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		<title><![CDATA[ Medical Imaging, IEEE Transactions on - new TOC ]]></title>
		<link>http://ieeexplore.ieee.org</link>
		<description>TOC Alert for Publication# 42 </description>
		<year>2009</year>
		<month>November </month>
		<day>19</day>
		<item>
			<title><![CDATA[Table of contents]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297442]]></link>
			<description><![CDATA[ ]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297442]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>C1</startPage>
			<endPage>C4</endPage>
			<fileSize>98</fileSize>
			<authors><![CDATA[]]></authors>
		</item>
		<item>
			<title><![CDATA[IEEE Transactions on Medical Imaging publication information]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297436]]></link>
			<description><![CDATA[ ]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297436]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>C2</startPage>
			<endPage>C2</endPage>
			<fileSize>43</fileSize>
			<authors><![CDATA[]]></authors>
		</item>
		<item>
			<title><![CDATA[<emphasis emphasistype="italic">B</emphasis>-Mode Ultrasound Image Simulation in Deformable 3-D Medium]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4799171]]></link>
			<description><![CDATA[<para> This paper presents an algorithm for fast image synthesis inside deformed volumes. Given the node displacements of a mesh and a reference 3-D image dataset of a predeformed volume, the method first maps the image pixels that need to be synthesized from the deformed configuration to the nominal predeformed configuration, where the pixel intensities are obtained easily through interpolation in the regular-grid structure of the reference voxel volume. This mapping requires the identification of the mesh element enclosing each pixel for every image frame. To accelerate this <emphasis emphasistype="boldital">point location</emphasis> operation, a fast method of projecting the deformed mesh on image pixels is introduced in this paper. The method presented was implemented for ultrasound <emphasis emphasistype="italic">B</emphasis>-mode image simulation of a synthetic tissue phantom. The phantom deformation as a result of ultrasound probe motion was modeled using the finite element method. Experimental images of the phantom under deformation were then compared with the corresponding synthesized images using sum of squared differences and mutual information metrics. Both this quantitative comparison and a qualitative assessment show that realistic images can be synthesized using the proposed technique. An ultrasound examination system was also implemented to demonstrate that real-time image synthesis with the proposed technique can be successfully integrated into a haptic simulation. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4799171]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1657</startPage>
			<endPage>1669</endPage>
			<fileSize>1435</fileSize>
			<authors><![CDATA[Goksel, O.;Salcudean, S. E.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Approaching Artery Rigid Dynamics in IVUS]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4814694]]></link>
			<description><![CDATA[Tissue biomechanical properties (like strain and stress) are playing an increasing role in diagnosis and long-term treatment of intravascular coronary diseases. Their assessment strongly relies on estimation of vessel wall deformation. Since intravascular ultrasound (IVUS) sequences allow visualizing vessel morphology and reflect its dynamics, this technique represents a useful tool for evaluation of tissue mechanical properties. Image misalignment introduced by vessel-catheter motion is a major artifact for a proper tracking of tissue deformation. In this work, we focus on compensating and assessing IVUS rigid in-plane motion due to heart beating. Motion parameters are computed by considering both the vessel geometry and its appearance in the image. Continuum mechanics laws serve to introduce a novel score measuring motion reduction in <i>in vivo</i> sequences. Synthetic experiments validate the proposed score as measure of motion parameters accuracy; whereas results in <i>in vivo</i> pullbacks show the reliability of the presented methodologies in clinical cases.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4814694]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1670</startPage>
			<endPage>1680</endPage>
			<fileSize>3188</fileSize>
			<authors><![CDATA[Hernandez-Sabate, A.;Gil, D.;Fernandez-Nofrerias, E.;Radeva, P.;Marti, E.;]]></authors>
		</item>
		<item>
			<title><![CDATA[<emphasis emphasistype="italic">In Vivo</emphasis> High-ResolutionConductivity Imaging of the Human Leg Using MREIT: The First Human Experiment]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4814693]]></link>
