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Mayo de 2006
Relationship between rupture process complexity and earthquake size.
Authors: K. Sato and J. Mori.
Link: www.agu.org/pubs/crossref/
2006/2005JB003614.shtml

Abstract
We studied the complexity of waveforms for two shallow crustal earthquake sequences in Japan. Using 47 earthquakes of the 2003 northern Miyagi sequence and 95 events of the 2004 mid-Niigata sequence, we estimated the number of complex and simple P waveforms for events with magnitudes from M3.1 to M6.6. Data were recorded at borehole and surface stations with

minimal site responses for close hypocentral distances of less than 30 km. The determination of complexity was done by counting the zero crossings of the accelerations waveforms. Our results show that for the smaller earthquakes, there are both simple and complex events but that all of the larger earthquakes are complex. There appears to be a threshold size over which the earthquakes always become complex. For both data sets this threshold is M4.0 to M4.5. We attribute this difference in complexity with earthquake size as an indication that larger earthquake grow with a complex ruptures that may be indicative of stochastic processes. There do not appear to be large earthquakes that grow smoothly to their final size.

Mayo de 2006
Ionospheric GPS total electron content (TEC) disturbances triggered by the 26 December 2004 Indian Ocean tsunami.
Authors: Jann-Yenq Liu, Yi-Ben Tsai et al.
Link: www.agu.org/pubs/crossref/
2006/2005JA011200.shtml

Abstract
Tsunami ionospheric disturbances (TIDs) of the 26 December 2004 M w 9.3 Sumatra earthquake are detected by the total electron content (TEC) of

ground-based receivers of the global positioning system (GPS) in the Indian Ocean area. It is found that the tsunami waves triggered atmospheric disturbances near the sea surface, which then traveled upward with an average velocity of about 730 m/s (2700 km/hr) into the ionosphere and significantly disturbed the electron density within it. Results further show that the TIDs, which have maximum height of about 8.6–17.2 km, periods of 10–20 min, and horizontal wavelengths of 120–240 km, travel away from the epicenter with an average horizontal speed of about 700 km/hr (190 m/s) in the ionosphere.

Mayo de 2006
Increase of shear wave velocity before the 1998 eruption of Merapi volcano (Indonesia)
Authors: U. Wegler, B.-G. Lühr, R. Snieder and A. Ratdomopurbo.
Link: www.agu.org/pubs/crossref/
2006/2006GL025928.shtml

Abstract
We infer temporal changes in the elastic

properties of the edifice of Merapi volcano (Java, Indonesia) before its eruption in 1998 by analyzing multiply scattered elastic waves excited by a repeatable controlled seismic source. A pre-eruptive increase of shear wave velocity, which correlates well with pre-eruptive seismicity and dome-growth is revealed. The method can be used as a "pressure-gauge" for pressure changes inside of volcanoes, because increasing pressures in rocks are known to cause proportionally increasing elastic wave velocities.

Mayo de 2006
A statistical investigation of preearthquake ionospheric anomaly.
Authors: J. Y. Liu, Y. I. Chen et al.
Link: www.agu.org/pubs/crossref/
2006/2005JA011333.shtml

Abstract
Empirical evidence of the preearthquake ionospheric anomalies (PEIAs) is reported by statistically investigating the relationship between

variations of the plasma frequency at the ionospheric F2 peak foF2 and 184 earthquakes with magnitude M = 5.0 during 1994–1999 in the Taiwan area. The PEIA, defined as the abnormal decrease more than about 25% in the ionospheric foF2 during the afternoon period, 1200–1800 LT, significantly occurs within 5 days before the earthquakes. Moreover, the odds of earthquakes with PEIA increase with the earthquake magnitude but decrease with the distance from the epicenter to the ionosonde station. These results indicate that the PEIA is energy related.

Mayo de 2006
Spiking modular neural networks: A neural network modeling approach for hydrological processes
Authors: K Parasuraman, A Elshorbagy et al.
Link: www.agu.org/pubs/crossref/
2006/2005WR004317.shtml

