著者

飯尾 能久 松本 聡 松島 健 植平 賢司 片尾 浩 大見 士朗 澁谷 拓郎 竹内 文朗 西上 欽也 廣瀬 一聖 加納 靖之 儘田 豊 宮澤 理稔 辰己 賢一 和田 博夫 河野 裕希 是永 将宏 上野 友岳 行竹 洋平 Bogdan ENESCU

出版者

公益社団法人 日本地震学会

雑誌

地震 第2輯 (ISSN:00371114)

巻号頁・発行日

vol.58, no.4, pp.463-475, 2006-03-31 (Released:2010-03-11)

参考文献数

44

被引用文献数

1 2

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The 2004 Mid Niigata Prefecture Earthquake (MJMA 6.8) occurred on 23 October 2004. The mainshock was followed by four aftershocks with MJMA≥6.0. This earthquake is located in the Niigata-Kobe Tectonic Zone in which large strain rates (>0.1ppm/y contraction) have been observed by GPS data. We deployed three temporary online seismic stations in the aftershock area. Combining data from the temporary stations and from permanent stations around the aftershock area, we determined aftershock locations, and estimated the structures and the stress change in and around the aftershock region. Based on these results, we suggested a generating process of the 2004 Mid Niigata Prefecture Earthquake supposing that a very weak region exists in the weak zone in the lower crust just beneath the seismogenic fault.

著者

澁谷 拓郎 平原 和朗 上野 友岳

出版者

公益社団法人 日本地震学会

雑誌

地震 第2輯 (ISSN:00371114)

巻号頁・発行日

vol.61, no.Supplement, pp.199-207, 2009-07-31 (Released:2013-11-21)

参考文献数

38

被引用文献数

2

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Receiver function analyses have been developed since the late 1970s. Receiver functions are calculated by deconvolving the vertical component from the horizontal components of teleseismic P waveforms in order to remove the complexities of the source time functions and to extract the structural information beneath seismic stations. The receiver functions are sensitive to impedance discontinuities of the earth’s interior, especially to the shear wave velocity discontinuities. Therefore, the receiver function analyses have advantages in estimating the shear wave velocity structure and imaging the shear wave velocity discontinuities. In this paper we introduce several basic topics of the receiver function analyses. Firstly, we discuss the method of the calculation of the receiver functions, pointing out weaknesses in the water level method and the multitaper method and introducing the extended-time multitaper method. Secondly, we describe the inversions of the receiver functions for the shear wave velocity structure. We show two examples with the genetic algorithm. Thirdly, we introduce the way and several examples to image the shear wave velocity discontinuities with the use of the receiver functions. Finally, we discuss issues in the receiver function analyses which have not been addressed yet but should be in the near future.