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On the measurement of Sdiff splitting caused by lowermost mantle anisotropy
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Seismic anisotropy has been detected at many depths of the Earth,
including its upper layers, the lowermost mantle, and the inner core.
While upper mantle seismic anisotropy is relatively straightforward to
resolve, lowermost mantle anisotropy has proven to be more complicated
to measure. Due to their long, horizontal raypaths along the core-mantle
boundary, S waves diffracted along the core-mantle boundary (Sdiff) are
potentially strongly influenced by lowermost mantle anisotropy. Sdiff
waves can be recorded over a large epicentral distance range and thus
sample the lowermost mantle everywhere around the globe. Sdiff therefore
represents a promising phase for studying lowermost mantle anisotropy;
however, previous studies have pointed out some difficulties with the
interpretation of differential SHdiff-SVdiff travel times in terms of
seismic anisotropy. Here, we provide a new, comprehensive assessment of
the usability of Sdiff waves to infer lowermost mantle anisotropy. Using
both axisymmetric and fully 3D global wavefield simulations, we show
that there are cases in which Sdiff can reliably detect and characterize
deep mantle anisotropy when measuring traditional splitting parameters
(as opposed to differential travel times). First, we analyze isotropic
effects on Sdiff polarizations, including the influence of realistic
velocity structure (such as 3D velocity heterogeneity and ultra-low
velocity zones), the character of the lowermost mantle velocity
gradient, mantle attenuation structure, and Earth’s Coriolis force.
Second, we evaluate effects of seismic anisotropy in both the upper and
the lowermost mantle on SHdiff waves. In particular, we investigate how
SHdiff waves are split by seismic anisotropy in the upper mantle near
the source and how this anisotropic signature propagates to the receiver
for a variety of lowermost mantle models. We demonstrate that, in
particular and predictable cases, anisotropy leads to Sdiff splitting
that can be clearly distinguished from other waveform effects. These
results enable us to lay out a strategy for the analysis of Sdiff
splitting due to anisotropy at the base of the mantle, which includes
steps to help avoid potential pitfalls, with attention paid to the
initial polarization of Sdiff and the influence of source-side
anisotropy. We demonstrate our Sdiff splitting method using three
earthquakes that occurred beneath the Celebes Sea, measured at many
Transportable Array (TA) stations at a suitable epicentral distance. We
resolve consistent and well-constrained Sdiff splitting parameters due
to lowermost mantle anisotropy beneath the northeastern Pacific Ocean.
Title: On the measurement of Sdiff splitting caused by lowermost mantle anisotropy
Description:
Seismic anisotropy has been detected at many depths of the Earth,
including its upper layers, the lowermost mantle, and the inner core.
While upper mantle seismic anisotropy is relatively straightforward to
resolve, lowermost mantle anisotropy has proven to be more complicated
to measure.
Due to their long, horizontal raypaths along the core-mantle
boundary, S waves diffracted along the core-mantle boundary (Sdiff) are
potentially strongly influenced by lowermost mantle anisotropy.
Sdiff
waves can be recorded over a large epicentral distance range and thus
sample the lowermost mantle everywhere around the globe.
Sdiff therefore
represents a promising phase for studying lowermost mantle anisotropy;
however, previous studies have pointed out some difficulties with the
interpretation of differential SHdiff-SVdiff travel times in terms of
seismic anisotropy.
Here, we provide a new, comprehensive assessment of
the usability of Sdiff waves to infer lowermost mantle anisotropy.
Using
both axisymmetric and fully 3D global wavefield simulations, we show
that there are cases in which Sdiff can reliably detect and characterize
deep mantle anisotropy when measuring traditional splitting parameters
(as opposed to differential travel times).
First, we analyze isotropic
effects on Sdiff polarizations, including the influence of realistic
velocity structure (such as 3D velocity heterogeneity and ultra-low
velocity zones), the character of the lowermost mantle velocity
gradient, mantle attenuation structure, and Earth’s Coriolis force.
Second, we evaluate effects of seismic anisotropy in both the upper and
the lowermost mantle on SHdiff waves.
In particular, we investigate how
SHdiff waves are split by seismic anisotropy in the upper mantle near
the source and how this anisotropic signature propagates to the receiver
for a variety of lowermost mantle models.
We demonstrate that, in
particular and predictable cases, anisotropy leads to Sdiff splitting
that can be clearly distinguished from other waveform effects.
These
results enable us to lay out a strategy for the analysis of Sdiff
splitting due to anisotropy at the base of the mantle, which includes
steps to help avoid potential pitfalls, with attention paid to the
initial polarization of Sdiff and the influence of source-side
anisotropy.
We demonstrate our Sdiff splitting method using three
earthquakes that occurred beneath the Celebes Sea, measured at many
Transportable Array (TA) stations at a suitable epicentral distance.
We
resolve consistent and well-constrained Sdiff splitting parameters due
to lowermost mantle anisotropy beneath the northeastern Pacific Ocean.
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