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        <rdf:li resource="http://hdl.handle.net/2122/8401" />
        <rdf:li resource="http://hdl.handle.net/2122/8344" />
        <rdf:li resource="http://hdl.handle.net/2122/8343" />
        <rdf:li resource="http://hdl.handle.net/2122/8324" />
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    <dc:date>2013-05-20T22:39:18Z</dc:date>
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  <item rdf:about="http://hdl.handle.net/2122/8499">
    <title>Geological and geophysical investigation of Kamil crater, Egypt</title>
    <link>http://hdl.handle.net/2122/8499</link>
    <description>Title: Geological and geophysical investigation of Kamil crater, Egypt
Authors: Urbini, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Nicolosi, I.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Zeoli, A.; Museo Nazionale dell’Antartide Universita` di Siena, Via Laterina 8, 53100 Siena, Italy; El Khrepy, S.; National Research Institute of Astronomy and Geophysics, Helwan, Egypt; Lethy, A.; National Research Institute of Astronomy and Geophysics, Helwan, Egypt; Hafez, M.; National Research Institute of Astronomy and Geophysics, Helwan, Egypt; El Gabry, M.; National Research Institute of Astronomy and Geophysics, Helwan, Egypt; El Barkooky, A.; Department of Geology, Faculty of Sciences, Cairo University, Giza, Egypt; Barakat, A.; Egyptian Mineral Resources Authority, 3 Salah Salem Road, Abassiya, Cairo, Egypt; Gomaa, M.; Museo Nazionale dell’Antartide Universita` di Siena, Via Laterina 8, 53100 Siena, Italy; Radwan, A. M.; Museo Nazionale dell’Antartide Universita` di Siena, Via Laterina 8, 53100 Siena, Italy; El Sharkawi, M.; Department of Geology, Faculty of Sciences, Cairo University, Giza, Egypt; D’Orazio, M.; Dipartimento di Scienze della Terra, Universita` di Pisa, Via S. Maria 53, 56126 Pisa, Italy; Folco, L.; Dipartimento di Scienze della Terra, Universita` di Pisa, Via S. Maria 53, 56126 Pisa, Italy
Abstract: We detail the Kamil crater (Egypt) structure and refine the impact scenario, based&#xD;
on the geological and geophysical data collected during our first expedition in February&#xD;
2010. Kamil Crater is a model for terrestrial small-scale hypervelocity impact craters. It is an&#xD;
exceptionally well-preserved, simple crater with a diameter of 45 m, depth of 10 m, and rayed&#xD;
pattern of bright ejecta. It occurs in a simple geological context: flat, rocky desert surface, and&#xD;
target rocks comprising subhorizontally layered sandstones. The high depth-to-diameter ratio&#xD;
of the transient crater, its concave, yet asymmetric, bottom, and the fact that Kamil Crater is not part of a crater field confirm that it formed by the impact of a single iron mass (or a tight cluster of fragments) that fragmented upon hypervelocity impact with the ground. The circular crater shape and asymmetries in ejecta and shrapnel distributions coherently indicate a direction of incidence from the NW and an impact angle of approximately 30 to 45 . Newly&#xD;
identified asymmetries, including the off-center bottom of the transient crater floor downrange, maximum overturning of target rocks along the impact direction, and lower crater rim elevation downrange, may be diagnostic of oblique impacts in well-preserved craters. Geomagnetic data reveal no buried individual impactor masses &gt;100 kg and suggest that the total mass of the buried shrapnel &gt;100 g is approximately 1050–1700 kg. Based on this mass value plus that of shrapnel &gt;10 g identified earlier on the surface during systematic search, the new estimate of the minimum projectile mass is approximately 5 t.</description>
    <dc:date>2012-12-13T23:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8401">
    <title>Automatic detection of landslides at Stromboli using neural network analysis of seismic signals</title>
    <link>http://hdl.handle.net/2122/8401</link>
    <description>Title: Automatic detection of landslides at Stromboli using neural network analysis of seismic signals
Authors: D'Auria, L.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Esposito, A.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Giudicepietro, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Martini, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Peluso, R.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; De Cesare, W.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Orazi, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Scarpato, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: Landslides along the Sciara del Fuoco flank of Stromboli volcano are generally accompanied&#xD;
