EGU23-8201, updated on 10 Jan 2024
https://doi.org/10.5194/egusphere-egu23-8201
EGU General Assembly 2023
© Author(s) 2024. This work is distributed under
the Creative Commons Attribution 4.0 License.

Does transient pore-pressure diffusion drive upper-plate aftershocks following megathrust earthquakes?

Carlos Peña1, Oliver Heidbach1,2, Bernd Schurr1, Sabrina Metzger1, Marcos Moreno3, Onno Oncken1,4, and Claudio Faccenna1,5
Carlos Peña et al.
  • 1Helmholtz Centre Potsdam, GFZ German Research Centre for Geosciences, Potsdam, Germany (carlosp@gfz-potsdam.de)
  • 2Institute of Applied Geosciences, Technical University Berlin, Germany
  • 3Departamento de Geofísica, Universidad de Concepción, Chile
  • 4Department of Earth Sciences, Freie Universität Berlin, Berlin, Germany
  • 5Dipartimento di Scienze, Università Roma Tre, Rome, Italy

Aftershocks are a time-dependent (exponential decay) phenomenon in the aftermath of large earthquakes. In subduction zones, those occurring in the upper plate are of special concern given their potential seismic hazard, as they may produce substantial surface shaking close to highly populated cities. Therefore, the understanding of the mechanisms that drive upper-plate aftershocks is of utmost importance to improving seismic hazard assessment. Transfer of static coseismic stresses has been commonly proposed to explain this; however, they fail to explain their exponential decay over time. This time-dependency is observed in postseismic geodetic measurements, suggesting that the processes that control the postseismic surface deformation also govern or at least are involved in the generation of upper-plate aftershocks. Here, the postseismic surface deformation is dominated by aseismic slip along the fault interface (afterslip), non-linear viscoelastic relaxation in the lower crust and upper mantle, and pore-pressure diffusion in the crust. Despite great research efforts, however, the key driver remains elusive.

In this study, we investigate which postseismic mechanism mainly controls the occurrence of aftershocks in the upper plate in subduction zones using the 2014 Mw=8.1 Iquique earthquake, northern Chile, as a study case. We employ a 4D numerical forward model to simulate the transient poroelastic and non-linear viscoelastic relaxation, whose contributions are subtracted from the cumulative Global Navigation Satellite System (GNSS) measurements to then invert for afterslip. Using realistic rock material properties, we first show that this approach explains the surface displacements during the first nine months of postseismic deformation recorded by continuous GNSS. For the same period, we then compute the spatiotemporal Coulomb Failure Stress changes (ΔCFS) that result from individual postseismic processes and compare them with the upper-plate aftershocks using a high-resolution seismicity catalog and focal mechanisms. We show for the first time that the ΔCFS produced by pore-pressure diffusion induced by the mainshock are unambiguously better correlated in space and time with the increase in upper-plate aftershocks than those from afterslip or non-linear viscous relaxation. In addition, pore-pressure diffusion lowers the effective normal stress of the stress tensor more effectively, while its resulting ΔCFS are relatively independent of the fault orientation. The latter would also explain the diversity of faulting styles in the upper plate exhibited by focal mechanisms following the 2014 Iquique earthquake and other subduction zone earthquakes. Our findings provide new insights into the link between pore-pressure diffusion and upper-plate deformation in subduction zones with implications for time-dependent seismic hazard.

How to cite: Peña, C., Heidbach, O., Schurr, B., Metzger, S., Moreno, M., Oncken, O., and Faccenna, C.: Does transient pore-pressure diffusion drive upper-plate aftershocks following megathrust earthquakes?, EGU General Assembly 2023, Vienna, Austria, 23–28 Apr 2023, EGU23-8201, https://doi.org/10.5194/egusphere-egu23-8201, 2023.