Bln. Kennett et al., THE UPPER-MANTLE S-VELOCITY AND P-VELOCITY STRUCTURE BENEATH NORTHERNAUSTRALIA FROM BROAD-BAND OBSERVATIONS, Physics of the earth and planetary interiors, 86(1-3), 1994, pp. 85-98
Good coverage of seismic wave propagation through the upper part of th
e mantle can be obtained for sources in the earthquake belt through In
donesia and New Guinea recorded at broad-band seismometers in the Nort
hern Territory of Australia. The midpoints of the propagation paths li
e along the northern margin of the Australian continent. Most of the o
bservations come from a Guralp CMG3 seismometer at the Warramunga Arra
y, but these have been supplemented by field deployments using compara
ble instrumentation. Two groups of sources, (1) along the Flores Are,
Indonesia, with propagation under northwestern Australia, and (2) in N
ew Guinea, with paths to the NNE of the array, have been used to const
ruct composite record sections for P, SV and SH waves over the distanc
e range 1250-3600 km. The choice of the two source zones was based on
earlier short-period studies, and the broad-band observations confirm
the presence of noticeable differences in P velocity profiles for path
s whose turning po;nts are separated by about 1000 km. The S waves rec
orded on the radial (SV) and tangential (SH) components are of compara
ble quality because the hard-rock recording sites minimise the influen
ce of coupling to P on the radial component. As the P and S sections a
re prepared from the same events, we are able to make direct estimates
of P/S velocity ratios for the mantle transition zone. This ratio inc
reases from 1.77 at the top of the mantle to 1.85 at the 410 km transi
tion, indicating that the S-wave velocity gradients are rather lower t
han might be expected. However, through the transition zone down to 66
0 km the S-wave gradients increase and the P/S velocity ratio is less
than 1.81 below the 660 km transition. There is a significant differen
ce in the frequency content of P and S waves beyond 2000 km. The P wav
es remain high frequency but the S waves returned from the transition
zone and below are of intermediate period (0.25-0.3 Hz), associated wi
th significant attenuation zone for S beneath 210 km.