Abstract
Artificial Neural Networks (ANNs) have been widely used for modeling hydrological processes that are embedded with high nonlinearity in both spatial and temporal scales. The input-output functional relationship does not remain the same over the entire modeling domain, varying at different spatial and temporal scales. In this study, a novel neural network model called the spiking modular neural networks (SMNNs) is proposed. An SMNN consists of an input layer, a spiking layer, and an associator neural network layer. The modular nature of the SMNN helps in finding domain-dependent relationships. The

performance of the model is evaluated using two distinct case studies. The first case study is that of streamflow modeling, and the second case study involves modeling of eddy covariance-measured evapotranspiration. Two variants of SMNNs were analyzed in this study. The first variant employs a competitive layer as the spiking layer, and the second variant employs a self-organizing map as the spiking layer. The performance of SMNNs is compared to that of a regular feed forward neural network (FFNN) model. Results from the study demonstrate that SMNNs performed better than FFNNs for both the case studies. Results from partitioning analysis reveal that, compared to FFNNs, SMNNs are effective in capturing the dynamics of high flows. In modeling evapotranspiration, it is found that net radiation and ground temperature alone can be used to model the evaporation flux effectively. The SMNNs are shown to be effective in discretizing the complex mapping space into simpler domains that can be learned with relative ease.

Mayo de 2006
Detailed imaging of tectonic structures by multiscale Earth resistivity tomographies: The Colfiorito normal faults (central Italy)
Authors: I. Diaferia, M. Barchi et al.
Link: www.agu.org/pubs/crossref/
2006/2006GL025828.shtml

Abstract
This study is aimed to show how cost effective geophysical surveying, integrated with detailed knowledge of the local geology, can give a significant contribution to image the subsurface structure of complex areas of active faulting. The combined inversion of a data set consisting of a large scale tomography and a target-dependent

multiresolution dipole-dipole measurements, the multiscale approach, is shown to yield detailed structural information and to infer some characteristics of the fault zone. The operating procedure, applied to the Colfiorito fault system, allowed to differentiate the electrical signatures of the crossed faults. Minor faults show sharp lateral variations generated by a contact between different geological formations, while the major faults are also characterized by a decrease in resistivity values distributed on the fault damage zones. A close interpretation was supported by detailed geological surface data. Besides, quantitative correlations between in situ resistivity distribution and geological units were supported by electrical logs.

Mayo de 2006
Equivalent hydraulic conductivity of an experimental stratigraphy: Implications for basin-scale flow simulations
Authors: Ye Zhang, Carl W. Gable and Mark Person
Link: www.agu.org/pubs/crossref/2006/
2005WR004720.shtml

Abstract
Critical issues facing basin-scale groundwater flow models are the estimation of representative hydraulic conductivity for the model units and the impact of nonrepresentation of within-unit conductivity heterogeneity on the model flow prediction. In this study, high-resolution, fully heterogeneous basin-scale hydraulic conductivity map is generated by scaling up an experimental stratigraphy created by physical sedimentation processes and by assuming increasing conductivity for increasing gray scale (proxy for sand content). A fully heterogeneous model is created, incorporating the complete conductivity variation. Two hydrogeologic framework models are also created, one of coarser stratigraphic division. A novel numerical up-scaling method is developed to compute an equivalent conductivity for each irregularly shaped framework model unit by conducting basin-scale flow experiments in the fully heterogeneous model. In each experiment, different boundary conditions are specified, subjecting the basin to various flow conditions. To evaluate the impact of using equivalent

conductivity on the prediction of basin-scale hydraulic head and groundwater flow, the flow experiments conducted in the fully heterogenous model are repeated in the framework models. Results indicate that for most deposits, the behavior of the equivalent conductivity with increasing ln(K) variance is consistent with the prediction of an analytic-stochastic theory. The equivalent conductivity is also insensitive to the boundary condition and the number of flow experiments performed, indicating the possible emergence of an effective conductivity. Although all equivalent conductivities are full tensors, the off-diagonal term is 2-3 orders of magnitude smaller than the diagonal terms. Ignoring the off-diagonal term has minimal impact on the framework-model-predicted hydraulic head and groundwater flow paths, when compared to the impact of nonrepresentation of within-unit conductivity heterogeneity. Under certain boundary conditions, significant head deviation can develop within framework model units that contain trended or strongly stratified deposits. However, the accuracy of head prediction is improved when the length of the no-flow boundary is increased. In a topography-driven system, progressive degradation is observed in the prediction of basin-scale flow pattern, flow rate, and location of recharge/discharge, when the progressively up-scaled framework models are used. In summary, the accuracy of the framework models is controlled by the level of stratigraphic division, conductivity heterogeneity, and boundary conditions.

