2022
DOI: 10.1029/2021jb022913
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Segmentation of Shallow Slow Slip Events at the Hikurangi Subduction Zone Explained by Along‐Strike Changes in Fault Geometry and Plate Convergence Rates

Abstract: Slow slip events (SSEs) are transient episodes of aseismic slip with longer durations and slower slip velocities than typical earthquakes. An SSE can generate millimeters to tens of centimeters of slip on a fault over periods of days to years (Schwartz & Rokosky, 2007). These events often occur at quasi-periodic intervals, spanning months to several years (Beroza & Ide, 2011), and play a significant role in the earthquake cycle where they occur, as they release part of the accumulated strain energy (e.g.,

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Cited by 8 publications
(4 citation statements)
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“…To save computational costs we set the background normal stress (σ) to 3 MPa, which is below the estimated range (10-30 MPa) along the shallow Hikurangi margin (Arnulf et al, 2021). We could scale up σ by reducing the constitutive parameters a and b so that aσ and bσ remain constant, and obtain the same results, as expected from Equations 1 and 2 (e.g., Perez-Silva et al, 2022).…”
Section: Fault Model Parametersmentioning
confidence: 65%
“…To save computational costs we set the background normal stress (σ) to 3 MPa, which is below the estimated range (10-30 MPa) along the shallow Hikurangi margin (Arnulf et al, 2021). We could scale up σ by reducing the constitutive parameters a and b so that aσ and bσ remain constant, and obtain the same results, as expected from Equations 1 and 2 (e.g., Perez-Silva et al, 2022).…”
Section: Fault Model Parametersmentioning
confidence: 65%
“…To save computational costs, we set σ = 3 MPa, which is below the estimated range (10-30 MPa) along the shallow Hikurangi margin (Arnulf et al, 2021). We could scale up σ by reducing the constitutive parameters a and b so that aσ and bσ remain constant, and obtain the same results, as expected from Equations 1 and 2 (e.g., Perez-Silva et al, 2022). 10, see Table 4.…”
Section: Fault Model Parametersmentioning
confidence: 99%
“…Within the rate‐and‐state friction (RSF) framework (Dieterich, 1979), SSEs commonly require rate‐weakening friction to nucleate, while different mechanisms (e.g., transition to rate‐strengthening friction at higher slip speeds, Shibazaki, 2003; dilatancy strengthening, Segall et al., 2010; transitional friction behavior, Liu & Rice, 2007) have been proposed to stabilize the growing unstable slip. These models, although successful in reproducing SSE characteristics (e.g., Dal Zilio et al., 2020; Li & Liu, 2016; Liu & Rice, 2009; Matsuzawa et al., 2013; Perez‐Silva et al., 2021, 2022; Shibazaki et al., 2012, 2019), do not account for the temporal variation in pore pressure nor the widespread occurrence of rate‐strengthening materials in slow slip regions (e.g., Bürgmann, 2018; Ikari et al., 2013; Saffer & Wallace, 2015). An alternative modeling approach, proposed by Perfettini and Ampuero (2008), suggests that transient slip is induced in rate‐strengthening conditions by external stress perturbations.…”
Section: Introductionmentioning
confidence: 99%
“…Various analytical solutions for displacement and stress caused by surface elements are readily available to represent a displacement discontinuity embedded within an elastic half-space [Comninou and Dundurs, 1975;Okada, 1992;Meade, 2007;Gimbutas et al, 2012;Nikkhoo and Walter, 2015]. A combination of rectangle and triangle surface elements can be used to shape realistic, non-planar fault geometries [e.g., Hori et al, 2004;Qiu et al, 2016;Li and Liu, 2017;Shibazaki et al, 2019;Perez-Silva et al, 2022]. The use of analytic solutions ensures high accuracy in simulating surface displacements by resolving the free surface exactly [Qiu et al, 2016;Wang and Barbot, 2020;Sathiakumar and Barbot, 2021].…”
Section: Plain Language Summarymentioning
confidence: 99%