2004
DOI: 10.1023/b:sgeg.0000037473.70906.08
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The k-2Rupture Model Parametric Study: Example of the 1999 Athens Earthquake

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Cited by 19 publications
(21 citation statements)
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“…Numerous SFFM generation algorithms have been proposed in the literature, and they often include parameters functionally similar to the S ∗ algorithm corner wave numbers [ Herrero and Bernard , ; Somerville et al , ; Mai and Beroza , ; Gallović and Brokešová , , ; Causse et al , , ]. To apply such algorithms a method to select parameter values is required (e.g., regressions with M w in this study), and to devise this it will usually be necessary to compute best fit model parameters from data.…”
Section: Discussionmentioning
confidence: 99%
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“…Numerous SFFM generation algorithms have been proposed in the literature, and they often include parameters functionally similar to the S ∗ algorithm corner wave numbers [ Herrero and Bernard , ; Somerville et al , ; Mai and Beroza , ; Gallović and Brokešová , , ; Causse et al , , ]. To apply such algorithms a method to select parameter values is required (e.g., regressions with M w in this study), and to devise this it will usually be necessary to compute best fit model parameters from data.…”
Section: Discussionmentioning
confidence: 99%
“…To apply such algorithms a method to select parameter values is required (e.g., regressions with M w in this study), and to devise this it will usually be necessary to compute best fit model parameters from data. If the SFFM algorithms include adjustments to slip values such as tapering, clipping, or absolute value transformation [ Herrero and Bernard , ; Gallović and Brokešová , , ; Causse et al , ; Løvholt et al , ], then the slip Fourier spectrum can deviate from the idealized spectral decay model (equation for the S ∗ algorithms used here) and ignoring this fact can lead to biased parameter estimates. The stochastic optimization algorithm devised in section 2.2.2 was designed to solve this problem and produced relatively accurate and unbiased corner wave number estimates for the S ∗ algorithms used here.…”
Section: Discussionmentioning
confidence: 99%
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“…The HIC technique simulates the rupture process in terms of slipping of elementary subsources with fractal number-size distribution (fractal dimension 2), randomly placed on the fault plane (Zeng et al, 1994). At low frequencies, the source description is based on the representation theorem (integral approach, Aki and Richards, 2002), assuming a final slip distribution composed from the subsources, which is characterized by a k-squared decay (Herrero and Bernard, 1994;Gallovič and Brokešová, 2004). At high frequency, instead, the ground-motion synthesis is obtained summing the contributions from each individual subsource treated as a point source (composite approach).…”
Section: Simulation Methodsmentioning
confidence: 99%
“…The kinematic rupture model considered for the 0 s fault is based on the study of Cocco and Pacor (1993): the final slip distribution is characterized by two main asperities, the largest located close to the southern edge of the fault and the other located close to the northern edge, both at a depth between 6.5 and 11 km. Starting from the slip and rupture time distributions originally proposed by the authors, we calculated a k 2 slip model (Herrero and Bernard, 1994;Gallovič and Brokešová, 2004) shown in Figure 2a. The position of the nucleation Figure 1.…”
Section: Source and Propagation Modelsmentioning
confidence: 99%