Modeling the Contribution of Poroelastic Deformation to Postseismic Geodetic Signals
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[1] Y. Fukuda,et al. Probing the Poisson's ratio of poroelastic rebound following the 2011 Mw 9.0 Tohoku earthquake , 2018, Geophysical Journal International.
[2] A. Gualandi,et al. Poroelasticity and Fluid Flow Modeling for the 2012 Emilia-Romagna Earthquakes: Hints from GPS and InSAR Data , 2018, Geofluids.
[3] M. Hesse,et al. Modeling the poroelastic response to megathrust earthquakes: A look at the 2012 Mw 7.6 Costa Rican event , 2017 .
[4] T. Dixon,et al. Slow slip events in the early part of the earthquake cycle , 2017 .
[5] C. Kyriakopoulos,et al. Large and primarily updip afterslip following the 2012 Mw 7.6 Nicoya, Costa Rica, earthquake , 2017 .
[6] C. Kyriakopoulos,et al. Large and primarily updip afterslip following the 2012 M w 7.6 Nicoya, Costa Rica, earthquake: Afterslip From 2012 Nicoya Earthquake , 2017 .
[7] C. Bignami,et al. Aftershocks, groundwater changes and postseismic ground displacements related to pore pressure gradients: Insights from the 2012 Emilia‐Romagna earthquake , 2017 .
[8] T. Dixon,et al. Strain release at the trench during shallow slow slip: The example of Nicoya Peninsula, Costa Rica , 2017 .
[9] Hiroshi P. Sato,et al. Resolving depth-dependent subduction zone viscosity and afterslip from postseismic displacements following the 2011 Tohoku-oki, Japan earthquake , 2017 .
[10] Andrew T. T. McRae,et al. Firedrake , 2016, Mathematics of Planet Earth.
[11] David A. Ham,et al. An Algorithm for the Optimization of Finite Element Integration Loops , 2016, ACM Trans. Math. Softw..
[12] S. Schwartz,et al. Monitoring transient changes within overpressured regions of subduction zones using ambient seismic noise , 2016, Science Advances.
[13] T. Dixon,et al. Multiscale postseismic behavior on a megathrust: The 2012 Nicoya earthquake, Costa Rica , 2015 .
[14] H. Villinger,et al. Slow and delayed deformation and uplift of the outermost subduction prism following ETS and seismogenic slip events beneath Nicoya Peninsula, Costa Rica , 2015 .
[15] T. Dixon,et al. Earthquake and tsunami forecasts: Relation of slow slip events to subsequent earthquake rupture , 2014, Proceedings of the National Academy of Sciences.
[16] X. Kuang,et al. An integrated permeability‐depth model for Earth's crust , 2014 .
[17] Yan Hu,et al. Contributions of poroelastic rebound and a weak volcanic arc to the postseismic deformation of the 2011 Tohoku earthquake , 2014, Earth, Planets and Space.
[18] Agustan,et al. A comprehensive model of postseismic deformation of the 2004 Sumatra–Andaman earthquake deduced from GPS observations in northern Sumatra , 2014 .
[19] S. Owen,et al. Nicoya earthquake rupture anticipated by geodetic measurement of the locked plate interface , 2014 .
[20] S. Owen,et al. The 5 September 2012 Nicoya, Costa Rica Mw 7.6 earthquake rupture process from joint inversion of high‐rate GPS, strong‐motion, and teleseismic P wave data and its relationship to adjacent plate boundary interface properties , 2013 .
[21] Anders Logg,et al. Unified form language: A domain-specific language for weak formulations of partial differential equations , 2012, TOMS.
[22] Eric J. Fielding,et al. Fault slip models of the 2010–2011 Canterbury, New Zealand, earthquakes from geodetic data and observations of postseismic ground deformation , 2012 .
[23] Michael Manga,et al. Hydrological effects of the M W 7.1 Darfield (Canterbury) earthquake, 4 September 2010, New Zealand , 2012 .
[24] Timothy H. Dixon,et al. Active deformation near the Nicoya Peninsula, northwestern Costa Rica, between 1996 and 2010: Interseismic megathrust coupling , 2012 .
[25] Anders Logg,et al. Automated Solution of Differential Equations by the Finite Element Method: The FEniCS Book , 2012 .
[26] Sylvain Barbot,et al. A unified continuum representation of post-seismic relaxation mechanisms: semi-analytic models of afterslip, poroelastic rebound and viscoelastic flow , 2010 .
[27] Walter D. Mooney,et al. Poroelastic stress-triggering of the 2005 M8.7 Nias earthquake by the 2004 M9.2 Sumatra–Andaman earthquake , 2010 .
[28] Anders Logg,et al. DOLFIN: Automated finite element computing , 2010, TOMS.
[29] Paul Segall,et al. Earthquake and Volcano Deformation , 2010 .
[30] Christophe Geuzaine,et al. Gmsh: A 3‐D finite element mesh generator with built‐in pre‐ and post‐processing facilities , 2009 .
[31] Y. Fialko,et al. Hydrologic detection and finite element modeling of a slow slip event in the Costa Rica prism toe , 2009 .
[32] B. E. Shaw,et al. Afterslip and aftershocks in the rate‐and‐state friction law , 2007, physics/0703249.
[33] S. Ge,et al. Hydrodynamic response of subduction zones to seismic activity: A case study for the Costa Rica margin , 2006 .
[34] Eric J. Fielding,et al. Coseismic and Postseismic Slip of the 2004 Parkfield Earthquake from Space-Geodetic Data , 2006 .
[35] Yuri Fialko,et al. Evidence of fluid-filled upper crust from observations of postseismic deformation due to the 1992 Mw7.3 Landers earthquake , 2004 .
[36] Hugo Perfettini,et al. Postseismic relaxation driven by brittle creep: A possible mechanism to reconcile geodetic measurements and the decay rate of aftershocks, application to the Chi-Chi earthquake, Taiwan , 2004 .
[37] Paul Lundgren,et al. Geodetic and Seismic Constraints on some Seismogenic Zone Processes in Costa Rica , 2003 .
[38] Paul Segall,et al. Post-earthquake ground movements correlated to pore-pressure transients , 2003, Nature.
[39] Herbert F. Wang. Theory of Linear Poroelasticity with Applications to Geomechanics and Hydrogeology , 2000 .
[40] Kenneth W. Hudnut,et al. Poroelastic rebound along the Landers 1992 earthquake surface rupture , 1998 .
[41] T. Dixon,et al. Seismogenic zone structure beneath the Nicoya Peninsula, Costa Rica, from three‐dimensional local earthquake P‐ and S‐wave tomography , 2006 .