The three-dimensional P and S wave structure of Redoubt Volcano, Alaska,
and the underlying crust to depths of 7-8 km is determined from 6219
P wave and 4008 S wave first-arrival times recorded by a 30-station
seismograph network deployed on and around the volcano. First-arrival
times are calculated using a finite-difference technique, which allows
for flexible parameterization of the slowness model and easy inclusion
of topography and source-receiver geometry. The three-dimensional
P wave velocity structure and hypocenters are determined simultaneously,
while the three-dimensional S wave velocity model is determined using
the relocated seismicity and an initial S wave velocity model derived
from the P wave velocity model assuming an average Vp/Vs ratio of
1.78. Convergence is steady with approximately 73\% and 52\% reduction
in P and S wave arrival time RMS, respectively, after 10 iterations.
The most prominent feature observed in the three-dimensional velocity
models derived for both P and S waves is a relative low-velocity,
near-vertical, pipelike structure approximately 1 km in diameter
that extends from 1 to 6 km beneath sea level. This feature aligns
axially with the bulk of seismicity and is interpreted as a highly
fractured and altered zone encompassing a magma conduit. The velocity
structure beneath the north flank of the volcano between depths of
1 and 6 km is characterized by large lateral velocity variations.
High velocities within this region are interpreted as remnant dikes
and sills and low velocities as regions along which magma migrates.
No large low-velocity body suggestive of a magma chamber is resolved
in the upper 7-8 km of the crust.
%0 Journal Article
%1 benz_etal:1996
%A Benz, H. M.
%A Chouet, B. A.
%A Dawson, P. B.
%A Lahr, J. C.
%A Page, R. A.
%A Hole, J. A.
%D 1996
%J Journal of Geophysical Research
%K geophysics seismology
%N B4
%P 8111--8128
%R 10.1029/95JB03046
%T Three-dimensional P and S wave velocity structure of Redoubt Volcano,
Alaska
%U http://dx.doi.org/10.1029/95JB03046
%V 101
%X The three-dimensional P and S wave structure of Redoubt Volcano, Alaska,
and the underlying crust to depths of 7-8 km is determined from 6219
P wave and 4008 S wave first-arrival times recorded by a 30-station
seismograph network deployed on and around the volcano. First-arrival
times are calculated using a finite-difference technique, which allows
for flexible parameterization of the slowness model and easy inclusion
of topography and source-receiver geometry. The three-dimensional
P wave velocity structure and hypocenters are determined simultaneously,
while the three-dimensional S wave velocity model is determined using
the relocated seismicity and an initial S wave velocity model derived
from the P wave velocity model assuming an average Vp/Vs ratio of
1.78. Convergence is steady with approximately 73\% and 52\% reduction
in P and S wave arrival time RMS, respectively, after 10 iterations.
The most prominent feature observed in the three-dimensional velocity
models derived for both P and S waves is a relative low-velocity,
near-vertical, pipelike structure approximately 1 km in diameter
that extends from 1 to 6 km beneath sea level. This feature aligns
axially with the bulk of seismicity and is interpreted as a highly
fractured and altered zone encompassing a magma conduit. The velocity
structure beneath the north flank of the volcano between depths of
1 and 6 km is characterized by large lateral velocity variations.
High velocities within this region are interpreted as remnant dikes
and sills and low velocities as regions along which magma migrates.
No large low-velocity body suggestive of a magma chamber is resolved
in the upper 7-8 km of the crust.
@article{benz_etal:1996,
abstract = {The three-dimensional P and S wave structure of Redoubt Volcano, Alaska,
and the underlying crust to depths of 7-8 km is determined from 6219
P wave and 4008 S wave first-arrival times recorded by a 30-station
seismograph network deployed on and around the volcano. First-arrival
times are calculated using a finite-difference technique, which allows
for flexible parameterization of the slowness model and easy inclusion
of topography and source-receiver geometry. The three-dimensional
P wave velocity structure and hypocenters are determined simultaneously,
while the three-dimensional S wave velocity model is determined using
the relocated seismicity and an initial S wave velocity model derived
from the P wave velocity model assuming an average Vp/Vs ratio of
1.78. Convergence is steady with approximately 73\% and 52\% reduction
in P and S wave arrival time RMS, respectively, after 10 iterations.
The most prominent feature observed in the three-dimensional velocity
models derived for both P and S waves is a relative low-velocity,
near-vertical, pipelike structure approximately 1 km in diameter
that extends from 1 to 6 km beneath sea level. This feature aligns
axially with the bulk of seismicity and is interpreted as a highly
fractured and altered zone encompassing a magma conduit. The velocity
structure beneath the north flank of the volcano between depths of
1 and 6 km is characterized by large lateral velocity variations.
High velocities within this region are interpreted as remnant dikes
and sills and low velocities as regions along which magma migrates.
No large low-velocity body suggestive of a magma chamber is resolved
in the upper 7-8 km of the crust.},
added-at = {2012-09-01T13:08:21.000+0200},
author = {Benz, H. M. and Chouet, B. A. and Dawson, P. B. and Lahr, J. C. and Page, R. A. and Hole, J. A.},
biburl = {https://www.bibsonomy.org/bibtex/23dade0a6a521c6aa4d108aa22ece5748/nilsma},
doi = {10.1029/95JB03046},
interhash = {c7f3372d22d36246174734d93a91c00f},
intrahash = {3dade0a6a521c6aa4d108aa22ece5748},
issn = {0148-0227},
journal = {Journal of Geophysical Research},
keywords = {geophysics seismology},
number = {B4},
pages = {8111--8128},
timestamp = {2021-02-09T13:26:58.000+0100},
title = {Three-dimensional P and S wave velocity structure of Redoubt Volcano,
Alaska},
url = {http://dx.doi.org/10.1029/95JB03046},
volume = 101,
year = 1996
}