Mayo de 2006
Optimal groundwater remediation design using an Adaptive Neural Network Genetic Algorithm
Authors: Shengquan Yan and Barbara Minsker.
Link: www.agu.org/pubs/crossref/2006/
2005WR004303.shtml

Abstract
Large-scale water resources optimization often involves using time-consuming simulation models to evaluate potential water resource designs or calibrate parameter values. Approximation models have been proposed for improving computational efficiency of the optimization. In most instances, multiple simulation runs have been done prior to the optimization, which are then used to fit an approximate model that is used during the optimization. This paper demonstrates that this

approach can lead to suboptimal solutions and proposes a dynamic modeling approach, called Adaptive Neural Network Genetic Algorithm (ANGA), in which artificial neural networks are adaptively and automatically trained directly within a genetic algorithm (GA) to replace the time-consuming water resource simulation models. A dynamic learning approach is proposed to periodically sample new solutions both to update the ANNs and to correct the GA's convergence. Different configurations of ANGA were tested on a hypothetical groundwater remediation design case, and then the best configuration was applied to a field-scale case. In these applications, ANGA saved 85-90% percent of the simulation model calls with no loss in accuracy of the optimal solutions. These results show that the method has substantial promise for reducing computational effort associated with large-scale water resources optimization.

Mayo de 2006 - Geofísica de la atmósfera
Modelo Neuronal Multiestación para el pronóstico del MP10
Autores: Patricio Perez y Jorge Reyes.
Link: Click Aquí

Abstract
Hemos desarrollado un modelo neuronal multiestación para pronosticar el valor máximo de la concentración promedio de 24 horas de PM10 con un día de anticipación y hemos aplicado la técnica al caso específico de cinco estaciones de monitoreo en Santiago de Chile. Las entradas del modelo son las concentraciones medidas hasta las 7 PM en las cinco estaciones en el día actual, junto con los valores medidos y predichos de las variables meteorológicas. Las salidas corresponden a las máximas concentraciones esperadas para el día siguiente en las cinco estaciones. La concentración máxima predicha define la calidad del aire para el día siguiente. De acuerdo con el rango en el que cae la máxima concentración predicha, se definen tres niveles o clases de calidad del aire: Buena (A), Mala (B) y Crítica (C). Los parámetros del modelo fueron ajustados utilizando datos de los años 2001 y 2002 para así pronosticar las condiciones del año 2003. Así mismo se utilizó datos del 2002 y del 2003 para pronosticar los valores del 2004. El pronóstico neuronal fue comparado con los resultados obtenidos con un modelo lineal que utilizaba las mismas entradas y con persistencia. De acuerdo con nuestros resultados, el modelo neuronal resulta ser el más confiable. Sin embargo, es muy importante una correcta elección de las variables de entrada.

Mayo de 2006 - Atmospheric Geophysics
An integrated neural network model for PM10 forecasting
Authors: Patricio Perez and Jorge Reyes.
Link: Click here

Abstract
We have developed an integrated artificial neural network model to forecast the maxima of 24 h average of PM10 concentrations 1 day in advance and we have applied it to the case of five monitoring stations in the city of Santiago, Chile. Inputs to the model are concentrations measured until 7 PM at the five stations on the present day plus measured and forecast values of meteorological variables. Outputs are the expected maxima concentrations for the following day at the site of the same five stations. The greatest of the concentrations among the five forecasts defines air quality for the following day. According to the range where the concentrations fall, three levels or classes of air quality are defined: good (A), bad (B) and critical (C). We have adjusted the parameters of the models using 2001 and 2002 data to forecast 2003 conditions and 2002 and 2003 data in order to forecast 2004 values. Forecast values using the neural model are compared with the results obtained with a linear model with the same input variables and with persistence. According to the results reported here, overall, the neural model seems more accurate, although a good choice of input variables appears to be very important.

Mayo de 2006
Polarization analysis and polarization filtering of three-component signals with the time-frequency S transform
Author: C. R. Pinnegar
Link: www.blackwell-synergy.com/doi/abs/10.1111/j.1365-246X.2006.02937.x