			<description><![CDATA[We present the first <i>in vivo</i> cross-sectional conductivity image of the human leg with 1.7 mm pixel size using the magnetic resonance electrical impedance tomography (MREIT) technique. After a review of its experimental protocol by an Institutional Review Board (IRB), we performed MREIT imaging experiments of four human subjects using a 3 T MRI scanner. Adopting thin and flexible carbon-hydrogel electrodes with a large surface area and good contact, we could inject as much as 9 mA current in a form of 15 ms pulse into the leg without producing a painful sensation and motion artifact. Sequentially injecting two imaging currents in two different directions, we collected induced magnetic flux density data inside the leg. Scaled conductivity images reconstructed by using the single-step harmonic <i>B</i> <sub>z</sub> algorithm well distinguished different parts of the subcutaneous adipose tissue, muscle, crural fascia, intermuscular septum and bone inside the leg. We could observe spurious noise spikes in the outer layer of the bone primarily due to the MR signal void phenomenon there. Around the fat, the chemical shift of about two pixels occurred obscuring the boundary of the fat region. Future work should include a fat correction method incorporated in the MREIT pulse sequence and improvements in radio-frequency coils and image reconstruction algorithms. Further human imaging experiments are planned and being conducted to produce conductivity images from different parts of the human body.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4814693]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1681</startPage>
			<endPage>1687</endPage>
			<fileSize>1931</fileSize>
			<authors><![CDATA[Hyung Joong Kim;Young Tae Kim;Minhas, A.S.;Woo Chul Jeong;Eung Je Woo;Jin Keun Seo;Kwon, O.J.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Statistical Sinogram Restoration in Dual-Energy CT for PET Attenuation Correction]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4804741]]></link>
			<description><![CDATA[<para> Dual-energy (DE) X-ray computed tomography (CT) has been found useful in various applications. In medical imaging, one promising application is using low-dose DECT for attenuation correction in positron emission tomography (PET). Existing approaches to sinogram material decomposition ignore noise characteristics and are based on logarithmic transforms, producing noisy component sinogram estimates for low-dose DECT. In this paper, we propose two novel sinogram restoration methods based on statistical models: penalized weighted least square (PWLS) and penalized likelihood (PL), yielding less noisy component sinogram estimates for low-dose DECT than classical methods. The proposed methods consequently provide more precise attenuation correction of the PET emission images than do previous methods for sinogram material decomposition with DECT. We report simulations that compare the proposed techniques and existing approaches. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4804741]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1688</startPage>
			<endPage>1702</endPage>
			<fileSize>1451</fileSize>
			<authors><![CDATA[Noh, J.;Fessler, J. A.;Kinahan, P. E.;]]></authors>
		</item>
		<item>
			<title><![CDATA[An Image Based Auto-Focusing Algorithm forDigital Fundus Photography]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4813255]]></link>
			<description><![CDATA[In fundus photography, the task of fine focusing the image is demanding and lack of focus is quite often the cause of suboptimal photographs. The introduction of digital cameras has provided an opportunity to automate the task of focusing. We have developed a software algorithm capable of identifying best focus. The auto-focus (AF) method is based on an algorithm we developed to assess the sharpness of an image. The AF algorithm was tested in the prototype of a semi-automated nonmydriatic fundus camera designed to screen in the primary care environment for major eye diseases. A series of images was acquired in volunteers while focusing the camera on the fundus. The image with the best focus was determined by the AF algorithm and compared to the assessment of two masked readers. A set of fundus images was obtained in 26 eyes of 20 normal subjects and 42 eyes of 28 glaucoma patients. The 95% limits of agreement between the readers and the AF algorithm were -2.56 to 2.93 and -3.7 to 3.84 diopter and the bias was 0.09 and 0.71 diopter, for the two readers respectively. On average, the readers agreed with the AF algorithm on the best correction within less than 3/4 diopter. The intraobserver repeatability was 0.94 and 1.87 diopter, for the two readers respectively, indicating that the limit of agreement with the AF algorithm was determined predominantly by the repeatability of each reader. An auto-focus algorithm for digital fundus photography can identify the best focus reliably and objectively. It may improve the quality of fundus images by easing the task of the photographer.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4813255]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1703</startPage>
			<endPage>1707</endPage>
			<fileSize>599</fileSize>
			<authors><![CDATA[Moscaritolo, M.;Jampel, H.;Knezevich, F.;Zeimer, R.;]]></authors>
		</item>
		<item>
			<title><![CDATA[A Stochastic Approach to Estimate the UncertaintyInvolved in B-Spline Image Registration]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4915790]]></link>
