IAG-IASPEI 2017

Presentation information

Oral

IASPEI Symposia » S14. Upper mantle and transition zone dynamics and structure

[S14-2] Upper mantle and transition zone dynamics and structure II

Wed. Aug 2, 2017 10:30 AM - 12:00 PM Room 402 (Kobe International Conference Center 4F, Room 402)

Chairs: Christine Houser (Tokyo Institute of Technology) , George Helffrich (Tokyo Institute of Technology)

11:00 AM - 11:15 AM

[S14-2-03] Mantle transition zone beneath a normal seafloor in the northwestern Pacific: Electrical conductivity, seismic thickness, and water content

Tetsuo Matsuno1, 2, Daisuke Suetsugu3, Kiyoshi Baba2, Noriko Tada2,3, Hisayoshi Shimizu2, Hajime Shiobara2, Takehi Isse2, Hiroko Sugioka4, Aki Ito3, Masayuki Obayashi3, Hisashi Utada2 (1.Kobe Ocean Bottom Exploration Center, Kobe University, Kobe, Japan, 2.Earthquake Research Institute, The University of Tokyo, Tokyo, Japan, 3.Department of Deep Earth Structure and Dynamics Research, Japan Agency for Marine-Earth Science and Technology, Yokosuka, Japan, 4.Department of Planetology, Kobe University, Kobe, Japan)

We conducted a joint electromagnetic (EM) and seismic experiment to reveal the mantle structure beneath a normal seafloor at 130-145 Ma in the northwestern Pacific, where the seafloor is relatively flat and the underlying mantle is expected to be normal (free from tectonic perturbations). In the experiment, we deployed state-of-the-art instruments in two arrays from 2010-2015. Here, we report the result of analyses of the EM and seismic data for investigating the mantle transition zone (MTZ) structure. The EM data analysis revealed that an electrical conductivity structure below both arrays was approximated by an average 1-D model of the north Pacific, and showed a possible downward increase in conductivity at the top of the MTZ. From the P-wave receiver function analysis, perturbations in the MTZ thickness from a global average were estimated to be +20 km and +2 km below the northern and southern arrays, respectively, from which temperature profiles in the MTZ below these two arrays were then estimated. We jointly interpreted the profiles of electrical conductivity and thus estimated temperature, with reference to the experimental values of the effects of water on the electrical conductivities of MTZ minerals (wadsleyite and ringwoodite) from mineral physics. The upper bound of the water content below the northern array was determined to be 0.4 wt.% or 0.04 wt.%, depending on different results of mineral physics, and that below the southern array was determined to be slightly smaller. The lower bound of the water content was not constrained by our data. Our results indicate that the MTZ beneath the normal seafloor in the northwestern Pacific is drier than subduction zones, and may be a water-poor region in a plum-pudding mantle model.