"Fluoroscopic imaging devices for interventional radiology and cardiovascular applications have traditionally used image-intensifiers optically coupled to either charge-coupled devices (CCDs) or video pick-up tubes. While such devices provide image quality sufficient for most clinical applications, there are several limitations, such as loss of resolution in the fringes of the image-intensifier, veiling glare and associated contrast loss, distortion, size, and degradation with time. This work is aimed at overcoming these limitations posed by image-intensifiers, while improving on the image quality. System design parameters related to the development of a high-resolution CCD-based imager are presented. The proposed system uses four 8 x 8-cm three-side buttable CCDs tiled in a seamless fashion to achieve a field of view (FOV) of 16 x 16-cm. Larger FOVs can be achieved by tiling more CCDs in a similar manner. The system employs a thallium-doped cesium iodide (CsI:Tl) scintillator coupled to the CCDs by straight (non-tapering) fiberoptics and can be operated in 78, 156 or 234-microns pixel pitch modes. Design parameters such as quantum efficiency and scintillation yield of CsI:Tl, optical coupling efficiency and estimation of the thickness of fiberoptics to provide reasonable protection to the CCD, linearity, sensitivity, dynamic range, noise characteristics of the CCD, techniques for tiling the CCDs in a seamless fashion, and extending the field of view are addressed. The signal and noise propagation in the imager was modeled as a cascade of linear-systems and used to predict objective image quality parameters such as the spatial frequency-dependent modulation transfer function (MTF), noise power spectrum (NPS) and detective quantum efficiency (DQE). The theoretical predictions were compared with experimental measurements of the MTF, NPS and DQE of a single 8 x 8-cm module coupled to a 450-microns thick CsI:Tl at x-ray beam quality appropriate for cardiovascular fluoroscopy. The measured limiting spatial resolution (10% MTF) was 3.9 cy/mm and 3.6 cy/mm along the two orthogonal axes. The measured DQE(0) was ~0.62 and showed no dependence with incident exposure rate over the range of measurement. The experimental DQE measurements demonstrated good agreement with the theoretical estimate obtained using the parallel-cascaded linear-systems model. The temporal imaging properties were characterized in terms of image lag and showed a first frame image lag of 0.9%. The imager demonstrated the ability to provide images of high and uniform spatial resolution, while preserving and potentially improving on DQE performance at dose levels lower than that currently used in clinical practice. These results provide strong support for potential adaptation of this type of imager for cardiovascular and pediatric angiography."