			<description><![CDATA[<para> Uncertainties in image registration may be a significant source of errors in anatomy mapping as well as dose accumulation in radiotherapy. It is, therefore, essential to validate the accuracy of image registration. Here, we propose a method to detect areas where mono modal <emphasis emphasistype="italic">B</emphasis>-spline registration performs well and to distinguish those from areas of the same image, where the registration is likely to be less accurate. It is a stochastic approach to automatically estimate the uncertainty of the resulting displacement vector field. The coefficients resulting from the <emphasis emphasistype="italic">B</emphasis>-spline registration are subject to moderate and randomly performed variations. A quantity is proposed to characterize the local sensitivity of the similarity measure to these variations. We demonstrate the statistical dependence between the local image registration error and this quantity by calculating their mutual information. We show the significance of the statistical dependence with an approach based on random redistributions. The proposed method has the potential to divide an image into subregions which differ in the magnitude of their average registration error. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4915790]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1708</startPage>
			<endPage>1716</endPage>
			<fileSize>774</fileSize>
			<authors><![CDATA[Hub, M.;Kessler, M. L.;Karger, C. P.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Generalized Algorithms for Direct Reconstruction of Parametric Images From Dynamic PET Data]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4915794]]></link>
			<description><![CDATA[Indirect and direct methods have been developed for reconstructing parametric images from dynamic positron emission tomography (PET) data. Indirect methods are simple and easy to implement because reconstruction and kinetic modeling are performed in two separate steps. Direct methods estimate parametric images directly from dynamic PET sinograms and, in theory, can be statistically more efficient, but the algorithms are often difficult to implement and are very specific to the kinetic model being used. This paper presents a class of generalized algorithms for direct reconstruction of parametric images that are relatively easy to implement and can be adapted to different kinetic models. The proposed algorithms use optimization transfer principle to convert the maximization of a penalized likelihood into a pixel-wise weighted least squares (WLS) kinetic fitting problem at each iteration. Thus, it can employ existing WLS algorithms developed for kinetic models. The proposed algorithms resemble the empirical iterative implementation of the indirect approach, but converge to a solution of the direct formulation. Computer simulations showed that the proposed direct reconstruction algorithms are flexible and achieve a better bias-variance tradeoff than indirect reconstruction methods.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4915794]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1717</startPage>
			<endPage>1726</endPage>
			<fileSize>697</fileSize>
			<authors><![CDATA[Guobao Wang;Jinyi Qi;]]></authors>
		</item>
		<item>
			<title><![CDATA[A Reconstruction Algorithm for Photoacoustic Imaging Based on the Nonuniform FFT]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4967959]]></link>
			<description><![CDATA[Fourier reconstruction algorithms significantly outperform conventional backprojection algorithms in terms of computation time. In photoacoustic imaging, these methods require interpolation in the Fourier space domain, which creates artifacts in reconstructed images. We propose a novel reconstruction algorithm that applies the one-dimensional nonuniform fast Fourier transform to photoacoustic imaging. It is shown theoretically and numerically that our algorithm avoids artifacts while preserving the computational effectiveness of Fourier reconstruction.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4967959]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1727</startPage>
			<endPage>1735</endPage>
			<fileSize>1666</fileSize>
			<authors><![CDATA[Haltmeier, M.;Scherzer, O.;Zangerl, G.;]]></authors>
		</item>
		<item>
			<title><![CDATA[A New Distortion Model for Strong Inhomogeneity Problems in Echo-Planar MRI]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4956987]]></link>
			<description><![CDATA[This paper proposes a new distortion model for strong inhomogeneity problems in echo planar imaging (EPI). Fast imaging sequences in magnetic resonance imaging (MRI), such as EPI, are very important in applications where temporal resolution or short total acquisition time is essential. Unfortunately, fast imaging sequences are very sensitive to variations in the homogeneity of the main magnetic field. The inhomogeneity leads to geometrical distortions and intensity changes in the image reconstructed via fast Fourier transform. Also, under strong inhomogeneity, the accelerated intravoxel dephase may overly attenuate signals coming from regions with higher inhomogeneity variations. Moreover, coarse discretization schemes for the inhomogeneity are not able to cope with this problem, producing discretization artifacts when large inhomogeneity variations occur. Most of the existing models do not attempt to solve this problem. In this paper, we propose a modification of the discrete distortion model to incorporate the effects of the intravoxel inhomogeneity and to minimize the discretization artifacts. As a result, these problems are significantly reduced. Extensive experiments are shown to demonstrate the achieved improvements. Also, the performance of the new model is evaluated for conjugate phase, least squares method (minimized iteratively using conjugated gradients), and regularized methods (using a total variation penalty).]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4956987]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1736</startPage>
