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  • 1
    Monograph available for loan
    Monograph available for loan
    Washington : American Geophysical Union
    Associated volumes
    Call number: 5/M 06.0058 ; M 07.0008
    In: Geophysical monograph
    Type of Medium: Monograph available for loan
    Pages: 280 S.
    ISBN: 087590422X
    Series Statement: Geophysical monograph 157
    Classification:
    Seismology
    Location: Reading room
    Location: Upper compact magazine
    Branch Library: GFZ Library
    Branch Library: GFZ Library
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  • 2
    Monograph available for loan
    Monograph available for loan
    Dordrecht [u.a.] : Reidel
    Call number: 14930
    Type of Medium: Monograph available for loan
    Pages: IX, 386 S. : Ill.
    ISBN: 9027725837
    Series Statement: Seismology and Exploration Geophysics
    Language: English
    Location: Upper compact magazine
    Branch Library: GFZ Library
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  • 3
    Call number: G 8971
    Type of Medium: Monograph available for loan
    Pages: 147 S. : graph. Darst., Kt.
    Location: Upper compact magazine
    Branch Library: GFZ Library
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  • 4
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 125 (1996), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: In an effort to determine the characteristics of seismic noise on the ocean bottom and its relationship to the structure of the sea-floor, we have adapted the method of nonlinear waveform fitting to accommodate multidimensional models (shear velocity β and shear damping Qs), and have applied it to invert several records of interface waves (Scholte 1958) from the THUMPER experiment off southern California. Waveform fitting is a very powerful tool to determine the S velocity in the top few metres of the sediment. Starting from β= 30 m s −1 at the top clay layer, the S velocity increases with a gradient of 2.8 m s−1 m−1 over the first 150m of sediment. A theoretical estimation of the source strength gives coherent estimates of Qs as a function of depth for distances between 400 and 1070 m from the source. the Qs models are characterized by very low values (10–20) in the top three metres, but by values in excess of 100 below that level. the results confirm the identification of the noise as harmonics of interface waves. In the area of this experiment, the largest noise amplitudes belong to the fundamental mode and penetrate to a depth of about 20 m into the sediment. the overtone energy can be appreciable too, and is noticeable to about 80 m depth. the Qs structure confirms the strong influence that the sea-floor structure has on the noise spectrum. the high attenuation at frequencies above 3–4 Hz suppresses noise propagation and produces low noise at higher frequencies. (Similarly, high attenuation in the asthenosphere suppresses noise propagation below 0.1 Hz.)
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 124 (1996), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: If body-wave phases in laterally heterogeneous media are modelled by surface-wave mode summation, mode coupling is required to bring out the ray character of the body-wave phases. However, it is frequently assumed that in laterally heterogeneous media surface-wave modes propagate without interacting with other modes. The effects of neglecting surface-wave mode coupling on the results from waveform inversions including body-wave arrivals have been studied by performing inversions with and without taking surface-wave mode coupling into account. The two inversion schemes are similar to the Partitioned Waveform Inversion (Nolet 1990) but differ in the approximations used to compute the synthetics: WKBJ, which neglects mode coupling, or SEA (Marquering & Snieder 1995), which does take mode coupling into account.Synthetic inversion experiments show that neglecting mode coupling can lead to biases in the deeper part of the model. Their most striking feature is that for ‘real’ shallow lateral heterogeneities, artificial anomalies with an opposite sign may show up in the deeper part of the model. When mode coupling is taken into account, as in the SEA inversion scheme, these biases do not occur.We have also studied possible bias effects as the result of using WKBJ in the EUR-S91 model of Zielhuis & Nolet (1994), which is characterized by strong velocity anomalies extending as deep as the transition zone. One of the most striking features in this model is the region of low velocities at larger depths beneath the fast Russian platform on the eastern side of the Tornquist–Teisseyre Zone (TTZ). Nolet & Zielhuis (1994) suggested that these low velocities are an indication for injection of water in the mantle by an earlier subduction. Our results show that the neglect of mode coupling indeed does bias the model towards a larger reversal of velocities with depth, and heterogeneities show up even where the S ray does not sample the mantle. However, low velocities deep below the eastern part of the TTZ persist even when mode coupling is taken into account.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 112 (1993), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 103 (1990), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: As originally formulated by Backus & Gilbert (1970), ill-posed linear inverse problems possess a unique minimum norm solution, and a locally averaged property of the model may be estimated with a resolution that is a monotonic function of its variance. Application of Backus–Gilbert theory requires the inversion of an N x N matrix, where N is the number of data, and therefore becomes cumbersome for large N. In this paper we show how Lanczos iteration may be used to project the original linear problem on a problem of much smaller size in order to obtain an approximation to the Backus–Gilbert solution without the need of matrix inversion. To calculate the resolution in the projected system one only needs to invert a symmetric tridiagonal matrix.