Several synthetic models are constructed to fit the first 40 sec of the transversely polarized displacement, as recorded at El Centro, of the April 9, 1968 Borrego Mountain earthquake. The modeling is done in the time domain using the response computed for a distributed set of point shear dislocations embedded in a layered half-space. The beginning 10 sec of the observed record is used to model the spatial and temporal distribution of faulting whereas the remaining portion is used to determine the upper crustal structure based on surface-wave periodicity. A natural depth criterion was provided by comparing the amplitude of the direct arrival with the surface-wave excitations. Trade-offs are found to exist between source models and velocity ...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
A least-squares point-by-point inversion of strong ground motion and teleseismic body waves is used ...
A least-squares point-by-point inversion of strong ground motion and teleseismic body waves is used ...
Several synthetic models are constructed to fit the first 40 sec of the transversely polarized displ...
Teleseismic P, SV, and SH waves recorded by the WWSS and Canadian networks from the 1971 San Fernand...
Teleseismic P, SV, and SH waves recorded by the WWSS and Canadian networks from the 1971 San Fernand...
Results from a synthetic seismogram analysis of the short-period P waves from the Borrego Mountain e...
The exact Cagniard-de Hoop solutions for a point dislocation in half-space are used to construct mod...
The exact Cagniard-de Hoop solutions for a point dislocation in half-space are used to construct mod...
The exact Cagniard-de Hoop solutions for a point dislocation in half-space are used to construct mod...
Strong-motion displacements, recorded at 33 km (IVC) and 36 km (ELC) from the November 4, 1976 Brawl...
Strong-motion displacements, recorded at 33 km (IVC) and 36 km (ELC) from the November 4, 1976 Brawl...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
Strong-motion displacements, recorded at 33 km (IVC) and 36 km (ELC) from the November 4, 1976 Brawl...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
A least-squares point-by-point inversion of strong ground motion and teleseismic body waves is used ...
A least-squares point-by-point inversion of strong ground motion and teleseismic body waves is used ...
Several synthetic models are constructed to fit the first 40 sec of the transversely polarized displ...
Teleseismic P, SV, and SH waves recorded by the WWSS and Canadian networks from the 1971 San Fernand...
Teleseismic P, SV, and SH waves recorded by the WWSS and Canadian networks from the 1971 San Fernand...
Results from a synthetic seismogram analysis of the short-period P waves from the Borrego Mountain e...
The exact Cagniard-de Hoop solutions for a point dislocation in half-space are used to construct mod...
The exact Cagniard-de Hoop solutions for a point dislocation in half-space are used to construct mod...
The exact Cagniard-de Hoop solutions for a point dislocation in half-space are used to construct mod...
Strong-motion displacements, recorded at 33 km (IVC) and 36 km (ELC) from the November 4, 1976 Brawl...
Strong-motion displacements, recorded at 33 km (IVC) and 36 km (ELC) from the November 4, 1976 Brawl...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
Strong-motion displacements, recorded at 33 km (IVC) and 36 km (ELC) from the November 4, 1976 Brawl...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
Spectral analysis of teleseismic body phases at several azimuths was used to determine the moment, ...
A least-squares point-by-point inversion of strong ground motion and teleseismic body waves is used ...
A least-squares point-by-point inversion of strong ground motion and teleseismic body waves is used ...