			<endPage>1753</endPage>
			<fileSize>7028</fileSize>
			<authors><![CDATA[Zibetti, M.V.W.;De Pierro, A.R.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Effect of Voxel Size and Computation Method on Tc-99m MAA SPECT/CT-Based Dose Estimation for Y-90 Microsphere Therapy]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4967961]]></link>
			<description><![CDATA[<para> The use of selective internal radiation therapy for treatment of hepatocellular carcinoma and liver metastases using Y-90 labeled microspheres has become an effective and widely used treatment regimen. However, dosimetric evaluations of this treatment are still primitive as uniform distribution models based only on injected activity are often used. This investigation attempts to quantify the effectiveness of several sophisticated patient-specific techniques which utilize the source distribution of Tc-99m MAA simulation studies to perform voxelized dosimetric computations. Among these techniques are complete Monte-Carlo radiation transport computation in patient-specific CT-based voxel phantoms, local energy deposition in patient specific phantoms and kernel transport techniques in water. Each technique was evaluated using three different phantom voxel dimensions and SPECT reconstruction matrix sizes. Dose evaluation results using all methods were compared to the exact solution, obtained using fully 3-D Monte-Carlo simulations with source distribution based not on SPECT data, but on the injected activity and exact boundaries of the anthropomorphic phantom used in the study. The results of this study show that at large voxel sizes and using SPECT reconstructions with a small matrix size (64<formula formulatype="inline"> <tex Notation="TeX">$,times,$</tex></formula>64), Monte-Carlo and local deposition methods are nearly equivalent. However, using a large SPECT reconstruction matrix (256<formula formulatype="inline"><tex Notation="TeX">$,times,$</tex> </formula>256) the local deposition method is significantly more accurate than full 3-D Monte-Carlo transport, and with a negligible computational burden. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4967961]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1754</startPage>
			<endPage>1758</endPage>
			<fileSize>432</fileSize>
			<authors><![CDATA[Pasciak, A. S.;Erwin, W. D.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Model-Based Iterative Reconstruction for Radial Fast Spin-Echo MRI]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5067386]]></link>
			<description><![CDATA[In radial fast spin-echo magnetic resonance imaging (MRI), a set of overlapping spokes with an inconsistent T2 weighting is acquired, which results in an averaged image contrast when employing conventional image reconstruction techniques. This work demonstrates that the problem may be overcome with the use of a dedicated reconstruction method that further allows for T2 quantification by extracting the embedded relaxation information. Thus, the proposed reconstruction method directly yields a spin-density and relaxivity map from only a single radial data set. The method is based on an inverse formulation of the problem and involves a modeling of the received MRI signal. Because the solution is found by numerical optimization, the approach exploits all data acquired. Further, it handles multicoil data and optionally allows for the incorporation of additional prior knowledge. Simulations and experimental results for a phantom and human brain <i>in vivo</i> demonstrate that the method yields spin-density and relaxivity maps that are neither affected by the typical artifacts from TE mixing, nor by streaking artifacts from the incomplete k-space coverage at individual echo times.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5067386]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1759</startPage>
			<endPage>1769</endPage>
			<fileSize>5935</fileSize>
			<authors><![CDATA[Block, K.T.;Uecker, M.;Frahm, J.;]]></authors>
		</item>
		<item>
			<title><![CDATA[<formula formulatype="inline"><tex Notation="TeX">${K}$</tex> </formula>-Space and Image-Space Combination for Motion-Induced Phase-Error Correction in Self-Navigated Multicoil Multishot DWI]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4967962]]></link>