by c1istinctive seismic signals which can be used for srudying this phenomenon.&#xD;
These signals are characterìzed by a spectral content with higher frequencies&#xD;
and a wider band than the typical explosion quakes and volcanic tremor signals which&#xD;
are continuously recorded at Stromboli. Furthermore their amplirude envelope usually&#xD;
shows a cigar-like shape. These two fearures make the detection of such signals quite&#xD;
easy. The detection of landslides at Stromboli has shown to be an important shortterm&#xD;
precursor of effusive eruptions. Before the Feb. 27th 2007 eruption, the opening&#xD;
of the effusive vents was preceded by few hours oI increased occurrence of landslide&#xD;
signals (Martini et al., 2007). Furthermore since the Sciara del Fuoco has shown significant&#xD;
instabilities during the 2002-2003 eruption, the automatic detection of landslide&#xD;
signals is an important monitoring tool for notifying variations in the stability of this&#xD;
flank. We propose a technique based on a Multi Layer Perceptron (MLP) neural network&#xD;
which has shown excellent performances. The network is composed of two layer&#xD;
of neurons, the hidden and the output. The hidden layer is composed of 4 neurons&#xD;
while the output layer is composed by a single neuron whose output value ranges&#xD;
between Oand 1, with values higher than a given threshold (e.g. 0.5) meaning positive&#xD;
detection. The continuous seismic signals are analysed using moving windows of 24 s,&#xD;
with an overlap of 12 s. For each of these windows the neural output is computed.&#xD;
The waveforms of each time window are parametrized using both their spectrogram&#xD;
and their amplirude envelope. The spectrogram is described using the Linear Preclictive&#xD;
Cocling (L'PC) technique which allows to represent the spectral content using a limited&#xD;
number of coefficients. The whole signal is c1ivided into 8 sub-windows of 5.12 s&#xD;
length, with an overlapping of 2.56 s. For each sub-window we compute 6 LPC coefficients,&#xD;
so each spectrogram is described by only 48 coefficients. The amplirude envelope&#xD;
is defined by computing the c1ifference between the maximum and minimum value&#xD;
over 1 s sub-windows obtaining 24 coefficients. In conclusion we use an input vector&#xD;
composed of 72 elements (48+24). This vector has shown to be an efficient and&#xD;
compact representation of the raw signal (composed of 1200 samples) (Esposito et al.&#xD;
2006). The dataset used for determining the network parameters is composed of 537&#xD;
signals, c1ivided in two classes: 267 landslide signals and 270 other signals (explosions&#xD;
and tremor). The classification of these signals has been performed by analysts. The training is carried out using subsets of 5/8 of the total dataset. The testing subsets are&#xD;
composed by the remaining 3/8. The network has shown a performance of about&#xD;
98.7%. This value is an average over 6 random permutations of the dataset. A preliminary&#xD;
real-rime automatic system has already been implemented. This system performs&#xD;
continuous analysis of the seismic signals, publishing them on internal web pages.&#xD;
It allows a detection of the landslides and a comparison with the past activity on&#xD;
arbitrary rime intervals.</description>
    <dc:date>2009-05-31T22:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8344">
    <title>Multiparametric data analysis for seismic source identification in the Campanian area: merging of seismological, structural and gravimetric data</title>
    <link>http://hdl.handle.net/2122/8344</link>
    <description>Title: Multiparametric data analysis for seismic source identification in the Campanian area: merging of seismological, structural and gravimetric data
Authors: Gaudiosi, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Alessio, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Cella, F.; Fedi, M.; Florio, G.; Nappi, R.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: This paper deals with an interdisciplinary research that has been carried out to&#xD;
investigate the neotectonic activity of the Campanian plain and surrounding areas&#xD;
(southern Italy), affected by Plio-Pleistocene tectonics and volcanic activity. Three&#xD;
thematic data sets have been generated for this area, “fault”, “earthquake” and&#xD;
“gravimetric” data sets, respectively. These data sets allow an integrated analysis of the&#xD;
