Nonsystematic Rupture Directivity of Geothermal Energy Induced Microseismicity in Helsinki, Finland
暂无分享,去创建一个
[1] G. Hillers,et al. Induced Earthquake Source Parameters, Attenuation, and Site Effects From Waveform Envelopes in the Fennoscandian Shield , 2022, Journal of Geophysical Research: Solid Earth.
[2] Younghee Kim,et al. Rupture Directivity of the 2021 ML 2.2 Gwangyang, Korea, Microearthquake: Toward Resolving High-Resolution Rupture Process of a Small Earthquake , 2022, The Seismic Record.
[3] Zhigang Peng,et al. Complex Source Behaviors and Spatiotemporal Evolution of Seismicity During the 2015–2016 Earthquake Sequence in Cushing, Oklahoma , 2021, Journal of Geophysical Research: Solid Earth.
[4] D. Eaton,et al. Large‐Scale Fracture Systems Are Permeable Pathways for Fault Activation During Hydraulic Fracturing , 2021, Journal of Geophysical Research: Solid Earth.
[5] P. Heikkinen,et al. Earthquake catalog of induced seismicity recorded during and after stimulation of Enhanced Geothermal System in Helsinki, Finland , 2021 .
[6] Y. Ben‐Zion,et al. Detection Limits and Near‐Field Ground Motions of Fast and Slow Earthquakes , 2020, Journal of Geophysical Research: Solid Earth.
[7] G. Hillers,et al. The 2018 Geothermal Reservoir Stimulation in Espoo/Helsinki, Southern Finland: Seismic Network Anatomy and Data Features , 2020, Seismological Research Letters.
[8] G. Dresen,et al. Seismicity during and after stimulation of a 6.1 km deep Enhanced Geothermal System in Helsinki, Finland , 2020 .
[9] J. Boatwright,et al. Directivity of M 3.1 Earthquake near Anza, California and the Effect on Peak Ground Motion , 2020 .
[10] G. Atkinson,et al. Stress Drops and Directivity of Induced Earthquakes in the Western Canada Sedimentary Basin , 2019, Bulletin of the Seismological Society of America.
[11] S. Wiemer,et al. Rupture Process of the Mw 3.3 Earthquake in the St. Gallen 2013 Geothermal Reservoir, Switzerland , 2019, Geophysical Research Letters.
[12] M. Gutierrez,et al. Patterns in complex hydraulic fractures observed by true-triaxial experiments and implications for proppant placement and stimulated reservoir volumes , 2019, Journal of Petroleum Exploration and Production Technology.
[13] G. Dresen,et al. Controlling fluid-induced seismicity during a 6.1-km-deep geothermal stimulation in Finland , 2019, Science Advances.
[14] J. Verdon,et al. Investigating the role of elastostatic stress transfer during hydraulic fracturing-induced fault activation , 2019, Geophysical Journal International.
[15] Yihe Huang,et al. Do Injection‐Induced Earthquakes Rupture Away from Injection Wells due to Fluid Pressure Change? , 2019, Bulletin of the Seismological Society of America.
[16] Yajing Liu,et al. Earthquake Stress Drop in the Charlevoix Seismic Zone, Eastern Canada , 2018, Geophysical Research Letters.
[17] W. Fan,et al. Investigating microearthquake finite source attributes with IRIS Community Wavefield Demonstration Experiment in Oklahoma , 2018 .
[18] J. Renner,et al. Sensitivity of Full Moment Tensors to Data Preprocessing and Inversion Parameters: A Case Study from the Salton Sea Geothermal Field , 2018 .
[19] Chris Van Houtte,et al. Improved Model Fitting for the Empirical Green's Function Approach Using Hierarchical Models , 2018 .
[20] Rachel E. Abercrombie,et al. Earthquake Directivity, Orientation, and Stress Drop Within the Subducting Plate at the Hikurangi Margin, New Zealand , 2017 .
[21] P. Mai,et al. Induced seismicity provides insight into why earthquake ruptures stop , 2017, Science Advances.
[22] S. Wiemer,et al. The induced earthquake sequence related to the St. Gallen deep geothermal project (Switzerland): Fault reactivation and fluid interactions imaged by microseismicity , 2017 .
[23] V. Vavryčuk,et al. Moment Tensor Inversion Based on the Principal Component Analysis of Waveforms: Method and Application to Microearthquakes in West Bohemia, Czech Republic , 2017 .
[24] W. Ellsworth,et al. Stress drops of induced and tectonic earthquakes in the central United States are indistinguishable , 2017, Science Advances.
[25] G. Prieto,et al. Earthquake rupture below the brittle-ductile transition in continental lithospheric mantle , 2017, Science Advances.
[26] C. Ji,et al. Moment rate scaling for earthquakes 3.3 ≤ M ≤ 5.3 with implications for stress drop , 2016 .
[27] S. Shapiro,et al. Rupture directivity of fluid‐induced microseismic events: Observations from an enhanced geothermal system , 2016 .
[28] Rachel E. Abercrombie,et al. Variability of earthquake stress drop in a subduction setting, the Hikurangi Margin, New Zealand , 2016, Geophysical Journal International.
[29] Peter M. Shearer,et al. New perspectives on self‐similarity for shallow thrust earthquakes , 2016 .