			<description><![CDATA[Motion during diffusion encodings leads to different phase errors in different shots of multishot diffusion-weighted acquisitions. Phase error incoherence among shots results in undesired signal cancellation when data from all shots are combined. Motion-induced phase error correction for multishot diffusion-weighted imaging (DWI) has been studied extensively and there exist multiple phase error correction algorithms. A commonly used correction method is the direct phase subtraction (DPS). DPS, however, can suffer from incomplete phase error correction due to the aliasing of the phase errors in the high spatial resolution phases. Furthermore, improper sampling density compensation is also a possible issue of DPS. Recently, motion-induced phase error correction was incorporated in the conjugate gradient (CG) image reconstruction procedure to get a nonlinear phase correction method that is also applicable to parallel DWI. Although the CG method overcomes the issues of DPS, its computational requirement is high. Further, CG restricts to sensitivity encoding (SENSE) for parallel reconstruction. In this paper, a new time-efficient and flexible <i>k</i>-space and image-space combination (KICT) algorithm for rigid body motion-induced phase error correction is introduced. KICT estimates the motion-induced phase errors in image space using the self-navigated capability of the variable density spiral trajectory. The correction is then performed in <i>k</i> -space. The algorithm is shown to overcome the problem of aliased phase errors. Further, the algorithm preserves the phase of the imaging object and receiver coils in the corrected <i>k</i> -space data, which is important for parallel imaging applications. After phase error correction, any parallel reconstruction method can be used. The KICT algorithm is tested with both simulated and in vivo data with both multishot single-coil and multishot multicoil acquisitions. We show that KICT correction results in diffusion-weighted -
images with higher signal-to-noise ratio (SNR) and fractional anisotropy (FA) maps with better resolved fiber tracts as compared to DPS. In peripheral-gated acquisitions, KICT is comparable to the CG method.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=4967962]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1770</startPage>
			<endPage>1780</endPage>
			<fileSize>2333</fileSize>
			<authors><![CDATA[Van, A.T.;Karampinos, D.C.;Georgiadis, J.G.;Sutton, B.P.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Effects of Different Imaging Models on Least-Squares Image Reconstruction Accuracy in Photoacoustic Tomography]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297445]]></link>
			<description><![CDATA[In the classic formulation of photoacoustic tomography (PAT), two distinct descriptions of the imaging model have been employed for developing reconstruction algorithms. We demonstrate that the numerical and statistical properties of unweighted least-squares reconstruction algorithms associated with each imaging model are generally very different. Specifically, some PAT reconstruction algorithms, including many of the iterative algorithms previously explored, do not work directly with the raw measured pressure wavefields, but rather with an integrated data function that is obtained by temporally integrating the photoacoustic wavefield. The integration modifies the statistical distribution of the data, introducing statistical correlations among samples. This change is highly significant for iterative algorithms, many of which explicitly or implicitly seek to minimize a statistical cost function. In this work, we demonstrate that iterative reconstruction by least-squares minimization yields better resolution-noise tradeoffs when working with the raw pressure data than with the integrated data commonly employed. In addition, we demonstrate that the raw-data based approach is less sensitive to certain deterministic errors, such as dc offset errors.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297445]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1781</startPage>
			<endPage>1790</endPage>
			<fileSize>1413</fileSize>
			<authors><![CDATA[Jin Zhang;Anastasio, M.A.;La Riviere, P.J.;Wang, L.V.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Distribution of Fiducial Registration Error in Rigid-Body Point-Based Registration]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297447]]></link>
			<description><![CDATA[<para> Rigid-body point-based registration is frequently used in computer assisted surgery to align corresponding points, or fiducials, in preoperative and intraoperative data. This alignment is mostly achieved by assuming the same homogeneous error distribution for all the points; however, due to the properties of the medical instruments used in measuring the point coordinates, the error distribution might be inhomogeneous and different for each point. In this paper, in an effort to understand the effect of error distribution in the localized points on the performed registration, we derive a closed-form solution relating the error distribution of each point with the performed registration accuracy. The solution uses maximum likelihood estimation to calculate the probability density function of registration error at each fiducial point. Extensive numerical simulations are performed to validated the proposed solution. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297447]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1791</startPage>
			<endPage>1801</endPage>
			<fileSize>312</fileSize>
			<authors><![CDATA[Moghari, M. H.;Abolmaesumi, P.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Rapid Dynamic Image Registration of the Beating Heart for Diagnosis and Surgical Navigation]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5071224]]></link>
