|
|
SOUTHWEST PACIFIC SEISMIC EXPERIMENT
Douglas A. Wiens, Patrick J. Shore, Jeffrey J. McGuire, and Erich Roth
Department of Earth and Planetary Sciences, Washington University, St. Louis
IRIS Newsletter, 14, No.1, Spring 1995.
Introduction
The Southwest PAcific Seismic Experiment (SPASE) is one of the
first extensive deployments of broadband, PASSCAL type instruments in a
subduction zone setting. 11 broadband sensors were deployed in Fiji,
Tonga, and Niue Island (Figure 1) during November, 1993 and August,
1994, and will remain deployed until December, 1995. The goals of the
experiment are to study the complex upper mantle velocity and
attenuation structure of the subducting Tonga Slab and Lau backarc
spreading center, as well as the source parameters of deep earthquakes
in Tonga slab. Since about two-thirds of the world's deep earthquakes
are located in the Tonga subduction zone, the Tonga-Fiji region is an
ideal site for this type of experiment. A related deployment of 29
Ocean Bottom Seismographs (LABATTS) in the Lau Backarc and Tonga forearc (Dorman,
Hildebrand, Webb, and Wiens, co-PIs) was carried out during September
through December, 1994, and should provide better imaging of small scale
structures than would be possible with the land stations alone.
Deployment
Instruments were deployed at 12 sites on 11 different islands.
The sites were chosen to maximize coverage of the northern part of the
Tonga slab as well as for logistical reasons. All of the sites are
reachable by scheduled air service, except Niuafo'ou Island, which was
deployed and picked up from ships servicing the OBS deployment, and
Tofua Island, with is reachable by a charter seaplane which lands in a
caldera lake.
Eight Streckeisen STS-2 and three Guralp CMG3-ESP sensors were
deployed, with each sensor connected to a REFTEK 24 bit DAS equipped
with GPS timing and 1.0 or 1.2 Gb disks. At most sites, the sensors
were housed inside 1 meter diameter fiberglass cylinders, which were
cemented to bedrock or coral and equipped with a fiberglass lid and
filled with Styrofoam insulation. The sensors were placed on a small
slab of concrete inside the cylinders and about 1 meter below the ground
surface. The electronic equipment and two automobile batteries were
placed inside wooden field boxes near the vaults, and powered by two 30
watt solar panels (Figure 2 and Figure 3).
Because of the high frequency-dependent seismic noise levels on
the islands, the REFTEK triggering algorithm misses many smaller events.
Therefore, we record only a single, continuous data stream at 20 or 25
samples/sec. The stations are serviced at 3 month intervals, when
disks are swapped and the data is downloaded on a field computer in
Suva, Fiji. A service trip to all the stations from North America takes
more than one month and entails about 30 separate plane flights. Kiti
Draunidalo of the Fiji Mineral Resources Department services the
stations on approximately one-half of the service runs. A copy of all
the data is retained in Suva for use by the local scientists in seismic
hazard studies. Data recovery over the first year of operation is about
85-90 percent.
The bankruptcy of Polynesian Airlines mid-way through the
experiment left Niue Island with only one weekly scheduled flight from
anywhere in the world, such that servicing this one station takes about
nine days. We are therefore cooperating with the PASSCAL Instrument
Center in testing an ARGOS satellite state-of-health communications
system. Data will be returned by using local people to swap out disks
and return them to the US by air cargo, and the station state-of
-health will be monitored via the ARGOS satellite. This system should
render it necessary to visit the island only in the case of equipment
failure.
Initial Results
We have now processed data from December, 1993 through June,
1994, which is enough to make some initial studies. Over 1000
earthquakes were located in the Tonga-Fiji region during the first seven
months of the experiment, most of which were not detected by the PDE or
other global earthquake compilations.
Deep Earthquakes: The March 9, 1994 large deep earthquake (MW
7.6, depth 570 km) was the largest deep earthquake in 20 years, and even
though now exceeded by the deep Bolivian event (June 9, 1994, MW 8.3),
it promises to provide a wealth of detail on the source processes of
deep earthquakes. Previous to this event, a true aftershock sequence
had not been observed for any deep earthquake, and rupture zones of deep
earthquakes were poorly constrained due to the lack of aftershocks to
delineate the fault planes. The March 9 event was unusually prolific in
producing aftershocks compared to other large deep events; we found a
sequence of 83 aftershocks ranging from mb 3.8 to 6.0 and extending for
at least 40 days. The aftershocks show a power law decay with time
similar to shallow aftershock sequences, and the number and magnitude
distribution of the aftershocks is similar to that observed for typical
shallow earthquakes. The contrast between this strong aftershock
sequence and the weak aftershock sequence of the Bolivia event is
particularly striking.