[30] Grzegorz Kwiatek,et al. HybridMT: A MATLAB/Shell Environment Package for Seismic Moment Tensor Inversion and Refinement , 2016 .
[31] K. Imanishi,et al. Small Earthquakes Deviate from the Omega‐Square Model as Revealed by Multiple Spectral Ratio Analysis , 2016 .
[32] Valentin Gischig,et al. The importance of earthquake interactions for injection‐induced seismicity: Retrospective modeling of the Basel Enhanced Geothermal System , 2016 .
[33] M. Vallée,et al. Stress-drop variability of shallow earthquakes extracted from a global database of source time functions , 2016 .
[34] David Dempsey,et al. Collective properties of injection‐induced earthquake sequences: 1. Model description and directivity bias , 2016 .
[35] M. O'Sullivan,et al. A damage mechanics approach to the simulation of hydraulic fracturing/shearing around a geothermal injection well , 2016 .
[36] M. Ishii,et al. Inversion for rupture properties based upon 3-D directivity effect and application to deep earthquakes in the Sea of Okhotsk region , 2015 .
[37] V. Gischig. Rupture propagation behavior and the largest possible earthquake induced by fluid injection into deep reservoirs , 2015 .
[38] Agust Gudmundsson. Elastic energy release in great earthquakes and eruptions , 2014, Front. Earth Sci..
[39] Serge A. Shapiro,et al. Magnitudes of induced earthquakes and geometric scales of fluid-stimulated rock volumes , 2011 .
[40] G. Dresen,et al. Source Parameters of Picoseismicity Recorded at Mponeng Deep Gold Mine, South Africa: Implications for Scaling Relations , 2011 .
[41] R. Horne,et al. Investigation of injection-induced seismicity using a coupled fluid flow and rate/state friction model , 2011 .
[42] Won-Young Kim,et al. The 2002 M5 Au Sable Forks, NY, earthquake sequence: Source scaling relationships and energy budget , 2010 .
[43] R. Abercrombie,et al. Source parameters and rupture velocity of small M ≤ 2.1 reservoir induced earthquakes , 2009 .
[44] G. A. Prieto,et al. A Fortran 90 library for multitaper spectrum analysis , 2009, Comput. Geosci..
[45] G. Kwiatek. Relative source time functions of seismic events at the Rudna copper mine, Poland: estimation of inversion uncertainties , 2008 .
[46] S. Gibowicz,et al. Comparison of source parameters estimated in the frequency and time domains for seismic events at the Rudna copper mine, Poland , 2008 .
[47] B. Chiou,et al. Directivity in NGA Earthquake Ground Motions: Analysis Using Isochrone Theory , 2008 .
[48] Hiroo Kanamori,et al. Static and Dynamic Scaling Relations for Earthquakes and Their Implications for Rupture Speed and Stress Drop , 2004 .
[49] W. Ellsworth,et al. Apparent break in earthquake scaling due to path and site effects on deep borehole recordings , 2003 .
[50] B. Domański,et al. Source Time Function of Seismic Events at Rudna Copper Mine, Poland , 2002 .
[51] Ralph J. Archuleta,et al. The Three-Dimensional Dynamics of Dipping Faults , 2000 .
[52] Yoshiaki Hisada,et al. A Theoretical Omega-Square Model Considering the Spatial Variation in Slip and Rupture Velocity , 2000 .
[53] Dino Bindi,et al. Source parameters of small events using constrained deconvolution with empirical Green’s functions , 1999 .
[54] Hans-Peter Harjes,et al. Source parameters of injection-induced microearthquakes at 9 km depth at the KTB Deep Drilling site, Germany , 1998, Bulletin of the Seismological Society of America.
[55] Rachel E. Abercrombie,et al. Earthquake source scaling relationships from −1 to 5 ML using seismograms recorded at 2.5‐km depth , 1995 .
[56] C. Doll,et al. Source characterization and fault plane determination for MbLg = 1.2 to 4.4 earthquakes in the Charlevoix Seismic Zone, Quebec, Canada , 1995, Bulletin of the Seismological Society of America.
[57] J. Kakkuri,et al. On horizontal crustal strain in Finland , 1992 .
[58] Jim Mori,et al. Source parameters for small events associated with the 1986 North Palm Springs, California, earthquake determined using empirical Green functions , 1990 .
[59] Frank L. Vernon,et al. Rupture characteristics and tomographic source imaging of ML ∼ 3 earthquakes near Anza, southern California , 1986 .
[60] Charles S. Mueller,et al. Source pulse enhancement by deconvolution of an empirical Green's function , 1985 .
[61] J. Boatwright,et al. A spectral theory for circular seismic sources; simple estimates of source dimension, dynamic stress drop, and radiated seismic energy , 1980 .
[62] S. Hartzell. Earthquake aftershocks as Green's functions , 1978 .
[63] C. Bufe,et al. Shear-wave attenuation along the San Andreas fault zone in central California , 1975, Bulletin of the Seismological Society of America.
[64] J. Brune. Tectonic stress and the spectra of seismic shear waves from earthquakes , 1970 .
[65] W. E. Williams,et al. Green's Functions , 1970, Nature.
[66] N. A. Haskell. Total energy and energy spectral density of elastic wave radiation from propagating faults , 1964 .