			<description><![CDATA[<para> Dynamic cardiac magnetic resonance imaging (MR) and computed tomography (CT) provide cardiologists and cardiac surgeons with high-quality 4-D images for diagnosis and therapy, yet the effective use of these high-quality anatomical models remains a challenge. Ultrasound (US) is a flexible imaging tool, but the US images produced are often difficult to interpret unless they are placed within their proper 3-D anatomical context. The ability to correlate real-time 3-D US volumes (RT3D US) with dynamic MR/CT images would offer a significant contribution to improve the quality of cardiac procedures. In this paper, we present a rapid two-step method for registering RT3D US to high-quality dynamic 3-D MR/CT images of the beating heart. This technique overcomes some major limitations of image registration (such as the correct registration result not necessarily occurring at the maximum of the mutual information (MI) metric) using the MI metric. We demonstrate the effectiveness of our method in a dynamic heart phantom (DHP) study and a human subject study. The achieved mean target registration error of CT+US images in the phantom study is 2.59 mm. Validation using human MR/US volumes shows a target registration error of 1.76 mm. We anticipate that this technique will substantially improve the quality of cardiac diagnosis and therapies. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5071224]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1802</startPage>
			<endPage>1814</endPage>
			<fileSize>1360</fileSize>
			<authors><![CDATA[Huang, X.;Ren, J.;Guiraudon, G.;Boughner, D.;Peters, T. M.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Robust Initial Detection of Landmarks in Film-Screen Mammograms Using Multiple FFDM Atlases]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5071222]]></link>
			<description><![CDATA[<para> Automated analysis of mammograms requires robust methods for pectoralis segmentation and nipple detection. Locating the nipple is especially important in multiview computer aided detection systems, in which findings are matched across images using the nipple-to-finding distance. Segmenting the pectoralis is a key preprocessing step to avoid false positives when detecting masses due to the similarity of the texture of mammographic parenchyma and the pectoral muscle. A multiatlas algorithm capable of providing very robust initial estimates of the nipple position and pectoral region in digitized mammograms is presented here. Ten full-field digital mammograms, which are easily annotated attributed to their excellent contrast, are robustly registered to the target digitized film-screen mammogram. The annotations are then propagated and fused into a final nipple position and pectoralis segmentation. Compared to other nipple detection methods in the literature, the system proposed here has the advantages that it is more robust and can provide a reliable estimate when the nipple is located outside the image. Our results show that the change in the correlation between nipple-to-finding distances in craniocaudal and mediolateral oblique views is not significant when the detected nipple positions replace the manual annotations. Moreover, the pectoralis segmentation is acceptable and can be used as initialization for a more complex algorithm to optimize the outline locally. A novel aspect of the method is that it is also capable of detecting and segmenting the pectoralis in craniocaudal views. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5071222]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1815</startPage>
			<endPage>1824</endPage>
			<fileSize>1037</fileSize>
			<authors><![CDATA[Iglesias, J. E.;Karssemeijer, N.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Kernel Granger Causality Mapping Effective Connectivity on fMRI Data]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5223585]]></link>
			<description><![CDATA[<para> Although it is accepted that linear Granger causality can reveal effective connectivity in functional magnetic resonance imaging (fMRI), the issue of detecting nonlinear connectivity has hitherto not been considered. In this paper, we address kernel Granger causality (KGC) to describe effective connectivity in simulation studies and real fMRI data of a motor imagery task. Based on the theory of reproducing kernel Hilbert spaces, KGC performs linear Granger causality in the feature space of suitable kernel functions, assuming an arbitrary degree of nonlinearity. Our results demonstrate that KGC captures effective couplings not revealed by the linear case. In addition, effective connectivity networks between the supplementary motor area (SMA) as the seed and other brain areas are obtained from KGC. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5223585]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1825</startPage>
			<endPage>1835</endPage>
			<fileSize>632</fileSize>
			<authors><![CDATA[Liao, W.;Marinazzo, D.;Pan, Z.;Gong, Q.;Chen, H.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Cardiac C-Arm CT: A Unified Framework for Motion Estimation and Dynamic CT]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5299272]]></link>
