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Magnetic Field Reversals and Secular Variation in a Bistable Geodynamo Model
D. Schmitt, M.A.J.H. Ossendrijver, P. Hoyng, Phys. of the Earth and Planet. Interiors, 125, 119-124 (2001)
A Theoretical Analysis of the Observed Variability of the Geomagnetic Dipole Field
P. Hoyng, D. Schmitt, M. Ossendrijver, Phys. of the Earth and Planet. Interiors, 130, 143-157 (2002)
Prospecting the Italian Agora in Delos Island
co-authored with Apostolos Sarris, G. Poulioudis, E. Kazelidou, Roland Etienne / postertext at CAA 2002 proceedings
Slawischer Burgwall Potzlow (Uckermark): Geomagnetische Prospektion und Ausgrabung Juli 2011
Co-authored with Felix Biermann & Eyub Eyub; Poster, presented at "20. Jahrestagung des Mittel- und Ostdeutschen Verbandes für Altertumskunde, April 16-19, 2012, Brandenburg an der Havel"
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Seen by: and 3 moreDevelopment of a three-dimensional velocity model for the crust and upper mantle in the greater Barents Sea region
H. Bungum, N. Maercklin, O. Ritzmann, J. I. Faleide, C. Weidle, A. Levshin, J. Schweitzer, W. D. Mooney, S. T. Detweiler (2005). 27th Seismic Research Review: Ground-based nuclear explosion monitoring technologies, LA-UR-05-6407, pages 13-22
We have compiled a 3D seismic velocity model for the crust and upper mantle in the greater Barents Sea region... more
We have compiled a 3D seismic velocity model for the crust and upper mantle in the greater Barents Sea region including northern Scandinavia, Svalbard, Novaya Zemlya, the Kara Sea, and the Kola-Karelia regions. While the general motivation for developing this model is basic geophysical research, a more specific goal is to create a model for research on the identification and location of small seismic events in the study region, and for operational use in locating and characterizing seismic events in the study region.
The observational basis for the velocity model are previous, crustal-scale 2D seismic reflection and refraction profiles, and passive seismological recordings, supplemented by potential field data to provide additional constraints on the crustal structure. The model is defined at grid tiles spaced every 50 km, and each tile is represented by up to two sedimentary and three crystalline crustal layers (plus water and ice). For crustal regions not constrained by primary velocity data, we developed an interpolation scheme based on several defined geological provinces that are characterized by individual tectono-sedimentary histories. The interpolation utilizes the observed strong correlation between sediment and crystalline crustal thickness within continental provinces. For comparison, an alternative interpolation approach applies a continuous curvature gridding algorithm within each of the provinces.
To provide a complete lithospheric model, we complemented the crustal model with an upper mantle velocity model based on surface wave inversion, thereby covering depths essential for Pn and Sn travel time modeling. As an extension to the previously existing data set, we recently retrieved a large amount of surface wave data recorded or excited in the European Arctic during the last three decades. The merged surface wave data set will enable us to refine the upper mantle velocity structure in the study region significantly. Preliminary group velocity maps for Rayleigh and Love waves reflect large-scale geological structures and demonstrate lateral velocity variations in the mantle.
Validation of our velocity model includes travel time modeling and relocation of seismic events. For this purpose we compiled a set of Ground Truth (GT) events comprising chemical and nuclear explosions, and natural earthquakes. Phase arrival times of multiple events at some sites provide timing error estimates at some stations. With the GT events we obtain a rather good Pn and Sn ray coverage in the main target region. Besides the comparison of observed and modeled travel times along selected transects, we have computed source-specific station corrections (SSSCs) from our 3D model.
The crustal velocity models are also evaluated by comparison of predicted gravity fields with the observed free-air gravity. To model the gravity field, we used standard velocity-density relationships for crustal rock types and the density structure of the upper mantle from previous studies. The inferred gravity fields both reflect and exaggerate the basic geological features. Accomplishments so far have been concerned with implementation of a forward modeling procedure and software development needed to support the complex 3D model structure. The forward modelling is done in order to reduce the misfit between observed and modelled gravity and finally to supplement our crustal velocity model with a density distribution.
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S-wave identification by polarization filtering and waveform coherence analyses
O. Amoroso, N. Maercklin, A. Zollo (2012). Bulletin of the Seismological Society of America, 102(2), 854-861, doi:10.1785/0120110140
High-resolution imaging with microseismic events requires the use of large and consistent data sets of seismic phase... more High-resolution imaging with microseismic events requires the use of large and consistent data sets of seismic phase arrival times. In particular the S-phase is important to derive physical parameters of the subsurface. Typically this phase is identified on one of the horizontal seismogram components by a change of signal amplitude and frequency as compared to the previous P-phase. However, reliable S-phase identification can be difficult for local events because of a signal overlap with the P coda, the presence of converted phases, and possible S-wave splitting due to anisotropy. In this study we propose a new data processing technique aiming at uniquely identifying the S-phase arrival using all available records from a seismic network. The technique combines polarization analysis of single three components recordings of an event with analysis of lateral waveform coherence across the network. This makes it possible to construct seismic sections in which the first arrival is the S-phase. This graphical representation can support an operator in both the analysis of single events and in semi-automatic analyses of large datasets. In addition, an automated stacking velocity analysis provides S-wave velocities from these sections. We demonstrate the applicability of this technique using synthetic seismograms, and we evaluate the efficacy on a dataset of three-component velocimeter records from local earthquakes of the Campania-Lucania Apennines (southern Italy) recorded by the Irpinia Seismic Network (ISNet).
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