13 research outputs found
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PDA-based system for monitoring electromagnetic signals
The development of a mobile system for receiving, storing, and displaying electromagnetic-signals (EM) at specific frequencies using mobile devices and wireless networks, is of extreme interest, especially when the final means of display is a PDA, a very light and compact handheld device. In the present study, an application is developed for remote monitoring of EM-signals preceding seismic events. The particular advantages and challenges faced when developing such application are explained and future work in this area is presented
Unified approach to catastrophic events: from the normal state to geological or biological shock in terms of spectral fractal and nonlinear analysis
An important question in geophysics is whether earthquakes (EQs) can be anticipated prior to their occurrence. Pre-seismic electromagnetic (EM) emissions provide a promising window through which the dynamics of EQ preparation can be investigated. However, the existence of precursory features in pre-seismic EM emissions is still debatable: in principle, it is difficult to prove associations between events separated in time, such as EQs and their EM precursors. The scope of this paper is the investigation of the pre-seismic EM activity in terms of complexity. A basic reason for our interest in complexity is the striking similarity in behavior close to irreversible phase transitions among systems that are otherwise quite different in nature. Interestingly, theoretical studies (Hopfield, 1994; Herz and Hopfield 1995; Rundle et al., 1995; Corral et al., 1997) suggest that the EQ dynamics at the final stage and neural seizure dynamics should have many similar features and can be analyzed within similar mathematical frameworks. Motivated by this hypothesis, we evaluate the capability of linear and non-linear techniques to extract common features from brain electrical activities and pre-seismic EM emissions predictive of epileptic seizures and EQs respectively. The results suggest that a unified theory may exist for the ways in which firing neurons and opening cracks organize themselves to produce a large crisis, while the preparation of an epileptic shock or a large EQ can be studied in terms of ''Intermittent Criticality''
Discrimination between pre-seismic electromagnetic anomalies and solar activity effects
Laboratory studies suggest that electromagnetic emissions in a wide frequency spectrum ranging from kilohertz (kHz) to very high megahertz (MHz) frequencies are produced by the opening of microcracks, with the MHz radiation appearing earlier than the kHz radiation. Earthquakes are large-scale fracture phenomena in the Earth's heterogeneous crust. Thus, the radiated kHz-MHz electromagnetic emissions are detectable not only in the laboratory but also at a geological scale. Clear MHz-to-kHz electromagnetic anomalies have been systematically detected over periods ranging from a few days to a few hours prior to recent destructive earthquakes in Greece. We should bear in mind that whether electromagnetic precursors to earthquakes exist is an important question not only for earthquake prediction but mainly for understanding the physical processes of earthquake generation. An open question in this field of research is the classification of a detected electromagnetic anomaly as a pre-seismic signal associated with earthquake occurrence. Indeed, electromagnetic fluctuations in the frequency range of MHz are known to be related to a few sources, including atmospheric noise (due to lightning), man-made composite noise, solar-terrestrial noise (resulting from the Sun-solar wind-magnetosphere-ionosphere-Earth's surface chain) or cosmic noise, and finally, the lithospheric effect, namely pre-seismic activity. We focus on this point in this paper. We suggest that if a combination of detected kHz and MHz electromagnetic anomalies satisfies the set of criteria presented herein, these anomalies could be considered as candidate precursory phenomena of an impending earthquake. © 2009 The Royal Swedish Academy of Sciences
On the response of Y3Al5O12 : Ce (YAG : Ce) powder scintillating screens to medical imaging X-rays
The aim of this study was to examine Y3Al5O12:Ce (also known as YAG:Ce)
powder scintillator under X-ray imaging conditions. This material shows
a very fast scintillation decay time and it has never been used in X-ray
medical imaging. In the present study various scintillator layers
(screens) with coating thickness ranging from 13 to 166 mg/cm(2) were
prepared in our laboratory by sedimentation of Y3Al5O12: Ce powder.
