JpGU-AGU Joint Meeting 2017

Presentation information

[EE] Oral

S (Solid Earth Sciences) » S-IT Science of the Earth's Interior & Tectonophysics

[S-IT31] [EE] Revisit Bullen's layer C - Mantle transition zone and beyond

Mon. May 22, 2017 10:45 AM - 12:15 PM 202 (International Conference Hall 2F)

convener:Teh-Ru Alex Song(University College London), Younghee Kim(Seoul National University), Xuzhang Shen(Lanzhou Insititute of Seismology, China Earthquake Administration), Yoshio Fukao(Center for Earthquake and Tsunami / Japan Agency for Marine-Earth Science & Technology), Chairperson:Teh-Ru Alex Song(University College London), Chairperson:YoungHee Kim(School of Earth and Environmental Sciences, Seoul National University Seoul)

11:30 AM - 11:45 AM

[SIT31-04] A sporadic low-velocity layer atop the 410-km discontinuity beneath the Pacific Ocean

*Songqiao Shawn Wei1, Peter M Shearer1 (1.Scripps Institution of Oceanography, UC San Diego)

Keywords:410-km discontinuity, SS precursor, Partial melting

The seismic discontinuity at 410 km depth is usually attributed to an isochemical phase transformation from olivine to wadsleyite. In addition to this globally observed feature, a low-velocity layer immediately above it has been observed regionally in many places, mainly under continents and continental margins. This low-velocity layer is thought to represent partial melting due to dehydration of ascending mantle across the 410-km discontinuity. Here we present seismic observations of a sporadic low-velocity layer atop the 410-km discontinuity beneath the Pacific Ocean by stacking and analysing long-period seismic body waves. The lateral variations of this low-velocity layer show no geographical correlation with 410-km discontinuity topography or tomographic models of seismic velocity, suggesting that it is not caused by regional thermal anomalies. If this low-velocity layer indeed indicates dehydration melting across the 410-km discontinuity, its strong lateral heterogeneity needs to be taken into account in future geodynamic models of mantle convection and the deep water cycle.