Coseismic slip gradient at the western terminus of the 1920 Haiyuan Mw 7.9 earthquake
Introduction
Fault geometrical complexities such as bends, branches and stepovers are common in strike-slip fault systems, separating the faults into multiple segments (King and Nabelek, 1985; Sibson, 1985). Faults comprising several disjointed segments can behave as distinct faults rupturing separately in individual earthquakes (e.g., Schwartz and Coppersmith, 1984; Wesnousky, 1994; Zhang et al., 1999) or coalesce to rupture simultaneously in large, multifault events (Elliott et al., 2015;; Hamling et al., 2017; Liu-Zeng et al., 2009; Sieh et al., 1993; Wesnousky, 1988, 2006;; Zhang et al., 1999). Earthquake ruptures often stop at geometrical complexities on faults (Wesnousky, 1988, Wesnousky, 2006). Wesnousky’s (2006) compilation of worldwide historical strike-slip earthquake rupture maps indicates that stepovers play a crucial role in controlling rupture length, constituting 2/3 of historical rupture endpoints, and there is a limiting dimension of fault stepover (3–4 km). An analysis of mapped surface ruptures for relationships between geometrical discontinuities in fault traces and earthquake rupture extents by Biasi and Wesnousky (2016) shows that ~90% of ruptures have at least one end at a mappable discontinuity, either a fault end or a step of 1 km or greater, especially along strike-slip faults. Harris and Day's (1993) numerical simulation also shows that a strike-slip rupture is unlikely to jump a stepover wider than 5 km. The basic controls on whether a rupture will stop at a step, however, are also related to the slip-behavior as it approaches the stepover (Elliott et al., 2009; Liu and Duan, 2016;; Oglesby, 2008). It is suggested that earthquake ruptures can jump through stepovers when their slip near the fault segment tip decreases rapidly and cannot propagate through fault stepovers when their slip decreases gradually, according to the compilation and comparative analysis of slip distributions from Elliott et al. (2009).
The 1920 Mw 7.9 Haiyuan earthquake was the latest major earthquake on the Haiyuan fault, forming a ~237-km-long surface rupture (Deng et al., 1986; IGCEA and NBCEA, 1990). This rupture broke through multiple stepovers along the fault while stopping at the ~4 km-wide Jingtai pull-apart basin at the western endpoint (Deng et al., 1986; IGCEA and NBCEA, 1990). However, why the surface rupture could break through multiple stepovers along the fault while stopping at the special structure of the left-stepping releasing Jingtai basin remains unclear. Therefore, a study on the mechanism of rupture cessation at the western stepover during the 1920 Haiyuan earthquake could provide important and valuable information for our understanding of the dynamic controls on rupture propagation and arrest.
To understand the interactions of earthquake ruptures and fault complexity, we need a detailed map of rupture geometry, coseismic slip, and its gradient along strike in the vicinity of the rupture endpoint (Wesnousky, 2006; Elliott et al., 2009). The quantification of slip data is usually based on reconstructing offset landforms along a fault trace, such as deflected stream channels, alluvial fans, and offset ridgelines (Sieh, 1978; McGill and Sieh, 1991). For the 1920 Haiyuan earthquake, such data were collected through field investigation in the 1980s (Deng et al., 1986; IGCEA and NBCEA, 1990). This early work provides valuable data but also poses some difficulties. The investigation was conducted 60 years after the earthquake and before the era of high-resolution satellite images and topographic maps (IGCEA and NBCEA, 1990). The surface rupture map was simplified, and offsets were measured with an old-fashioned simple measuring tape; thus, the numbers lack precise coordinates for coseismic slip measurements to be checked with reliability and uncertainty (IGCEA and NBCEA, 1990). Recent advances in remotely sensed high-resolution topography and optical imaging have improved upon this approach; for example, light detection and ranging (LiDAR) systems can acquire high-resolution topographic data, enabling the detailed characterization of landforms and measurements of small displacements (e.g., Arrowsmith and Zielke, 2009; Behr et al., 2010; Chen et al., 2018; Frankel and Dolan, 2007; Liu et al., 2013; Oskin et al., 2012; Ren et al., 2016; Salisbury et al., 2012; Zielke et al., 2010; 2012; Zielke and Arrowsmith, 2012).
