F. Kruger, SEDIMENT STRUCTURE AT GRF FROM POLARIZATION ANALYSIS OF P-WAVES OF NUCLEAR-EXPLOSIONS, Bulletin of the Seismological Society of America, 84(1), 1994, pp. 149-170
Near-vertical incidence angles and quasi-elliptical particle motions c
haracterize broadband P waves from nuclear explosions recorded at the
three 3-component stations of the Grafenberg array (GRF) in southern G
ermany, which is situated on the Jurassic sediments of the Franconian
Jura. Comparison with data from the broadband stations KHC (Kaperske H
ory, Czech Republic) and KSP (Ksiaz, Poland), located on gneiss in the
Bohemian Massif and Precambrian sediments, respectively, show that th
e observed effect is caused by local receiver conditions. Polarization
analysis shows that P- to SV-wave conversions at the basement/sedimen
t boundary and multiples in the sedimentary layers are mainly responsi
ble for these observations at the GRF array. Borehole and refraction d
ata confirm low P-wave velocities in the sediments under the GRF stati
ons. By modeling the broadband particle motions of the P waves of nucl
ear explosions, average models for the sedimentary layers below the GR
F stations are derived. The main modifications to the model of Aichele
(1976) are one (GRF-C1) and two low-velocity layers (GRF-B1 and GRF-A
1) between the outcropping limestone and the basement. The first low-v
elocity layer has an S-wave velocity of about 1.0 km/sec and a thickne
ss of about 200 m below the three 3-component stations and a P-wave ve
locity about 2.8 km/sec, which is not well constrained. The second low
-velocity layer underlying the first low-velocity layer at the station
s GRF-B1 and GRF-A1 has a lower P-wave velocity of about 2.4 km/sec bu
t a higher S-wave velocity of about 1.6 km/sec. Together with the surf
icial limestone layer (about 200 m thick), the total thickness of the
sediment column increases from about 400 m below GRF-C1 in the south t
o about 750 m below GRF-BI and to about 1150 m below GRF-A1 in the nor
th. Slow sediment layers near the surface are important for the polari
zation of telescismic P waves. In turn, polarization analysis of broad
band recordings can be used to analyze the structure of shallow sedime
nt layers.