日本地球惑星科学連合2016年大会

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セッション記号 S (固体地球科学) » S-CG 固体地球科学複合領域・一般

[S-CG63] 変動帯ダイナミクス

2016年5月23日(月) 15:30 〜 17:00 A08 (アパホテル&リゾート 東京ベイ幕張)

コンビーナ:*深畑 幸俊(京都大学防災研究所)、重松 紀生(独立行政法人産業技術総合研究所活断層・火山研究部門)、加藤 愛太郎(名古屋大学大学院環境学研究科)、岩森 光(海洋研究開発機構・地球内部物質循環研究分野)、池田 安隆(東京大学大学院理学系研究科地球惑星科学専攻)、竹下 徹(北海道大学大学院理学院自然史科学専攻)、座長:西村 卓也(京都大学防災研究所)、小林 健太(新潟大学理学部地質科学科)

15:45 〜 16:00

[SCG63-20] 新潟ー神戸ひずみ集中帯における定常的プレート変形の意義

*鷺谷 威1,2Meneses Angela2 (1.名古屋大学減災連携研究センター、2.名古屋大学大学院環境学研究科)

キーワード:プレート内変形、非弾性変形、地殻ひずみ速度

We found a persistent localized contraction along the Niigata-Kobe Tectonic Zone (NKTZ) before and after the 2011 Tohoku-oki earthquake through an analysis of GEONET coordinate data (Menese-Gutierrez and Sagiya, 2016). This persistent pattern is identified as short-wavelength components in the strain rate pattern after removing the long-wavelength components. Persistency of deformation pattern under both interseismic and postseismic periods indicates that the localized contraction results from aseismic process driven by the tectonic stress field. Strain rate of this localized contraction is about 0.06 ppm/year, generally consistent with geologically estimated strain rate (Wesnousky et al., 1982, Sato, 1989). The localized pattern can be reproduced by ~10mm/year aseismic slip on a fault cutting the crust up to the depth of a few km. This implies inelastic processes have significant contribution in the crustal deformation of the Japanese island arc. Similar inelastic deformation is expected for other fault zones. However, slip rate of major active faults are smaller and the deeper locking depth makes associated deformation pattern much broader. Thus it is more difficult to detect related signals with a similar approach. The long-wavelength components in the strain rate pattern are considered to be elastic deformation caused by interaction at the plate boundary. Since our precise geodetic observation is limited for the last 20 years, we have not figured out how elastic strain accumulation and release are balanced through an earthquake cycle. Modeling effort of earthquake cycles with realistic lithospheric structure to reproduce the observed deformation pattern is essential to solve the problem.