			<description><![CDATA[<para> Generating 3-D images of the heart during interventional procedures is a significant challenge. In addition to real time fluoroscopy, angiographic C-arm systems can also now be used to generate 3-D/4-D CT images on the same system. One protocol for cardiac CT uses ECG triggered multisweep scans. A 3-D volume of the heart at a particular cardiac phase is then reconstructed by applying Feldkamp (FDK) reconstruction to the projection images with retrospective ECG gating. In this work we introduce a unified framework for heart motion estimation and dynamic cone-beam reconstruction using motion corrections. The benefits of motion correction are 1) increased temporal and spatial resolution by removing cardiac motion which may still exist in the ECG gated data sets and 2) increased signal-to-noise ratio (SNR) by using more projection data than is used in standard ECG gated methods. Three signal-enhanced reconstruction methods are introduced that make use of all of the acquired projection data to generate a 3-D reconstruction of the desired cardiac phase. The first averages all motion corrected back-projections; the second and third perform a weighted averaging according to 1) intensity variations and 2) temporal distance relative to a time resolved and motion corrected reference FDK reconstruction. In a comparison study seven methods are compared: nongated FDK, ECG-gated FDK, ECG-gated, and motion corrected FDK, the three signal-enhanced approaches, and temporally aligned and averaged ECG-gated FDK reconstructions. The quality measures used for comparison are spatial resolution and SNR. Evaluation is performed using phantom data and animal models. We show that data driven and subject-specific motion estimation combined with motion correction can decrease motion-related blurring substantially. Furthermore, SNR can be increased by up to 70% while maintaining spatial resolution at the same level as is provided by the ECG-gated FDK. The presented framework provides exce-
llent image quality for cardiac C-arm CT. </para>]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5299272]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1836</startPage>
			<endPage>1849</endPage>
			<fileSize>1880</fileSize>
			<authors><![CDATA[Prummer, M.;Hornegger, J.;Lauritsch, G.;Wigstrom, L.;Girard-Hughes, E.;Fahrig, R.;]]></authors>
		</item>
		<item>
			<title><![CDATA[Correction for Susceptibility-Induced Distortion in Echo-Planar Imaging Using Field Maps and Model-Based Point Spread Function]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5165029]]></link>
			<description><![CDATA[Susceptibility-induced distortion is one of the major artifacts in echo-planar imaging (EPI), and many solutions have been proposed for the problem, including the Fourier method and the point spread function (PSF) method. In this paper, a framework unifying both methods is presented. Under this framework, a model-based PSF method is proposed in which the PSF of the source object is modeled along with a single field map measured by TE-offset reference scans. EPI images of a phantom and a healthy human subject were acquired, and the results of distortion correction by the Fourier method, linear interpolation method, and the model-based PSF method were compared. The results showed that the model-based PSF method could correct for geometric distortion and signal intensity distortion satisfactorily, avoiding the rippling artifact shown in the Fourier method. In conclusion, the proposed framework gave us an overall picture of how different correction methods work. The model-based PSF method, which required fewer reference scans and less computational load, was more clinically feasible than other methods.]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5165029]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1850</startPage>
			<endPage>1857</endPage>
			<fileSize>1139</fileSize>
			<authors><![CDATA[Yung-Chin Hsu;Ching-Han Hsu;Tseng, W.-Y.I.;]]></authors>
		</item>
		<item>
			<title><![CDATA[ISBI 2010]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297439]]></link>
			<description><![CDATA[ ]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297439]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1858</startPage>
			<endPage>1858</endPage>
			<fileSize>601</fileSize>
			<authors><![CDATA[]]></authors>
		</item>
		<item>
			<title><![CDATA[Special issue on multivariate microscopy image analysis]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5299255]]></link>
			<description><![CDATA[ ]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5299255]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1859</startPage>
			<endPage>1859</endPage>
			<fileSize>157</fileSize>
			<authors><![CDATA[]]></authors>
		</item>
		<item>
			<title><![CDATA[Explore IEL IEEE's most comprehensive resource]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297438]]></link>
			<description><![CDATA[ ]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297438]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>1860</startPage>
			<endPage>1860</endPage>
			<fileSize>345</fileSize>
			<authors><![CDATA[]]></authors>
		</item>
		<item>
			<title><![CDATA[IEEE Transactions on Medical Imaging information for authors]]></title>
			<link><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297437]]></link>
			<description><![CDATA[ ]]></description>
			<pubDate><![CDATA[Nov.  2009]]></pubDate>
			<guid><![CDATA[http://ieeexplore.ieee.org/xpls/abs_all.jsp?isnumber=5297435&arnumber=5297437]]></guid>
			<volume>28</volume>
			<issue>11</issue>
			<startPage>C3</startPage>
			<endPage>C3</endPage>
			<fileSize>26</fileSize>
			<authors><![CDATA[]]></authors>
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