<?xml version="1.0" encoding="UTF-8"?>
<rss xmlns:slash="http://purl.org/rss/1.0/modules/slash/" xmlns:apple-wallpapers="http://www.apple.com/ilife/wallpapers" xmlns:itunes="http://www.itunes.com/dtds/podcast-1.0.dtd" xmlns:g-custom="http://base.google.com/cns/1.0" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:creativeCommons="http://backend.userland.com/creativeCommonsRssModule" xmlns:taxo="http://purl.org/rss/1.0/modules/taxonomy/" xmlns:content="http://purl.org/rss/1.0/modules/content/" xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:g-core="http://base.google.com/ns/1.0" xmlns:cc="http://web.resource.org/cc/" xmlns:media="http://search.yahoo.com/mrss/" xmlns:opensearch="http://a9.com/-/spec/opensearch/1.1/" xmlns:georss="http://www.georss.org/georss" xmlns:geo="http://www.w3.org/2003/01/geo/wgs84_pos#" version="2.0">
  <channel>
    <title>DSpace Collection:</title>
    <link>http://hdl.handle.net/2122/248</link>
    <description />
    <pubDate>Tue, 21 May 2013 14:18:36 GMT</pubDate>
    <dc:date>2013-05-21T14:18:36Z</dc:date>
    <item>
      <title>Magnitude scale for LP events: a quantification scheme for volcanic quakes</title>
      <link>http://hdl.handle.net/2122/8682</link>
      <description>Title: Magnitude scale for LP events: a quantification scheme for volcanic quakes
Authors: Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Bianco, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Borgna, I.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: The peculiar source characteristics of long-period seismic events (time persistency of the source, low-frequency peaks in the source spectrum, absence of high-frequency radiation) prevent the formation of a definite high-frequency coda in the seismograms. In contrast, this is well formed in volcano–tectonic quakes. For this reason, the widely used duration magnitude scale that is based on the proportionality between the energy and the coda duration cannot be used for long-period estimation. In observatory practice, the long-period magnitude is sometimes estimated using the same duration magnitude scale, leading to confusing results. In this report, we show a new method to estimate the magnitude of long-period events that generally occur for volcanoes, with some application examples from data for Mt Etna (Italy), Colima Volcano (Mexico) and Campi Flegrei (Italy).</description>
      <pubDate>Sun, 28 Apr 2013 22:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8682</guid>
      <dc:date>2013-04-28T22:00:00Z</dc:date>
    </item>
    <item>
      <title>Joint observation of coherent coda waves at surface and underground arrays</title>
      <link>http://hdl.handle.net/2122/8668</link>
      <description>Title: Joint observation of coherent coda waves at surface and underground arrays
Authors: La Rocca, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Galluzzo, D.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Scarpa, R.; Università di Salerno
Abstract: Local and regional seismicity jointly recorded by two dense small aperture arrays, one installed at surface and one at 1.3 km depth, constitutes an interesting data set useful for coda observations. Applying array techniques to earthquakes recorded at the two arrays we measure slowness, backazimuth and correlation coefficient of the coherent coda wave signals in five frequency bands in the range 1–10 Hz. Slowness distributions show marked differences between surface and underground, with slow signals at surface (slowness greater than 1.0 s km−1) that&#xD;
are not observed underground. We interpret these coherent signals as surface waves produced by the interaction of body waves with the free surface characterized by rough topography.&#xD;
The backazimuth values measured in the frequency bands centred at 1.5 and 3 Hz are almost uniformly distributed between 0 and 360◦, while those measured at higher frequencies show different distributions between surface and underground. On the contrary, the earthquake envelopes&#xD;
show very similar coda shapes between surface and underground recordings, with an&#xD;
almost constant coda-amplitude ratio (between 4 and 8) in a wide frequency range.</description>
      <pubDate>Mon, 15 Apr 2013 22:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8668</guid>
      <dc:date>2013-04-15T22:00:00Z</dc:date>
    </item>
    <item>
      <title>A Multidisciplinary Study of the DPRK Nuclear Tests</title>
      <link>http://hdl.handle.net/2122/8652</link>
