Geological Society of America | GEOLOGY | Volume 50 | Number 11 | www.gsapubs.org 1229
Manuscript received 28 August 2021
Revised manuscript received 7 June 2022
Manuscript accepted 15 June 2022
https://doi.org/10.1130/G49639.1
© 2022 The Authors. Gold Open Access: This paper is published under the terms of the CC-BY license.
CITATION: Tobin, H.J., et al., 2022, Direct constraints on in situ stress state from deep drilling into the Nankai subduction zone, Japan: Geology, v. 50,
p. 1229–1233, https://doi.org/10.1130/G49639.1
Direct constraints on in situ stress state from deep drilling into
the Nankai subduction zone, Japan
Harold J. Tobin
1
, Demian M. Saffer
2
, David A. Castillo
3
and Takehiro Hirose
4
1
Department of Earth and Space Sciences, University of Washington, Box 351310, Seattle, Washington 98195, USA
2
Institute for Geophysics and Department of Geological Sciences, University of Texas at Austin, 10601 Exploration Way, Austin,
Texas 78758, USA
3
Insight Geomechanics, 8 Joffre Road, Trigg, Western Australia 6029, Australia
4
Kochi Institute for Core Sample Research (X-star), Japan Agency for Marine-Earth Science and Technology, 200 Monobe-otsu Nankoku,
Kochi 783-8502, Japan
ABSTRACT
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 seafoor (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 frst
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
), defnitively
ruling out a thrust-faulting stress regime to at least 3 km depth, and to within ∼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 mega-
thrust, lies in a normal or strike-slip faulting regime (S
v
≥ S
Hmax
> S
hmin
). Total differential
stresses are below ∼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 décollement
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 ∼5000 mbsf, S
Hmax
must transi-
tion 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.
ULTRADEEP SCIENTIFIC DRILLING
IN A SUBDUCTION ZONE
The Nankai Trough Seismogenic Zone
Experiment (NanTroSEIZE) is a comprehensive
investigation of subduction zone faulting and
stress conditions (Tobin and Kinoshita, 2006;
Tobin et al., 2019). NanTroSEIZE has combined
seismic imaging with Integrated Ocean Drilling
Program (IODP) drilling for direct sampling,
in situ measurements, and long-term borehole
monitoring to better understand the nature of
the megathrust seismic cycle, fault locking, and
the spectrum of fault slip. A transect of bore-
holes (Fig. 1) was drilled on a series of IODP
expeditions from 2007 through 2019 (Tobin
et al., 2019). The centerpiece is ultradeep drill-
ing at IODP Site C0002 (Fig. 1B), which was
targeted to cross and sample a seismic refector
interpreted as the main plate-boundary fault (the
“megathrust”), which lies at ∼5000 m below the
seafoor (mbsf) based on refection and refrac-
tion depth imaging (Moore et al., 2007; Bangs
et al., 2009; Kamei et al., 2012).
The principal borehole (Fig. 2) at this site
(Hole C0002F/N/P) was drilled by the riser
drilling vessel Chikyu to 3058 mbsf, with steel
casing cemented in place to a depth of 2922
mbsf (Tobin et al., 2015a, 2019; Strasser et al.,
2014). One key objective at Site C0002 is to
characterize the present-day state of stress in
the inner accretionary wedge, which forms the
upper plate of the primary plate-boundary fault
(Fig. 1B). The orientations and absolute magni-
tudes of the three principal stresses—and their
temporal evolution—drive fault strength, slip,
and earthquakes (e.g., Scholz, 1998; Brodsky
et al., 2020) throughout the seismic cycle (e.g.,
Magee and Zoback, 1993; Wang and Hu, 2006).
Decades of effort to measure stress and pore-
fuid pressure conditions, either directly or indi-
rectly, however, have met with limited success
(summarized in Saffer and Tobin, 2011), and
the quantitative state of stress at depth in any
subduction setting is not known with confdence.
Previous NanTroSEIZE work using borehole
breakouts and induced tensile fracture orien-
tations from resistivity log imaging has estab-
lished the orientation of the principal stress axes
but not their magnitudes (Chang et al., 2010;
Lin et al., 2015).
Unlike nearly all other scientifc ocean drill-
ing, this hole was drilled with a riser system,
using a closed loop of drilling mud designed to
clean the hole and provide pressure support to
the borehole, permitting a number of otherwise
impossible stress- and pore pressure-related
observations (e.g., Saffer et al., 2013). We ana-
lyzed a suite of data sets collected during drilling
that, taken together, provide quantitative con-
straints on the in situ stress tensor, including all
three principal stresses and pore-fuid pressure.
ESTIMATES OF IN SITU STRESS STATE
We determined the vertical stress (S
v
) directly
using bulk density measurements from core
samples and borehole cuttings returns (Kitajima
et al., 2017). Values of bulk density ranged from
∼1500 kg/m
3
near the seafoor to ∼2400 kg/m
3
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