Most of the well-located aftershocks locate along a steeply
dipping plane (Figure 4) consistent with one of the main shock nodal
planes and appear to delineate a 50 km by 65 km main shock rupture zone.
Inversion of broadband body waveforms, recorded on-scale by six regional
stations, also suggests this plane denotes the fault plane. Both the
region of moment release and the aftershock zone cuts entirely through
the active seismic zone and extends about 20 kilometers into the
surrounding aseismic region. Thus there must be a mechanism for
producing both rupture and aftershocks within the normally aseismic
region surrounding the active slab. The width of the rupture zone is
hard to reconcile with predictions of the transformational faulting
hypothesis for the origin of deep earthquakes, which suggests that deep
earthquakes should be confined to a thin zone of metastable olivine (see
report in Dec 8, 1994 issue of Nature).
Several other deep earthquakes with MW > 5.5 have occurred during the experiment. Most of these events have showed several aftershocks,
including one MW 6.4 event which showed 9. These results, combined with
the March 9 aftershock sequence, suggests that Tonga deep earthquakes
show more active aftershock sequences than deep earthquakes in other
subduction zones.
Attenuation Structure: The broadband body waveforms show first
order differences in attenuation between paths following the slab and
various paths within the backarc region. We are developing a 3
dimensional Q model for the upper mantle beneath the Lau backarc using a
differential attenuation method which determines the dt* along the
raypaths of regionally propagating P- and S-waves. The dt*
measurements and the raypaths can then be inverted to determine the
lateral and depth dependent Q variations. Initial results suggest that
Q increases rapidly with depth. A low Q region is found in the upper
several hundred kilometers beneath the Lau backarc spreading center,
possibly suggesting the presence of partial melt, and much higher Q is
found beneath the South Fiji Basin, an older, inactive region.
Anisotropy: Shear wave splitting is readily observed on records
of intermediate and deep earthquakes recorded in Fiji, and we are
currently investigating anisotropy beneath the Lau backarc and Fiji
platform in collaboration with Karen Fischer (Brown University). All
Fiji stations generally show about 1 s. of splitting, with an average
fast direction of about N60W. There appears to be little
variation in the amount of splitting with event depth or path length for
sources between depths of 400 to 650 km, and several teleseismic SKS
phases show similar splitting results. This suggests that the splitting
occurs largely within the upper 400 km of the mantle beneath the
station. These results are consistent with a 1% azimuthal anisotropy
uniformly distributed in the upper 400 km or the mantle, or greater
anisotropy if the splitting occurs at shallower depths. The fast
direction of the anisotopy is approximately parallel with the
convergence direction of the Pacific plate and the spreading direction
in the Lau backarc, suggesting the anisotropy may be produced by
counterflow induced within the backarc by the subducting slab or the
back arc extension.
Other studies of the velocity structure of the subducting slab
and backarc basin using arrival time data and waveforms are also
underway, as well as source parameter studies of regional earthquakes.
The Southwest Pacific Seismic experiment will produce a better
understanding of the seismic structure and geodynamnics of island arc -
backarc systems, as well as a better understanding of the rupture
processes of deep earthquakes. The data will be made available to the
entire community through the IRIS data center one year after the end of
the experiment.
Acknowledgements: We thank Michael Bevis (Hawaii), Kitione
Draunidalo (Mineral Resources Dept, Fiji)
George Hade (Cornell), Paul Friberg (PASSCAL), George Sionhalo (Niue Dept. of Survey), Saimone Helu and Tavita
Fatai (Tonga Minestry of Lands and Survey) for assistance with the
deployment of the seismographs. We also thank Bob Busby (PASSCAL)
for assistance with the equipment and planning of the experiment, and
Hersh Gilbert, Brian Park-Li and Rachel Sakata for carrying out various
aspects of the analysis...
back to SPaSE home
|