      <description>Title: A Multidisciplinary Study of the DPRK Nuclear Tests
Authors: Carluccio, R.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Giuntini, A.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Materni, V.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Chiappini, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Bignami, C.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione CNT, Roma, Italia; D'Ajello Caracciolo, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Pignatelli, A.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia; Stramondo, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione CNT, Roma, Italia; Console, R.; Chiappini, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma2, Roma, Italia
Abstract: The Democratic People Republic of Korea announced&#xD;
two underground nuclear tests carried out in their territory respectively&#xD;
on October 9th, 2006 and May 25th, 2009. The scarce&#xD;
information on the precise location and the size of those explosions&#xD;
has stimulated various kinds of studies,mostly based on seismological&#xD;
observations, by several national agencies concerned with theNuclear&#xD;
Test Ban Treaty verification.Weanalysed the available seismological&#xD;
data collected through a global high-quality network for the two tests.&#xD;
After picking up the arrival times at the various stations, a standard&#xD;
location program has been applied to the observed data. If we use all&#xD;
the available data for each single event, due to the different magnitude&#xD;
and different number of available stations, the locations appear quite&#xD;
different. On the contrary, if we use only the common stations, they&#xD;
happen to be only few km apart from each other and within their&#xD;
respective error ellipses. A more accurate relative location has been&#xD;
carried out by the application of algorithms such as double difference&#xD;
joint hypocenter determination (DDJHD) and waveform alignment.&#xD;
The epicentral distance between the two events obtained by these&#xD;
methods is 2 km, with the 2006 event shifted to the ESE with respect&#xD;
to that of 2009. We then used a dataset of VHR TerraSAR-X satellite&#xD;
images to detect possible surface effects of the underground tests. This&#xD;
is the first ever case where these highly performing SAR data have&#xD;
been used to such aim. We applied InSAR processing technique to&#xD;
fully exploit the capabilities of SAR data to measure very short displacements&#xD;
over large areas. Two interferograms have been&#xD;
computed, one co-event and one post-event, to remove possible&#xD;
residual topographic signals. A clear displacement pattern has been&#xD;
highlighted over a mountainous area within the investigated region,&#xD;
measuring a maximum displacement of about 45 mm overall the&#xD;
relief. Hypothesizing that the 2009 nuclear test had been carried out&#xD;
close to the area where the displacement has been observed through&#xD;
the DInSAR technique, its relation with the epicenter location&#xD;
obtained through seismological processing has been discussed as a&#xD;
possible alternative hypothesis with respect to the preferred solutions&#xD;
reported by the nuclear explosion database (NEDB). The distance of&#xD;
about 10 km between the two places can be considered acceptable in&#xD;
light of the possible systematic location shifts commonly observed in&#xD;
the seismological practice over a global scale. The difference between&#xD;
the mb magnitudes of the two tests could reflect differences in geological&#xD;
conditions of the two test sites, even if the yield of the two&#xD;
explosions had been the same.</description>
      <pubDate>Fri, 28 Dec 2012 23:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8652</guid>
      <dc:date>2012-12-28T23:00:00Z</dc:date>
    </item>
    <item>
      <title>Frequency dependent Qα and Qβ in the Umbria-Marche (Italy) region using a quadratic approximation of the coda-normalization method</title>
      <link>http://hdl.handle.net/2122/8639</link>
      <description>Title: Frequency dependent Qα and Qβ in the Umbria-Marche (Italy) region using a quadratic approximation of the coda-normalization method
Authors: De Lorenzo, S.; Dipartimento di Scienze della Terra e geoambientali, University of Bari; Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Bianco, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: The coda normalization method is one of the most used methods in the inference of attenuation&#xD;
