Description: This paper describes results from a geophysical study in the area between the ultraslow Knipovich Ridge and Bear Island, western Barents Sea. The objective was to map the crustal structure along a profile crossing a pull-apart rifted continental margin and oceanic crust generated by ultraslow spreading. The results are based on modeling of wide-angle seismic and gravity data, together with interpretation of multichannel reflection data. Our results show a two layered oceanic crust in the western part of the profile. The thickness of the oceanic crust is variable in the western 130 km, ranging from 3.5 to 5.5 km. East of km 130 the crustal thickness is relatively constant, with values close to the global average for oceanic crust. The oceanic crust is buried by a thick package of Cenozoic sedimentary rocks. The continent–ocean transition (COT) is placed in the interval 207–255 km, between unequivocal oceanic crust and the foot of the westernmost fault in the Hornsund Fault Zone. It is not possible to conclude whether this interval is oceanic crust or thinned and intruded continental crust, but we favor the latter interpretation, at least for the eastern part of the COT. Stretched continental crust is observed between Hornsund Fault Zone and the Knølegga Fault. Here the sedimentary rocks have high velocities and are interpreted to be mainly of Mesozoic and Late Paleozoic age. In this interval Moho depths increase abruptly from 15 km in the west to 27 km in the east. Crystalline basement velocities are observed close to the seafloor east of the Knølegga Fault. We suggest that continental breakup north of Greenland–Senja Fracture Zone occurred around 33 Ma, after a period of pull-apart tectonics. The spreading rate of the earliest seafloor spreading may have been higher than the present day spreading, creating thicker oceanic crust close to the COT.

Description: The current effort represents a systematic regional study of the vast and poorly sampled area, linking the Barents Sea and the Arctic Ocean. The deep structure of the Northern Barents Sea was examined by means of integration various geophysical techniques, including numerical geodynamic modeling. Ocean Bottom Seismometers data have been acquired east of Svalbard and processed using a seismic refraction/reflection tomography method. A series of crustal-scale geotransects, illustrating the architecture of the Cenozoic Northern Barents Sea margin were constructed using gravity modeling, sparse seismic reflection profiles and depth to magnetic sources estimates. The structure of the Mesozoic passive margin, facing to the Amerasia Basin, was inferred based on a similar technique, involving plate reconstructions. Numerical simulations of the lithosphere extension, leading to formation of the Eurasia Basin, was performed using the finite element method. The velocity structure east of Svalbard exhibits evidences of Cretaceous magmatism. In particular, funnel-shaped high-velocity anomalies, reaching 10% relative to the 1D background model, are interpreted as Early Cretaceous magmatic intrusions. Further to the north, a narrow and steep continent-ocean transition was observed. The conjugate northern (and eastern) Barents Sea - Lomonosov Ridge margins are symmetric and narrow whereas the continent-ocean transition on the Podvodnikov Basin's side of the Lomonosov Ridge is broad. On the continental side, the Northern Barents Sea margin is underlain by Paleozoic-Early Mesozoic deep sedimentary basins separated from the oceanic side by the marginal basement uplift. The Northern Barents Sea, including Svalbard, was not affected by the major Late Jurassic - Early Cretaceous rifting which gave rise to deep basins in the South Western Barents Sea. However, the area experienced widespread Early Cretaceous magmatism. The emplacement of mafic magmas was controlled by Paleozoic rift structures which were reactivated in the Early Cretaceous. The magmatism east of Svalbard developed without significant crustal thinning, but was probably triggered by localized lithospheric weakness zones. The Mesozoic passive margin, originated due to the opening of the Podvodnikov Basin, was subjected to significant crustal thinning. The Northern Barents Sea region together with the Lomonosov Ridge was standing high during most of the Late Cretaceous. The regional uplift sourced from the Alpha Ridge area. The Eurasia Basin's breakup in the Paleocene preceded the opening of the Norwegian Sea, implying a connection to the Labrador Sea. A short-lived lithosphere-scale shear zone has likely facilitated to the detachment of the Lomonosov Ridge microcontinent and onset of seafloor spreading. Shear heating in the mantle lithosphere accompanied the development of the proposed shear zone and served as a mechanism for strain localization.

Description: P -wave polarization at the Gräfenberg array (GRF) in southern Germany is analysed in terms of azimuthal deviations and deviations in the vertical polarization using 20 yr of broad-band recordings. An automated procedure for estimating P -wave polarization parameters is suggested, based on the definition of a characteristic function, which evaluates the polarization angles and their time variability as well as the amplitude, linearity and the signal-to-noise ratio of the P wave. P -wave polarization at the GRF array is shown to depend mainly on frequency and backazimuth and only slightly on epicentral distance indicating depth-dependent local anisotropy and lateral heterogeneity. A harmonic analysis is applied to the azimuthal anomalies to analyse their periodicity as a function of backazimuth. The dominant periods are 180° and 360°. At low frequencies, between 0.03 and 0.1 Hz, the observed fast directions of azimuthal anisotropy inferred from the 180° periodicity are similar across the array. The average fast direction of azimuthal anisotropy at these frequencies is N20°E with an uncertainty of about 8° and is consistent with fast directions of Pn -wave propagation. Lateral velocity gradients determined for the low-frequency band are compatible with the Moho topography of the area. A more complex pattern in the horizontal fast axis orientation beneath the GRF array is observed in the high-frequency band between 0.1 and 0.5 Hz, and is attributed to anisotropy in the upper crust. A remarkable rotation of the horizontal fast axis orientation across the suture between the geological units Moldanubicum and Saxothuringicum is observed. In contrast, the 360° periodicity at high frequencies is rather consistent across the array and may either point to lower velocities in the upper crust towards the Bohemian Massif and/or to anisotropy dipping predominantly in the NE–SW direction. Altogether, P -wave polarization analysis indicates the presence of layered lithospheric anisotropy in the area of the GRF array. Seismic anisotropy is more variable in the brittle upper crust compared to lower crustal and subcrustal depths.