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IUGG XXIV General Assembly July 2-13, 2007 Perugia, Italy<br />

(S) - <strong>IASPEI</strong> - International Association of Seismology and Physics of the Earth's<br />

Interior<br />

JSS007 Poster presentation 1968<br />

Shallow Resistivity Structure of Asama Volcano and Its Implication for<br />

Magma Ascent Process of 2004 Eruptions<br />

Dr. Koki Aizawa<br />

Tokyo Institute of Technology Tokyo Institute of Technology IAGA<br />

Yasuo Ogawa, Takeshi Hashimoto, Takao Koyama, Wataru Kanda, Electromagnetic<br />

Research Group For Asama Volcano<br />

Asama volcano, which sits 150km northwest of Tokyo, is one of the most active volcanoes in Japan.<br />

Historical records show many eruptions that are mainly characterized by Vulcanian eruptions. Its recent<br />

eruptions took place in 2004 at the summit crater without remarkable precursors. Geodetic data and the<br />

hypocenter distributions [e.g., Takeo et al., 2006] suggest that magma ascent route is not simple, and<br />

the conduit does not directly link the summit crater to deep magma chamber. Because shallow structure<br />

may give the constraints on volcanic activities [Tanaka et al., 2002] and can control type of eruptions<br />

[Kagiyama et al., 1999], imaging the upper part of volcanoes is important. In this paper, we will argue<br />

the resistivity structure shallower than 5km obtained by dense magnetotelluric (MT) survey. The MT<br />

data were taken along the four survey lines across the volcano. The total number of measurement sites<br />

was 74. The resistivity profiles obtained by two-dimensional inversions are mainly characterized by<br />

resistive surface layer and underlying conductive layer. Important feature of the profiles is that in a<br />

depth range of a few hundred meters to a few kilometers, three resistive bodies exist, being surrounded<br />

by highly conductive regions. Two of three resistive bodies correspond to the old eruption centers; one<br />

corresponds to the 24ka collapse caldera, and the other does to the 21ka lava dome. Taking into<br />

account that the geothermal activities exist near the old eruption centers, the highly conductive zone is<br />

considered to be hydrothermal system. In this study, we interpret the resistive bodies as old and<br />

solidified intrusive magma that are still driving hydrothermal system in the surrounding area. The<br />

solidified magma bodies are considered to be resistive due to its low porosity. Self-potential survey was<br />

also conducted along the MT profiles. The obtained SP data show the distinct "W"-shaped SP profiles<br />

[Ishido, 2004], and suggests the existence of hydrothermal and hydrogeological zone within the<br />

volcano. The SP profiles seem to have correlation with the top surface of the highly conductive regions,<br />

which is interpreted as hydrothermal system. The SP data may support our interpretation of the<br />

resistivity structure. The resistive body beneath the 24ka collapse caldera is located above the swarm of<br />

tectonic earthquakes at the depth of 3km. Geodetic data suggests that magma intruded beneath this<br />

resistive body. We suggest that magma ascent was hampered by old and solidified remnant magma at<br />

the depth of 3km beneath the collapse caldera, and that a part of the magma migrated horizontally to<br />

the east and finally ascended to the summit, resulting in the 2004 eruptions. This study raises the<br />

possibility that solidified remnant magma in volcanoes is controlling present magma movement.<br />

Keywords: magnetotellurics, resistivity, self potential

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