<?xml version="1.0" encoding="UTF-8"?>
<rdf:RDF xmlns:rdf="http://www.w3.org/1999/02/22-rdf-syntax-ns#" xmlns:dcterms="http://purl.org/dc/terms/" xmlns:prism="http://prismstandard.org/namespaces/1.2/basic/" xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns="http://purl.org/rss/1.0/"><channel rdf:about="http://www.physicamedicaonline.com/?rss=yes"><title>Physica Medica: European Journal of Medical Physics</title><description>Physica Medica: European Journal of Medical Physics RSS feed: Current Issue.    Physica Medica is the official journal of the  Associazione Italiana 
di Fisica Medica , the  European Federation of Organisations for Medical Physics  
and the  Irish Association of Physicists in Medicine  . 
 
Physica Medica, European 
Journal of Medical Physics, publishing with Elsevier from 2007, provides an international forum for research and reviews on the following 
main topics: 
 
  Medical Imaging 
  Radiation Therapy	 
  Radiation Protection 
 Measuring Systems and 
Signal Processing 
 Education and training in Medical Physics 
 Professional issues in Medical Physics 
 
 
 
Contributions 
on other topics related to Applications of Physics to Biology and Medicine and in particular related to new emerging fields such as Molecular 
Imaging, Hadrontherapy, System biology, Nanoparticles and Nanotechnologies, etc. are strongly encouraged.   </description><link>http://www.physicamedicaonline.com/?rss=yes</link><dc:publisher>Elsevier Inc.</dc:publisher><dc:language>en</dc:language><dc:rights> © 2010 Published by Elsevier Inc. All rights reserved. </dc:rights><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:issn>1120-1797</prism:issn><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:publicationDate>April 2012</prism:publicationDate><prism:copyright> © 2010 Published by Elsevier Inc. All rights reserved. </prism:copyright><prism:rightsAgent>healthpermissions@elsevier.com</prism:rightsAgent><items><rdf:Seq><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179712000087/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179712000191/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS112017971200004X/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000287/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000226/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000238/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000275/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000299/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000305/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000214/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000251/abstract?rss=yes"/><rdf:li rdf:resource="http://www.physicamedicaonline.com/article/PIIS1120179711000263/abstract?rss=yes"/></rdf:Seq></items></channel><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179712000087/abstract?rss=yes"><title>Aims &amp; Scope &amp; Editorial Board</title><link>http://www.physicamedicaonline.com/article/PIIS1120179712000087/abstract?rss=yes</link><description></description><dc:title>Aims &amp; Scope &amp; Editorial Board</dc:title><dc:creator></dc:creator><dc:identifier>10.1016/S1120-1797(12)00008-7</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2012-04-01</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2012-04-01</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section></prism:section><prism:startingPage>IFC</prism:startingPage><prism:endingPage>IFC</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179712000191/abstract?rss=yes"><title>Announcement: Galileo Galilei Award</title><link>http://www.physicamedicaonline.com/article/PIIS1120179712000191/abstract?rss=yes</link><description></description><dc:title>Announcement: Galileo Galilei Award</dc:title><dc:creator></dc:creator><dc:identifier>10.1016/S1120-1797(12)00019-1</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2012-04-01</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2012-04-01</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section></prism:section><prism:startingPage>93</prism:startingPage><prism:endingPage>93</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS112017971200004X/abstract?rss=yes"><title>Iterative reconstruction methods in X-ray CT</title><link>http://www.physicamedicaonline.com/article/PIIS112017971200004X/abstract?rss=yes</link><description>Abstract: Iterative reconstruction (IR) methods have recently re-emerged in transmission x-ray computed tomography (CT). They were successfully used in the early years of CT, but given up when the amount of measured data increased because of the higher computational demands of IR compared to analytical methods. The availability of large computational capacities in normal workstations and the ongoing efforts towards lower doses in CT have changed the situation; IR has become a hot topic for all major vendors of clinical CT systems in the past 5 years.This review strives to provide information on IR methods and aims at interested physicists and physicians already active in the field of CT. We give an overview on the terminology used and an introduction to the most important algorithmic concepts including references for further reading. As a practical example, details on a model-based iterative reconstruction algorithm implemented on a modern graphics adapter (GPU) are presented, followed by application examples for several dedicated CT scanners in order to demonstrate the performance and potential of iterative reconstruction methods. Finally, some general thoughts regarding the advantages and disadvantages of IR methods as well as open points for research in this field are discussed.