parameters Qα and Qβ . Since, in this method, the geometrical spreading exponent γ is an&#xD;
unknown model parameter, the most part of studies assumes a fixed γ , generally equal to&#xD;
1. However γ and Q could be also jointly inferred from the non-linear inversion of codanormalized&#xD;
logarithms of amplitudes, but the trade-off between γ and Q could give rise to&#xD;
unreasonable values of these parameters. To minimize the trade-off between γ and Q, an&#xD;
inversion method based on a parabolic expression of the coda-normalization equation has&#xD;
been developed. The method has been applied to the waveforms recorded during the 1997&#xD;
Umbria-Marche seismic crisis. The Akaike criterion has been used to compare results of the&#xD;
parabolic model with those of the linear model, corresponding to γ = 1. A small deviation&#xD;
from the spherical geometrical spreading has been inferred, but this is accompanied by a&#xD;
significant variation of Qα and Qβ values. For almost all the considered stations, Qα smaller&#xD;
than Qβ has been inferred, confirming that seismic attenuation, in the Umbria-Marche region,&#xD;
is controlled by crustal pore fluids.</description>
      <pubDate>Mon, 31 Dec 2012 23:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8639</guid>
      <dc:date>2012-12-31T23:00:00Z</dc:date>
    </item>
    <item>
      <title>Qc, Qb, Qi and Qs attenuation parameters in the Umbria–Marche (Italy) region</title>
      <link>http://hdl.handle.net/2122/8638</link>
      <description>Title: Qc, Qb, Qi and Qs attenuation parameters in the Umbria–Marche (Italy) region
Authors: De Lorenzo, S.; Dipartimento di Scienze della Terra e geoambientali, University of Bari; Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Bianco, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: The attenuation of coda and S waves has been inferred for the Umbria–Marche region (central Italy) using&#xD;
seismic waveforms collected during the 1997 seismic crisis. The selected dataset is composed of 343&#xD;
small magnitude (1.4 &lt; ML &lt; 4.2) earthquakes recorded at a temporary array composed of 23 seismic stations.&#xD;
The Sato (1977) method, based on the assumption of single isotropic scattering has been used to&#xD;
infer Qc, considering three different lapse times (20, 30 and 40 s). The coda normalization method (Aki,&#xD;
1980) has been used to infer Qb. Both Qc and Qb show a clear frequency dependence with a different frequency&#xD;
dependent parameter. The frequency dependence of Qc is comparable with that previously found&#xD;
in the same area and around it. Using the method of Wennerberg (1993), intrinsic and scattering attenuation&#xD;
have been separated. Intrinsic attenuation is found to be close to coda attenuation and dominates&#xD;
over scattering dissipation. Coda Q increases with increasing lapse time but at a rate smaller than that&#xD;
observed in other areas of the Earth. Coda and intrinsic attenuation in the Umbria–Marche region are very&#xD;
high compared to other seismic active regions of the Earth. The retrieved high values of intrinsic attenuation&#xD;
may be explained in terms of the previously hypothesized fluid-pressurized regime of the crust in&#xD;
the central Apennines (Miller et al., 2004).</description>
      <pubDate>Mon, 31 Dec 2012 23:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8638</guid>
      <dc:date>2012-12-31T23:00:00Z</dc:date>
    </item>
    <item>
      <title>Overview on the strong motion data recorded during the May-June 2012 Emilia seismic sequence</title>
      <link>http://hdl.handle.net/2122/8590</link>
      <description>Title: Overview on the strong motion data recorded during the May-June 2012 Emilia seismic sequence
Authors: Luzi, L.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Pacor, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Ameri, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Puglia, R.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Burrato, P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Massa, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Augliera, P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Franceschina, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Lovati, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Milano-Pavia, Milano, Italia; Castro, R.; Departamento de Sismología, División Ciencias de la Tierra, centro de Investigación Científica y de Educación Superior de Ensenada (CICESE), Ensenada, Baja California, 22860, México.
