Thesis submitted in fulfilment of the requirements for the degree Master of Technology: Electrical Engineering in the Faculty of Engineering at the Cape Peninsula University of Technology, 2012 / In order to effectively determine the occurrences of space weather anomalies in near Earth orbit, a highly sensitive space-grade magnetometer system is needed for measuring changes in the Earth’s magnetic field, which is the aftermath of space weather storms. This research is a foundational work, aimed at evaluating a commercial-off-the-shelf (COTS) high temperature DC SQUID (superconducting quantum interference device) magnetometer, and establishing the possibility of using it for space weather applications. A SQUID magnetometer is a magnetic field measuring in strument that produces an electrical signal relative to the sensed external magnetic field intensity.

Orientadores: Abner de Siervo e Flavio Garcia / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Fisica Gleb Wataghin. / Made available in DSpace on 2018-08-12T11:00:44Z (GMT). No. of bitstreams: 1 Figueiredo_JoseJadsomSampaiode_M.pdf: 4194889 bytes, checksum: 489e23ac30c4fa90808ef2de00ae46d4 (MD5) Previous issue date: 2008 / Resumo: Nanopartículas (NPs) metálicas, filmes ultrafinos e sistemas nano-estruturados têm motivado vários estudos teóricos e experimentais devido a novas propriedades eletrônicas, óticas e magnéticas destes materiais. Nas NPs, tais propriedades estão diretamente relacionadas aos efeitos de tamanho (size effect) e superfície, os quais afetam suas estruturas eletrônica e cristalográfica, concentrando um maior número de átomos na superfície em relação ao seu volume. Estudos recentes têm sugerido que alguns metais nobres sem nenhum tipo de ordenamento ferromagnético espontâneo podem apresentá-lo, mesmo a temperatura ambiente, quando segmentados em forma de nanopartículas. Exemplos desses metais são Au e Pd. Apesar dos esforços para provar a existência de comportamento ferromagnético nestes materiais, não existem medidas que demonstrem de forma não ambígua a polarização ferromagnética nos átomos de Pd. Na maioria dos trabalhos mostrados na literatura, o ferromagnetismo é quantificado por magnetometria SQUID. Faz-se necessário, portanto, verificar a existência de ferromagnetismo nestes materiais utilizando-se de técnicas elemento específicas, tais como XMCD (dicroísmo circular magnético de raios X). Esta técnica é muito importante para determinação quantitativa e seletiva dos momentos magnéticos de spin e orbital para cada elemento separadamente. O nosso trabalho se diferencia em relação a estes, pois ao invés de estudarmos cada elemento individualmente trabalhamos com nanopartículas do composto bimetálico Aux Pd1-x (x =0,00, 0,25, 0,50, 0,75) passivadas por tiol. Medidas de SQUID indicaram claramente um sinal magnético nestas nanopartículas, inclusive à temperatura ambiente. Neste trabalho apresentaremos os resultados preliminares da caracterização destas nanopartículas por medidas de SQUID, XANES, XPS, bem como XMCD nas bordas L2,3 do Pd e L3 do Au . Ressaltamos também, o desenvolvimento de uma instrumentação para medidas de XMCD em ambientes de UHV onde é possível submeter às amostras a altos campos magnéticos e condições de baixas temperaturas. Com base nos resultados obtidos discutiremos a possibilidade de ferromagnetismo nestas nanopartículas e sua origem. / Abstract: Metallic Nanoparticles (NP's), ultra-thin films and nano-structured systems have motivated several theoretical and experimental works because of their new electronic optical and magnetic properties of these materials. In NP's, such properties are directly related to the size and surface effects, which affect its electronic and crystallographic structures, by concentrating a larger number of atoms on the surface in relation to their volume. Recent studies have suggested that some noble metals without any kind of spontaneous ferromagnetic order can exhibit it, even at room temperature, when segmented as nanoparticles. Examples of these metals are Au and Pd. Despite the efforts to prove the existence of a ferromagnetic behavior in such materials, there are no measurements that demonstrate unambiguously the ferromagnetic polarization in Pd atoms, for example. Most of the works shown in the literature have used SQUID measurements to characterize the ferromagnetism in these materials. It is therefore necessary to verify the existence of ferromagnetism in these materials by using element specific techniques, such as XMCD (X-ray magnetic circular dichroism). XMCD is a very important technique, which is element selective and performs quantitative determination of the spin and orbital magnetic contributions for each element separately. Our work has a particular difference when compared to others in literature because instead of studying each element individually we have worked with NP's of the bimetallic compound Aux Pd1-x (x = 0.00, 0.25, 0.50, 0.75) capped by thiol. SQUID measurements clearly showed ferromagnetic behavior in these nanoparticles, even at room temperature. In this thesis we will present results of a systematic characterization of these nanoparticles by a multi-technique approach which involves measurements with SQUID, XANES, XPS and XMCD in the L2,3 edges of the Pd and Au L3 edge. We also emphasize the development of a new instrumentation for XMCD measurements at UHV where samples can be submitted to high magnetic fields and conditions of low temperatures. Based on these findings we discuss the possibility of ferromagnetism in these nanoparticles and its origin. / Mestrado / Física da Matéria Condensada / Mestre em Física

