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 U (ユニオン) » ユニオン

[U-04] 地球惑星科学における高速過程を捉える

2019年5月29日(水) 13:45 〜 15:15 103 (1F)

コンビーナ:芳野 極(岡山大学惑星物質研究所)、丹下 慶範(高輝度光科学研究センター)、座長:芳野 極(岡山大学)、河野 義生(愛媛大学地球深部ダイナミクスセンター)、丹下 慶範

14:30 〜 14:45

[U04-04] Semi-brittle flow in dunite and harzburgite at upper mantle pressures

★Invited Papers

*大内 智博1雷 興林2肥後 祐司3丹下 慶範3 (1.愛媛大学地球深部ダイナミクス研究センター、2.産業技術総合研究所、3.高輝度光科学研究センター)

キーワード:水、半脆性流動、断層形成

The mechanism of intraslab earthquakes (> 40 km depth) is fundamentally different from those of shallower ones. This is because the frictional strength is much higher and fracture process associates ductile flow (i.e., semi-brittle flow) at deeper parts. The location of the double seismic zone in the subducting Pacific slab corresponds to the main dehydration field in the pressure-temperature diagram of the hydrous peridotite (Omori et al., 2002). The cause of intraslab seismicity at intermediate depths has been attributed to breakdown of hydrous minerals such as serpentinite (e.g., Ferrand et al., 2017) and lawsonite (Okazaki et al., 2016) because it causes unstable fault slip or shear localization. However, the role of aqueous fluid in fracturing at high pressures is still unclear.

To evaluate the effect of water on semi-brittle behavior of dunite and harzburgite, we conducted in-situ uniaxial deformation experiments on as-is/water-saturated dunite and harzburgite at pressures 1-3 GPa and temperatures 670-1250 K with a constant displacement rate using a deformation-DIA apparatus. Pressure, stress, and strain were measured in situ by using x-ray diffraction patterns and radiographs. Radiographs were taken at each several minutes in most of deformation experiments, though radiographs were continuously taken (each 5 seconds) during a deformation run (at 2 GPa and 860 K). Acoustic emissions (AEs) were also recorded continuously on six sensors, and three-dimensional AE source location were determined.

Formation of throughgoing faults was observed in water-saturated dunite and harzburgite at 860 K and lower temperatures. Fault slip rate is between 3E-5 and 4E-4 s-1 which are comparable to the background strain rate just before a faulting (1E-5 and 3E-4 s-1), showing that shear localization is ineffective under water-saturated conditions. Addition of the aqueous fluid resulted in the reduction in the number of AE events in the faulted sample (i.e., aseismic faulting). A high time-resolution strain monitoring revealed that fault slip rate fluctuate within several ten seconds (i.e., stick-slip phenomena). Because the high time-resolution strain monitoring is a preliminary experiment, the relationship between stick-slip phenomena and aqueous fluid is unclear. We will investigate that point in near future.