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  • 1
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    In:  Geophysical Journal International, Luxembourg, Conseil de l'Europe, vol. 155, no. 3, pp. 839-856, pp. B04313, (ISBN: 0-12-018847-3)
    Publication Date: 2003
    Keywords: Intensity ; Attenuation ; Earthquake hazard ; Tomography ; GJI ; attenuation, ; macroseismic ; intensity, ; tomography
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  • 2
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    In:  Geophys. J. Int., Basel, Inst. f. Geophys., Ruhr-Univ. Bochum, vol. 163, no. 3, pp. 1203-1218, pp. 1009, (ISSN: 1340-4202)
    Publication Date: 2005
    Keywords: Volcanology ; Stress ; Micro-tremor (seismic noise) ; Seismicity ; Statistical investigations ; Pattern recognition ; Earthquake precursor: prediction research ; GJI ; flank ; eruptions, ; regional ; tectonic ; stress, ; statistical ; pattern ; recognition, ; time ; predictability
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  • 3
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    In:  Physics of The Earth and Planetary Interiors, Berlin, Inst. Electrical & Electronics Engineers, vol. 156, no. 1-2, pp. 41-58, pp. B04307, (ISBN: 0534351875, 2nd edition)
    Publication Date: 2006
    Keywords: Seismicity ; Statistical investigations ; Gutenberg-Richter magnitude frequency b-value ; Correlation ; PEPI ; Aftershocks ; forecasting ; Omori ; law ; Gutenberg-Richter ; law ; Parameters ; correlation
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  • 4
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    In:  Annals Geophysics, Luxembourg, Conseil de l'Europe, vol. 47, no. 1, pp. 307-334, pp. L12309, (ISSN: 1340-4202)
    Publication Date: 2004
    Keywords: Earthquake catalog ; Seismicity ; Fault plane solution, focal mechanism ; Seismology
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  • 5
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    In:  Annals of Geophysics, Luxembourg, Conseil de l'Europe, vol. 47, no. 1, pp. FROTH, pp. L12309, (ISSN: 1340-4202)
    Publication Date: 2004
    Keywords: Earthquake catalog ; Seismicity
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  • 6
    Publication Date: 2012-07-19
    Description: SUMMARY With the goal of constructing a homogeneous data set of moment magnitudes ( M w ) to be used for seismic hazard assessment, we compared M w estimates from moment tensor catalogues available online. We found an apparent scaling disagreement between M w estimates from the National Earthquake Information Center (NEIC) of the US Geological Survey and from the Global Centroid Moment Tensor (GCMT) project. We suspect that this is the effect of an underestimation of M w 〉 7.0 ( M 0 〉 4.0 × 10 19 Nm) computed by NEIC owing to the limitations of their computational approach. We also found an apparent scaling disagreement between GCMT and two regional moment tensor catalogues provided by the ‘Eidgenössische Technische Hochschule Zürich’ (ETHZ) and by the European–Mediterranean Regional Centroid Moment Tensor (RCMT) project of the Italian ‘Istituto Nazionale di Geofisica e Vulcanologia’ (INGV). This is probably the effect of the overestimation of M w 〈 5.5 ( M 0 〈 2.2 × 10 17 Nm), up to year 2002, and of M w 〈 5.0 ( M 0 〈 4.0 × 10 16 Nm), since year 2003, owing to the physical limitations of the standard CMT inversion method used by GCMT for the earthquakes of relatively low magnitude. If the discrepant data are excluded from the comparisons, the scaling disagreements become insignificant in all cases. We observed instead small absolute offsets (≤0.1 units) for NEIC and ETHZ catalogues with respect to GCMT whereas there is an almost perfect correspondence between RCMT and GCMT. Finally, we found a clear underestimation of about 0.2 units of M w magnitudes computed at the INGV using the time-domain moment tensor (TDMT) method with respect to those reported by GCMT and RCMT. According to our results, we suggest appropriate offset corrections to be applied to M w estimates from NEIC, ETHZ and TDMT catalogues before merging their data with GCMT and RCMT catalogues. We suggest as well to discard the probably discrepant data from NEIC and GCMT if other M w estimates from different sources are available for the same earthquakes. We also estimate approximately the average uncertainty of individual M w estimates to be about 0.07 magnitude units for the GCMT, NEIC, RCMT and ETHZ catalogues and about 0.13 for the TDMT catalogue.
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
    Published by Oxford University Press on behalf of The Deutsche Geophysikalische Gesellschaft (DGG) and the Royal Astronomical Society (RAS).
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  • 7
    Publication Date: 2012-06-07
    Description: SUMMARY Until a decade ago, regression analyses for conversions between different types of magnitude were using only the ordinary least squares method, which assumes that the independent variable is error free, or the simple orthogonal regression method, which assumes equal uncertainties for the two variables. The recent literature became aware of the inadequacy of such approaches and proposes the use of general orthogonal regression methods that account for different uncertainties of the two regression variables. Under the common assumption that only the variance ratio between the dependent and independent variables is known, we compared three of such general orthogonal regression methods that have been applied to magnitude conversions: the chi-square regression, the general orthogonal regression, and the weighted total least squares. Although their formulations might appear quite different, we show that, under appropriate conditions, they all compute almost exactly the same regression coefficients and very similar (albeit slightly different) formal uncertainties. The latter are in most cases smaller than those estimated by bootstrap simulation but the amount of the deviation depends on the data set and on the assumed variance ratio.