structural, seismic and gravimetric data in GIS environment with the aim of&#xD;
identifying the active structural lineaments that accommodate the local stress through&#xD;
seismic activity. In detail, an original map with Plio-Quaternary tectonic structures of&#xD;
the Campanian plain and its margins, constrained by morpho-structural analysis&#xD;
and/or geophysical exploration data, is presented. The available earthquake data sets&#xD;
have been merged in a single data set, including seismicity in the Campanian area&#xD;
from 217 b.C. to 2010; processing of seismic data for new precise earthquake&#xD;
locations have been carried out for some clusters of events with poor data, for better&#xD;
constraining existence and activity of some outcropping and buried tectonic&#xD;
structures. As regards the gravimetric data set, a Multiscale Derivative Analysis&#xD;
(MDA) of the gravity field of the area has been performed, relying on the high&#xD;
resolution properties of the Enhanced Horizontal Derivative (EHD). MDA of gravity&#xD;
data allowed localization of several linear and close trends, identifying anomaly&#xD;
sources whose presence was not previously detected. Our integrated analysis shows&#xD;
that a strong correlation occurs among the new hypocentral locations of the seismic&#xD;
clusters matching the fault systems of the Massico Mt. and Avella Mts., and the MDA&#xD;
lineaments from gravity data relative to the same tectonic structures.</description>
    <dc:date>2012-09-11T22:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8343">
    <title>High-resolution controlled-source seismic tomography across the Middle Aterno basin in the epicentral area of the 2009, Mw 6.3, L’Aquila earthquake (central Apennines, Italy)</title>
    <link>http://hdl.handle.net/2122/8343</link>
    <description>Title: High-resolution controlled-source seismic tomography across the Middle Aterno basin in the epicentral area of the 2009, Mw 6.3, L’Aquila earthquake (central Apennines, Italy)
Authors: Improta, L.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Villani, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Bruno, P. P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Castiello, A.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; De Rosa, D.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Varriale, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Punzo, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Brunori, C. A.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione CNT, Roma, Italia; Civico, R.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Pierdominici, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Berlusconi, A.; Università dell'Insubria, Facoltà di Scienze M.F.N.; Giacomuzzi, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione CNT, Roma, Italia
Abstract: We present high-resolution Vp models of the Middle Aterno basin obtained by multi-scale non-linear controlled-source tomography. Seismic data have been collected along four dense wide-aperture profiles, that run SW-NE for a total length of ~ 6 km in the hangingwall of the Paganica - S. Demetrio Fault, source of the 6th April 2009 (Mw 6.3) L'Aquila normal-faulting earthquake. Seismic tomography expands the knowledge of the basin with high spatial resolution and depth penetration (&gt; 300 m), illuminating the Meso-Cenozoic substratum that corresponds to high-Vp regions (Vp &gt; 3500-4000 m/s). Low Vp (1500-2000 m/s) lacustrine sediments (Early Pleistocene in age) are imaged only in the SW sector of the basin, where they are up to 200 m thick and lie below coarse fluvial and alluvial fan deposits. The overall infill consists of Early to Late Pleistocene alluvial fan and fluvial sediments between the Paganica Fault and the Bazzano ridge, with Vp reaching 3000 m/s for the oldest conglomeratic bodies. The substratum has an articulated topography. The main depocenter, ~ 350 m deep, is in the SW sector of the basin south of the Bazzano ridge. Remarkably, this depocenter and the overlying thick lacustrine body match the area of maximum coseismic subsidence observed after the 2009 earthquake. In the Paganica area, Vp images unravel large steps in the substratum related to two unreported SW-dipping buried strands, synthetic to the Paganica Fault, with ~ 250 m associated total vertical throw. This finding has important implications on the long-term history of the Paganica – S. Demetrio Fault system, whose total vertical displacement has been previously underestimated. An additional ~ 250 m vertical offset along this complex Quaternary extensional structure should therefore be considered.</description>