Abstract
From basic Fourier theory, a one-component signal can be expressed as a superposition of sinusoidal oscillations in time, with the Fourier amplitude and phase spectra describing the contribution of each sinusoid to the total signal. By extension, three-component signals can be thought of as superpositions of sinusoids oscillating in the x-, y-, and z-directions, which, when considered one frequency at a time, trace out elliptical motion in three-space. Thus the total three-component signal can be thought of as a superposition of ellipses. The information contained in the Fourier spectra of the x-, y-, and z-components of the signal can then be re-

expressed as Fourier spectra of the elements of these ellipses, namely: the lengths of their semi-major and semi-minor axes, the strike and dip of each ellipse plane, the pitch of the major axis, and the phase of the particle motion at each frequency. The same type of reasoning can be used with windowed Fourier transforms (such as the S transform), to give time-varying spectra of the elliptical elements. These can be used to design signal-adaptive polarization filters that reject signal components with specific polarization properties. Filters of this type are not restricted to reducing the whole amplitude of any particular ellipse; for example, the 'linear' part of the ellipse can be retained while the 'circular' part is rejected. This paper describes the mathematics behind this technique, and presents three examples: an earthquake seismogram that is first separated into linear and circular parts, and is later filtered specifically to remove the Rayleigh wave; and two shot gathers, to which similar Rayleigh-wave filters have been applied on a trace-by-trace basis.

Mayo de 2006
Computation of Large Anisotropic Seismic Heterogeneities (CLASH)
Authors: Éric Beucler and Jean-Paul Montagner
Link: www.blackwell-synergy.com/doi/abs/10.1111/j.1365-246X.2005.02813.x

Abstract
A general tomographic technique is designed in order (i) to operate in anisotropic media; (ii) to account for the uneven seismic sampling and (iii) to handle massive data sets in a reasonable computing time. One modus operandi to compute a 3-D body wave velocity model relies on surface wave phase velocity measurements. An intermediate step, shared by other approaches, consists in translating, for each period of a given mode branch, the phase velocities integrated along ray paths into local velocity perturbations. To this end, we develop a method, which accounts for the azimuthal anisotropy in its comprehensive form. The weakly non-linear forward problem

allows to use a conjugate gradient optimization. The Earth's surface is regularly discretized and the partial derivatives are assigned to the individual grid points. Possible lack of lateral resolution, due to the inescapable uneven ray path coverage, is taken into account through the a priori covariances on parameters with laterally variable correlation lengths. This method allows to efficiently separate the 2psi and the 4psi anisotropic effects from the isotropic perturbations. Fundamental mode and overtone phase velocity maps, derived with real Rayleigh wave data sets, are presented and compared with previous maps. The isotropic models concur well with the results of Trampert & Woodhouse. Large 4psi heterogeneities are located in the tectonically active regions and over the continental lithospheres such as North America, Antarctica or Australia. At various periods, a significant 4psi signature is correlated with the Hawaii hotspot track. Finally, concurring with the conclusions of Trampert & Woodhouse, our phase velocity maps show that Rayleigh wave data sets do need both 2psi and 4psi anisotropic terms.

Abril de 2006
Equivalent transmissivity of heterogeneous leaky aquifers for steady state radial flow
Authors: Nadim K. Copty, Murat Savas Sarioglu and Angelos N. Findikakis.
Link: www.agu.org/pubs/crossref/2006/
2005WR004673.shtml

Abstract
The purpose of this study is to estimate the equivalent transmissivity for two-dimensional steady state radial flow toward a fully penetrating well in a heterogeneous leaky aquifer. The log transmissivity of the pumped aquifer is modeled as a multivariate random spatial function with stationary mean and exponential semivariogram, while the aquitard conductance is assumed to be spatially uniform. An approximate expression for

the upscaled or block transmissivity, defined as the transmissivity of an equivalent homogeneous leaky aquifer system with the same pumping, is proposed. The proposed relation expresses the upscaled transmissivity as a weighted average of the log transforms of the point transmissivity values. Monte Carlo simulations are used to numerically validate the proposed upscaling expression for wide ranges of aquifer parameters. The relation of the weighing function to the statistical parameters of the transmissivity field is discussed. The first and second moments of the upscaled transmissivity are also estimated as a function of the problem parameters. The expected value of the equivalent transmissivity is shown to increase from the geometric mean to the arithmetic mean as the aquitard conductance increases from zero to infinity.

