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    <title>ERA Community:</title>
    <link>http://hdl.handle.net/1842/1631</link>
    <description />
    <pubDate>Wed, 22 May 2013 10:18:06 GMT</pubDate>
    <dc:date>2013-05-22T10:18:06Z</dc:date>
    <item>
      <title>Seismic body-wave anisotropy beneath continents</title>
      <link>http://hdl.handle.net/1842/6537</link>
      <description>Title: Seismic body-wave anisotropy beneath continents
Authors: Singh, Jasbinder
Abstract: A search for the effects of anisotropy on seismic body-waves predicted&#xD;
by theory is described. Preliminary studies were based on long-period&#xD;
data from the WWSSN, HGLP and SRO networks. These showed that data from&#xD;
the WWSSN network are unsuitable for anisotropy studies because of&#xD;
features in the geometry of the recording system which lead to misalignment&#xD;
of the digitizer relative to the galvanometer-swing (which it is&#xD;
not always possible to correct) and the fact that the horizontal components&#xD;
are not always well matched. Digital data from the HGLP&#xD;
(recorded after 1976) and SRO networks are more suitable for anisotropy&#xD;
studies but eventually it was found that the anisotropic differences are&#xD;
too small to be resolved by long-period instruments. Analysis of&#xD;
short-period teleseismic shear-waves observed at LRSM stations located&#xD;
in United States and southern Canada has revealed shear-wave splitting&#xD;
diagnostic of anisotropy somewhere along the path. The shear-wave&#xD;
splitting is often seen as two separate shear-wave arrivals on the rotated&#xD;
horizontal components. All cases of shear-wave splitting are indicated&#xD;
by an abrupt change in the direction of particle-motion in the&#xD;
horizontal plane. A selection of seismograms and associated particlemotion&#xD;
diagrams is presented in order to illustrate shear-wave splitting.&#xD;
The polarizations of the first arrival shear-waves and the delays&#xD;
between the shear-wave arrivals were measured and are presented in the&#xD;
form of stereograms. The maximum shear-wave delay observed is 2.75&#xD;
seconds and on the basis of this, we calculate the thickness of the anisotropic&#xD;
layer to be 248 kms for a model with 4.5% differential shearwave&#xD;
velocity anisotropy. For a model with much higher differential shear-wave velocity anisotropy (8.4%), the thickness of the layer is&#xD;
only 136 kms. Our results do not allow us to constrain the depth to the&#xD;
top of the anisotropic layer, although on the basis of other studies we&#xD;
believe the anisotropic layer to be situated immediately below the&#xD;
Mohorovicic discontinuity. The polarizations are broadly similar to&#xD;
those obtained theoretically for the y- and z-cuts of olivine,&#xD;
transversely isotropic olivine and mixture of transversely isotropic&#xD;
olivine/isotropic material. On the basis of this, we tentatively identify&#xD;
N50°E as a direction of symmetry and note that it is approximately&#xD;
parallel to the absolute motion of the North-American plate. We therefore&#xD;
suspect a causal relationship between plate motion and the generation&#xD;
of anisotropy. The most likely hypothesis is that as the continental&#xD;
lithosphere moves across the asthenosphere, the drag on the lithosphere&#xD;
sets up a horizontal compression in the direction of motion of&#xD;
the lithosphere relative to the asthenosphere and olivine crystals align&#xD;
by {Okl} [100] pencil glide so that the a-axis points into the direction&#xD;
of plate motion while the b and c axes form girdles perpendicular to the&#xD;
a-axis. This would result in transverse isotropy with the axis of symmetry&#xD;
horizontal, an orientation which is consistent with our results.&#xD;
The existence of anisotropy in the upper mantle has implications for&#xD;
other seismological studies. In particular, focal mechanism studies&#xD;
which rely solely on S-wave polarizations will be erroneous and studies&#xD;
of travel-time residuals will need to take account of the anisotropy.</description>
      <pubDate>Sat, 01 Jan 1983 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/1842/6537</guid>
      <dc:date>1983-01-01T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Complexity, aftershock sequences, and uncertainty in earthquake statistics</title>
      <link>http://hdl.handle.net/1842/6224</link>
      <description>Title: Complexity, aftershock sequences, and uncertainty in earthquake statistics
Authors: Touati, Sarah
Abstract: Earthquake statistics is a growing field of research with direct application to probabilistic&#xD;
seismic hazard evaluation. The earthquake process is a complex spatio-temporal phenomenon,&#xD;
and has been thought to be an example of the self-organised criticality (SOC) paradigm, in&#xD;
which events occur as cascades on a wide range of sizes, each determined by fine details of the&#xD;
rupture process. As a consequence, deterministic prediction of specific event sizes, locations,&#xD;
and times may well continue to remain elusive. However, probabilistic forecasting, based on&#xD;
statistical patterns of occurrence, is a much more realistic goal at present, and is being actively&#xD;