    <dc:date>2011-12-31T23:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8324">
    <title>Biogenic/Abiogenic Hydrocarbons’ Origin</title>
    <link>http://hdl.handle.net/2122/8324</link>
    <description>Title: Biogenic/Abiogenic Hydrocarbons’ Origin
Authors: Scalera, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia
Editors: Scalera, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Cwojdzinski, S.; Polish Geologic Survey
Abstract: The creation of hydrocarbons is linked to tectono-geologic processes and particularly&#xD;
to orogenesis, rifting, overthrusts, erosion, deposition of sediments, deep gas emissions,&#xD;
etc.. Many have claimed the inadequacy of plate tectonics in linearly explain a number&#xD;
of phenomena involved in hydrocarbons generation and geological processes, and many&#xD;
others defended the synthesis of hydrocarbons starting from inorganic minerals, proposing&#xD;
di erent geochemical processes. In this paper a possible mechanism for production of&#xD;
abiogenic hydrocarbons is proposed, linking it to a previously proposed orogenic isostatic&#xD;
model. While in plate tectonics the cold slab travels in contact with the lithosphere of the&#xD;
continental side, oxidizing materials faced to oxidizing materials, in this model a hightemperature&#xD;
reducing environment of undepleted mantle rises up and come in contact with&#xD;
the relatively cold oxidizing lithospheric environment. Non-lithostatic overpressures and a&#xD;
number of chemical reactions are then favoured in this sort of tectonic oxidizing-reducing&#xD;
pile, leading to a multiple origin of hydrocarbons. The actual situation along the Italian&#xD;
Apennines orogenic belt seems in accord to the proposed model in which an important&#xD;
role should have the abiogenic hydrocarbons in particular those produced by the tectonic&#xD;
working at the western margin of the Adriatic plate. However, albeit a continuous accumulation&#xD;
of hydrocarbons is witnessed by a number of planetary bodyes of the Solar system,&#xD;
no evaluation of the abiogenic/biogenic hydrocarbons rate is yet possible on our planet.</description>
    <dc:date>2011-12-31T23:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8104">
    <title>Buried archeological remains connected to the Greek-Roman harbor at Tindari (north-east Sicily): results from geomorphological and geophysical investigations</title>
    <link>http://hdl.handle.net/2122/8104</link>
    <description>Title: Buried archeological remains connected to the Greek-Roman harbor at Tindari (north-east Sicily): results from geomorphological and geophysical investigations
Authors: Bottari, C.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Urbini, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Bianca, M.; Università della Basilicata, Dipartimento di Strutture, Geotecnica, Geologia applicata all'Ingegneria,; D'Amico, M.; Università di Messina, Osservatorio sismologico; Marchetti, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Pizzolo, F.; Università di Messina, Osservatorio sismologico
Abstract: In recent years, detailed geoarcheological investigations have been&#xD;
carried out to search for traces of the ancient Tindari harbor (north-east&#xD;
Sicily, Italy). A digital terrain model supported the hypothesis that 2,000&#xD;
yr ago the Oliveri Basin was a suitable landing place that was protected&#xD;
from prevailing winds. This model was generated from uplift data, sea&#xD;
level changes, historical cartographic data and three-dimensional&#xD;
reconstruction of the sedimentary succession of the cover. The present&#xD;
position of some historical buildings represent an archeological marker&#xD;
of the shoreline progression. Recent excavations during the construction&#xD;
of the Messina-to-Palermo motorway brought to light some portions of an&#xD;
ancient archeological complex. The thickness of the walls and the volume&#xD;
of the collected archeological material suggests dating between the 1st&#xD;
century BC and the 4th century AD. After that time, heavy environmental&#xD;
changes due to human activities in the area led to inaccurate&#xD;
underestimation of the role of Tindari harbor in the past. A geophysical&#xD;
investigation was carried out in the area surrounding the archeological&#xD;
complex to search for new buried structures related to the ancient&#xD;
settlement, and to be open to any results of the paleotopographic&#xD;
reconstruction of the area. The applied geophysical techniques included&#xD;
