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Magnetic Resonance Imaging (MRI) is a widely used soft tissue imaging technique that has gained considerable success because of its sensitivity to several tissue parameters. However, commercially available whole-body imaging systems with large encircling radio frequency (RF) and gradient coils are less efficient when the goal is to obtain detailed, high-resolution images with high specificity and sensitivity from localized regions of the body such as the female breast. This research addresses these problems by proposing a new design in RF coil development for breast cancer screening in a conventional 1.5T MRI system. The new design provides two resonant receiving modes that operate in a quadrature configuration, and a region of interest (ROI) that closely conforms to the shape of the female breast. We adopted an optimum design strategy that combined the analytic Biot-Savart intergral equation with the Method of Moment formulation in the development of electromagnetic models and simulation tools. These models were used to analyze the magnetic field distribution and the spatial field coverage, as well as the magnetic field uniformity in the ROI. Results from our analysis were employed in the construction of a highly scalable prototype. The validation of our design strategy is confirmed by comparisons with the commercial Ansoft HFSS v8.5 finite element package.

Ce projet de thèse porte sur le développement d'un dispositif instrumental basé sur les propriétés de non linéarité intrinsèques au matériau supraconducteur YBa2Cu3O7, qui restent jusqu'à présent peu explorées dans le régime radiofréquence (RF). Ceci, dans l'objectif de contrôler la commutation d'antennes supraconductrices ultrasensibles dédiées à l'Imagerie par Résonance Magnétique (IRM), de l'état supraconducteur à un état dissipatif. L'implémentation des antennes SHTC en imagerie permet d'atteindre les plus grandes sensibilités de détection observées actuellement en IRM à champ clinique, ce qui ouvre la voie au développement de l'imagerie moléculaire d'agents de contraste. Leur utilisation demeure cependant trop minoritaire et ce, entre autre, à cause de l'incompatibilité de la mise en œuvre des antennes YBa2Cu3O7 avec les méthodes de détection quantitative actuellement implémentées en imagerie moléculaire. Comme les techniques habituelles de découplage d'antennes ne sont pas transposables aux matériaux supraconducteurs, l'inactivation des antennes YBa2Cu3O7 à des échelles de temps compatibles avec une séquence IRM (< 1 msec) est un véritable défi, à la fois scientifique et technologique. Ce travail de recherche a pour but d'évaluer les performances de matériaux supraconducteurs à haute température critique tels que l' YBa2Cu3O7 en champ magnétique et dans le domaine des RF, en fonction de leurs propriétés nano-structurales et géométriques, et de développer un système permettant une commutation ultra rapide (ms) de l'état supraconducteur à l'état dissipatif et réciproquement, afin d'éviter le phénomène de concentration du flux magnétique lors de la phase émission, et de préserver la sensibilité du résonateur supraconducteur lors de la phase détection. / The aim of this work is to develop an instrumental device based on the nonlinear behaviour of superconducting materials such as YBa2Cu3O7 as a function of the emitted rf power, with the objective of controlling the switch between the zero resistance state and a dissipative state. This will then be applied to superconducting ultra-sensitive coils dedicated to magnetic resonance imaging (MRI). The implementation of HTS coils for biomedical imaging improves the sensitivity of the acquired images in standard clinical MRI devices. The superconducting coils are currently not implemented because of their incompatibility with quantitative detection methods used in molecular imaging today. As usual decoupling techniques for pick-up coils are not transferable to superconducting materials, the inactivation of superconducting YBa2Cu3O7 coils is a technical and a scientific challenge. The overall objective of this research work is to evaluate the performance of HTS materials in non-zero magnetic fields, in the radiofrequency regime, as a function of the nanostructural and geometric attributes of the material. Based on this, I shall develop a system for ultra-fast switch (msec) from the superconducting state to the dissipative state and vice versa, to avoid the phenomenon of of magnetic flux concentration during the emission phase.

A novel experimental setup has been realized to measure weak magnetic moments which can be modulated at radio frequencies (~1–5 MHz). Using an optimized radio-frequency (RF) pickup coil and lock-in amplifier, an experimental sensitivity of 10 -15 Am2 corresponding to 10 -18 emu has been demonstrated with a one second time constant. The detection limit at room temperature is 9.3 10 -16 Am2/√Hz limited by Johnson noise of the coil. In order to demonstrate the sensitivity of this technique it was used to electrically detect the polarized spins in semiconductors in zero applied magnetic fields. For example in GaAs, the magnetic moment due to a small number (~ 7 x 108) of spin polarized electrons generated by polarization modulated optical radiation was detected. Spin polarization was generated by optical injection using circularly polarized light which is modulated rapidly using an electro-optic cell. The modulated spin polarization generates a weak time-varying magnetic field which is detected by the sensitive radio-frequency coil. Using a radio-frequency lock-in amplifier, clear signals were obtained for bulk GaAs and Ge samples from which an optical spin orientation efficiency of ~ 10–20% could be determined for Ge at 1342 nm excitation wavelength at 127 K. In the presence of a small external magnetic field, the signal decayed according to the Hanle Effect, from which a spin lifetime of 4.6 ± 1.0 ns for electrons in bulk Ge at 127 K was extracted. The spin dynamics in n-Ge was further explored and the temperature dependence of the spin lifetime was plotted for a temperature range of about 90 K to 180 K. The temperature dependence of the optical pumping efficiency was also measured though no quantitative conclusions could be derived. The signals observed for semi-insulating GaAs, n-GaAs, GaSb and CdTe which are direct gap semiconductors are much larger than expected (almost two orders of magnitude). An attempt was made to explain this unexpected behavior of these direct gap semiconductors using the spin hall effect.