explored and tested in global initiatives.&#xD;
This thesis focuses on the temporal statistics of earthquake populations, exploring the uncertainties&#xD;
in various commonly-used procedures for characterising seismicity and explaining&#xD;
the origins of these uncertainties. Unlike many other SOC systems, earthquakes cluster in&#xD;
time and space through aftershock triggering. A key point in the thesis is to show that the&#xD;
earthquake inter-event time distribution is fundamentally bimodal: it is a superposition of a&#xD;
gamma component from correlated (co-triggered) events and an exponential component from&#xD;
independent events. Volcano-tectonic earthquakes at Italian and Hawaiian volcanoes exhibit a&#xD;
similar bimodality, which in this case, may arise as the sum of contributions from accelerating&#xD;
and decelerating rates of events preceding and succeeding volcanic activity. Many authors, motivated&#xD;
by universality in the scaling laws of critical point systems, have sought to demonstrate&#xD;
a universal data collapse in the form of a gamma distribution, but I show how this gamma form&#xD;
is instead an emergent property of the crossover between the two components. The relative size&#xD;
of these two components depends on how the data is selected, so there is no universal form.&#xD;
The mean earthquake rate—or, equivalently, inter-event time—for a given region takes time&#xD;
to converge to an accurate value, and it is important to characterise this sampling uncertainty.&#xD;
As a result of temporal clustering and non-independence of events, the convergence is found to&#xD;
be much slower than the Gaussian rate of the central limit theorem. The rate of this convergence&#xD;
varies systematically with the spatial extent of the region under consideration: the larger the&#xD;
region, the closer to Gaussian convergence. This can be understood in terms of the increasing&#xD;
independence of the inter-event times with increasing region size as aftershock sequences overlap&#xD;
in time to a greater extent. On the other hand, within this high-overlap regime, a maximum&#xD;
likelihood inversion of parameters for an epidemic-type statistical model suffers from lower&#xD;
accuracy and a systematic bias; specifically, the background rate is overestimated. This is&#xD;
because the effect of temporal overlapping is to mask the correlations and make the time&#xD;
series look more like a Poisson process of independent events. This is an important result&#xD;
with practical relevance to studies using inversions, for example, to infer temporal variations&#xD;
in background rate for time-dependent hazard estimation.</description>
      <pubDate>Mon, 25 Jun 2012 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/1842/6224</guid>
      <dc:date>2012-06-25T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Analysis of P-wave seismic response for fracture detection: modelling and case studies</title>
      <link>http://hdl.handle.net/1842/6185</link>
      <description>Title: Analysis of P-wave seismic response for fracture detection: modelling and case studies
Authors: Xu, Yungui
Abstract: This thesis addresses a few specific issues in the use of wide azimuth P-wave seismic&#xD;
data for fracture detection based on numerical modelling and real data. These issues&#xD;
include the seismic response of discrete fractures, the effects of anticline and&#xD;
uncertainties in real data analysis. For this, I implemented the finite difference&#xD;
scheme for modelling the seismic response in 3D fractured media; appropriate&#xD;
approaches are then selected to study discrete fracture models and the effect of the&#xD;
anticline with 3D seismic modelling, followed by an integrate real case study.&#xD;
Finite difference (FD) is widely used in seismic modelling. There are three FD&#xD;
schemes described in this thesis, the standard staggered grid (SSG), the rotated&#xD;
staggered grid (RSG), and the diamond staggered grid (DSG). Both qualitative and&#xD;
quantitative comparison has been made to reveal their capability in modelling 3D&#xD;
fractured media. The SSG has shown best performance for anisotropic media with&#xD;
orthorhombic symmetry or higher symmetry system. For lower anisotropy symmetry,&#xD;
the DSG is preferred than the RSG in terms of computation efficiency. A new&#xD;
solution to the diamond grid issue is developed which can simplify the DSG&#xD;
implementation, and an optimized workflow is proposed to simulate large 3D&#xD;
fractured models. The SSG scheme is implemented in three dimensions and it&#xD;
provides a useful tool for various practical modelling studies.&#xD;
With the above tool, two modelling studies have been carried out, on the effects of&#xD;
the discrete fractures and of the presence of anticline: the Discrete Fracture Model&#xD;
(DFM) study provides many insights into seismic response of discrete fracture and&#xD;
the link between the discrete fractures and aligned micro cracks, as well as the&#xD;
features in scattering waves. The modelling results demonstrate that, P-wave seismic&#xD;