</description><dc:title>Iterative reconstruction methods in X-ray CT</dc:title><dc:creator>Marcel Beister, Daniel Kolditz, Willi A. Kalender</dc:creator><dc:identifier>10.1016/j.ejmp.2012.01.003</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2012-02-10</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2012-02-10</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Reviews</prism:section><prism:startingPage>94</prism:startingPage><prism:endingPage>108</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000287/abstract?rss=yes"><title>From analytic inversion to contemporary IMRT optimization: Radiation therapy planning revisited from a mathematical perspective</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000287/abstract?rss=yes</link><description>Abstract: In this paper we look at the development of radiation therapy treatment planning from a mathematical point of view. Historically, planning for Intensity-Modulated Radiation Therapy (IMRT) has been considered as an inverse problem. We discuss first the two fundamental approaches that have been investigated to solve this inverse problem: Continuous analytic inversion techniques on one hand, and fully-discretized algebraic methods on the other hand. In the second part of the paper, we review another fundamental question which has been subject to debate from the beginning of IMRT until the present day: The rotation therapy approach versus fixed angle IMRT. This builds a bridge from historic work on IMRT planning to contemporary research in the context of Intensity-Modulated Arc Therapy (IMAT).</description><dc:title>From analytic inversion to contemporary IMRT optimization: Radiation therapy planning revisited from a mathematical perspective</dc:title><dc:creator>Yair Censor, Jan Unkelbach</dc:creator><dc:identifier>10.1016/j.ejmp.2011.04.002</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-05-27</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-05-27</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Reviews</prism:section><prism:startingPage>109</prism:startingPage><prism:endingPage>118</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000226/abstract?rss=yes"><title>On impulse response functions computed from dynamic contrast-enhanced image data by algebraic deconvolution and compartmental modeling</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000226/abstract?rss=yes</link><description>Abstract: Concentration-time courses measured by dynamic contrast-enhanced (DCE) imaging can be described by a convolution of the arterial input with an impulse response function, QT(t), characterizing tissue microcirculation. Data analysis is based on two different approaches: computation of QT(t) by algebraic deconvolution (AD) and subsequent evaluation according to the indicator dilution theory (IDT) or parameterization of QT(t) by analytical expressions derived by compartmental modeling. Pitfalls of both strategies will be addressed in this study.Tissue data acquired by DCE-CT in patients with head-and-neck cancer and simulated by a reference model (MMID4) were analyzed by a two-compartment model (TCM), a permeability-limited two-compartment model (PL-TCM) and AD. Additionally, MMID4 was used to compute the ‘true’ response function that corresponds to the simulated tumor data.TCM and AD yielded accurate fits, whereas PL-TCM performed worse. Nevertheless, the corresponding response functions diverge markedly. The response curves obtained by TCM decrease exponentially in the early perfusion phase and overestimate the tissue perfusion, QT(0). AD also resulted in response curves starting with a negative slope and not – as the ‘true’ response function in accordance with the IDT – with a horizontal plateau. They are thus not valid responses in the sense of the IDT that can be used unconditionally for parameter estimation.Response functions differing considerably in shape can result in virtually identical tissue curves. This non-uniqueness makes a strong argument not to use algebraic but rather analytical deconvolution to reduce the class of solutions to representatives that are in accordance with a-priori knowledge. To avoid misinterpretations and systematic errors, users must be aware of the pitfalls inherent to the different concepts.