日本地球惑星科学連合2015年大会

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セッション記号 S (固体地球科学) » S-EM 固体地球電磁気学

[S-EM33] 電気伝導度・地殻活動電磁気学

2015年5月26日(火) 09:00 〜 10:45 102A (1F)

コンビーナ:*神田 径(東京工業大学火山流体研究センター)、市來 雅啓(東北大学大学院理学研究科)、座長:松野 哲男(東京大学地震研究所)

10:00 〜 10:15

[SEM33-05] 磁場変換関数データとNetwork-MTデータによる九州地方の3次元比抵抗構造

*畑 真紀1上嶋 誠1半田 駿2下泉 政志3田中 良和4橋本 武志5鍵山 恒臣4歌田 久司1宗包 浩志6市來 雅啓7藤田 清士8 (1.東京大学地震研究所、2.佐賀大学農学部、3.九州職業能力開発大学校、4.京都大学理学研究科、5.北海道大学大学院理学研究院、6.国土地理院、7.東北大学大学院理学研究科、8.大阪大学院工学研究科)

The Kyushu Island in the Southwest Japan Arc has many Quaternary active volcanoes, which exist along the volcanic front of N30oE-S30oW, in relation to the subduction of the Philippine Sea Plate (PSP). The volcanoes are located in northern and southern regions of the island, and no volcano is located in the central region between the two volcanic regions of the island. We have performed three-dimensional (3-D) inversion analyses to obtain a lithospheric-scale electrical resistivity structure (model) beneath the entire Kyushu Island by using a data set of Network-Magnetotelluric (MT) response functions [Hata et al., 2015]. One of two major findings from a distribution of conductive anomalies in the model is that the volcanoes in the northern and southern volcanic regions have two different origins bordering the non-volcanic region at deep depths. Secondly, the degrees of magmatism and the relative contributions of slab-derived fluids to the magmatism vary spatially in the one non-volcanic and two volcanic regions.
A shallow depth resolution of the lithospheric-scale resistivity model, however, was too low to examine small-scale resistivity structures of the crust because of the period range between 480 and 40,960 s of the Network-MT data. Thus we have started to perform 3-D inversion analyses by using a data set of geomagnetic transfer functions whose period range is from 20 to 960 s to obtain a resistivity structure model, in which we can examine smaller-scale structures. The geomagnetic transfer functions were determined at 167 sites in the Kyushu district. Original raw data sets for the geomagnetic transfer functions were measured at the entire Kyushu island and several islands off the western coast of Kyushu from 1980,s to 1990,s [e.g., Handa et al., 1992; Shimoizumi et al., 1997; Munekane et al., 1997]. In this presentation, we will show a new electrical resistivity model, which is obtained through a two-stage inversion process as follows. We determine a resistivity structure mainly at a shallow depth by applying 3-D inversion analyses for the geomagnetic transfer functions of 20-960 s first and then determine a lithospheric-scale resistivity structure by applying 3-D inversion analyses for the Network-MT response functions of 480-40,960 s, which is based on values of the previous resistivity model determined by using the geomagnetic transfer functions. In the two-stage inversion process, we use two types of DASOCC inversion code [Siripunvaraporn et al., 2004; Uyeshima et al., 2008; Siripunvaraporn and Egbert, 2009].