Please use this identifier to cite or link to this item: http://hdl.handle.net/2122/6773
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dc.contributor.authorallHainzl, S.; GFZ German Research Centre for Geosciences, Potsdam, Germanyen
dc.contributor.authorallEnescu, B.; GFZ German Research Centre for Geosciences, Potsdam, Germanyen
dc.contributor.authorallCocco, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italiaen
dc.contributor.authorallWoessner, J.; Institute of Geophysics, ETH Zurich, Zurich, Switzerlanden
dc.contributor.authorallCatalli, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italiaen
dc.contributor.authorallWang, R.; Helmholtz Centre Potsdam, GFZ German Research Centre for Geosciences,Potsdam, Germanyen
dc.contributor.authorallRoth, F.; Helmholtz Centre Potsdam, GFZ German Research Centre for Geosciences,Potsdam, Germanyen
dc.date.accessioned2011-01-19T13:51:04Zen
dc.date.available2011-01-19T13:51:04Zen
dc.date.issued2009en
dc.identifier.urihttp://hdl.handle.net/2122/6773en
dc.descriptionAn edited version of this paper was published by AGU. Copyright (2009) American Geophysical Union.en
dc.description.abstractWe discuss the impact of uncertainties in computed coseismic stress perturbations on the seismicity rate changes forecasted through a rate- and state-dependent frictional model. We aim to understand how the variability of Coulomb stress changes affects the correlation between predicted and observed changes in the rate of earthquake production. We use the aftershock activity following the 1992 M7.3 Landers (California) earthquake as a case study. To accomplish these tasks, we first analyze the variability of stress changes resulting from the use of different published slip distributions. We find that the standard deviation of the uncertainty is of the same size as the absolute stress change and that their ratio, the coefficient of variation (CV), is approximately constant in space. This uncertainty has a strong impact on the forecasted aftershock activity if a rate-and-state frictional model is considered. We use the early aftershocks to invert for friction parameters and the coefficient of variation by means of the maximum likelihood method. We show that, when the uncertainties are properly taken into account, the inversion yields stable results, which fit the spatiotemporal aftershock sequence. The analysis of the 1992 Landers sequence demonstrates that accounting for realistic uncertainties in stress changes strongly improves the correlation between modeled and observed seismicity rate changes. For this sequence, we measure a friction parameter Aσn ≈ 0.017 MPa and a coefficient of stress variation CV = 0.95.en
dc.language.isoEnglishen
dc.relation.ispartofJournal of Geophysical Researchen
dc.relation.ispartofseries/114 (2009)en
dc.subjectrate dependent and state dependent frictional modelen
dc.subjectseismicityen
dc.subjectearthquake forecastingen
dc.subjectCoulomb stress changeen
dc.titleAftershock modeling based on uncertain stress calculationsen
dc.typearticleen
dc.description.statusPublisheden
dc.type.QualityControlPeer-revieweden
dc.description.pagenumberB05309en
dc.subject.INGV04. Solid Earth::04.06. Seismology::04.06.01. Earthquake faults: properties and evolutionen
dc.subject.INGV04. Solid Earth::04.06. Seismology::04.06.02. Earthquake interactions and probabilityen
dc.identifier.doi10.1029/2008JB006011en
dc.description.obiettivoSpecifico3.1. Fisica dei terremotien
dc.description.journalTypeJCR Journalen
dc.description.fulltextopenen
dc.contributor.authorHainzl, S.en
dc.contributor.authorEnescu, B.en
dc.contributor.authorCocco, M.en
dc.contributor.authorWoessner, J.en
dc.contributor.authorCatalli, F.en
dc.contributor.authorWang, R.en
dc.contributor.authorRoth, F.en
dc.contributor.departmentGFZ German Research Centre for Geosciences, Potsdam, Germanyen
dc.contributor.departmentGFZ German Research Centre for Geosciences, Potsdam, Germanyen
dc.contributor.departmentIstituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italiaen
dc.contributor.departmentInstitute of Geophysics, ETH Zurich, Zurich, Switzerlanden
dc.contributor.departmentIstituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italiaen
dc.contributor.departmentHelmholtz Centre Potsdam, GFZ German Research Centre for Geosciences,Potsdam, Germanyen
dc.contributor.departmentHelmholtz Centre Potsdam, GFZ German Research Centre for Geosciences,Potsdam, Germanyen
item.openairetypearticle-
item.cerifentitytypePublications-
item.languageiso639-1en-
item.grantfulltextopen-
item.openairecristypehttp://purl.org/coar/resource_type/c_18cf-
item.fulltextWith Fulltext-
crisitem.author.deptDeutschelGeoForschungsZentrum-
crisitem.author.deptGFZ German Research Centre for Geosciences, Potsdam, Germany-
crisitem.author.deptIstituto Nazionale di Geofisica e Vulcanologia (INGV), Sezione Roma1, Roma, Italia-
crisitem.author.deptETH, Zurich,Switzerland-
crisitem.author.deptIstituto Nazionale di Geofisica e Vulcanologia (INGV), Sezione Roma1, Roma, Italia-
crisitem.author.deptDept. Physics of the Earth, Helmholtz-Zentrum Potsdam, Deutsches, GeoForschungsZentrum (GFZ), Telegrafenberg, 14473 Potsdam, Germany-
crisitem.author.deptHelmholtz Centre Potsdam, GFZ German Research Centre for Geosciences,Potsdam, Germany-
crisitem.author.orcid0000-0002-2875-0933-
crisitem.author.orcid0000-0001-6798-4225-
crisitem.author.parentorgIstituto Nazionale di Geofisica e Vulcanologia-
crisitem.author.parentorgIstituto Nazionale di Geofisica e Vulcanologia-
crisitem.classification.parent04. Solid Earth-
crisitem.classification.parent04. Solid Earth-
crisitem.department.parentorgIstituto Nazionale di Geofisica e Vulcanologia-
crisitem.department.parentorgIstituto Nazionale di Geofisica e Vulcanologia-
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