</description><dc:title>On impulse response functions computed from dynamic contrast-enhanced image data by algebraic deconvolution and compartmental modeling</dc:title><dc:creator>Gunnar Brix, Mona Salehi Ravesh, Stefan Zwick, Jürgen Griebel, Stefan Delorme</dc:creator><dc:identifier>10.1016/j.ejmp.2011.03.004</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-04-15</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-04-15</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Original Papers</prism:section><prism:startingPage>119</prism:startingPage><prism:endingPage>128</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000238/abstract?rss=yes"><title>A dosimetry method in the transverse plane of HDR Ir-192 brachytherapy source using gafchromic EBT2 film</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000238/abstract?rss=yes</link><description>Abstract: Radiochromic film dosimetry is increasingly used in brachytherapy applications for its higher resolution ability as compared to other experimental methods. The present study was aimed to assess the accuracy and suitability of use of the improved radiochromic film model, Gafchromic EBT2, to evaluate the dose distribution in the transverse plane of microselectron HDR 192Ir source.A specially designed and locally fabricated Polymethyl methacrylate (PMMA) phantom was used in this work for the experimental measurement of dose distribution around the source in its transverse plane. The AAPM TG-43U1 recommended radial dose function, g (r), and dose rate constant, Λ, for the source were measured using Gafchromic EBT2 film and thermoluminescent dosimeters (TLD). The EBT2 film measured dosimetric quantities were validated against their values obtained from the TLD measurements and previously published values for the same source available in literature.The dose rate constant and radial dose function for microselectron HDR 192Ir source obtained from Gafchromic EBT2 film measurements are in agreement with their TLD measured results within 3.9% and 2.8% respectively. They also agree within the accepted range of uncertainty with their experimental and Monte Carlo calculated results reported in literature.This work demonstrates the suitability of using Gafchromic EBT2 film dosimetry in characterization of dose distribution in the transverse plane of HDR Ir-192 source. This is a more efficient method than TLD dosimetry at discrete and distant positions. Relative to TLD dosimetry, it is found to be better reproducible, easy to use and a less expensive method of dosimetry.</description><dc:title>A dosimetry method in the transverse plane of HDR Ir-192 brachytherapy source using gafchromic EBT2 film</dc:title><dc:creator>S.C. Uniyal, S.D. Sharma, U.C. Naithani</dc:creator><dc:identifier>10.1016/j.ejmp.2011.03.005</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-04-21</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-04-21</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Original Papers</prism:section><prism:startingPage>129</prism:startingPage><prism:endingPage>133</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000275/abstract?rss=yes"><title>Kilovoltage beam model for flat panel imaging system with bow-tie filter for scatter prediction and correction</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000275/abstract?rss=yes</link><description>Abstract: Purpose: Kilovoltage flat-panel imaging systems are used for cone-beam Computed Tomography (CBCT) and digital Tomosynthesis (DTS). Hereby, the presence of scatter and relatively large dose from imaging are challenging factors. In this study a phenomenological beam model was developed to characterize imager response to imaging beams with a bow-tie filter (Varian OBI system).Materials and method: The kilovoltage beam model was based on dose ratio formalism and thus was using standard concepts of megavoltage dose calculation such as scatter factors, tissue maximum ratio and off-axis ratio. Primary and scatter (head and phantom scatter) were modeled with three Gaussian kernels. Parameters were based on measured transmission images for slabs of solid water of different total thickness and various jaw settings.Results: The beam model was used to evaluate contributions from primary, secondary and tertiary contributions for different geometrical objects such as cylinders and step-like phantoms. Theoretical predictions of radiographs using the model for known objects are consistent with the measurements.Conclusion: Secondary and tertiary contributions were interpreted as scatter and can be subtracted from CBCT projections based on the analytical model. Therefore our model can provide a basis for improvement of image quality (less artifacts due to scatter, better contrast and resolution) in CBCT reconstruction.</description><dc:title>Kilovoltage beam model for flat panel imaging system with bow-tie filter for scatter prediction and correction</dc:title><dc:creator>M. Blessing, M.S. Bhagwat, Y. Lyatskaya, J.R. Bellon, J. Hesser, P. Zygmanski</dc:creator><dc:identifier>10.1016/j.ejmp.2011.04.001</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-05-16</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-05-16</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Original Papers</prism:section><prism:startingPage>134</prism:startingPage><prism:endingPage>143</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000299/abstract?rss=yes"><title>Clinical investigations of a CVD diamond detector for radiotherapy dosimetry</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000299/abstract?rss=yes</link><description>Abstract: X-ray detectors based on single crystal diamond film made via chemical vapor deposition were investigated to evaluate their performance under clinically relevant conditions for radiotherapy dosimetry. Studies focused on repeatability, dose rate dependence, tissue phantom ratios, output factors and beam