passive seismic and ground-penetrating radar. This survey indicates the&#xD;
presence of buried structures, such as walls and floors, that probably&#xD;
belong to a Roman villa. Furthermore, it defines the depth of the Holocene&#xD;
sedimentary cover of the Oliveri coastal plain, which strengthens the&#xD;
hypothesis formulated for its morphological evolution.</description>
    <dc:date>2011-12-31T23:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8098">
    <title>Multivariate time series clustering on geophysical data recorded at Mt. Etna from 1996 to 2003</title>
    <link>http://hdl.handle.net/2122/8098</link>
    <description>Title: Multivariate time series clustering on geophysical data recorded at Mt. Etna from 1996 to 2003
Authors: Di Salvo, R.; Dipartimento di Ingegneria Elettrica, Elettronica e Informatica, Università degli Studi di Catania, Facoltà di Ingegneria, Italy; Montalto, P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Catania, Catania, Italia; Nunnari, G.; Dipartimento di Ingegneria Elettrica, Elettronica e Informatica, Università degli Studi di Catania, Facoltà di Ingegneria, Italy; Neri, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Catania, Catania, Italia; Puglisi, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Catania, Catania, Italia
Abstract: Time series clustering is an important task in data analysis issues in order to extract implicit, previously unknown,&#xD;
and potentially useful information froma large collection of data. Finding useful similar trends inmultivariate time&#xD;
series represents a challenge in several areas including geophysics environment research. While traditional time&#xD;
series analysis methods deal only with univariate time series, multivariate time series analysis is a more suitable&#xD;
approach in the field of researchwhere different kinds of data are available. Moreover, the conventional time series&#xD;
clustering techniques do not provide desired results for geophysical datasets due to the huge amount of data&#xD;
whose sampling rate is different according to the nature of signal. In this paper, a novel approach concerning geophysical&#xD;
multivariate time series clustering is proposed using dynamic time series segmentation and Self Organizing&#xD;
Maps techniques. This method allows finding coupling among trends of different geophysical data&#xD;
recorded from monitoring networks at Mt. Etna spanning from 1996 to 2003, when the transition from summit&#xD;
eruptions to flank eruptions occurred. This information can be used to carry out a more careful evaluation of the&#xD;
state of volcano and to define potential hazard assessment at Mt. Etna.</description>
    <dc:date>2012-12-31T23:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/8072">
    <title>Flank instability structure of Mt. Etna inferred by a magnetotelluric survey</title>
    <link>http://hdl.handle.net/2122/8072</link>
    <description>Title: Flank instability structure of Mt. Etna inferred by a magnetotelluric survey
Authors: Siniscalchi, A.; Dipartimento di Scienze della Terra e Geoambientali, Università di Bari, Bari, Italy; Tripaldi, S.; Dipartimento di Scienze della Terra e Geoambientali, Università di Bari, Bari, Italy; Neri, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Catania, Catania, Italia; Balasco, M.; Istituto di Metodologie per l’Analisi Ambientale, Consiglio Nazionale delle Ricerche, Tito, Potenza, Italy; Romano, G.; Dipartimento di Scienze della Terra e Geoambientali, Università di Bari, Bari, Italy; Ruch, J.; Dipartimento di Scienze Geologiche, Università di Roma Tre, Rome, Italy; Schiavone, D.; Dipartimento di Scienze Geologiche, Università di Roma Tre, Rome, Italy
Abstract: This paper presents a magnetotelluric (MT) survey of the unstable eastern flank of&#xD;
Mt. Etna. We take thirty soundings along two profiles oriented in the N-S and NW-SE&#xD;
directions, and from these data recover two 2D resistivity models of the subsurface.&#xD;
Both models reveal three major layers in a resistive-conductive-resistive sequence, the&#xD;
deepest extending to 14 km bsl. The shallow layer corresponds to the volcanic cover, and&#xD;
the intermediate conductive layer corresponds to underlying sediments segmented by&#xD;
faults. These two electrical units are cut by   E-W-striking faults. The third layer&#xD;
(basement) is interpreted as mainly pertinent to the Apennine-Maghrebian Chain associated&#xD;
with   SW-NE-striking regional faults. The detailed shapes of the resistivity profiles&#xD;
