Journal
GEOLOGY
Volume 50, Issue 11, Pages 1229-1233Publisher
GEOLOGICAL SOC AMER, INC
DOI: 10.1130/G49639.1
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This study successfully constrained the in situ pore pressure and stress state in the deep interior of an accretionary wedge using data from drilling in the Nankai subduction zone. The estimated stress components helped reveal the tectonic stress characteristics in the region, indicating a normal or strike-slip faulting regime with low stress variations.
Stress state is a long-sought but poorly known parameter on subduction megathrusts and in overlying accretionary wedges in general. We used direct observations made during drilling of Integrated Ocean Drilling Program (IODP) borehole C0002 to a depth of 3058 m below the seafioor (mbsf) in the Nankai subduction zone of southwestern Japan to constrain in situ pore pressure and stress state in the deep interior of an accretionary wedge for the first time. These data included downhole pressure, active pumping tests, and logging and sample measurements. We found a nearly linear gradient in minimum horizontal principal stress (S-hmin) and show that it remained consistently smaller than the vertical stress (S-v), definitively ruling out a thrust-faulting stress regime to at least 3 km depth, and to within similar to 2 km above the subduction megathrust. At 3000 mbsf, the estimated effective stresses were: S-v = 33 MPa, S-Hmax = 25-36 MPa, and S-hmin = 18.5-21 MPa. We therefore interpret that the stress state throughout the drilled interval, which lies entirely in the hanging wall of the active megathrust, lies in a normal or strike-slip faulting regime (S-v >= S-Hmax > S-hmin). Total differential stresses are below similar to 18 MPa. We conclude that (1) basal traction along the megathrust must be small in order to permit both locking (and frictional sliding at failure) of the decollement and such low differential stresses deep within the upper plate; and (2) although differential stresses may remain low all the way to the plate boundary at similar to 5000 mbsf, S-Hmax must transition to become greater than the vertical stress-either spatially below the base of the borehole or temporally leading up to megathrust fault rupture-in order to drive thrust motion along the plate boundary as observed in great earthquakes and in recurring very low-frequency earthquakes and slow-slip events.
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