anisotropy increases with the decrease of discrete fracture spacing, and different spacing leads to different patterns in scattering waves. The study also reveals the&#xD;
azimuthal AVO variation on the top of discrete fracture layer, which is similar to that&#xD;
we find in homogenous anisotropic media. The study of the anticline structure with&#xD;
vertical fractures, which is built with the parameters from a real case, is to assess the&#xD;
anticline structure effect on fracture parameter inversion based on the Singular Value&#xD;
Decomposition (SVD) method. The fracture density can be resolved accurately at the&#xD;
top of the anticline, whilst that on the flanks tends to be over-estimated. The results&#xD;
also indicate that the SVD method is a reliable approach for directly estimating the&#xD;
fracture density.&#xD;
P-wave azimuthal attributes are commonly employed to invert fracture density and&#xD;
orientation. Many factors may affect the accuracy of the inversion results. The&#xD;
integrated study in this thesis shows that azimuthal coverage, offset-depth ratio, data&#xD;
quality and geological structures all affect the final prediction, and different&#xD;
attributes shows different sensitivities to these factors. Furthermore, the combined&#xD;
analysis of both geological observation and pre- and post-stack seismic attributes can&#xD;
reduce the uncertainties for fracture detection.</description>
      <pubDate>Mon, 25 Jun 2012 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/1842/6185</guid>
      <dc:date>2012-06-25T00:00:00Z</dc:date>
    </item>
    <item>
      <title>Non-physical energy in seismic interferometry</title>
      <link>http://hdl.handle.net/1842/6184</link>
      <description>Title: Non-physical energy in seismic interferometry
Authors: King, Simon James
Abstract: Non-physical arrivals produced by seismic interferometry, the process whereby&#xD;
Green’s functions are synthesized between two points by cross-correlation, crossconvolution&#xD;
or deconvolution, are often considered to provide little information&#xD;
about the Earth’s subsurface. Their contributions are usually suppressed in&#xD;
interferometric Green’s function estimates to suit existing methods of seismic&#xD;
velocity estimation which favour the more familiar physical arrivals. In this thesis&#xD;
we show that the non-physical arrivals retrieved in exploration-type settings are&#xD;
useful for determining the long-wavelength seismic velocity structure and can be&#xD;
used to obtain improved Green’s function estimates.&#xD;
First, we estimate the seismic velocity and layer thickness by measuring the&#xD;
signal coherency along traveltime curves between two receivers in a collection of&#xD;
traces consisting of cross-correlated wavefields, known as the correlation gather.&#xD;
The traveltime curves represent the traveltime differences between wavefields&#xD;
recorded at the two receivers. When the procedure is used to find the velocity and&#xD;
thickness of the uppermost layer, the traveltime curves implicitly incorporate the&#xD;
physical and non-physical wavefields in the Green’s function estimates. When the&#xD;
procedure is applied to a model with more than one layer, the traveltime curves&#xD;
correspond to non-physical wavefields only in the Green’s function estimates.&#xD;
Instead of suppressing multiple reflections as in conventional methods, the&#xD;
procedure incorporates the traveltimes of multiple reflections to constrain velocity&#xD;
and thickness estimates.&#xD;
The procedure above is most suitable for recovering the first-layer seismic&#xD;
velocity. We propose a simpler method to estimate the seismic velocities&#xD;
corresponding to deeper layers. We find that the Green’s functions contain very&#xD;
weak reflections, but are dominated by non-physical refractions if retrieved using a&#xD;
limited source aperture. The seismic velocities are easily identifiable as repeating&#xD;
bright spots after transforming the refraction-dominated Green’s functions to the&#xD;
  − p domain.&#xD;
We show that non-physical reflections can be used constructively to provide&#xD;
physical reflections, and therefore improved Green’s function estimates, by using a cross-convolution operation in a new variant of seismic interferometry,&#xD;
called source-receiver interferometry. We also show that non-physical reflections&#xD;
associated with the cross-correlation of reflections from different interfaces allow&#xD;
for the direct estimation of interval velocities and layer thicknesses. This method&#xD;
removes the necessity to first find the root-mean-square velocities and two-way&#xD;
traveltimes required to compute the interval velocities by Dix inversion.&#xD;
Overall, this thesis significantly improves our understanding of how nonphysical&#xD;
energy in seismic interferometry both provides useful information&#xD;
about the Earth’s subsurface and contributes to physical energy in particular&#xD;
interferometric methods.</description>
      <pubDate>Mon, 25 Jun 2012 00:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/1842/6184</guid>
      <dc:date>2012-06-25T00:00:00Z</dc:date>
    </item>
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