日本地球惑星科学連合2022年大会

講演情報

[J] 口頭発表

セッション記号 S (固体地球科学) » S-SS 地震学

[S-SS07] 地震発生の物理・断層のレオロジー

2022年5月23日(月) 13:45 〜 15:15 105 (幕張メッセ国際会議場)

コンビーナ:大谷 真紀子(東京大学地震研究所)、コンビーナ:岡崎 啓史(海洋研究開発機構)、奥脇 亮(筑波大学生命環境系山岳科学センター)、コンビーナ:金木 俊也(京都大学防災研究所)、座長:金木 俊也(京都大学防災研究所)、岡崎 啓史(海洋研究開発機構)

13:45 〜 14:00

[SSS07-01] 高変成度白亜紀付加体に産する礫質砂岩起源のマイロナイト

★招待講演

*山口 飛鳥1山本 一平1中村 佳博2針金 由美子2奥田 花也1 (1.東京大学大気海洋研究所、2.産業技術総合研究所)

The Kerama formation in the Kerama Islands, the Ryukyu Arc, located at the southwestern end of the Shimanto Belt, has a maximum temperature of 470-530°C. Presence of greenstones intruded into the clastic rocks is considered to record 100-90 Ma ridge subduction along the Ryukyu Arc (Yamamoto et al., this meeting). In the Kerama formation, foliation of greenstone, sandstone, and pelitic phyllite is parallel to bedding plane and dips SW in general. Stretching mineral lineations and fibers of layer-parallel quartz veins on the foliation exhibit NW–SE trend. Axes of asymmetric folds observed in pelitic phyllite show NE–SW trend, suggesting top-to-SE thrusting shear. Fold axes are perpendicular to stretching lineations. High-angle normal faults branching from low-angle normal fault are found in pelitic phyllite. These deformation features are classified into three deformation stages: D1 (underthrusting), D2 (underplating) and D3 (exhumation), respectively.
Strongly deformed rocks of D2 stage originated from conglomeratic sandstone occur in the Kerama Formation. The deformed rocks show myronitic texture with shear bands of fine-grained quartz, and such rocks have not reported from other areas of the Shimanto Belt. Here we call it conglomeratic sandstone mylonite.
We performed SEM-EBSD analysis of the crystallographic preferred orientation of recrystallized quartz in the conglomeratic sandstone mylonite. The EBSD patterns of most of the samples show random fabric, but some shows a type II crossed girdle fabric. The deformation temperature was estimated as 530°C according to the thermometer of Faleiros et al. (2017), and differential stress was estimated to be 27 MPa by the piezometer of Cross et al. (2016). These values are consistent with flow law of quartz (Hirth et al., 2001).
In the Shimanto Belt in Kyushu, Palazzin et al. (2016) reported that plastic deformation of quartz begins at about 300°C. Considering the temperature conditions, the strength of the subduction plate boundary may be primarily controlled by plastic deformation of quartz at temperatures of ~300-530°C.