clearly show that the NE Rift is shallow-rooted ( 0–1 km bsl), thus presumably fed by&#xD;
lateral dikes from the central volcano conduit. The NW-SE profile suggests by a series of&#xD;
listric faults reaching up to 3 km bsl, then becoming almost horizontal. Toward the SE, the&#xD;
resistive basement dramatically dips (from  3 km to  10 km bsl), in correspondence with&#xD;
the Timpe Fault System. Several high-conductivity zones close to the main faults suggest&#xD;
the presence of hydrothermal activity and fluid circulation that could enhance flank&#xD;
instability. Our results provide new findings about the geometry of the unstable Etna flank&#xD;
and its relation to faults and subsurface structures.</description>
    <dc:date>2012-03-29T22:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/7970">
    <title>crustal fracturing field and presence of fluid as revealed by seismic anisotropy: case-histories from seismogenic areas in the Apennines</title>
    <link>http://hdl.handle.net/2122/7970</link>
    <description>Title: crustal fracturing field and presence of fluid as revealed by seismic anisotropy: case-histories from seismogenic areas in the Apennines
Authors: Pastori, Marina; Università degli studi di Perugia
Abstract: During the last decades, the study of seismic anisotropy has provided useful information for the interpretation and evaluation of the stress field and active crustal deformation. Seismic anisotropy can yield valuable information on upper crustal structure, fracture field, and presence of fluid-saturated rocks crossed by shear waves. Several studies worldwide demonstrate that seismic anisotropy is related to stress-aligned, filled-fluid micro-cracks (EDA model, Crampin et al., 1984b; Crampin, 1993).&#xD;
The seismic anisotropy is an almost ubiquitous property of the Earth and the Shear Wave Splitting is the most unambiguous indicator of anisotropy, but the automatic estimation of the splitting parameters is difficult because the effect of the anisotropy on a seismogram is a second order, not easily detectable effect. Different researchers developed automated techniques aimed to study the Shear Wave Splitting: in this study, the results of different codes are compared in order to evaluate the best method for automatic anisotropy evaluation.&#xD;
In the last three years, an automatic analysis code, “Anisomat+”, was developed, tested and improved to calculate the anisotropic parameters: fast polarization direction () and delay time (∂t). “Anisomat+” consists of a set of MatLab scripts able to retrieve automatically crustal anisotropy parameters from three-component seismic recordings of local earthquakes. It needs waveforms and hypocentral parameters in the format routinely archived by the Istituto Nazionale di Geofisica e Vulcanologia (INGV). &#xD;
The code uses horizontal component cross-correlation method: a mathematical algorithm aimed to measure the similarity of the pulse shape between two shear waves. &#xD;
Anisomat+ has been compared to other two automatic analysis codes (SPY and SHEBA) and tested on three zones of the Apennines (Val d’Agri, Tiber Valley and L’Aquila surroundings). It was observed that, if the number of measures is large enough, at each station the average values of the parameters (fast direction and delay time) are comparable.&#xD;
The main goal in developing of an automatic code was to have tool able to work on a big amount of data, in a short time, by reducing the errors due to the subjectivity. These two acquirements are very useful and are the basis to develop a quasi real-time monitoring of the anisotropic parameters.&#xD;
The anisotropic parameters, resulting from the automatic computation, have been interpreted to determine the fracture field geometries; for each area, I defined the dominant fast direction and the intensity of the anisotropy, interpreting these results in the light of the geological and structural setting and of two anisotropic interpretative models, proposed in the literature. In the first one, proposed by Zinke and Zoback (2000), the local stress field and cracks are aligned by tectonics phases and are not necessarily related to the presently active stress field. Therefore the anisotropic parameters variations are only space-dependent. In the second, EDA model (Crampin, 1993), and its development in the APE model (Zatsepin and Crampin, 1995) fluid-filled micro-cracks are aligned or ‘opened’ by the active stress field and the variation of the stress field might be related to the evolution of the pore pressure in time; therefore in this case the variation of the anisotropic parameters are both space- and time- dependent.&#xD;
