{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1363388845401010944.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1002/2013jb010118"}},{"identifier":{"@type":"URI","@value":"https://api.wiley.com/onlinelibrary/tdm/v1/articles/10.1002%2F2013JB010118"}},{"identifier":{"@type":"URI","@value":"https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1002/2013JB010118"}}],"dc:title":[{"@value":"Inferring fault rheology from low‐frequency earthquakes on the San Andreas"}],"description":[{"type":"abstract","notation":[{"@value":"<jats:title>Abstract</jats:title><jats:p>Families of recurring low‐frequency earthquakes (LFEs) within nonvolcanic tremor (NVT) on the San Andreas fault in central California show strong sensitivity to shear stress induced by the daily tidal cycle. LFEs occur at all levels of the tidal shear stress and are in phase with the very small, ~400 Pa, stress amplitude. To quantitatively explain the correlation, we use a model from the existing literature that assumes the LFE sources are small, persistent regions that repeatedly fail during shear of a much larger scale, otherwise aseismically creeping fault zone. The LFE source patches see tectonic loading, creep of the surrounding fault which may be modulated by the tidal stress, and direct tidal loading. If the patches are small relative to the surrounding creeping fault then the stressing is dominated by fault creep, and if patch failure occurs at a threshold stress, then the resulting seismicity rate is proportional to the fault creep rate or fault zone strain rate. Using the seismicity rate as a proxy for strain rate and the tidal shear stress, we fit the data with possible fault rheologies that produce creep in laboratory experiments at temperatures of 400 to 600°C appropriate for the LFE source depth. The rheological properties of rock‐forming minerals for dislocation creep and dislocation glide are not consistent with the observed fault creep because strong correlation between small stress perturbations and strain rate requires perturbation on the order of the ambient stress. The observed tidal modulation restricts ambient stress to be at most a few kilopascal, much lower than rock strength. A purely rate dependent friction is consistent with the observations only if the product of the friction rate dependence and effective normal stress is ~ 0.5 kPa. Extrapolating the friction rate strengthening dependence of phyllosilicates (talc) to depth would require the effective normal stress to be ~50 kPa, implying pore pressure is lithostatic. If the LFE source is on the order of tens of meters, as required by the model, rate‐weakening friction rate dependence (e.g., olivine) at 400 to 600°C requires that the minimum effective pressure at the LFE source is ~ 2.5 MPa.</jats:p>"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380848661784345476","@type":"Researcher","foaf:name":[{"@value":"N. M. Beeler"}],"jpcoar:affiliationName":[{"@value":"Cascades Observatory U.S. Geological Survey  Vancouver Washington USA"}]},{"@id":"https://cir.nii.ac.jp/crid/1383388845401010945","@type":"Researcher","foaf:name":[{"@value":"Amanda Thomas"}],"jpcoar:affiliationName":[{"@value":"University of California  Berkeley California USA"}]},{"@id":"https://cir.nii.ac.jp/crid/1383388845401010946","@type":"Researcher","foaf:name":[{"@value":"Roland Bürgmann"}],"jpcoar:affiliationName":[{"@value":"University of California  Berkeley California USA"}]},{"@id":"https://cir.nii.ac.jp/crid/1383388845401010944","@type":"Researcher","foaf:name":[{"@value":"David Shelly"}],"jpcoar:affiliationName":[{"@value":"U.S. Geological Survey  Menlo Park California USA"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"21699313"},{"@type":"EISSN","@value":"21699356"}],"prism:publicationName":[{"@value":"Journal of Geophysical Research: Solid Earth"}],"dc:publisher":[{"@value":"American Geophysical Union (AGU)"}],"prism:publicationDate":"2013-11","prism:volume":"118","prism:number":"11","prism:startingPage":"5976","prism:endingPage":"5990"},"reviewed":"false","dc:rights":["http://onlinelibrary.wiley.com/termsAndConditions#vor"],"url":[{"@id":"https://api.wiley.com/onlinelibrary/tdm/v1/articles/10.1002%2F2013JB010118"},{"@id":"https://agupubs.onlinelibrary.wiley.com/doi/pdf/10.1002/2013JB010118"}],"createdAt":"2013-11-08","modifiedAt":"2023-10-10","relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1360004233291525504","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Why Do Aftershocks Occur Within the Rupture Area of a Large Earthquake?"}]},{"@id":"https://cir.nii.ac.jp/crid/1360017282189567872","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Frictional and Hydraulic Properties of Plate Interfaces Constrained by a Tidal Response Model Considering Dilatancy/Compaction"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285704781147648","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Tidal sensitivity of tectonic tremors in Nankai and Cascadia subduction zones"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285704783172864","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Tidal sensitivity of shallow very low frequency earthquakes in the Ryukyu Trench"}]},{"@id":"https://cir.nii.ac.jp/crid/1360285708268797696","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Tidal Modulation and Tectonic Implications of Tremors in Taiwan"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567179759821696","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Slip‐behavior transitions of a heterogeneous linear fault"}]},{"@id":"https://cir.nii.ac.jp/crid/1390001205532988416","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"ja","@value":"深部微動が明らかにする潮汐のプレート運動への影響"},{"@language":"en","@value":"Controls on plate motion by oscillating tidal stress: Evidence from deep tremors in western Japan"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842042471296","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Variations in precursory slip behavior resulting from frictional heterogeneity"}]},{"@id":"https://cir.nii.ac.jp/crid/2051151842066365056","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Forecasting tectonic tremor activity using a renewal process model"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1002/2013jb010118"},{"@type":"CROSSREF","@value":"10.1029/2022jb024112_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1002/2014gl060035_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1002/2015jb012250_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1002/2016jb013348_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1002/2016jb013132_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1029/2018gl077843_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1186/s40645-018-0201-x_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1029/2018jb015663_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"},{"@type":"CROSSREF","@value":"10.1186/s40645-022-00523-1_references_DOI_GEnxgGPuLjXZplmZDZNfdU3qVHX"}]}