Earthquake catalogs most commonly represent events as point sources, specified
by a moment tensor and a centroid (location and time), which are the zeroth and
first degree polynomial moments of the earthquake's source distribution
respectively. We have begun cataloging the 2nd degree moments of the source
distributions of earthquakes between MW=7.0 and MW=8.2 occurring since 1994.
We invert frequency dependent measurements of amplitude and arrival time
anomalies for fundamental mode Rayleigh waves and P-waves recorded at global
stations for the 0th, 1st, and 2nd degree moments of an earthquake. The
inversion procedure enforces the non-linear, physical constraint that the source
region have non-negative volume. The 2nd moments describe the spatial and
temporal extent of a rupture, as well as its average propagation velocity. They
can be interpreted in terms of a characteristic rupture length, Lc, and a
characteristic rupture duration, tauc, whose ratio gives the apparent
rupture velocity, vc = Lc / tauc. Because the 2nd spatial moment describes the
extent and orientation of the source, it can be used to resolve the fault-plane
ambiquity associated with an event's moment-tensor. The mixed moment between
space and time represents the average velocity of the instantaneous centroid
during rupture, v0.
One of the initial results to come out of cataloging 2nd moments is an apparent
statistical preference for unilateral rather than bilateral rupture. For a
perfectly symmetric bi-lateral rupture, v0= 0, whereas for uniform-slip
unilateral ruptures, v0=vc. Thus by comparing v0 and vc we can infer the
nature of rupture propagation during an event. Approximately 85% of the events
in our catalog have v0 = 0.5*vc indicating a dominately unilateral rupture.
This predominance of unilateral propagation as the mode of rupture appears to
hold for both strike-slip and subduction zone thrust-fault events. We will
discuss several potential explanations for the predominance of unilateral
ruptures in large earthquakes, including fault interface waves and the control
of rupture nucleation by features such as asperities or fault segment
boundaries.