboratoire d’Astrophysique de Bordeaux, BP 89 33271 Floirac Cedex, France

Context. Rapid gas accretion onto gas giants requires the prior formation of ~10 M⊕ cores, and this presents a continuing challenge to planet formation models. Recent studies of oligarchic growth indicate that in the region around 5 AU growth stalls at ~2 M⊕. Earth-mass bodies are expected to undergo Type I migration directed either inward or outward depending on the thermodynamical state of the protoplanetary disc. Zones of convergent migration exist where the Type I torque cancels out. These “convergence zones” may represent ideal sites for the growth of giant planet cores by giant impacts between Earth-mass embryos.
Aims. We study the evolution of multiple protoplanets of a few Earth masses embedded in a non-isothermal protoplanetary disc. The protoplanets are located in the vicinity of a convergence zone located at the transition between two different opacity regimes. Inside the convergence zone, Type I migration is directed outward and outside the zone migration is directed inward.
Methods. We used a grid-based hydrodynamical code that includes radiative effects. We performed simulations varying the initial number of embryos and tested the effect of including stochastic forces to mimic the effects resulting from disc turbulence. We also performed N-body runs calibrated on hydrodynamical calculations to follow the evolution on Myr timescales.
Results. For a small number of initial embryos (N = 5–7) and in the absence of stochastic forcing, the population of protoplanets migrates convergently toward the zero-torque radius and forms a stable resonant chain that protects embryos from close encounters. In systems with a larger initial number of embryos, or in which stochastic forces were included, these resonant configurations are disrupted. This in turn leads to the growth of larger cores via a phase of giant impacts between protoplanets, after which the system settles to a new stable resonant configuration. Giant planets cores with masses ≥ 10 M⊕ formed in about half of the simulations with initial protoplanet masses of mp = 3 M⊕ but in only 15% of simulations with mp = 1 M⊕, even with the same total solid mass.
Conclusions. If 2−3 M⊕ protoplanets can form in less than ~1 Myr, convergent migration and giant collisions can grow giant planet cores at Type I migration convergence zones. This process can happen fast enough to allow for a subsequent phase of rapid gas accretion during the disc’s lifetime.

Reference
Pierens A, Cossou C and Raymond SN (in press) Making giant planet cores: convergent migration and growth of planetary embryos in non-isothermal discs. Astronomy & Astrophysics
[doi:10.1051/0004-6361/201322123]
Reproduced with permission © ESO

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Stratified Ejecta Boulders as Indicators of Layered Plutons on the Moon

Kickapoo Lunar Research Teama, Georgiana Kramerb,c,*

aAbby Delawder, Austen Beason, Victoria Wilson, and Richard D. Snyder, Kickapoo High School, 3710 S. Jefferson Avenue, Springfield, MO 65807, USA
bCenter for Lunar Science and Exploration, Lunar and Planetary Institute, 3600 Bay Area Blvd., Houston, TX 77058, USA
cNASA Lunar Science Institute, USA

High resolution images of stratified ejecta boulders on the lunar nearside reveal layers of alternating low and high albedo material. We measured the thickness and albedo of each alternating light and dark layer from twenty nine stratified boulders located in Aristarchus Crater and Mare Undarum. The results were used to test hypotheses to explain the origins of the observed strata in these impact ejected boulders. Morphologically, these boulders demonstrate cross-bedding, trough-shaped layering, tapered layering and cumulate enclaves. We interpret these characteristics to be evidence that these layers result from periodic disruption by convection or density currents within a cooling layered igneous intrusion. We demonstrate that the layering observed in these boulders cannot be the result of known processes occurring on the surface, but instead suggests a history of complex intrusive igneous processes within the lunar crust.

Reference
Kickapoo Lunar Research Team and Georgiana Kramer G (in press) Stratified Ejecta Boulders as Indicators of Layered Plutons on the Moon. Icarus
[doi:10.1016/j.icarus.2013.10.003]
Copyright Elsevier

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