Abril de 2006
Solar activity reconstructed over the last 7000 years: The influence of geomagnetic field changes.
Authors: I. G. Usoskin, S. K. Solanki and M. Korte.
Link: www.agu.org/pubs/crossref/2006/
2006GL025921.shtml

Abstract
The long-term solar activity, as manifested by sunspot number, has been recently reconstructed on multi-millennium time scales by S. K. Solanki et al. (2004) from the measured concentration of 14C in tree rings. The exact level of the reconstructed solar activity depends, however, on independently evaluated data of the geomagnetic dipole strength variations. Recently, a new series

of the palaeomagnetic dipole moment reconstruction for the last 7000 years has been presented by M. Korte and C. G. Constable (2005a) on the basis of a thorough analysis of global samples. The new palaeomagnetic series yields a systematically lower dipole moment in the past, compared to the earlier geomagnetic reconstructions. We have revised the earlier sunspot activity reconstruction since 5000 BC, using the new geomagnetic data series, and found that it is roughly consistent with the previous results during most of the period, although the revised sunspot number values are in general higher. Nonetheless, it is confirmed with the new palaeomagnetic series that the Sun spends only 2-3% of the time in a state of high activity, similar to the modern episode. This strengthens the conclusion that the modern high activity level is very unusual during the last 7000 years.

Abril de 2006
Seismology: Breaking new ground (Nature)
Author: Naomi Lubick
Link: www.nature.com/nature/journal
/v440/n7086/full/440864a.html

Abstract
In 1906, a great earthquake destroyed San Francisco, and galvanized US seismologists. Naomi Lubick looks back at the event that changed the country's geological scene.
The Great Earthquake and subsequent fire that destroyed San Francisco in 1906 began at 5:12 a.m. on 18 April. More than 3,000 people are thought to have died following the magnitude-7.9 tremor. The metropolis of San Francisco, built on gold-rush fortunes, was almost utterly destroyed in three days of fire, and officials spent years playing down the possibility of another 'big one'. Yet the earthquake also jump-started seismology in the United States, inspiring it to catch up with

countries such as Britain, Japan and Germany. The US scientific community had already encountered several major earthquakes. Three tremors of magnitude 8 or more racked the New Madrid region in the US Midwest in 1811 and 1812. And the city of Charleston, South Carolina, was seriously damaged during an 1886 earthquake.
But the 1906 earthquake happened in the right time and place to act as a catalyst for science. Chance brought together several ingredients: the right people, the right technology, key ideas in need of testing - and a huge earthquake delivering the data. "It took that large an event to make seismology a national priority," says Jack Boatwright, a seismologist at the US Geological Survey (USGS) in Menlo Park, California.
Around the world, the discipline of seismology began to coalesce in the late nineteenth century, as non-specialists interested in earthquakes began to work together. In India ...

Abril de 2006
Distinct regional differences in crustal thickness along the axis of the Mariana Trough, inferred from gravity anomalies
Authors: Kazuya Kitada , Nobukazu Seama, Toshitsugu Yamazaki, Yoshifumi Nogi, Kiyoshi Suyehiro
Link: www.agu.org/pubs/crossref/
2006/2005GC001119.shtml

Abstract
We have compiled extensive gravity and bathymetry data for the whole Mariana Trough, which were collected during several Japanese scientific cruises over the last few years. This study aims to clarify the lateral distribution of the local differences in geochemical signatures, which have been observed locally in the Mariana Trough. Shipboard free-air gravity anomaly data from eight Japan Agency for Marine-Earth Science and Technology (JAMSTEC) cruises were compiled with those crossover errors of 2.85 mgal. Mantle Bouguer anomalies (MBA) were calculated by subtracting the predictable gravity signal due to the seawater/crust and crust/mantle density boundaries. The crustal thickness variation along the spreading axis was estimated from the MBA. Different features in crustal thickness, its variation, and segment length for each segment, allow us to identify four distinct regional differences in magmatic activity along the spreading axis of the Mariana Trough. Segment in

region A (to the north of 20°35'N) shows the largest sectional dimensions of crust along the axis and it is probably affected by an additional supply from island arc magma sources. A variety of crustal thickness values and of along-axis crustal thickness variations in region B (between 15°38'N and 20°35'N) suggests two types of segments. One is similar to a slow spreading ridge segment that has a plume-like mantle upwelling under the spreading axis, and the other is a magma-starved segment. Region C (between 14°22'N and 15°38'N) is a less magmatic region (individual crustal thickness averages of 3.4-4.1 km). Region D (to the south of 14°22'N) has higher individual crustal thickness averages of 5.9-6.9 km, suggesting higher magmatic activity with a sheet-like mantle upwelling under the spreading axis. Different features in the MBA for off-axis areas suggest that these four regions have existed since the Mariana Trough started spreading. Moreover, comparison between our results of crustal thickness and previous geochemical results indicates that less magmatic spreading segments with thin crust, which are locally distributed in both regions B and C, probably result from mantle source depleted of water and incompatible elements. This suggests that lateral compositional variation of water and incompatible elements exists on a segment scale in the mantle source beneath the spreading axis of the Mariana Trough.

