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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 />

JSS016 Poster presentation 2352<br />

Seafloor borehole seismic observatories in the western Pacific and upper<br />

mantle and crustal structure beneath the northwestern Pacific basin<br />

Dr. Masanao Shinohara<br />

Earthquake Research Institute University of Tokyo <strong>IASPEI</strong><br />

Tetsuo Fukano, Toshihiko Kanazawa, Eiichiro Araki, Kiyoshi Suyehiro, Masashi<br />

Mochizuki, Kazuo Nakahigashi, Yuka Kaiho, Tomoaki Yamada<br />

Geophysical networks provide data for better understanding of the dynamics in the Earth. However, a<br />

great limitation on existing networks is the uneven distribution of stations, especially lack of stations in<br />

the ocean such as the Pacific. For uniform distribution of stations on the Earth, we need to construct<br />

observatories in the sea. The western Pacific area has been selected for installation of ocean-bottom<br />

observatories because it is ideal for problems related to plate subduction. Boreholes are considered to<br />

give best environment for geophysical observations in the sea. Four borehole geophysical observatories<br />

at three areas have been installed during ODP Leg186, 191 and 195. Two stations (JT-1 and JT-2) are<br />

located on the landward side of the Japan Trench. The observatories WP-1 and WP-2 are effectively<br />

located to complete a 1000-km span network in the western Pacific area. The WP-1 site is in the west<br />

Philippine Basin west of the Kyushu-Palau Ridge. The WP-2 observatory is situated in the northwestern<br />

Pacific Basin. Both the stations fill gap for global seismic networks. The WP-1 observatory was activated<br />

in March 2002 using an ROV and long-term observation started. In June 2006, an ROV dived to the WP-<br />

1 (fourth visit) and recovered the data. At this visit, data recording was discontinued. At present,<br />

seismic records of 692-days (Mar. 2002 - Feb, 2004) have been obtained from the WP-1. The WP-2<br />

observatory was activated in October 2000 using an ROV. In June 2005, an ROV made fourth visit to<br />

the WP-2 and recovered the data. Recording at the WP-2 has been suspended from the fourth ROV<br />

visit. In total, 436-days data (Oct. 2000 - Jan. 2001, Aug. 2001 - July 2002) were retrieved. A detailed<br />

structure of an oceanic plate is important information to consider a dynamics of oceanic plate.<br />

Geomagnetic studies in the WP-2 area indicate the crust was formed 129 Ma. The seismic experiments<br />

with ocean bottom seismometers (OBSs), the WP-2 and airguns were performed around the WP-2 in<br />

July 2001, July 2002 and July 2005. To detect a seismic anisotropy in the uppermost mantle, the<br />

experiments had four profiles with different directions. Broadband seismic records for 436 days in total<br />

were retrieved from the WP-2. Reflecting low noise environment, many teleseismic events were<br />

recorded. The purposes of the present study are to obtain a detail seismic structure of crust and<br />

uppermost mantle including a seismic anisotropy from the seismic surveys and to estimate a upper<br />

mantle structure including depths of discontinuities using the WP-2 records. Shallow seismic velocity<br />

models just below OBS were derived from using tau-p method and records of a hydrophone streamer.<br />

The obtained seismic models were confirmed using the ODP logging data. Deep structures were<br />

estimated by forward modeling using a two dimensional ray tracing method. The estimated crustal<br />

structures beneath each line are almost identical. In a sediment layer, P-wave structure is 1.6km/s, S-<br />

wave is about 0.2km/s, the thickness of this layer is approximately 0.4km. The layer 2 is divided into<br />

two layers which have different vertical velocity gradients (layer 2A and layer 2B). The P- and S-wave<br />

velocities at the top of the layer 2A are 4.6km/s and 2.7km/s, respectively. The layer 2B has P- and S-<br />

wave velocities of 5.3km/s and 3.1km/s at the top of the layer, respectively. Total thickness of the layer<br />

2 is about 1.4 km. The data from the WP-2 were useful to estimate the detailed structure of the layer 2.<br />

The uppermost Layer 3 has P- and S-wave velocities of 6.8km/s and 3.8km/s, respectively. The layer 3<br />

is about 5km thick. To explain large amplitudes of Pn phase, a crust-mantle transition layer is required<br />

at the bottom of the crust. The Pn velocities are different in each profile. Average velocities of Pn and

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