Aj. Rodgers et al., PROPAGATION CHARACTERISTICS OF SHORT-PERIOD SR AND LG IN THE MIDDLE-EAST, Bulletin of the Seismological Society of America, 87(2), 1997, pp. 396-413
We present propagation characteristics of the short-period regional se
ismic phases Sn and Lg for the Middle East. Digital waveform data from
the Iranian Long Period Array (ILPA) and the Global Seismic Network (
GSN) stations ABKT (Alibek, Turkmenistan), ANTO (Ankara, Turkey), KEG
(Kottamya, Egypt), and KIV (Kislovodsk, Georgia) were used in this stu
dy, Three-component rotated seismograms were bandpass filtered (0.5 to
5.0 Hz) and examined for the presence and strength (amplitude) of Sn
and Lg relative to the Pn and Pg phases. The short-period Sn and Lg wa
veforms show great variability, Sn propagates efficiently for paths cr
ossing the Mediterranean, Black, and Caspian Seas as well as for paths
passing north of the Greater Caucasus, Alborz, and Kopet-Dag Mountain
s. Generally, Sn is not observed or propagates inefficiently for paths
with segments beneath the Turkish plateau and northern Iranian platea
u, consistent with a previous study by Kadinsky-Cade et al. (1981). Th
is study finds that the zone of inefficient Sn propagation coincides w
ith a zone of low Pn velocities (<7.9 km/sec) determined by Hearn and
Ni (1994) from Pn tomography. Lg is consistently not observed for path
s crossing the Mediterranean, Black, and Caspian Seas, Lg propagates e
fficiently for paths crossing the northern Arabian shield. Generally,
Lg propagates efficiently for paths contained within the Turkish-Irani
an plateau. Paths in the Middle East greater than about 2000 km consis
tently show no or little Lg energy. The correspondence of zones of ine
fficient Sn propagation and low Pn velocities suggests that high tempe
ratures and partial melt lie at shallow depths in the upper mantle ben
eath the Turkish plateau and northern Iranian plateau. The presence of
water, presumably due to subduction of hydrated oceanic crust, lowers
the solidus temperature and enhances partial melt. Lg is blocked by o
ceanic crustal structures as well as by structural and topographic var
iations associated with tectonic boundaries.