Japan Geoscience Union Meeting 2021

Presentation information

[J] Poster

S (Solid Earth Sciences ) » S-CG Complex & General

[S-CG50] Dynamics in mobile belts

Thu. Jun 3, 2021 5:15 PM - 6:30 PM Ch.15

convener:Yukitoshi Fukahata(Disaster Prevention Research Institute, Kyoto University), Hikaru Iwamori(Earthquake Research Institute, The University of Tokyo), Kiyokazu Oohashi(Graduate School of Sciences and Technology for Innovation, Yamaguchi University)

5:15 PM - 6:30 PM

[SCG50-P07] Characteristic of fault geometry and the subducting plate boundary in the focal area of the 2016 Mw7.8 Kaikoura earthquake, New Zealand inferred from high precision aftershock distribution

*Yuta Kawamura1, Satoshi Matsumoto1, Tomomi Okada2, Miu Matsuno2, Yoshihisa Iio3, Tadashi Sato2, Stephen Bannister4, John Ristau4, Martha Savage5, Richard Sibson6 (1.Kyushu University, 2.Tohoku University, 3.Kyoto University, 4.GNS Science, 5.Victoria University of Wellington, 6.University of Otago)

Keywords:Kaikoura Earthquake, New Zealand, high precision aftershock distribution, fault geometry, plate boundary

On 14 November 2016, in the northeast region of South Island, New Zealand, the Kaikoura earthquake (Mw 7.8) occurred. One of the main characteristics of this event, which is pointed out by previous studies, is the complexity of the rupture process involved with several faults. Our temporary observation group had installed more than 70 sites surrounding the target area before the mainshock and it has successfully recorded the mainshock and the aftershocks. In this study, we applied a double-difference relocation algorithm (Waldhauser and Ellsworth, 2000) to the dense observations and we determined fault geometries based on the high precision hypocenter distribution.
In order to evaluate the fault structure quantitatively, we employed multivariate analysis and a statistical method used in Yukutake and Iio (2017). As a result, we identified 11 fault planes in total. In particular, one of them is the fault where the rupture of the Kaikoura earthquake initiated, which is consistent with the structure shown by other studies and the nodal plane of the mainshock focal mechanism. Furthermore, the bottom of the aftershock distribution in the northern area reveals a curved surface deepening towards the northwest direction. The result is almost parallel to, but approximately 3 km above, the slab interface determined by Williams et al. (2013). We detected many aftershocks in reverse fault type above this interface, which showed similarity in dip angle of the events to the interface. We consider whether the curved surface could represent the top of the subducting slab, or another type of interface.