4.3 Article

Deformation of olivine under mantle conditions: An in situ high-pressure, high-temperature study using monochromatic synchrotron radiation

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Publisher

AMER GEOPHYSICAL UNION
DOI: 10.1029/2011JB008498

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Funding

  1. GRC
  2. Electron Microscopy Center at Argonne National Laboratory
  3. NSF [EAR-0652574, EAR-0968456]
  4. National Science Foundation, Earth Sciences [EAR-0622171]
  5. Department of Energy, Geosciences [DE-FG02-94ER14466]
  6. U.S. Department of Energy, Office of Science, Office of Basic Energy Sciences [DE-AC02-06CH11357]
  7. U.S. Department of Energy Office of Science Laboratory [DE-AC02-06CH11357]
  8. Division Of Earth Sciences
  9. Directorate For Geosciences [0968456, 0968823, 1045832] Funding Source: National Science Foundation
  10. Division Of Earth Sciences
  11. Directorate For Geosciences [0968863] Funding Source: National Science Foundation

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Polycrystalline samples of San Carlos olivine were deformed at high-pressure (2.8-7.8 GPa), high-temperature (1153 to 1670 K), and strain rates between 7.10(-6) and 3.10(-5) s(-1), using the D-DIA apparatus. Stress and strain were measured in situ using monochromatic X-rays diffraction and imaging, respectively. Based on the evolution of lattice strains with total bulk strain and texture development, we identified three deformation regimes, one at confining pressures below 3-4 GPa, one above 4 GPa, both below 1600 K, and one involving growth of diffracting domains associated with mechanical softening above similar to 1600 K. The softening is interpreted as enhanced grain boundary migration and recovery. Below 1600 K, elasto-plastic self-consistent analysis suggests that below 3-4 GPa, deformation in olivine occurs with large contribution from the so-called a-slip system [100](010). Above similar to 4 GPa, the contribution of the a-slip decreases relative to that of the c-slip [001](010). This conclusion is further supported by texture refinements. Thus for polycrystalline olivine, the evolution in slip systems found by previous studies may be progressive, starting from as low as 3-4 GPa and up to 8 GPa. During such a gradual change, activation volumes measured on polycrystalline olivine cannot be linked to a particular slip system straightforwardly. The quest for the activation volume of olivine at high pressure should cease at the expense of detailed work on the flow mechanisms implied. Such evolution in slip systems should also affect the interpretation of seismic anisotropy data in terms of upper mantle flow between 120 and 300 km depth.

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