日本地震学会2019年度秋季大会

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ポスター会場(3日目)

一般セッション » S08. 地震発生の物理

S08P

2019年9月18日(水) 13:00 〜 14:30 P会場 (時計台国際交流ホールII・III)

13:00 〜 14:30

[S08P-01] 2018年11月11日東アフリカ・マヨッテ島付近の単振動地震 -イラン広帯域地震観測網による観測ー

サデギ ホセイン1、*鈴木 貞臣2 (1. フェルドウシ大学マッシャド 、理学部地質学科、イラン、2. (公財)地震予知総合研究振興会、東濃地震科学研究所)

The 11 November 2018 Mayotte event was first introduced in the media by Maya Wei-Haas (2018) on National Geographic Magazine as a strange earthquake of which seismic waves were recorded by instruments around the world, but unusually nobody felt them. The Mayotte event in the absence of body waves caused long-period surface waves traveling around the globe. Tono Research Institute of Earthquake Science recorded the data with the broadband seismometer (STS-1) and gravimeter (gPhone) installed in Mizunami (Murakami et al., 2019). The records by Iranian broadband stations clearly showed the long period seismic signals around 10 (UTC) on November 11, 2018. We studied records by 28 stations (Figure 1) distributed throughout the country. Among them, 26 stations were operated by National Center of Broadband Seismic Network of Iran, while two other stations were operated by the Ferdowsi University of Mashhad. Since the frequency content of Fourier amplitude spectra appeared the signal of the surface waves as a peak around 0.06 Hz, we applied a bandpass filter of 0.05-0.07 Hz to the waveform data. To separate Rayleigh from love in surface waves, the filtered horizontal components were rotated to the radial and transverse components based on an assumed epicenter location at the latitude of 12.7S and longitude of 45.4E degrees. The stations considered as an array and the investigation was carried out in two ways. First, the position of each station was taken as the reference point of the array coordinate, and arrival delay times at the other stations relative to the reference were calculated. The phase velocity and the back-azimuth of each station were estimated through the least-square regression method. The estimated back azimuths were within 13 degrees from the back azimuths from the assumed epicenter. The average phase velocity for Rayleigh (Figure 2a) and Love phases (Figure 2b) are calculated as 3.31 and 2.97 km/sec, respectively. Second, we applied semblance analysis to six stations (red triangles in Fugure 1) with the shortest spacing distances. However, the distance between the adjacent stations relative to the signal wavelength was not enough short to prevent spatial aliasing. Nevertheless, the interesting was that the semblance results were different for radial and transverse components.

(References)
Maya Wei-Haas (2018) Strange waves rippled around the world, and nobody knows why, National Geographic, published November 28, 2018.
Murakami O., Tanaka T., and Asai Y. (2019) Observation of the extremely monotonic seismic waves generated on November 11, 2018 at the Tono Research Institute of Earthquake Science, Report of the Tono Research Institute of Earthquake Science, Seq. No.42, 17-22 (in Japanese).