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 M (領域外・複数領域) » M-TT 計測技術・研究手法

[M-TT05] Cryoseismology - a new proxy for detecting surface environmental variations of the Earth -

2016年5月26日(木) 10:45 〜 12:15 202 (2F)

コンビーナ:*金尾 政紀(国立極地研究所)、坪井 誠司(海洋研究開発機構)、伊藤 武男(名古屋大学大学院環境学研究科附属 地震火山研究センター)、Wiens Douglas(Washington University in St Louis)、Anandakrishnan Sridhar(Penn State University)、Winberry Jeremy(Central Washington University)、Anderson Kent(Incorporated Research Institutions for Seismology)、座長:豊国 源知(東北大学 大学院理学研究科 地震・噴火予知研究観測センター)、伊藤 武男(名古屋大学大学院環境学研究科附属 地震火山研究センター)

12:00 〜 12:15

[MTT05-04] May 30, 2015 Bonin Islands, Japan deep earthquake (Mw7.8) recorded by broadband seismographic station on Greenland ice sheet

*坪井 誠司1中村 武史1 (1.海洋研究開発機構)

キーワード:deep earthquake, Greenland icesheet, theoretical seismograms

May 30, 2015 Bonin Islands, Japan earthquake (Mw 7.8, depth 679.9km GCMT) was one of the deepest earthquakes ever recorded. We apply the waveform inversion technique (Kikuchi & Kanamori, 1991) to obtain slip distribution in the source fault of this earthquake in the same manner as our previous work (Nakamura et al., 2010). We use 60 broadband seismograms of IRIS GSN seismic stations with epicentral distance between 30 and 90 degrees. The broadband original data are integrated into ground displacement and band-pass filtered in the frequency band 0.002-1 Hz. We use the velocity structure model IASP91 to calculate the wavefield near source and stations. We assume that the fault is squared with the length 50 km. We obtain source rupture model for both nodal planes with high dip angle (74 degree) and low dip angle (26 degree) and compare the synthetic seismograms with the observations to determine which source rupture model would explain the observations better. We calculate broadband synthetic seismograms with these source propagation models using the spectral-element method (Komatitsch & Tromp, 2001). We use new Earth Simulator system in JAMSTEC to compute synthetic seismograms using the spectral-element method. The simulations are performed on 7,776 processors, which require 1,944 nodes of the Earth Simulator. On this number of nodes, a simulation of 50 minutes of wave propagation accurate at periods of 3.8 seconds and longer requires about 5 hours of CPU time. Comparisons of the synthetic waveforms with the observation at Greenland ice sheet station, ICESG (epicentral distance 83.4 degree), show that the arrival time of pP wave calculated for depth 679km matches well with the observation, which demonstrates that the earthquake really happened below the 660 km discontinuity. In our present forward simulations, the source rupture model with the low-angle fault dipping is likely to better explain the observations.