Abril de 2006
Unusually quick development of a 4000 nT substorm during the initial 10 min of the 29 October 2003 magnetic storm
Authors: M. Yamauchi , T. Iyemori, H. Frey, M. Henderson
Link: www.agu.org/pubs/crossref/
2006/2005JA011285.shtml

Abstract
Global geomagnetic field data, IMAGE FUV data, and many other in situ observations are presented for the initial 10 min of the magnetic storm starting 29 October 2003 at around 0610 UT. Within 1 min after sudden commencement (SC), two independent strong westward ionospheric electrojets (>2000 nT) at the inner magnetospheric region started simultaneously, one in the evening-midnight sector and the other in the morning sector. Both activities expanded and accompanied auroral expansion. The locations (inner magnetosphere), morphologies (expansion), and intensities (>2000 nT) of both

activities fall into substorm expansive phases. Having such simultaneous independent 2000 nT level expansions makes this event unique. The interplanetary magnetic field condition before the SC was not favorable in causing an AL < -2000 nT activity. A timing analysis indicates that these strong westward electrojets were most likely triggered by the interplanetary shock, with the triggering location not farther than the geosynchronous distance. They are also probably maintained by the direct energy pumping from the solar wind because cross-tail current derived from the closely located GOES-10 and Polar did not decrease very much during this period. A local but even stronger geomagnetic (nearly 4000 nT) and auroral activity started only 6 min after the start of SC at postmidnight where and when the above two expanding activities met each other, although the relation between the onset of 4000 nT activity and the preceding expansions is not clear. The suddenness of this third activity (3000 nT change within 2 min) is another unique feature.

Abril de 2006
A least-squares variance analysis method for shape and depth estimation from gravity data
Authors: E M Abdelrahman et al
Link: www.iop.org/EJ/abstract/1742-2140/3/2/005

Abstract
We have developed a simple method to estimate the shape (shape factor) and the depth of a buried structure simultaneously from modified first moving average residual anomalies (second moving average residuals) obtained from gravity data using filters of successively greater window

lengths. The method is based on computing the variance of the depths determined from all second moving average residual anomaly profiles using the least-squares method for each shape factor. The minimum variance is used as a criterion for determining the correct shape and depth of the buried structure. When the correct shape factor is used, the variance of the depths is always less than the variances computed using wrong shape factors. The method is applied to synthetic data with and without random errors, complex regional anomalies and interference from neighbouring structures, and tested on a field example from the USA.

Abril de 2006
Exploration of a geothermal reservoir using geoelectrical resistivity inversion: case study at Hammam Mousa, Sinai, Egypt
Author: Gad El-Qady
Link: www.iop.org/EJ/abstract/1742-2140/3/2/002

Abstract
Geoelectrical resistivity is a pioneer geophysical technique used in geothermal exploration. With the advent of computing technology, it has become convenient to apply sophisticated data analysis and inversion to geoelectrical resistivity field data. In this work, a geoelectrical resistivity survey was conducted in the Hammam Mousa area to explore the geothermal resources and groundwater aquifer. The survey comprises 19 vertical electrical soundings (VES) using the well-known Schlumberger array with AB/2 up to 1000 m. Interpretation of one-dimensional (1D)

inversion gave a layered-earth resistivity model using a nonlinear least-squares method. However, some resistivity sections of the 1D inversion were not fully resolved for the complicated geologic structure. Therefore, we carried out a two-dimensional (2D) inversion based on the ABIC least-squares method for the same data set. The general distribution of resistivity shows a very low value near Hammam Mousa Hot Spring. The 2D resistivity cross section clearly elaborates the subsurface structure in the spring area and it elucidates and gives an explanation for the hot water source in the area. It is concluded that the hydrothermal system in the Hammam Mousa area is adequately delineated from the 1D and 2D inversions of vertical electric sounding data using a Schlumberger electrode array. Accordingly, a proposal for geothermal drilling in the study area is recommended.