Optical emission spectra and light emission efficiency (spectrum area
over X-ray exposure) of the layers were measured under X-ray excitation
using X-ray tube voltages (80-120 kVp) often employed in general medical
radiography and fluoroscopy. Spectral compatibility with various optical
photon detectors (photodiodes, photocathodes, charge coupled devices,
films) and intrinsic conversion efficiency values were determined using
emission spectrum data. In addition, parameters related to X-ray
detection, energy absorption efficiency and K-fluorescence
characteristic emission were calculated. A theoretical model describing
radiation and light transfer through scattering media was used to fit
experimental data. Intrinsic conversion efficiency (eta(C) approximate
to 0.03-0.05) and light attenuation coefficients (sigma approximate to
26.5 cm(2)/g) were derived through this fitting. Y3Al5O12:Ce showed peak
emission in the wavelength range 530-550 nm. The light emission
efficiency was found to be maximum for the 107 mg/cm(2) layer. Due to
its “green” emission spectrum, Y3Al5O12:Ce showed excellent
compatibility (of the order of 0.9) with the sensitivity of many
currently used photodetectors. Taking into account its very fast
response Y3Al5O12:Ce could be considered for application in X-ray
imaging especially in various digital detectors. (C) 2004 Published by
Elsevier B.V
Light emission efficiency and imaging performance of Y3Al5O12: Ce (YAG : Ce) powder screens under diagnostic radiology conditions
In this study Y3Al5O12: Ce powder scintillator was evaluated for use in
X-ray imaging detectors. This phosphor, also known as YAG: Ce
scintillator or P-46 phosphor, is a non-hygroscopic, emitting green
light with very short decay time. These properties are very attractive
for X-ray imaging. Y3Al5O12: Ce powder was used to prepare various test
screens ( 33 - 166 mg/cm(2)). Absolute luminescence efficiency
measurements were performed for various X-ray tube voltages ( 50 - 130
kVp). In addition parameters related to image quality such as the
modulation transfer function and the detective quantum efficiency were
examined. A theoretical model, describing radiation and light transfer,
was employed to fit experimental data and to estimate values of optical
parameters. Absolute efficiency was found to decrease with X-ray tube
voltage. Highest efficiency was obtained for the 107 mg/cm(2) screen.
Light attenuation coefficients were close to those of green emitting
rare earth scintillators. At low spatial frequencies the detective
quantum efficiency was high for the 107 - 166 mg/cm(2) screens. The
light emission efficiency and imaging performance of Y3Al5O12: Ce was
not better than currently employed scintillators. However due to its
very fast response and high spectral compatibility to optical sensors it
may be considered for use in digital imaging detectors
Imaging properties of cerium doped Yttrium Aluminum Oxide (YAP:Ce) powder scintillating screens under X-ray excitation
The aim of the present study was to evaluate the imaging performance of YAP:Ce powder scintillating screens under exposure conditions employed in diagnostic radiology (50-140 kV). Various screens were prepared in our laboratory from YAP: Ce powder (Phosphor Technology, Ltd.), with coating thickness ranging from 53 to 110 mg/cm2. The imaging performance of the screens was assessed by experimental determination of the modulation transfer function (MTF) and the noise transfer function (NTF). MTF was determined by the edge spread function (ESF) method while NTF was estimated by noise power spectrum (NPS) measurements after uniform screen irradiation. In addition, parameters related to overall image quality, such as the signal-to-noise ratio transfer (MTF/NTF), were estimated. MTF curves were affected by the beam hardening effects caused by the patient simulating 20 mm thick aluminum phantom. Under these conditions MTF values were found to increase with the mean X-ray photon energy. A similar effect was observed for NTF curves. Results were compared with data obtained on CsI:Tl scintillator. Taking into consideration the very fast response of YAP:Ce, these data may be of interest in designing X-ray imaging detectors. © 2006 Elsevier B.V. All rights reserved
Imaging properties of cerium doped Yttrium Aluminum Oxide (YAP:Ce) powder scintillating screens under X-ray excitation
The aim of the present study was to evaluate the imaging performance of YAP:Ce powder scintillating screens under exposure conditions employed in diagnostic radiology (50-140 kV). Various screens were prepared in our laboratory from YAP: Ce powder (Phosphor Technology, Ltd.), with coating thickness ranging from 53 to 110 mg/cm2. The imaging performance of the screens was assessed by experimental determination of the modulation transfer function (MTF) and the noise transfer function (NTF). MTF was determined by the edge spread function (ESF) method while NTF was estimated by noise power spectrum (NPS) measurements after uniform screen irradiation. In addition, parameters related to overall image quality, such as the signal-to-noise ratio transfer (MTF/NTF), were estimated. MTF curves were affected by the beam hardening effects caused by the patient simulating 20 mm thick aluminum phantom. Under these conditions MTF values were found to increase with the mean X-ray photon energy. A similar effect was observed for NTF curves. Results were compared with data obtained on CsI:Tl scintillator. Taking into consideration the very fast response of YAP:Ce, these data may be of interest in designing X-ray imaging detectors. © 2006 Elsevier B.V. All rights reserved