S. Kodaira et al., V-P V-S RATIO STRUCTURE OF THE LOFOTEN CONTINENTAL-MARGIN, NORTHERN NORWAY, AND ITS GEOLOGICAL IMPLICATIONS/, Geophysical journal international, 124(3), 1996, pp. 724-740
In 1988, an extensive seismic refraction and wide-angle reflection stu
dy was performed at the Lofoten passive continental margin, off northe
rn Norway, by using three-component ocean bottom seismographs. The Lof
oten margin was formed by continental rifting and sea-floor spreading
with extensive volcanism, which is responsible for landward flood basa
lts and seaward-dipping reflectors (SDR). The P-wave structure beneath
the seaward side of the Voring Plateau escarpment at the Lofoten marg
in is characterized by a thick oceanic lower crust and the existence o
f an additional high-velocity layer at the bottom of the crust. In thi
s study, the distribution of the P-wave velocity (V-p) to S-wave veloc
ity (V-s) ratio down to the uppermost mantle is obtained by studying P
-to-S converted shear-wave data. V-p/V-s ratios of 3.0-5.5 are obtaine
d in the sedimentary layers. These high ratios are attributed to uncon
solidated sediments. In the upper crust, a significant difference in V
-p/V-s ratios is found between oceanic-side profiles and land-side pro
files, i.e. 1.86 oceanward of the SDRs and 1.76 landward of the SDRs.
This variation may have been caused by a difference in porosity, due t
o the difference in extrusive processes: the upper crust of the oceani
c side of the SDRs was created by submarine eruptions, while the land
side of the SDRs was formed by subaerial eruptions. The V-p/V-s ratios
in the middle crust and lower crust are estimated as 1.76-1.78 and 1.
80, respectively. Comparing V-p and V-s data from the lower crust to t
hose in previous studies clearly indicates the presence of mafic gneis
ses. This result represents new seismic evidence for the hotspot hypot
hesis concerning the formation of passive volcanic continental margins
. Clear S-wave upper-mantle refractions can be observed at offsets of
up to 100 km, even where P-wave arrivals cannot be identified. In orde
r to model these S-wave arrivals, a V-s = 4.8 km s(-1) layer is necess
ary 2 km below the Moho.