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 124 (1996), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: In seismic tomography the problem is generally underdetermined. The solution to the tomographic problem depends on the specific optimization condition used and is inherently distorted due lo noise in the data and approximations in the theory. Smoothing is often applied to reduce inversion artefacts with short correlation lengths. However, a posteriori smoothing generally affects the data fit. For more sophisticated, non-linear filters this effect can be severe. We present a technique to conserve data fit for filters of arbitrary complexity. The difference between the ‘optimal’ solution and a filtered version is projected onto the nullspace of the model space in order to preserve the data fit. Thus, we only allow changes to the image that do not conflict with the data. We demonstrate the benefits of such conservative filters using several different non-linear filters to reduce noise, smooth the image, and highlight edges.The method is exact in small-scale experiments, where we can use the method of singular value decomposition: eigenvectors with large eigenvalues are used to project the difference between the original model and the filtered version onto the nullspace. With large-scale tomographic problems, calculation of all of the large eigenvectors is unrealistic. We show how to use the iterative method of conjugate gradients to apply conservative filters to large-scale tomographic problems with minimum computational effort.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 117 (1994), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: A new model, EUR-S91, of shear-wave velocity variations in the upper mantle beneath central Europe and surrounding regions, down to a depth of 670km, is presented. The model is derived from the inversion of the waveforms of 217 seismograms, using the partitioned waveform-inversion method for the seismogram in the time window from the S-wave arrival to the fundamental mode of the Rayleigh wave. The seismograms were mostly assembled from digitally recording long-period and broad-band stations in Europe. The resulting 3-D model accurately predicts most of the observed waveforms, in a wide band of frequencies. Body waves were fit for frequencies up to 60mHz. The fundamental Rayleigh mode, which at high frequencies is more prone to scattering and multipathing, was generally low passed at 25 mHz. The resolving power of the data set depends strongly on the density of available wave paths and varies as a function of geographical position. Small-scale heterogeneities like the subducted lithosphere in the Hellenic collision zone were imaged in the region with the highest density of wave paths, which indicates an optimum resolution of better than 200 km.The main new results of this study pertain to the transition between east and central Europe. We present new information about the structure below the Tornquist-Teisseyre Zone (TTZ). The TTZ is generally regarded as the boundary between the Precambrian crust of the Baltic Shield/Russian Platform and the younger crust of central Europe. Our 3-D S-velocity model reveals that below this line a sharp lateral boundary extends down to at least 140 km depth, with high velocities beneath the Baltic Shield and Russian Platform contrasting to the low velocities beneath the younger regions of Europe. The observed velocity contrast across the TTZ is largest between the Pannonian Basin and the Russian Platform, where it is equal to 12 per cent at 80 km depth. At depths of 300–400 km, the TTZ is underlain by a zone of low S velocity, which indicates a local thinning of the deeply rooted high-velocity structure or tectosphere that underlies most of eastern Europe.In addition to these new results on the transition region between east and central Europe, a number of features that are present in other tomographic results have been confirmed: the Precambrian provinces of Europe are characterized by high S velocities; low velocities are found beneath the Pannonian Basin, the western Mediterranean, northern Aegean Sea/Turkey and a small region south-west of the Massif Central. The lithosphere beneath the Paris Basin has a positive S-velocity anomaly. The resolution of all these anomalies has been established with sensitivity tests.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 114 (1993), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: When the earliest measurements of the Earth's normal modes became available, it was soon noticed that Vs models satisfying this new data set were generally slower than models based on S traveltimes. This S discrepancy has since then been attributed to the influence of dispersion that accompanies attenuation, but it ignores a competing process that may have the same effect: in a heterogeneous earth, seismic rays will bend to take advantage of local high-velocity anomalies. This effect is difficult to quantify because of the computational problems associated with the determination of minimum traveltime paths in heterogeneous earth models in three dimensions.We have developed a new method to find absolute minimum traveltimes even in very complicated earth models and applied this to a large number of rays generated in different random earth models. the S discrepancy is a function of correlation length and amplitude of Vs heterogeneity. A standard deviation s̀ of 0.15 km s−1, with a correlation length of 200 km in the whole mantle, would give a discrepancy even larger than observed at Δ〉60° and must be discarded. A s̀ of 0.15 km s−1 in the upper mantle and 0.05 km s−1 elsewhere explains a discrepancy of 1-2s, depending on the correlation length. Since the total discrepancy is estimated to be about 4s, this still allows for effects of attenuation.We conclude that the S-wave discrepancy can be used to set limits to the heterogeneity in the lower mantle at short correlation lengths. With our present-day knowledge of the magnitude of the discrepancy a heterogeneity larger than 1 per cent with correlation length 200 km is unlikely.
    Type of Medium: Electronic Resource
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