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Experimental deformation of olivine single crystals at mantle pressures and temperatures

Deformation experiments were carried out in a deformation-DIA high-pressure apparatus (D-DIA) on oriented San Carlos olivine single crystals, at pressure ( P) ranging from 3.5 to 8.5 GPa, temperature ( T) from 1373 to 1673 K, and in poor water condition. Oxygen fugacity ( fO 2) was maintained within...

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Published in:Physics of the earth and planetary interiors 2009-01, Vol.172 (1), p.74-83
Main Authors: Raterron, Paul, Amiguet, Elodie, Chen, Jiuhua, Li, Li, Cordier, Patrick
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description Deformation experiments were carried out in a deformation-DIA high-pressure apparatus (D-DIA) on oriented San Carlos olivine single crystals, at pressure ( P) ranging from 3.5 to 8.5 GPa, temperature ( T) from 1373 to 1673 K, and in poor water condition. Oxygen fugacity ( fO 2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity a opx = 1. Two compression directions were tested, promoting either [1 0 0] slip alone or [0 0 1] slip alone in (0 1 0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress ( σ) and specimen strain rates ( ε ˙ ) were monitored in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high- P deformation data with the data obtained at room- P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable T– σ– fO 2– a opx conditions – allowed quantifying the P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume V a * = 12 ± 4   c m 3 /mol in the corresponding rheological law, while pressure has little effect on c-slip with V c * = 3 ± 4   c m 3 /mol . These results may explain the discrepancy between olivine low- P and high- P deformation data which has been debated in the literature for more than a decade.
doi_str_mv 10.1016/j.pepi.2008.07.026
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Oxygen fugacity ( fO 2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity a opx = 1. Two compression directions were tested, promoting either [1 0 0] slip alone or [0 0 1] slip alone in (0 1 0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress ( σ) and specimen strain rates ( ε ˙ ) were monitored in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high- P deformation data with the data obtained at room- P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable T– σ– fO 2– a opx conditions – allowed quantifying the P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume V a * = 12 ± 4   c m 3 /mol in the corresponding rheological law, while pressure has little effect on c-slip with V c * = 3 ± 4   c m 3 /mol . 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Oxygen fugacity ( fO 2) was maintained within the olivine stability field and contact with enstatite powder ensured an orthopyroxene activity a opx = 1. Two compression directions were tested, promoting either [1 0 0] slip alone or [0 0 1] slip alone in (0 1 0) crystallographic plane, here called, respectively, a-slip and c-slip. Constant applied stress ( σ) and specimen strain rates ( ε ˙ ) were monitored in situ using time-resolved X-ray synchrotron diffraction and radiography, respectively. Transmission electron microscopy (TEM) investigation of run products revealed that dislocation creep was responsible for sample deformation. Comparison of the obtained high- P deformation data with the data obtained at room- P by Bai et al. [Bai, Q., Mackwell, S.L., Kohlstedt D.L., 1991, High-temperature creep of olivine single crystals. 1. Mechanical results for buffered samples, Journal of Geophysical Research, 96, 2441–2463] – on identical materials deformed at comparable T– σ– fO 2– a opx conditions – allowed quantifying the P effect on a-slip and c-slip rheological laws. A slip transition with increasing pressure, from dominant a-slip to dominant c-slip, is documented. a-slip appears sensitive to pressure, which translates into the high activation volume V a * = 12 ± 4   c m 3 /mol in the corresponding rheological law, while pressure has little effect on c-slip with V c * = 3 ± 4   c m 3 /mol . 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ispartof Physics of the earth and planetary interiors, 2009-01, Vol.172 (1), p.74-83
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1872-7395
0031-9201
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recordid cdi_osti_scitechconnect_980204
source ScienceDirect Journals
subjects Activation volume
COMPRESSION
CREEP
DEFORMATION
DIFFRACTION
Dislocation creep
DISLOCATIONS
ENSTATITE
High pressure
MONOCRYSTALS
national synchrotron light source
OLIVINE
OXYGEN
PARTICLE ACCELERATORS
Rheological law
San Carlos olivine
SLIP
Slip systems
STABILITY
STRAIN RATE
SYNCHROTRONS
TRANSMISSION ELECTRON MICROSCOPY
Upper mantle
WATER
title Experimental deformation of olivine single crystals at mantle pressures and temperatures
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