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dc.contributor.authorMORII, Wataruen
dc.date.accessioned2010-09-08T08:30:46Z-
dc.date.available2010-09-08T08:30:46Z-
dc.date.issued1996-03-
dc.identifier.issn0454-7675-
dc.identifier.urihttp://hdl.handle.net/2433/125013-
dc.description.abstractThe generation mechanism of X_3 was investigated. It was concluded that X_3 is a packet of spheroidal overtones. It was already proved in the previous study that X_1 and X_2 are composed of successive arrivals of converted body waves while X_4 is a packet of spheroidal overtones. From the point of view that X_3 and X_4 can be treated as higher modes, the velocity dispersions of X_3 and X_4 were examined. The results show that group velocities of X_3 and X_4 separate into segments corresponding to the extrema of velocity dispersion curves of some higher Rayleigh modes. It can be said that X_3 and X_4 are composed of Airy phases of some higher Rayleigh modes. As to X_l and X_2, the relation between the predominant periods and magnitudes was examined. The results exhibited an correlation between them. The predominant periods of X_1 and X_2 are related directly to the duration of the source process. It was also revealed that the predominant periods grow longer under the influence of focusing of seismic rays.en
dc.format.mimetypeapplication/pdf-
dc.language.isoeng-
dc.publisherDisaster Prevention Research Institute, Kyoto Universityen
dc.titleThe Generation Mechanism and Some Properties of the X Phaseen
dc.typedepartmental bulletin paper-
dc.type.niitypeDepartmental Bulletin Paper-
dc.identifier.ncidAA00581033-
dc.identifier.jtitleBulletin of the Disaster Prevention Research Instituteen
dc.identifier.volume45-
dc.identifier.issue4-
dc.identifier.spage85-
dc.identifier.epage98-
dc.textversionpublisher-
dc.sortkey02-
dcterms.accessRightsopen access-
出現コレクション:Vol.45 Pt.4

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