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On the geometry of an earthquake fault system
Y. Y. Kagan
Institute of Geophysics and Planetary Physics, University of California, Los Angeles, CA 90024-1567, USA
Received 7 October 1991; accepted 28 October 1991. Available online 16 October 2002.
Invariants of a two-point correlation function of the seismic moment tensor were used to investigate an earthquake fault system. The geometry of the fault system is significantly different from the standard model of an earthquake fault, i.e. coherent rupture on a planar surface. Contrary to the `flat-fault' model, we see clear evidence for non-planarity of the fault system geometry, and observe that the focal mechanisms of neighboring events may have very different orientation, i.e. they undergo large three-dimensional rotations. Therefore, earthquake deformation models need to be fully three-dimensional and should include large rotations.
The spatial
behavior of the invariants is approximately the same for earthquakes in
different depth intervals: shallow, intermediate, and deep. The
temporal behavior of the invariants differs only in that shallow
earthquakes are clustered in time, whereas for deeper events the
clustering is much less pronounced; as soon as we `decluster' shallow
seismicity, the invariants' temporal properties become similar for
earthquakes of all depths. This demonstrates that the basic geometrical
properties of earthquake rupture do not depend on depth, and therefore
they are generally independent of rheological properties of rocks,
lithostatic pressure, or the presence of a free boundary for strong
shallow earthquakes.
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