T69 Impact Cratering on the Earth, Moon, and Planets: Remote, Field, and Lab Studies
Sunday, 9 October 2011
1:30 PM - 5:30 PM
Room L100H-J
CRYSTALLOGRAPHIC MODELING AND OBSERVATIONS OF {112} PLANAR FRACTURES IN NATURALLY SHOCKED ZIRCON
Paper number: T69-12
Program: Technical Sessions
Time: 4:30 PM – 4:45 PM
Authors
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Aaron J. CavosieUniversity of Puerto Rico, Mayaguez, PR
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Henri A. RadovanUniversity of Puerto Rico, Mayaguez, PR
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Desmond E. MoserUniversity of Western Ontario, London, ON
Abstract
Modeling four {ΙΙ2} orientations produces variable lineation patterns on {Ι00} and {ΙΙ0} forms. Two lineations form on {Ι00} that create an acute angle of ~49˚. Only two form because on (Ι00), for example, the (ΙΙ2) and (ĪΙ2) set and the (ΙĪ2) and (ĪĪ2) set are parallel. Three lineations form on {ΙΙ0}. On (ΙΙ0) for example, the (ΙΙ2) and (ĪĪ2) sets, which are parallel, form one lineation 90˚ to the c-axis. The other two PFs, (ĪΙ2) and (ΙĪ2), form lineations with an acute angle of ~65˚. Along all other c-axis parallel crystallographic orientations (e.g., {Ι20}) four lineations will be formed by the {ΙΙ2} PFs.
Imaging a subhedral detrital zircon with {Ι00} and {ΙΙ0} prisms confirms the presence of {ΙΙ2} PFs in 4 orientations; additional PFs on (Ι00) and (0ΙΙ) result in 6 PF orientations. PFs and deformation micro-twins in {ΙΙ2} orientation have been reported in zircon shocked experimentally to 60 GPa (TEM, Leroux et al. 1999) and in bedrock samples from Vredefort shocked to >20 GPa (EBSD, Moser et al. 2011). Factors that favor formation of specific PF orientations in zircon are not well understood, but likely include shock pressure, grain orientation relative to the shock wave, and rheological properties of surrounding phases.