日本地球惑星科学連合2023年大会

講演情報

[E] オンラインポスター発表

セッション記号 S (固体地球科学) » S-IT 地球内部科学・地球惑星テクトニクス

[S-IT16] 地球深部科学

2023年5月26日(金) 09:00 〜 10:30 オンラインポスターZoom会場 (2) (オンラインポスター)

コンビーナ:土屋 旬(愛媛大学地球深部ダイナミクス研究センター)、太田 健二(東京工業大学理学院地球惑星科学系)、河合 研志(東京大学大学院理学系研究科地球惑星科学専攻)、飯塚 毅(東京大学)

現地ポスター発表開催日時 (2023/5/25 17:15-18:45)

09:00 〜 10:30

[SIT16-P02] The direction of mantle flow beneath Thailand inferred from shear wave splitting measurements

*Tarudee Autaijaratrasmee1Satoru Tanaka2Kenji Kawai1Sutthipong Noisagool3 (1.Department of Earth and Planetary Science, School of Science, The University of Tokyo, Hongo 7-3-1, Bunkyo, Tokyo 113-0033, Japan、2.Research Institute for Marine Geodynamics (IMG) Volcanoes and Earth’s Interior Research Center (VERC) Geophysical Research Group, Japan Agency for Marine-Earth Science and Technology、3.Department of Physics, Mahidol University, 999 Phutthamonthon Sai 4 Rd, Salaya, Phutthamonthon District, Nakhon Pathom 73170, Thailand)

キーワード:Mantle flow, Shear wave splitting, Anisotropy, Transverse energy minimization method

We infer the anisotropic properties of the mantle beneath Thailand based on shear wave splitting analyses. The magnitude of anisotropy is quantified by the travel time difference (dt) between the fast and slow shear waves. The fast axis orientation of anisotropic minerals is related to the angle (φ) between the P-wave and the fast shear wave. We made a Matlab code based on the transverse energy minimization method (Silver and Chan, 1991) to infer dt and φ. To validate the code, we compared our results with Yu et al. (2017) result. The graph after minimization, the particle motion, and the fast and slow shear waves before time shift delay time(dt), are the same. So, we applied it to the data from Incorporated Research Institutions for Seismology (IRIS) seismic data for 3 stations in Thailand, Chiang Mai station (CHTO; 18.8140°N, 98.9440°E), Chiang Mai station (CMMT; 18.8128°N, 98.9476°E), and Phuket station (PKDT; 7.8464°N, 98.3230°E). We got preliminary results for CHTO 3 events, CMMT 8 events, and PKDT 1 event as follows: dtCHTO = 2.98 ± 0.25 s and φCHTO = 49.26 ± 4.64°, dtCMMT = 2.18 ± 0.82 s and φCMMT = 79.47 ± 21.25°, and dtPKDT = 1.93 s and φPKDT = -2.15°. But the results are not good enough because the data set was a small size and the phases were not suitable to use the method to find φ and dt. Therefore, we are analyzing the data observed by the Thai Seismic Array (TSAR) Project which are suitable phases to investigate the more detailed anisotropic structure in the upper mantle beneath Thailand. We will show the results and discuss their geophysical interpretation in the presentation.