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To investigate the role of grain boundary sliding during dislocation creep of dunite, a series of deformation experiments were carried out under anhydrous conditions on fine-grained (～15 μm) samples synthesized from powdered San Carlos olivine and powdered San Carlos olivine+1.5 vol.% MORB. Triaxial compressive creep tests were conducted at a temperature of 1 473 K and con-fining pressures of 200 and 400 MPa using a high-resolution, gas-medium deformation apparatus. Each sample was deformed at several levels of differential stress between 100 and 250 MPa to yield strain rates in the range of 10-6 to 10-4 s-1. Under these conditions, the dominant creep mechanism involves the motion of dislocations, largely on the easy slip system (010)[100], accommodated by grain boundary sliding (gbs). This grain size-sensitive creep regime is characterized by a stress ex-ponent of n=3.4±0.2 and a grain size exponent of p=2.0±0.2. The activation volume for this gbs-accommodated dislocation creep regime is V*=(26±3)×10-6 m2·mol-1. Comparison of our flow law for gbs-accommodated dislocation creep with those for diffusion creep and for dislocation creep reveals that the present flow law is important for the flow of mantle rocks with grain sizes of <100 μm at differential stresses >20 MPa. Hence, gbs-accommodated dislocation creep is likely to be an important deformation mechanism in deep-rooted, highly localized shear zones in the lithospheric upper mantle.
To investigate the role of grain boundary sliding during dislocation creep of dunite, a series of deformation experiments carried carried under anhydrous conditions on fine-grained (~ 15 μm) samples composed from powdered San Carlos olivine and powdered San Carlos olivine + 1.5 vol. % MORB. Triaxial compressive creep tests were conducted at a temperature of 1 473 K and con-fining pressures of 200 and 400 MPa using a high-resolution, gas-medium deformation apparatus. Each sample was deformed at several levels of differential stress between 100 Under these conditions, the dominant creep mechanism involves the motion of dislocations, largely on the easy slip system (010) [100], accommodated by grain boundary sliding (gbs). This grain size-sensitive creep regime is characterized by a stress ex-ponent of n = 3.4 ± 0.2 and a grain size exponent of p = 2.0 ± 0.2. The activation volume for this gbs-accommodating dislocation creep r Egime is V * = (26 ± 3) × 10-6 m2 · mol-1. Comparison of our flow law for gbs-accommodating dislocation creep with those for diffusion creep and for dislocation creep reveals that the present flow flow is important for the flow of mantle rocks with grain sizes <100 μm at 60 MPa. Therefore, gbs-accommodating dislocation creep is likely to be an important deformation mechanism in deep-rooted, highly localized shear zones in the lithospheric upper mantle.