Abstract: On 20 May 2012, at 02:03:52 GMT, an earthquake with Mw 6.1 (RCMT, http://www.bo.ingv.it/RCMT) occurred in northern Italy striking a densely populated area. The mainshock was followed a few hours later by two severe aftershocks having the same local magnitude (Ml 5.1, 1 and 2 in Figure 1a), and by hundreds of smaller aftershocks. Nine days later, on 29 May, at 07:00:03 GMT, a second event with moment magnitude Mw 6.0 (RCMT, http://www.bo.ingv.it/RCMT) occurred to the west, on an adjacent fault segment. This event was also followed by hundreds of aftershocks, three of them having local magnitude 5.3, 5.2 and 5.1 (3, 4 and 5, respectively, in Figure 1a) (locations from Istituto Nazionale di Geofisica e Vulcanologia, hereinafter INGV, http://iside.rm.ingv.it/; Malagnini et al., 2012; Scognamiglio et al., 2012). Despite the moderate number of casualties if compared to other major events in the Italian history, the economic loss was extremely high, resulting in about EUR 5 billion (AON Benfield, 2012, http://www.aon.com/), as the majority of Italian industrial activities and infrastructures concentrate in this area, the eastern Po plain, which is the largest sedimentary basin in Italy.&#xD;
The mainshocks are associated to two thrust faults with an approximate E-W trend dipping to the South (Figure 1b). The majority of the faults in this region are located in the upper crust, at depths lower than 10 km. The two main shocks are among the strongest earthquakes generated by thrust faults ever recorded in Italy in the instrumental era. The Emilia sequence has been extensively recorded by several strong-motion networks, operating in the Italian territory and neighbouring countries. Some of the networks acquire continuous data streams at their national data centres, which are nodes of EIDA (European Integrated Data Archive, hhtp://eida.rm.ingv.it), a federation of several archives, so that the waveforms can be obtained immediately after the occurrence of an event. Other networks, such as the Italian accelerometric network (RAN), managed by the Italian Department of the Civil Protection (hereinafter DPC), distribute the acceleration waveforms through their web site (http://protezionecivile.gov.it). The data set explored in this study is relative to the six events of the sequence having Ml &gt; 5 (Table 1) and consists in 365 accelerograms recorded within a distance of 200 km from the epicentres, that were provided by the permanent and temporary seismic networks of INGV, the Swiss Seismological Service (SED, http://www.seismo.ethz.ch/index) and the DPC.</description>
      <pubDate>Mon, 31 Dec 2012 23:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8590</guid>
      <dc:date>2012-12-31T23:00:00Z</dc:date>
    </item>
    <item>
      <title>Detection of Seismic Signals from Background Noise in the Area of Campi Flegrei: Limits of the Present Seismic Monitoring</title>
      <link>http://hdl.handle.net/2122/8553</link>
      <description>Title: Detection of Seismic Signals from Background Noise in the Area of Campi Flegrei: Limits of the Present Seismic Monitoring
Authors: Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Bianco, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Castellano, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Cusano, P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Galluzzo, D.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; La Rocca, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Petrosino, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: In the present paper, we will describe the field survey&#xD;
(Fig. 1) and the data analysis of an experiment carried out&#xD;
to put constraints on the magnitude detection threshold in the area of Campi Flegrei. Results show that seismic radiation&#xD;
emitted from VT seismic events at frequency lower than 2 Hz&#xD;
has a high detection threshold (minimum magnitude around&#xD;
1.5). In the range between 2 and 20 Hz, VT events with magnitudes smaller than about 0.5 have a high probability to be undetected. This result indicates that noise reduction through borehole stations and/or small arrays is essential for an accurate seismic monitoring in the Campi Flegrei area.</description>
      <pubDate>Thu, 28 Feb 2013 23:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8553</guid>
