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Creators/Authors contains: "Meade, Brendan J"

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  1. Geometric moment is accumulated and released throughout the earthquake cycle and can be imaged over both co- and inter-seismic time intervals with geodetic data. Recent dynamic earthquake cycle models have shown that substantial coseismic slip may occur in regions that exhibit low levels of moment accumulation during decadal-scale pre-earthquake epochs. We estimate that <1% of the region that slipped coseismically during the 2024 MW = 7.1 Hyuganada Sea (offshore southeastern Japan) earthquake was co-located with a region of pre-event moment accumulation. This stands in contrast with the behavior of the 2011 MW = 9.1 Tohoku-Oki(offshore northeastern Japan) earthquake, where ∼98% of the coseismic rupture area was co-located with pre-seismic moment accumulation. This co-location of coseismic slip and pre-seismic moment release proximal to the 2024 Hyuganada Sea earthquake serves as a real-world observation consistent with a novel theoretical prediction and is consistent with a perspective that decadal-scale pre-earthquake coupling estimates may provide snapshots of a highly time-variable fault system behavior, and may not necessarily serve as diagnostic identifiers of regions facing short-term earthquake hazard. 
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    Free, publicly-accessible full text available April 3, 2026
  2. Abstract Following large earthquakes, viscoelastic stress relaxation may contribute to postseismic deformation observed at Earth's surface. Mechanical representations of viscoelastic deformation require a constitutive relationship for the lower crust/upper mantle material where stresses are diffused and, for non‐linear rheologies, knowledge of absolute stress level. Here, we describe a kinematic approach to representing geodetically observed postseismic motions that does not require an assumed viscoelastic rheology. The core idea is to use observed surface motions to constrain time‐dependent displacement boundary conditions applied at the base of the elastic upper crust by viscoelastic motions in the lower crust/upper mantle, approximating these displacements as slip on a set of dislocation elements. Using three‐dimensional forward models of viscoelastically modulated postseismic deformation in a thrust fault setting, we show how this approach can accurately represent surface motions and recover predicted displacements at the base of the elastic layer. Applied to the 1999 Chi‐Chi (Taiwan) earthquake, this kinematic approach can reproduce geodetically observed displacements and estimates of the partitioning between correlated postseismic deformation mechanisms. Specifically, we simultaneously estimate afterslip on the earthquake source fault that is similar to previous estimates, along with slip on dislocations at the base of the elastic layer that mimic predictions from viscous stress dissipation models in which viscosity is inferred to vary three‐dimensionally. A use case for the dislocation approach to modeling viscoelastic deformation is the estimation of spatiotemporally variable fault slip processes, including across sequential interseismic phases of the earthquake cycle, without assuming a lower crust/upper mantle rheology. 
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    Free, publicly-accessible full text available August 1, 2026
  3. Abstract Geologic and geodetic observations provide constraints on tectonic and earthquake cycle kinematics. Block models offer one approach to integrating the effects of plate rotations, elastic strain accumulation, applied basal displacements, internal block strain, and idealized pressure sources. Here, we describe the construction of block models where spatially variable slip rates are parameterized by distance‐weighted eigenmodes operating over meshes of triangular dislocation elements. This dimensionally reduced model is recast as a quadratic programming problem with upper and lower bounds on both geologic fault slip rates and spatially variable slip deficit rates. We propose iterating over successive quadratic programming estimates with evolving slip rate bounds to find a solution consistent with specified coupling at all points on geometrically complex fault surfaces. 
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    Free, publicly-accessible full text available July 1, 2026