日本地震学会2020年度秋季大会

講演情報

B会場

一般セッション » S09. 地震活動とその物理

[S09]PM-1

2020年10月30日(金) 13:00 〜 14:15 B会場

座長:尾鼻 浩一郎(海洋研究開発機構)、座長:小木曽 仁(気象研究所)

13:30 〜 13:45

[S09-20] 高精度震源決定による2016年ニュージーランドカイコウラ地震におけるプレート境界面と断層形状の関係

〇河村 優太1、松本 聡1、岡田 知己2、松野 弥愛2、飯尾 能久3、佐藤 将2、Bannister Stephen4、Ristau John4、Savage Martha5、Thurber Clifford6、Sibson Richard7 (1.九州大学、2.東北大学、3.京都大学、4.GNS Science、5.Victoria University of Wellington、6.University of Wisconsin - Madison、7.University of Otago)

On November 14, 2016, the Kaikoura earthquake (Mw. 7.8) occurred in northeastern South Island, New Zealand. The main characteristic of this earthquake is that the co-seismic rupture process of the main shock was composed of slip on many faults. Clark et al. (2017) pointed out that the aftershocks of both strike-slip and reverse fault types frequently occurred and more than 20 faults were ruptured during the main shock. Moreover, Cesca et al. (2017) proposed a simple model that the complex rupture proceeded on three major faults in the northern, central and southern areas based on the aftershock distribution, focal mechanisms, geodetic and seismic waveform inversion. Two previous studies have relocated aftershocks using double-difference techniques (Mouslopoulou et al., 2019; Lanza et al., 2019). However, in these studies, it was difficult to determine the fault geometry in detail because of the sparse seismic station density within about 50 km. In this research, we added phase data from seismic stations that we deployed before the main shock in order to improve the accuracy of hypocenter location. Furthermore, we apply the double-difference earthquake relocation algorithm (Waldhauser and Ellsworth, 2000) and time-domain waveform cross-correlation (Poupinet et al., 1984), which further enhance the precision of the hypocenter locations.

As a result, the variance of the hypocenter distribution is reduced and the depth is also concentrated to 15 km or less. There are 10-kilometer long clusters that mainly show a north-south-southwest orientation. Nine fault planes were found from the relocated aftershock distribution through a principal component analysis and bootstrap resampling method. The bottom of the aftershock distribution reveals a curved surface deepening in the southwest direction, which is parallel to the slab determined by Williams et al. (2013).