      <dc:date>2013-02-28T23:00:00Z</dc:date>
    </item>
    <item>
      <title>Rete Mobile e Laboratorio Analisi aVanzate (LAV) - Rendiconto 2012</title>
      <link>http://hdl.handle.net/2122/8532</link>
      <description>Title: Rete Mobile e Laboratorio Analisi aVanzate (LAV) - Rendiconto 2012
Authors: Cusano, P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Galluzzo, D.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; La Rocca, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Petrosino, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Bianco, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Castellano, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: In the text</description>
      <pubDate>Mon, 31 Dec 2012 23:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8532</guid>
      <dc:date>2012-12-31T23:00:00Z</dc:date>
    </item>
    <item>
      <title>Rete Mobile e Laboratorio Analisi aVanzate (LAV) - Rendiconto I semestre 2012</title>
      <link>http://hdl.handle.net/2122/8531</link>
      <description>Title: Rete Mobile e Laboratorio Analisi aVanzate (LAV) - Rendiconto I semestre 2012
Authors: Cusano, P.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Galluzzo, D.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; La Rocca, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Petrosino, S.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Bianco, F.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Castellano, M.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia; Del Pezzo, E.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione OV, Napoli, Italia
Abstract: In the text</description>
      <pubDate>Sat, 30 Jun 2012 22:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8531</guid>
      <dc:date>2012-06-30T22:00:00Z</dc:date>
    </item>
    <item>
      <title>Mapping the Moho Across the Northern and Central Apennine Chain and Eastern Sicily - The Teleseismic Receiver Functions Method</title>
      <link>http://hdl.handle.net/2122/8517</link>
      <description>Title: Mapping the Moho Across the Northern and Central Apennine Chain and Eastern Sicily - The Teleseismic Receiver Functions Method
Authors: Mele, Giuliana; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia
Editors: Scalera, G.; Istituto Nazionale di Geofisica e Vulcanologia, Sezione Roma1, Roma, Italia; Boschi, E.; Cwojdzinski, S.
Abstract: Waveforms of seismic events occurred at epicentral distances ranging from 30 &#xD;
to 90 , and recorded by 3-component stations installed in peninsular Italy and in eastern&#xD;
Sicily, were analyzed using the receiver function technique. Receiver functions are time&#xD;
series where the arrivals of P-to-S waves converted at marked velocity contrasts beneath a&#xD;
seismometer are enhanced. Teleseismic receiver functions are frequently used to identify&#xD;
waves converted at the Moho discontinuity to infer crustal thickness. Across the northern&#xD;
Apennines, receiver functions show that west of this chain (i.e. beneath the Elba island and&#xD;
Tuscany) the Moho is flat and shallow, while it deepens from the eastern coast of the peninsula&#xD;
toward the chain. Two Ps conversions are observed at a station located in the Tiberina&#xD;
valley, indicating the presence of the Moho at depths of about 20 and 52 km. More to the&#xD;
south, across the central Apennines, the Moho is shallower beneath the Tyrrhenian margin&#xD;
of the peninsula than beneath the Adriatic margin, and deepens from both sides toward the&#xD;
Apennines. The largest crustal thickness is inferred in the area of highest topography. The&#xD;
Moho depths estimated with the receiver function technique are in agreement with the interpretation&#xD;
of active seismic data in the western margin of peninsular Italy and along the&#xD;
Adriatic coast, while they are significantly larger beneath the Apennines. Results of an ongoing&#xD;
study in eastern Sicily show that Moho depth increases from north to south. In this&#xD;
area, the northernmost stations show a also a later Ps converted by a lower interface.</description>
      <pubDate>Mon, 03 Oct 2011 22:00:00 GMT</pubDate>
      <guid isPermaLink="false">http://hdl.handle.net/2122/8517</guid>
      <dc:date>2011-10-03T22:00:00Z</dc:date>
    </item>
  </channel>
</rss>