Abril de 2006
Reconciling a geophysical model to data using a Markov chain Monte Carlo algorithm: An application to the Yellow Sea-Korean Peninsula region
Authors: Michael E. Pasyanos, Gregory A. Franz et al
Link: www.agu.org/pubs/crossref/2006
/2005JB003851.shtml

Abstract
In an effort to build seismic models that are the most consistent with multiple data sets we have applied a new probabilistic inverse technique. This method uses a Markov chain Monte Carlo (MCMC) algorithm to sample models from a prior distribution and test them against multiple data types to generate a posterior distribution. While computationally expensive, this approach has several advantages over deterministic models, notably the seamless reconciliation of different data types that constrain the model, the proper handling of both data and model uncertainties, and the ability to easily incorporate a variety of prior information, all in a straightforward, natural fashion. A real advantage of the technique is

that it provides a more complete picture of the solution space. By mapping out the posterior probability density function, we can avoid simplistic assumptions about the model space and allow alternative solutions to be identified, compared, and ranked. Here we use this method to determine the crust and upper mantle structure of the Yellow Sea and Korean Peninsula region. The model is parameterized as a series of seven layers in a regular latitude-longitude grid, each of which is characterized by thickness and seismic parameters (Vp, Vs, and density). We use surface wave dispersion and body wave traveltime data to drive the model. We find that when properly tuned (i.e., the Markov chains have had adequate time to fully sample the model space and the inversion has converged), the technique behaves as expected. The posterior model reflects the prior information at the edge of the model where there is little or no data to constrain adjustments, but the range of acceptable models is significantly reduced in data-rich regions, producing values of sediment thickness, crustal thickness, and upper mantle velocities consistent with expectations based on knowledge of the regional tectonic setting.

Abril de 2006
Unsolved problems in the lowermost mantle
Authors: Kei Hirose, Shun-ichiro Karato et al
Link: www.agu.org/pubs/crossref/2006/
2006GL025691.shtml

Abstract
Many characteristics of D" layer may be attributed to the recently discovered MgSiO3 post-perovskite phase without chemical heterogeneities. They include a sharp discontinuity at the top of D", regional variation in seismic anisotropy, and a steep Clapeyron slope. However, some features remain unexplained. The seismically inferred

velocity jump is too large in comparison to first principles calculations, and the sharpness of the discontinuity may require a chemical boundary. Chemical heterogeneity may play an important role in addition to the phase transformation from perovskite to post-perovskite. Phase transformation and chemical heterogeneity and the attendant changes in physical properties, such as rheology and thermal conductivity, are likely to play competing roles in defining the dynamical stability of the D" layer. Revealing the relative roles between phase transition and chemical anomalies is an outstanding challenge in the study of the role of D" in thermal-chemical evolution of the Earth.

Marzo de 2006
Monte Carlo modeling of toroidal ion distributions and ion temperatures at high altitudes equatorward of the cusp: Effect of finite gyroradius
Authors: I. A. Barghouthi and M. A. Atout
Link: www.agu.org/pubs/crossref/2006
/2005JA011437.shtml

Abstract
We report that the effect of finite gyroradius is responsible for production of the H+ and O+ toroids at high altitudes equatorward of the cusp that are observed by TIDE and TIMAS ion instruments on board the polar spacecraft. The energization of charged particles, owing to interaction with electromagnetic turbulence, has an important influence on the plasma outflow in space. The effect of wave-particle interactions (WPI) on H+ and O+ outflow at high altitudes equatorward of the cusp was investigated by using Monte Carlo method. The Monte Carlo model includes the effect of WPI, gravity, polarization electrostatic field, and the divergence of the geomagnetic field within the simulation tube (1.2-10 Earth radii, R E ). As the ions drift upward along the geomagnetic field lines, they

interact with the electromagnetic turbulence and consequently get heated in the direction perpendicular to the geomagnetic field. The mirror force converts some of the gained ion energy in the perpendicular direction into parallel kinetic energy. These effects combine to form an ion-conic velocity distribution. However, as the ions are heated and move to higher altitudes, the ion gyroradius ? i may become comparable to the perpendicular wavelength of the electromagnetic turbulence lambda . As the ratio Rho/lambda becomes >1, then the heating rate turns to be self-limited and the ion velocity distribution displays toroidal features. A comparison has been made between the Monte Carlo calculations obtained in this study and observations of H+ and O+ ion velocity distributions and temperatures. The comparison showed a remarkably close agreement in the corresponding results for the ion velocity distribution and its temperature. As a result of the comparison, we were able to predict the characteristic value of the perpendicular wavelength of the electromagnetic turbulence lambda at high altitudes equatorward of the cusp. To our knowledge, this represents the first successful comparison of observed toroids with a theoretical model.

