Oblique subduction is a form of subduction (i.e. a tectonic process involving the convergence of two plates where the denser plate descends into Earth's interior) for which the convergence direction differs from 90° to the plate boundary. Most convergent boundaries involve oblique subduction, particularly in the Ring of Fire including the Ryukyu, Aleutian, Central America and Chile subduction zones. In general, the obliquity angle is between 15° and 30°. Subduction zones with high obliquity angles include Sunda trench (ca. 60°) and Ryukyu arc (ca. 50°). Obliquity in plate convergence causes differences in dipping angle and subduction velocity along the plate boundary. Tectonic processes including slab roll-back, trench retreat (i.e. a tectonic response to the process of slab roll-back that moves the trench seaward) and slab fold (i.e. buckling of subducting slab due to phase transition) may also occur. Moreover, collision of two plates leads to strike slip deformation of the forearc, thus forming a series of features including forearc slivers and strike slip fault systems that are sub-parallel to ocean trenches. In addition, oblique subduction is associated with the closure of ancient ocean, tsunami and block rotations in several regions.
Deformation features
Forearc slivers
Forearc slivers are partly detached continental blocks of the overriding plates. They are bounded by the trenches and trench parallel strike slip fault systems. The motion of forearc slivers depend on the obliquity of the subducting slabs. Moreover, some forearc slivers occur in the absence of well defined strike-slip fault systems, and sliver motions are not purely strike-slip.
Trench parallel strike-slip fault systems Trench parallel strike-slip faults are deformational products contributed by trench parallel component of strain partitioning. They are located between the forearc slivers and the remaining overriding plates.
Orientation of strike slip faults Vertical strike slip fault systems are generally accepted by the early literature of oblique subduction. However, modern technology, such as seismic profiling, reveals that the faults are not necessarily vertical. Several other models concerning the orientations of the faults are proposed.
Slip accommodating mechanisms Trench parallel slip component from oblique subduction may not be fully accommodated by the aforementioned trench parallel strike slip faults. Several models suggest that there are other slip accommodating mechanisms formed by oblique subduction as means to take up the remaining slip component.
Margin parallel strike-slip faults in subducting plates
Ishii et al., (2013) suggested that the trench parallel strike-slip faults may appear in the obliquely subducting slabs to accommodate a portion of the trench parallel slip component. In the Sumatra subduction zone, the trench parallel slip component is measured to be approximately 45 mm per year, the motion rate of northern Great Sumatra Fault ranges from 1 to 9 mm per year with the maximum rate of 13 mm per year. The result shows that the trench parallel slip component of at least 32 mm per year is left. On 11 April 2012, a Mw 8.6 earthquake occurred in the subducting plate (i.e. the Indo-Australian Plate). Strike-slip seismicity was recorded in the earthquake. This infers strike slip fault systems are present in the descending slab and they may potentially accommodate slip component from oblique subduction.
Strain partitioning
Strain partitioning is a form of deformation. In oblique subduction zone, strain partitioning is initiated into trench parallel component and trench normal component. The trench parallel component is accommodated by localized shear zones (short-term deformation) or trench parallel strike slip fault systems (long-term deformation) in the overriding plates. Likewise, this component commonly leads to the formation of forearc slivers. The trench normal component is taken up by thrust structures. These thrusts are generally discontinuous and their geometries change progressively.
Short-term deformation: Localized shear zone
Short-term deformation is mainly elastic and acts at human time scale (i.e. perceptible during a human lifetime, unlike changes that take place on a geologic time scale). When the denser plate subducts beneath the upper plate, they are coupled at the interface (i.e. plate coupling). The process of plate coupling thus generates tectonic force that follows the subduction direction. The orientation of tectonic force gradually rotates toward the trench normal direction. This attributes to the decline of trench parallel component when the force leaves the plate coupling zone. In this way, only the frontal part, rather than the whole upper plate, is dragged by the subducting slab.
Long-term deformation: Formation of forearc sliver and strike slip fault
Long-term deformation occurs at geological time scale. Under continuous oblique subduction, the aforementioned frontal part of the upper plate permanently accommodates the trench parallel component. In this way, the orientation of tectonic force rotates gradually toward the trench parallel direction. Strong and continuing tectonic force in trench parallel direction leads to the development of trench parallel strike slip fault system. The fault thus separate a portion of the forearc from the overriding plate, forming the forearc sliver.
Tectonic events related to oblique subduction
The 1771 Great Yaeyama Tsunami
The tsunami occurred in the southwestern part of the Ryukyu arc. Yukinobu et al., (2018) suggested that oblique subduction was the primary reason leading to the occurrence of the tsunami.
Tectonic setting In the plate boundary, an approximately 80 km long and 30 km wide depression is observed. It obscures trench parallel strike slip fault and the topographic ridge of the wedge.
Oblique subduction and tsunami
Block rotation
Oblique subduction has led to rotation of microblocks about nearby poles of rotation (See also: Euler poles) in some oblique subduction zones. In these regions, the trench parallel strike slip fault systems are less prominent. This is because a portion of the trench parallel component is accommodated by the microblock rotation. Examples of oblique subduction-induced block rotation are identified in North Island, Cascadia and New Guinea.
Example: North Island oblique subduction zone
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![Oblique subduction: Simplified model of oblique subduction. The oblique subduction motion is composed of motion vectors that are parallel and orthogonal to plate boundary.[1] The obliquity of plate convergence is compensated by the relative motion between forearc sliver and the remaining overriding plate.[1] In this way, the relative motion between the overriding plate and the subducting plate is almost perpendicular to the plate boundary.[1] Adapted from Westbrook, 2005.[1]](https://upload.wikimedia.org/wikipedia/commons/thumb/4/4e/Subduction_motions.png/1280px-Subduction_motions.png?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)
![Oblique subduction: Oblique subduction model with the development of forearc sliver and margin parallel strike slip fault. Forearc sliver is a microplate bounded by the oceanic trench and strike slip fault.[14] Trench parallel strike slip fault develops when the forearc sliver moves away from stable continent.[14] Adapted from Haq and Davis, 2010.[14]](https://upload.wikimedia.org/wikipedia/commons/thumb/c/c0/Oblique_subduction_%2B_features.png/1280px-Oblique_subduction_%2B_features.png?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)
![Oblique subduction: A vertical strike slip fault model. The red line indicates the vertical fault. The fault extends from surface down to the subducting slab.[10]](https://upload.wikimedia.org/wikipedia/commons/thumb/7/74/Vertical_fault3.png/1280px-Vertical_fault3.png?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)
![Oblique subduction: A mega splay fault system model. The strike slip fault is suggested to be one of the branches in the mega splay fault, which also links thrust faults in the forearc.[21] The mega splay fault is subparallel to the subducting plate at depth.[21] Modified from Tsuji et al., 2014.[21]](https://upload.wikimedia.org/wikipedia/commons/thumb/b/b3/Splay_fault5.png/1280px-Splay_fault5.png?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)
![Oblique subduction: A curved strike slip fault model. Adapted from Ormeño. et al., 2017[19]](https://upload.wikimedia.org/wikipedia/commons/thumb/9/9d/Curved_fault3.png/1280px-Curved_fault3.png?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)
