The accuracy of ED measurement, Z determination, and iodine quantitation derived from DL-DECT was demonstrated with phantom measurements. The accuracies were not sensitive to scan and reconstruction parameters, namely tube potential, dose, rotation time, and spectral reconstruction level, especially in the case of electron density.

CARDIAC IMAGINGC oronary CT angiography (CCTA) is currently recommended for the assessment of many cardiovascular diseases, including coronary artery disease (CAD) evaluation (1). CCTA is particularly important for its high negative predictive value for CAD in a low-and intermediaterisk acute chest pain population, with a high sensitivity and specificity for CAD in a low-and intermediate-risk chronic coronary syndrome population (2-5). This had been made possible by the recent technical evolution of the CT systems and the existence of large-scale validation cohort studies (6,7). However, conventional CCTA still has a limited spatial resolution and soft-tissue contrast, which impairs its diagnostic performance for small arteries (ie, ,2 mm) and high-contrast (eg, stent, calcification) and low-contrast (eg, noncalcified plaque) tasks, and carries the risks of relatively high x-ray dose delivery.Over the past 5 years, photon-counting CT (PCCT) technology has emerged in the field of CT imaging. Compared with conventional CT, this new modality has better spatial resolution and soft-tissue contrast and reduced noise, blooming, and beam-hardening artifacts (8). This is because of new energy-resolving detectors, called photon-counting Background. Spatial resolution, soft-tissue contrast, and dose-efficient capabilities of photon-counting CT (PCCT) potentially allow a better quality and diagnostic confidence of coronary CT angiography (CCTA) in comparison to conventional CT. Purpose:To compare the quality of CCTA scans obtained with a clinical prototype PCCT system and an energy-integrating detector (EID) dual-layer CT (DLCT) system. Materials and Methods:In this prospective board-approved study with informed consent, participants with coronary artery disease underwent retrospective electrocardiographically gated CCTA with both systems after injection of 65-75 mL of 400 mg/mL iodinated contrast agent at 5 mL/sec. A prior phantom task-based quality assessment of the detectability index of coronary lesions was performed. Ultra-high-resolution parameters were used for PCCT (1024 matrix, 0.25-mm section thickness) and EID DLCT (512 matrix, 0.67-mm section thickness). Three cardiac radiologists independently performed a blinded analysis using a five-point quality score (1 = insufficient, 5 = excellent) for overall image quality, diagnostic confidence, and diagnostic quality of calcifications, stents, and noncalcified plaques. A logistic regression model, adjusted for radiologists, was used to evaluate the proportion of improvement in scores with the best method.Results: Fourteen consecutive participants (12 men; mean age, 61 years 6 17) were enrolled. Scores of overall quality and diagnostic confidence were higher with PCCT images with a median of 5 (interquartile range [IQR], 2) and 5 (IQR, 1) versus 4 (IQR, 1) and 4 (IQR, 3) with EID DLCT images, using a mean tube current of 255 mAs 6 0 versus 349 mAs 6 111 for EID DLCT images (P , .01). Proportions of improvement with PCCT images for quality of calcification, stent, and non...

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We have continuously measured in situ reflectance and transmittance of percolating gold films over the entire range of surface coverage P, in the IR regime (1.7 and 2.2 μm). The samples present similar optical and electrical behavior, when compared on a normalized thickness scale. In the fractal region, close to the percolation threshold, the optical properties show a linear dependence on the surface coverage parameter, in agreement with a renormalization argument previously suggested. A strong absorption (about 40%), whose origin is not well understood, is found in the fractal region. The interpretations previously proposed by other authors are not applicable. We conclude that geometrical effects must dominate the optical properties over a large range of surface coverage.

The breakdown current I c of a percolating system is measured on real materials. We find I c ccB~x; B is the weakly nonlinear response determined by third-harmonic generation. A new criterion for I c is suggested, defined as the current at which a hot spot reaches the melting temperature of the metallic grains, T m . This criterion remains valid in the presence of nonlinear effects. It is also consistent with the experimental observations: At I c the resistance either increases to infinity or decreases, i.e., the local geometry is changed at T m . Modeling the breakdown by hot spots yields the above power law with 0.5 >: x > 0.36, in excellent agreement with the measured data: x =0.48 and 0.41 for Ag and Au films.

The three CT components with the greatest impact on image quality are the X-ray source, detection system and reconstruction algorithms. In this paper, we focus on the first two. We describe the state-of-the-art of CT detection systems, their calibrations, software corrections and common performance metrics. The components of CT detection systems, such as scintillator materials, photodiodes, data acquisition electronics and anti-scatter grids, are discussed. Their impact on CT image quality, their most important characteristics, as well as emerging future technology trends for each, are reviewed. The use of detection for multi-energy CT imaging is described. An overview of current CT X-ray sources, their evolution to support major trends in CT imaging and future trends is provided.

BackgroundTo evaluate the feasibility of multicolour quantitative imaging with spectral photon-counting computed tomography (SPCCT) of different mixed contrast agents.MethodsPhantoms containing eleven tubes with mixtures of varying proportions of two contrast agents (i.e. two selected from gadolinium, iodine or gold nanoparticles) were prepared so that the attenuation of each tube was about 280 HU. Scans were acquired at 120 kVp and 100 mAs using a five-bin preclinical SPCCT prototype, generating conventional, water, iodine, gadolinium and gold images. The correlation between prepared and measured concentrations was assessed using linear regression. The cross-contamination was measured for each material as the root mean square error (RMSE) of its concentration in the other material images, where no signal was expected. The contrast-to-noise ratio (CNR) relative to a phosphate buffered saline tube was calculated for each contrast agent.ResultsThe solutions had similar attenuations (279 ± 10 HU, mean ± standard deviation) and could not be differentiated on conventional images. However, a distinction was observed in the material images within the same samples, and the measured and prepared concentrations were strongly correlated (R2 ≥ 0.97, 0.81 ≤ slope ≤ 0.95, -0.68 ≤ offset ≤ 0.89 mg/mL). Cross-contamination in the iodine images for the mixture of gold and gadolinium contrast agents (RMSE = 0.34 mg/mL) was observed. CNR for 1 mg/mL of contrast agent was better for the mixture of iodine and gadolinium (CNRiodine = 3.20, CNRgadolinium = 2.80) than gold and gadolinium (CNRgadolinium = 1.67, CNRgold = 1.37).ConclusionsSPCCT enables multicolour quantitative imaging. As a result, it should be possible to perform imaging of multiple uptake phases of a given tissue/organ within a single scan by injecting different contrast agents sequentially.

The weak nonlinear electrical response of two-dimensional semicontinuous Ag and Au films was measured over three decades of sheet resistance. The third-harmonic component generated by the films, due to local Joule heating, is interpreted as a measure of the fourth moment of the current distribution. Higher harmonics corresponding to higher moments of the current distribution were also observed. Under certain conditions, measurement of the third harmonic lends the same critical exponent as that of