Numerically Calculated 3D Space-Weighting Functions to Image Crustal Volcanic Structures Using Diffuse Coda Waves
Metadatos
Mostrar el registro completo del ítemAutor
Pezzo, Edoardo del; Torre Vega, Ángel De La; Bianco, Francesca; Ibáñez Godoy, Jesús Miguel; Gabrielli, Simona; Siena, Luca DeEditorial
MDPI
Materia
Seismic attenuation Seismic coda Seismic scattering Diffusion Coda imaging
Fecha
2018-05-11Referencia bibliográfica
Del Pezzo, E. [et al.]. Numerically Calculated 3D Space-Weighting Functions to Image Crustal Volcanic Structures Using Diffuse Coda Waves. Geosciences 2018, 8, 175; doi:10.3390/geosciences8050175.
Patrocinador
This research was partly supported by the Projects TEC2015-68752 (MINECO/FEDER), TEC2015-68752 (KNOWAVES).Resumen
Seismic coda measurements retrieve parameters linked to the physical characteristics of
rock volumes illuminated by high frequency scattered waves. Space weighting functions (SWF)
and kernels are different tools that model the spatial sensitivity of coda envelopes to scattering
and absorption anomalies in these rock matrices, allowing coda-wave attenuation (Qcoda) imaging.
This note clarifies the difference between SWF and sensitivity kernels developed for coda wave
imaging. It extends the SWF previously developed in 2D to the third dimension by using radiative
transfer and the diffusion equation, based on the assumption that variations of Qcoda depend solely
on variations of the extinction length. When applied to active data (Deception Island, Antarctica),
3D SWF images strongly resemble 2D images, making this 3D extension redundant. On the other
hand, diffusion does not efficiently model coda waveforms when using earthquake datasets spanning
depths between 0 and 20 km, such as at Mount St. Helens volcano. In this setting, scattering
attenuation and absorption suffer tradeoffs and cannot be separated by fitting a single seismogram
energy envelope for SWF imaging. We propose that an approximate analytical 3D SWF, similar
in shape to the common coda kernels used in literature, can still be used in a space weighted
back-projection approach. While Qcoda is not a physical parameter of the propagation medium,
its spatially-dependent modeling allows improved reconstruction of crustal-scale tectonic and
geological features. It is even more efficient as a velocity independent imaging tool for magma
and fluid storage when applied to deep volcanism.