In this study, we present slip measurements based on a high-resolution digital elevation model (DEM) near the western end of the 1920 Haiyuan earthquake rupture. We calculate the coseismic slip gradient as the rupture approached the Jingtai releasing stepover. This value is compared with the dataset of worldwide historical earthquakes compiled by Elliott et al. (2009). We also investigate the possible westward extension section of the surface rupture of the 1920 Mw 7.9 Haiyuan earthquake. In addition, we compare the section with discontinuities in the line-of-sight (LOS) velocity field revealed by synthetic aperture radar interferometry (InSAR) on the northern boundary of the Jingtai basin with the extension segment of the Haiyuan fault to discuss additional factors that stopped the earthquake rupture as it approached the releasing stepover.
Section snippets
Seismotectonic setting
The Indo-Asia collision has formed a series of large left-lateral strike-slip faults in and around the Tibetan Plateau, such as the Altyn Tagh fault, Haiyuan fault, Kunlun fault, Karakoram fault and Xianshuihe-Xiaojiang fault (Tapponnier and Molnar, 1977; Tapponnier et al., 2001). The Haiyuan fault is a major left-lateral strike-slip fault on the margin of the northeastern Tibetan Plateau and plays an important role in accommodating the deformation as a consequence of the collision and poses a
Methods
The main methods of obtaining high-resolution topographic data are LiDAR and high-resolution optical imagery. The ability to generate high-resolution “bare-earth” DEMs through the removal of vegetation coverage has become one of the most attractive benefits of airborne LiDAR, enabling the fine-scale mapping and surveying of fault geometry and displaced geomorphic markers (Barth et al., 2012; Zielke et al., 2012). For high-resolution optical imagery, tectono-geomorphic investigations can be
Observations and results
The western terminus of the 1920 rupture was located at point M from field investigation in the 1980s (Fig. 7d; Deng et al., 1986; IGCEA and NBCEA, 1990). The fault extends to the Jingtai basin, where the trace is obliterated due to building construction in the village. Topographically, there is a ~3 m scarp in the extension section of the fault (Fig. 7e&g&h) and a ~500 m-long ditch man-dug along an original scarp in the 1970s by local residents coincides with and lies exactly along the
Interpretation
The 1920 Mw 7.9 Haiyuan earthquake rupture broke through multiple restraining stepovers (PU1-PU2) and releasing stepovers (PB1-PB8) along the fault and finally ended at the ~4 km-wide Jingtai pull-apart basin (releasing stepover) at the western end (Deng et al., 1986; IGCEA and NBCEA, 1990). What are the factors that prevented the 1920 rupture from continuing to propagate westward and jump the Jingtai pull-apart basin at the western end? Is the Jingtai pull-apart basin a persistent barrier to
Discussion
We have analysed various factors (e.g., slip gradient, geometric complexity and aseismic creep) affecting the termination of the 1920 earthquake rupture at the western end. It is possible that a certain factor dominated or that the combined impact of these factors terminated the 1920 earthquake rupture. Are the above-mentioned multiple factors met during other earthquakes, and will future earthquake ruptures also stop in the Jingtai basin?
The offset value of the most recent event (1920 Mw 7.9
Conclusion
The factors noted in this paper could help assess the reasons why the 1920 rupture was impeded/arrested by the Jingtai basin (releasing stepover) at the western end. Currently, multiple factors are considered to have blocked the 1920 rupture, such as geometric complexity, slip gradients and aseismic creep. The coseismic slip gradients calculated in this study have high values for a 4 km-wide releasing stepover compared to the dataset of worldwide earthquakes compiled by Elliott et al. (2009),
CRediT authorship contribution statement
Longfei Han: Conceptualization, Methodology, Software, Validation, Formal analysis, Investigation, Writing – original draft, Writing – review & editing. Jing Liu-Zeng: Conceptualization, Validation, Formal analysis, Resources, Writing – original draft, Writing – review & editing. Wenqian Yao: Software, Formal analysis, Investigation, Writing – review & editing. Yanxiu Shao: Software, Writing – review & editing. Zhaode Yuan: Software, Writing – review & editing. Yan Wang: Writing – review &
Declaration of competing interest
The authors declare that they have no known competing financial interests or personal relationships that could have appeared to influence the work reported in this paper.
Acknowledgements
This work is supported jointly by the grants of State Key Laboratory of Earthquake Dynamics, China Earthquake Administration (No. LED2017A01), the National Natural Science Foundation of China (U1839203, 41802228, 42011540385). We thank the associate editor and two anonymous reviewers for their constructive comments that greatly improve this manuscript.
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