SHEAR-WAVE VELOCITY STRUCTURE BENEATH EUROPE, THE NORTHEASTERN ATLANTIC AND WESTERN ASIA FROM WAVE-FORM INVERSIONS INCLUDING SURFACE-WAVE MODE-COUPLING
H. Marquering et R. Snieder, SHEAR-WAVE VELOCITY STRUCTURE BENEATH EUROPE, THE NORTHEASTERN ATLANTIC AND WESTERN ASIA FROM WAVE-FORM INVERSIONS INCLUDING SURFACE-WAVE MODE-COUPLING, Geophysical journal international, 127(2), 1996, pp. 283-304
Waveforms of 449 seismograms have been inverted for S-wave velocity st
ructures beneath Europe, the northeastern Atlantic, and western Asia d
own to a depth of 670 km. Recorded waveforms were used in the time win
dow starting at the S-wave arrival and ending after the fundamental-mo
de Rayleigh-wave arrival. The inversion method is based on the partiti
oned waveform inversion (Nolet 1990), with the difference that synthet
ic seismograms are calculated taking surface-wave mode coupling into a
ccount in order to model body waves in laterally heterogeneous media m
ore accurately. The partitioning of the inversion procedure makes non-
linear optimization feasible, even for inversions including surface-wa
ve mode coupling. The non-linear inversion of the waveforms resulted i
n linear constraints on the 3-D velocity structure. In a second step,
these constraints were used in a linear inversion for the 3-D shear-wa
ve velocity model beneath Europe, the northeastern Atlantic and wester
n Asia. The EUR-SC'95 model is presented, which is characterized by a
wide range of length-scales of the velocity structures. In central Eur
ope, where the ray density is highest, small-scale structures are reco
vered, such as the presence of high velocities associated with the Hel
lenic subduction zone. On the edges of the inversion model, where the
ray density (and therefore also the resolution) is poorer, we find lar
ger-scale features, such as the relatively laterally homogeneous high-
velocity structure beneath the Russian Platform to a depth of 300 km.
In this paper we discuss the inversion method, data processing, parame
trization difficulties due to the introduction of surface-wave mode co
upling, spatial resolution of the model, and structures in the EUR-SC'
95 model.