profiling. Repeatability experiments revealed a temporary loss in sensitivity due to charge detrapping effects following irradiation, which was modeled to make corrections that improved short-term precision. Dose rate dependence was observed (Fowler fitting parameter Δ = 0.96 ± 0.2) using dose rates up to ∼2 Gy min^−1. The detector statistically distinguished (n = 5, P &lt; 0.05) between dose values separated by 7.7 × 10^−3 Gy (1 MU). Depth dose measurements from 1 to 15 cm and output factors using 3 × 3 to 10 × 10 cm^2 field sizes compared well with a Farmer ion chamber (&lt;1.3% difference). Output factor measurements indicate encouraging results for fields sizes &lt;4 × 4 cm^2. Off-axis measurements showed that perturbation of the beam could be reduced when the detector is used in the edge-on orientation due to its thin-film sandwich configuration and ∼200 nm thick Ag contacts. This relatively inexpensive detector has potential to be used for routine dosimetry using conventional radiotherapy instrumentation.</description><dc:title>Clinical investigations of a CVD diamond detector for radiotherapy dosimetry</dc:title><dc:creator>G.T. Betzel, S.P. Lansley, F. Baluti, L. Reinisch, J. Meyer</dc:creator><dc:identifier>10.1016/j.ejmp.2011.04.003</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-05-18</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-05-18</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Original Papers</prism:section><prism:startingPage>144</prism:startingPage><prism:endingPage>152</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000305/abstract?rss=yes"><title>Monte Carlo derivation of AAPM TG-43 dosimetric parameters for GZP6 Co-60 HDR sources</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000305/abstract?rss=yes</link><description>Abstract: Cobalt 60 source is generally available on high dose rate (HDR) afterloading equipment especially for treatment of gynecological lesions. The GZP6 remote afterloader (Nuclear Power Institute of China) utilizes 60Co sources for treatment of intracavitary and intraluminal malignancies. In this study, the AAPM TG-43 dosimetric parameters of three sources in GZP6 system have been studied using MCNP4C Monte Carlo (MC) code; and the results are compared with other available 60Co HDR sources. The presented parameters consist of air kerma strength, dose rate constant, radial dose function and anisotropy function. They show less than 1% uncertainty. The TG-43 based dosimetry data can be used not only to validate the dedicated treatment planning software (TPS), but also to introduce new complementary software to enhance the system performance in gynecological treatments.</description><dc:title>Monte Carlo derivation of AAPM TG-43 dosimetric parameters for GZP6 Co-60 HDR sources</dc:title><dc:creator>Sanaz Hariri Tabrizi, Alireza Kamali Asl, Zohreh Azma</dc:creator><dc:identifier>10.1016/j.ejmp.2011.04.004</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-05-30</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-05-30</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Original Papers</prism:section><prism:startingPage>153</prism:startingPage><prism:endingPage>160</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000214/abstract?rss=yes"><title>CT iterative reconstruction in image space: A phantom study</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000214/abstract?rss=yes</link><description>Abstract: Although iterative reconstruction is widely applied in SPECT/PET, its introduction in clinical CT is quite recent, in the past the demand for extensive computer power and long image reconstruction times have stopped the diffusion of this technique. Recently Iterative Reconstruction in Image Space (IRIS) has been introduced on Siemens top CT scanners. This recon method works on image data area, reducing the time-consuming loops on raw data and noise removal is obtained in subsequent iterative steps with a smoothing process. We evaluated image noise, low contrast resolution, CT number linearity and accuracy, transverse and z-axis spatial resolution using some dedicated phantoms in single, dual source and cardiac mode. We reconstructed images with a traditional filtered back-projection algorithm and with IRIS. The iterative procedure preserves spatial resolution, CT number accuracy and linearity moreover decreases image noise. These preliminary results support the idea that dose reduction with preserved image quality is possible with IRIS, even if studies on patients are necessary to confirm these data.