I recognized that the average of fast directions, in the three selected areas, are oriented NW-SE, in agreement with the orientation of the active stress field, as suggested by the EDA model, proposed by Crampin (1993), but also, by the  proposed by Zinke and Zoback model; in fact, NW-SE direction corresponds also to the strike of the main fault structures in the three study regions. The mean values of the magnitude of the normalized delay time range from 0.005 s/km to 0.007 s/km and to 0.009 s/km, respectively for the L'Aquila (AQU) area, the High Tiber Valley (ATF) and the Val d'Agri (VA), suggesting a 3-4% of crustal anisotropy (Piccinini et al., 2006). &#xD;
In each area are also examined the spatial and temporal distribution of anisotropic parameters, which lead to some innovative observations, listed below.&#xD;
o	The higher values of normalized delay times have been observed in those zones where most of the seismic events occur. This aspect was further investigated, by evaluating the average seismic rate, in a time period, between years 2005 and 2010, longer than the lapse of time, analyzed in the anisotropic studies. This comparison has highlighted that the value of the normalised delay time is larger where the seismicity rate is higher.&#xD;
o	In the Alto Tiberina Fault area the higher values of normalised delay time are not only related to the presence of a high seismicity rate but also to the presence of a tectonically doubled carbonate succession. Therefore, also the lithology, plays a important role in hosting and preserving the micro-fracture network responsible for the anisotropic field. &#xD;
o	The observed temporal variations of anisotropic parameters, have been observed and related to the fluctuation of pore fluid pressure at depth possibly induced by different mechanisms in the different regions, for instance, changes in the water table level in Val D’Agri (Valoroso et al., GJI submitted), occurrence of the April 6th Mw=6.1 earthquake in L’Aquila (Lucente et al., 2010). &#xD;
Since these variations have been recognized, it is possible to affirm that the models that better fit my results, both in term of fast directions and of delay times, seems to be those proposed by Crampin (1993) and Zatsepin &amp; Crampin (1995), respectively EDA and APE models.</description>
    <dc:date>2011-02-16T23:00:00Z</dc:date>
  </item>
  <item rdf:about="http://hdl.handle.net/2122/7965">
    <title>A RESPER probe for measurements of RESistivity and PERmittivity</title>
    <link>http://hdl.handle.net/2122/7965</link>
    <description>Title: A RESPER probe for measurements of RESistivity and PERmittivity
Authors: Settimi, A.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia
Editors: Beatrice besson; LAP LAMBERT Academic Publishing GmbH &amp; Co. KG Heinrich-Böcking-Str. 6-8 66121; LAP LAMBERT Academic Publishing GmbH &amp; Co. KG Heinrich-Böcking-Str. 6-8 66121; LAP LAMBERT Academic Publishing GmbH &amp; Co. KG Heinrich-Böcking-Str. 6-8 66121; LAP LAMBERT Academic Publishing GmbH &amp; Co. KG Heinrich-Böcking-Str. 6-8 66121, Saarbrücken, Germany
Abstract: The electrical RESistivity and dielectric PERmittivity measuring device (RESPER) for non-invasive investigation of media is an exploiting electrical induction by means of capacitive coupling with media as terrestrial soils and concretes. The device utilizes a four-electrode probe to inject a radio frequency into a medium and register an induced current. Complex transfer impedance can be determined from a ratio between a potential measured across two electrodes, and an induced current flowing in the medium. Electrical parameters of resistivity and permittivity characterizing the medium can be established from the transfer impedance, using inversion formulas that also take into account the geometric ratio and position of the electrodes. The device exploits the in-phase and quadrature under sampling technique which, together with numerical operations performed by a microcontroller, allows the device to attain a required performance. It is possible to execute a number of numerical integrations which, combined with some circuit solutions, can reduce the amplitude and phase errors of the acquired signal. The device can operate at variable frequency, maintaining a suitable under-sampling frequency to fully exploit the analogical-digital acquisition performance both in velocity and dynamic range.</description>
    <dc:date>2012-05-15T22:00:00Z</dc:date>
  </item>
</rdf:RDF>