Marzo de 2006
Probabilistic seismic hazard estimation in low-seismicity regions considering non-Poissonian seismic occurrence
Authors: Céline Beauval, Sebastian Hainzl and Frank Scherbaum
Link: http://www.blackwell-synergy.com/doi/abs/10.1111/j.1365-246X.2006.02863.x

Abstract
In low-seismicity regions, such as France or Germany, the estimation of probabilistic seismic hazard must cope with the difficult identification of active faults and with the low amount of seismic data available. Since the probabilistic hazard

method was initiated, most studies assume a Poissonian occurrence of earthquakes. Here we propose a method that enables the inclusion of time and space dependences between earthquakes into the probabilistic estimation of hazard. Combining the seismicity model Epidemic Type Aftershocks-Sequence (ETAS) with a Monte Carlo technique, aftershocks are naturally accounted for in the hazard determination. The method is applied to the Pyrenees region in Southern France. The impact on hazard of declustering and of the usual assumption that earthquakes occur according to a Poisson process is quantified, showing that aftershocks contribute on average less than 5 per cent to the probabilistic hazard, with an upper bound around 18 per cent.

Marzo de 2006
Simulation of active tectonic processes for a convecting mantle with moving continents
Authors: Valeriy Trubitsyn, Mikhail Kaban, Walter Mooney, Christoph Reigber and Peter Schwintzer
Link: http://www.blackwell-synergy.com/doi/abs/10.1111/j.1365-246X.2006.02832.x

Abstract
Numerical models are presented that simulate several active tectonic processes. These models include a continent that is thermally and mechanically coupled with viscous mantle flow. The assumption of rigid continents allows use of solid body equations to describe the continents' motion and to calculate their velocities. The starting point is a quasi-steady state model of mantle convection with temperature/pressure-dependent viscosity. After placing a continent on top of the mantle, the convection pattern changes.

The mantle flow subsequently passes through several stages, eventually resembling the mantle structure under present-day continents: (a) Extension tectonics and marginal basins form on boundary of a continent approaching to subduction zone, roll back of subduction takes place in front of moving continent; (b) The continent reaches the subduction zone, the extension regime at the continental edge is replaced by strong compression. The roll back of the subduction zone
still continues after closure of the marginal basin and the continent moves towards the upwelling. As a result the ocean becomes non-symmetric and (c) The continent overrides the upwelling and subduction in its classical form stops. The third stage appears only in the upper mantle model with localized upwellings overrides the upwelling and subduction in its classical form stops. The third stage appears only in the upper mantle model with localized upwellings.
01-mar-06
Detectan hidratos de gas de fácil explotación en costa chilena (Noticias Ambientales ACHS)
Auspiciosos resultados preliminares tuvo la expedición científica de la comisión encargada de explorar la presencia de hidratos de gas en la costa chilena. Un estudio realizado durante 20 días a bordo del buque oceanográfico Vidal Gormaz de la Armada, ubicó vastos yacimientos
de hidratos de gas (forma sólida) y gas libre, cuyo estado en forma de burbujas facilita su potencial explotación como fuente energética. Ya se había establecido la existencia de yacimientos de gas en el océano, pero la exploración entre el 3 y 22 de febrero permitió un análisis más acotado del sector entre la desembocadura de los ríos Maule y Bio Bío. Los resultados de la exploración estarán listos en forma parcial a fines de año.

Diciembre 2005
Layer stripping of azimuthal anisotropy from P-wave reflection moveout in orthogonal survey lines
Authors: Shangxu Wang et al 2006 J. Geophys. Eng. 3 1-11 doi:10.1088/1742-2132/3/1/001
Link: http://www.iop.org/EJ/abstract/1742-2140/3/1/001

Abstract
This paper presents a layer-stripping procedure to determine interval measurements of fracture parameters in multi-layered fractured media with vertically varying strike directions. The procedure is based on the P-wave travel time difference between two orthogonal seismic survey lines, and this difference is referred to as the P-wave

Azimuthal Moveout Response (AMR). The interval AMR of a fracture target for a fixed offset is a function of cos(x) with respect to the line azimuth and the fracture-strike azimuth i. Consequently two pairs of orthogonal survey lines can be used to determine the local fracture strike i if the interval AMR of the target is known. In the case of a weakly fractured overburden underlain by a fractured target, layer stripping can be achieved through the alignment of the top-target event by performing NMO correction separately for all survey lines. The interval AMR of the target layer may then be calculated from the residual moveout the bottom-target event, if any. In the general case, a ray-tracing procedure, similar to that used in AVO analysis, is required to perform effective layer stripping. Full-wave modelling is used to verify and illustrate these procedures.

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