</description><dc:title>CT iterative reconstruction in image space: A phantom study</dc:title><dc:creator>C. Ghetti, O. Ortenzia, G. Serreli</dc:creator><dc:identifier>10.1016/j.ejmp.2011.03.003</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-04-18</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-04-18</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Technical Notes</prism:section><prism:startingPage>161</prism:startingPage><prism:endingPage>165</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000251/abstract?rss=yes"><title>Analysis of image sharpness reproducibility on a novel engineered micro-CT scanner with variable geometry and embedded recalibration software</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000251/abstract?rss=yes</link><description>Abstract: This study investigates the reproducibility of the reconstructed image sharpness, after modifications of the geometry setup, for a variable magnification micro-CT (μCT) scanner. All the measurements were performed on a novel engineered μCT scanner for in vivo imaging of small animals (Xalt), which has been recently built at the Institute of Clinical Physiology of the National Research Council (IFC-CNR, Pisa, Italy), in partnership with the University of Pisa. The Xalt scanner is equipped with an integrated software for on-line geometric recalibration, which will be used throughout the experiments. In order to evaluate the losses of image quality due to modifications of the geometry setup, we have made 22 consecutive acquisitions by changing alternatively the system geometry between two different setups (Large FoV – LF, and High Resolution – HR). For each acquisition, the tomographic images have been reconstructed before and after the on-line geometric recalibration. For each reconstruction, the image sharpness was evaluated using two different figures of merit: (i) the percentage contrast on a small bar pattern of fixed frequency (f = 5.5 lp/mm for the LF setup and f = 10 lp/mm for the HR setup) and (ii) the image entropy. We have found that, due to the small-scale mechanical uncertainty (in the order of the voxel size), a recalibration is necessary for each geometric setup after repositioning of the system’s components; the resolution losses due to the lack of recalibration are worse for the HR setup (voxel size = 18.4 μm). The integrated on-line recalibration algorithm of the Xalt scanner allowed to perform the recalibration quickly, by restoring the spatial resolution of the system to the reference resolution obtained after the initial (off-line) calibration.</description><dc:title>Analysis of image sharpness reproducibility on a novel engineered micro-CT scanner with variable geometry and embedded recalibration software</dc:title><dc:creator>D. Panetta, N. Belcari, A. Del Guerra, A. Bartolomei, P.A. Salvadori</dc:creator><dc:identifier>10.1016/j.ejmp.2011.03.006</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-04-18</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-04-18</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Technical Notes</prism:section><prism:startingPage>166</prism:startingPage><prism:endingPage>173</prism:endingPage></item><item rdf:about="http://www.physicamedicaonline.com/article/PIIS1120179711000263/abstract?rss=yes"><title>First application of total skin electron beam irradiation in Greece: Setup, measurements and dosimetry</title><link>http://www.physicamedicaonline.com/article/PIIS1120179711000263/abstract?rss=yes</link><description>Abstract: Total Skin Electron Beam (TSEB) irradiation is considered as the treatment of choice for cutaneous T-cell lymphoma internationally, for either curative purposes or palliative care. An attempt for the first application of this external radiation therapy technique in Greece took place at the Radiation Therapy Unit of 2nd Department of Radiology of University of Athens at University General Hospital “Attikon”. TSEB modality was developed on a linear accelerator VARIAN Clinac 2100C. To create a uniform and sufficiently large field () at , two symmetrical 6 MeV electron beams are combined with 17.5° tilts concerning the horizontal direction. An immobilization system was constructed to support patient during treatment and to modulate the composite electron field. Irradiation procedure demands a standing patient that takes, in total, six treatment positions. For the confirmation of treatment suitability and the determination of physical features of the clinical electron field, specific measurements were carried out using a parallel-plate ionization chamber and TLDs at water equivalent plastic and anthropomorphic phantoms. Measurements at the referred conditions showed a homogeneous total field with intensity variation of ±2% in the longitudinal axis and ±4% at horizontal axis. The mean energy of the composite field () is 3.4 MeV, the most probable energy () is 4.4 MeV and the half-value depth in water () is 1.5 g/cm2. The maximum X-ray background of the TSEB field is 2.1% at head and feet. The above results lead us to conclude that TSEB treatment using “Six-dual-field” technique can be applied in our department safely.</description><dc:title>First application of total skin electron beam irradiation in Greece: Setup, measurements and dosimetry</dc:title><dc:creator>K. Platoni, S. Diamantopoulos, G. Panayiotakis, V. Kouloulias, P. Pantelakos, N. Kelekis, E. Efstathopoulos</dc:creator><dc:identifier>10.1016/j.ejmp.2011.03.007</dc:identifier><dc:source>Physica Medica: European Journal of Medical Physics 28, 2 (2012)</dc:source><dc:date>2011-04-25</dc:date><prism:publicationName>Physica Medica: European Journal of Medical Physics</prism:publicationName><prism:publicationDate>2011-04-25</prism:publicationDate><prism:volume>28</prism:volume><prism:number>2</prism:number><prism:issueIdentifier>S1120-1797(12)X0002-4</prism:issueIdentifier><prism:section>Technical Notes</prism:section><prism:startingPage>174</prism:startingPage><prism:endingPage>182</prism:endingPage></item></rdf:RDF>