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
    Published by Oxford University Press on behalf of The Deutsche Geophysikalische Gesellschaft (DGG) and the Royal Astronomical Society (RAS).
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  • 8
    Publication Date: 2011-02-26
    Description: SUMMARY We analysed the time evolution of the decay parameters of the L’Aquila aftershock sequence, neglecting spatial variability. During the first two months after the main shock, the sequence showed quite unusual properties: a particularly slow decay of the aftershock rate that progressively accelerated and a very scarce sensitivity to the occurrence of strong aftershocks. In the first few days, the decrease of the aftershock rate was compatible with an Omori's process with power-law exponent  p  ≈ 0.5. The successive increase of the exponent up to about  p  = 1.2 in the following months can be interpreted as the emergence of a negative exponential regime that has been found to control the decay of other sequences occurred in Italy and California. In fact, two decay models, even including a negative exponential term, reproduce the aftershock rate in the first 60 days significantly better than the Omori's law according to the Akaike information criteria. In this time interval, the strongest aftershocks do not seem to have produced significant increases of the aftershock rate while a couple of them seem to be preceded, rather than followed, by a slight increase of the rate. Consequently, epidemic models do not perform significantly better than non-epidemic ones for durations shorter than 60–80 days. A slow change of decay parameters seems to have been preceded a clear increase of the rate occurred 80 days after the main shock in correspondence of a relatively strong aftershock in the main fault area and of the activation of a previously silent fault segment in the NW. As a consequence of such reactivation, epidemic models become preferable with respect to non-epidemic ones for longer durations. The L’Aquila main shock productivity is the highest ever observed in Italy since the installation of a modern seismic network in Italy in mid 1980s, as the number of generated aftershock is from three to 10 times higher than for any previous earthquake of similar magnitude.
    Print ISSN: 0956-540X
    Electronic ISSN: 1365-246X
    Topics: Geosciences
    Published by Oxford University Press on behalf of The Deutsche Geophysikalische Gesellschaft (DGG) and the Royal Astronomical Society (RAS).
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  • 9
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 120 (1995), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Notes: The applicability of the time- and slip-predictable earthquake recurrence models to Italian seismicity is tested through a more stringent statistical procedure than previously employed. This procedure has the following main features:(1) the original definition, which applied to ‘megafault’ planar geometries is extended to 3-D source volumes;(2) seismic regions are defined by two independent regionalization criteria based on (a) neotectonics and (b) the spatial clustering of epicenters;(3) analysis is restricted to the complete part of the catalogue, inferring completeness through statistics;(4) the common simple inspection for alignment in the cumulative (or noncumulative) sequence of coseismic slips is translated into an equivalent regression problem, which is studied through the analysis of variance in two stages for the data being compatible with the models;(5) clustered large events within each region are accounted for by ‘attaching’ to each main event all the following occurrences within a given time window;(6) different magnitude thresholds are used to ensure that each event releases strain in a whole region.The procedure is applied to two different sets of data, which, in order to maximize the number of analysable recurrences, both rely or, the moment-magnitude scaling law to estimate the coseismic slip, and have therefore an intrinsic accuracy similar to that of the sets used in previous studies. The first set of data considers the complete catalogue for Italian seismicity and, capitalizing on the most extended and reliable historical seismic record in the world, contains several recurrences in each region. The second one, based only on instrumental recording, considers the recent activity of a more detailed subset of three low-seismicity regions. Each region is analysed separately to avoid bias in the regression and since it does not appear feasible to assume that the tectonic setting and the mechanical properties are identical everywhere. This analysis yields that the time- and the slip-predictable models offer a satisfactory fit to reality, respectively, in just two regions and one region out of the 19 globally analysed. The reasons for this negative result, at odds with the positive evidence which has been reported in the literature for the time-predictable model, are analysed. The potential causes might be several, but applying the same procedure to the flagships of these models, i.e. Bufe, Harsh & Burford (1977), Shimazaki & Nakata (1980) and Papazachos (1989, 1992), yields similar negative results. The origin of this general incapability (with very few exceptions) of the time-and slip-predictable models to represent the data appears therefore to be the stringent validation procedure adopted here. Such models appear thus too crude to be a tool of general practical utility, and can be tentatively used for time-dependent hazard estimates in just a very few regions. This suggests also that seismogenesis obeys constitutive laws more complex than simple linear elastic laws.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    Oxford, UK : Blackwell Publishing Ltd
    Geophysical journal international 115 (1993), S. 0 
    ISSN: 1365-246X
    Source: Blackwell Publishing Journal Backfiles 1879-2005
    Topics: Geosciences
    Type of Medium: Electronic Resource
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