La tomographie d'émission monophotonique (TEMP) dédiée au petit animal est une technique d'imagerie nucléaire qui joue un rôle important en imagerie moléculaire. Les systèmes TEMP, à l'aide de collimateurs pinholes ou multi-pinholes, peuvent atteindre des résolutions spatiales submillimétriques et une haute sensibilité pour un petit champ de vue, ce qui est particulièrement attractif pour imager des souris. Une géométrie de collimation originale a été proposée, dans le cadre d'un projet, appelé SIGAHRS, piloté par la société Biospace. Ce collimateur présente des longueurs focales qui varient spatialement dans le plan transaxial et qui sont fixes dans le plan axial. Une haute résolution spatiale est recherchée au centre du champ de vue, avec un grand champ de vue et une haute sensibilité. Grâce aux simulations Monte Carlo, dont nous pouvons maîtriser tous les paramètres, nous avons étudié cette collimation originale que nous avons positionnée par rapport à un collimateur parallèle et un collimateur monofocal convergent. Afin de générer des données efficacement, nous avons développé un module multi-CPU/GPU qui utilise une technique de lancer de rayons dans le collimateur et qui nous a permis de gagner un facteur ~ 60 en temps de calcul, tout en conservant ~ 90 % du signal, pour l'isotope ⁹⁹^mTc (émettant à 140,5 keV), comparé à une simulation Monte Carlo classique. Cependant, cette approche néglige la pénétration septale et la diffusion dans le collimateur. Les données simulées ont ensuite été reconstruites avec l'algorithme OSEM. Nous avons développé quatre méthodes de projection (une projection simple (S-RT), une projection avec volume d'intersection (S-RT-IV), une projection avec calcul de l'angle solide (S-RT-SA) et une projection tenant compte de la profondeur d'interaction (S-RT-SA-D)). Nous avons aussi modélisé une PSF dans l'espace image, anisotrope et non-stationnaire, en nous inspirant de la littérature existante. Nous avons étudié le conditionnement de la matrice système pour chaque projecteur et collimateur, et nous avons comparé les images reconstruites pour chacun des collimateurs et pour chacun des projecteurs. Nous avons montré que le collimateur original proposé est le système le moins bien conditionné. Nous avons aussi montré que la modélisation de la PSF dans l'image ainsi que de la profondeur d'intéraction améliorent la qualité des images reconstruites ainsi que le recouvrement de contraste. Cependant, ces méthodes introduisent des artefacts de bord. Comparé aux systèmes existants, nous montrons que ce nouveau collimateur a un grand champ de vue (~ 70 mm dans le plan transaxial), avec une résolution de 1,0 mm dans le meilleur des cas, mais qu'il a une sensibilité relativement faible (1,32x10⁻² %). / Small animal single photon emission computed tomography (SPECT) is a nuclear medicine imaging technique that plays an important role in molecular imaging. SPECT systems using pinhole or multi-pinhole collimator can achieve submillimetric spatial resolution and high sensitivity in a small field of view, which is particularly appropriate for imaging mice. In our work, we studied a new collimator dedicated to small animal SPECT, in the context of a project called SIGAHRS, led by the Biospace company. In this collimator, focal lengths vary spatially in the transaxial plane and are fixed in the axial plane. This design aims at achieving high spatial resolution in the center of the field of view, with a large field of view and high sensitivity. Using Monte Carlo simulations, where all parameters can be controlled, we studied this new collimator geometry and compared it to a parallel collimator and a cone-beam collimator. To speed up the simulations, we developed a multi-CPU/GPU module that uses a technique of ray tracing. Using this approach, the acceleration factor was ~ 60 and we restored ~ 90 % of the signal for ⁹⁹^mTc (140.5 keV emission), compared to a classical Monte Carlo simulation. The 10 % difference is due to the fact that the multi-CPU/GPU module neglects the septal penetration and scatter in the collimator. We demonstrated that the data acquired with the new collimator could be reconstructed without artifact using an OSEM algorithm. We developed four forward projectors (simple projector (S-RT), projector accounting for the surface of the detecting pixel (S-RT-IV), projection modeling the solid angle (S-RT-SA) of the projection tube, and projector modeling the depth of interaction (S-RT-SA-D)). We also modeled the point spread function of the collimator in the image domain, using an anisotropic non-stationary function. To characterize the reconstruction, we studied the conditioning number of the system matrix for each projector and each collimator. We showed that the new collimator was more ill-conditioned than a parallel collimator or a cone-beam collimator. We showed that the image based PSF and the modeling of the depth of interaction improved the quality of the images, but edge artefacts were introduced when modeling the PSF in the image domain. Compared to existing systems, we showed that this new collimator has a large field of view (~ 70 mm in the transaxial plane) with a resolution of 1.0 mm in the best case but suffers from a relatively low sensitivity (1.32x10⁻² %).

Current positron emission mammography (PEM) depth of interaction (DOI) enabling detectors have low scintillator to photodetector encoding ratios, RE causing high system complexity and cost. The modularized dual-ended readout block (DERB) detector combines the Anger logic block detector with dual-ended readout to increase RE while measuring DOI. To investigate the trade-off between RE and spatial resolution, scalable DERB detectors with varying RE and light guide thickness were modelled with Monte- Carlo. Simulation showed RE can increase up to six-fold compared to the dual-ended readout design without significantly degrading spatial resolution. Experimental characterization of a RE = 9 : 8 DERB detector was found to achieve super-resolution <0.5 mm for resolving crystal indices, DOI resolution of ~5 mm FWHM, and mean energy resolution of 20% without recovering photons lost to neighbouring detector modules. The model was validated by agreement of simulation results adjusted for detector quantum efficiency with experimental results.

Current positron emission mammography (PEM) depth of interaction (DOI) enabling detectors have low scintillator to photodetector encoding ratios, RE causing high system complexity and cost. The modularized dual-ended readout block (DERB) detector combines the Anger logic block detector with dual-ended readout to increase RE while measuring DOI. To investigate the trade-off between RE and spatial resolution, scalable DERB detectors with varying RE and light guide thickness were modelled with Monte- Carlo. Simulation showed RE can increase up to six-fold compared to the dual-ended readout design without significantly degrading spatial resolution. Experimental characterization of a RE = 9 : 8 DERB detector was found to achieve super-resolution <0.5 mm for resolving crystal indices, DOI resolution of ~5 mm FWHM, and mean energy resolution of 20% without recovering photons lost to neighbouring detector modules. The model was validated by agreement of simulation results adjusted for detector quantum efficiency with experimental results.