日本地球惑星科学連合2019年大会

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[J] 口頭発表

セッション記号 S (固体地球科学) » S-MP 岩石学・鉱物学

[S-MP32] 変形岩・変成岩とテクトニクス

2019年5月29日(水) 15:30 〜 17:00 A08 (東京ベイ幕張ホール)

コンビーナ:針金 由美子(産業技術総合研究所)、中村 佳博(国立研究開発法人産業技術総合研究所 地質調査総合センター)、座長:遠藤 俊祐(島根大学 総合理工学部 地球科学科)、大柳 良介(国立研究開発法人 海洋研究開発機構 地球内部物質循環研究分野)

16:45 〜 17:00

[SMP32-18] High- and low-stress subduction zones recognized in the rock record

*石井 和彦1ウォリス サイモン2 (1.大阪府立大学大学院理学系研究科物理科学専攻、2.東京大学大学院理学系研究科地球惑星科学専攻)

キーワード:高圧型変成岩、沈み込み境界の応力、三波川帯、フランシスカン コンプレックス

Knowledge of the frictional strength along subduction plate boundaries is an essential part of understanding the conditions necessary for plate tectonics, the processes leading to great earthquakes occur along subduction megathrusts and the thermal structure of subduction zones. The frictional strength of faults increases with depth until ductile deformation becomes dominant and is usually expressed as the ratio of shear to normal stress known as the coefficient of friction, mu or the apparent coefficient, mu’, when the effects of fluid pressure are taken into account. Lamb (2006) uses force balance for forearc domains to infer mu’ = 0.03-0.09 along subduction boundaries. Gao and Wang (2014) infer mu’ = 0.02-0.13 based on the comparison between heat flow data and numerical modeling, while England (2018) estimates relatively uniform values mu’ = 0.05-0.07 from analytical modeling of heat flow data. In addition, a global 3D thermo-mechanical model presented by Osei Tutu et al. (2018) suggests the average mu’ along plate boundaries is required to be <= 0.05 to match the observed present-day plate motion and net rotation.

The published estimates of mu’ for subduction boundaries are significantly lower than Byerlee’s Law (mu’ ~ 0.4, assuming hydrostatic fluid pressure) and closer to values published for seismic slip rates with mu’ ~ 0.1 (Di Toro et al., 2011). However, estimates for different subduction zones or obtained by different methods show variations over an order of magnitude. It is desirable to obtain direct estimates of shear stresses from ancient subduction zones both as an independent test of the suggested values and because if high- and low-stress subduction zones can be identified in the ancient record then observations of the associated geology can help identify those characteristics that are responsible for differences in shear strength along subduction zone boundaries.

Thermal modelling shows that high- and low-stress subduction zones can potentially be recognized in the ancient record based on the shape of the prograde P-T path in the forearc region. For all but very young and very slowly subducting slabs, high-stress subduction can be distinguished by curved P–T paths with higher P/T gradients at greater depths. Low-stress subduction over the same domain results in straight paths.

The Cretaceous Sanbagawa belt of SW Japan records metamorphism developed as a result of rapid (20-24 cm/yr) subduction of the Izanagi plate with a slab age of around 60 Ma. The prograde P-T paths show the characteristics predicted for high-stress subduction. Comparisons with thermal modelling suggest an apparent coefficient of friction, mu’, of > 0.11, and the corresponding peak shear stresses are ~60 MPa.

Prograde P–T paths and geochronological information from high grade blocks of the Franciscan Complex, USA, indicate rapid cooling during the initial 10-20 Myr subduction with low mu’ <= 0.02.

P–T paths in subduction-type metamorphic belts have the potential to be used as paleo stress indicators. Examining differences between high- and low-stress subduction-type metamorphic belts can help determine what controls the strength of different subduction boundaries and assess the potential for great earthquakes in modern settings.