Cette thèse s'articule autour de l'étude de la cohérence de la lumière produite à partir de sources de paires de photons intriqués et de micro-lasers. Nous avons produit et manipulé des états photoniques intriqués, et conduit des investigations à la fois fondamentales et appliquées. Les deux études menées sur les aspects fondamentaux de la non localité avaient pour but de relaxer partiellement deux contraintes sur lesquelles s'appuie l'inégalité de Bell standard en vue d'applications à la cryptographie quantique. Ainsi, en collaboration avec l'Université de Genève, nous avons redéfini la notion de localité en prenant en compte les influences sur les mesures de corrélations des choix des configurations expérimentales et d'une efficacité globale de détection limitée. Cela a permis de définir des inégalités de Bell généralisées et les violations expérimentales qui en découlent permettent d'attester de la non localité des états quantiques observés. Nous avons aussi étudié et mis en place une solution expérimentale autorisant l'émission de photons intriqués dans des pairs de canaux télécoms pour la cryptographie quantique. Nous avons montré la préservation de l'intrication sur 150 km et obtenu des débits records en comparaison avec les réalisations similaires. Enfin, nous avons étudié les propriétés de l’émission de lasers à semi-conducteurs aux dimensions réduites. L’émission de ces composants microscopiques s'accompagne de grandes fluctuations en intensité lorsque ceux-ci sont pompés en-dessous du seuil laser. Cette étude a permis de mieux comprendre comment se construit la cohérence laser dans ces systèmes. / In this thesis we study the coherence of light emitted by entangled photon-pair sources and micro-lasers. We have generated an manipulated entangled photonic states and investigated both fundamental (non locality) and applied (quantum cryptography) research directions. The objective of two fundamental studies on non locality was to partially relax the strong assumptions on which standard Bell tests rely. To this end, we redefined, in collaboration with the University of Geneva, the formalism of locality taking into account the influence, on correlation measurements, of the freedom of choice (in the basis settings) and of the limitation of the overall detection efficiency. Both assumptions allow devising generalized Bell inequalities whose experimental violations indicate that we can still attest for non locality for the observed states. In addition, we have studied and realized an experimental setup allowing to distribute entangled photon pairs in paired telecom channels for high bit rate quantum cryptography. We have shown that entanglement is preserved over a distance of 150 km with record rates for similar realizations, by mimicking classical network solutions exploiting, in an optimal fashion, the capacity of an optical fiber link via dense spectral multiplexing. Finally, we have studied the properties of light emitted by semiconductor lasers showing reduced dimensionality. This micro-lasers actually provide output light under high intensity fluctuations when they are pumped below the threshold. Their study allowed to refine our understanding on how the coherence builds up in these systems as the cavity is filled with photons.

No description available.

Die Transporteigenschaften eines Elektronengases mit reduzierter Dimensionalität werden von den Welleneigenschaften der Elektronen bestimmt. Dies ermöglicht es, verschiedene Quanteneffekte, wie Quanteninterferenz, zu beobachten. Im ersten Teil dieser Arbeit werden geätzte Quantenringe und eindimensionale (1D) Verengungen, basierend auf AlxGa1-xAs/GaAs-Heterostrukturen, hinsichtlich ihrer Transporteigenschaften untersucht. Messungen des thermischen Rauschens im Gleichgewichtszustand zeigen, dass der Erwartungswert mit den Rauschspektren aller 1D Verengungen übereinstimmt, jedoch um bis zu 60 % bei allen Quantenringen überschritten wird. Rauschmessungen im thermischen Nichtgleichgewicht ergeben, dass der Wärmefluss in Quantenringen mithilfe einer globalen Steuerelektrode (Topgate) an- und ausgeschaltet werden kann. Die magnetische Widerstandsänderung der Quantenringe zeigt Oszillationen, die dem Aharonov-Bohm-Effekt zugeordnet werden. Die Beobachtbarkeit dieser Oszillationen hängt stark von dem Abkühlvorgang der Probe ab und die Oszillationen zeigen Hinweise auf ein Schwebungsmuster sowie auf Phasenstarre. Im zweiten Teil der Arbeit werden die Oberflächenzustände von exfolierten Bi2Se3 Mikroflocken untersucht. Für Mikroflocken mit metallischen Temperaturabhängigkeiten des Widerstandes wurde schwache Anti-Lokalisierung beobachtet. Diese Beobachtung deutet darauf hin, dass sich die magnetische Widerstandsänderung weniger ausschließlich aus den 2D Oberflächenkanälen als vielmehr aus einem geschichtetem Transport von 2D Kanälen im Volumenkörper zusammensetzt. Eine Mikroflocke mit halbleitenden Eigenschaften zeigt keine Hinweise auf solch einen geschichteten 2D Transport und es wird angenommen, dass ihre magnetische Widerstandsänderung ausschließlich von den 2D Oberflächenzuständen verursacht wird. / The transport properties of an electron gas with reduced dimensionality are dominated by the electron’s wave nature. This allows to observe various quantum effects, such as quantum interference. In the first part of this thesis etched quantum rings and one-dimensional (1D) constrictions, based on AlxGa1-xAs/GaAs heterostructures, are investigated with respect to their transport properties. Thermal noise measurements in equilibrium show that the expectation value agrees with the noise spectra of all 1D constrictions but is exceeded by up to 60 % for the noise spectra of all quantum rings. Noise measurements in thermal non-equilibrium reveal that the heat flow can be switched on and off for a quantum ring by a global top-gate. The measured magnetoresistance of the quantum rings shows oscillations that are attributed to the Aharonov-Bohm effect. The observability of these oscillations strongly depends on the cooling process of the sample and the oscillations show indications of a beating as well as phase rigidity. In the second part of the thesis the surface states of exfoliated Bi2Se3 microflakes are studied. For microflakes that show a metallic temperature dependence of the resistance weak anti-localization is observed. This observation suggests that the magnetoresistance is a result of layered transport of 2D channels in the bulk rather than just the surface 2D channels. A microflake with semiconducting characteristics does not show indications of such a 2D layered transport and its magnetoresistance is considered to be carried by the 2D surface states only.

L'imagerie par résonance magnétique (IRM) est une modalité qui offre de bons contrastes et une bonne résolution spatiale, mais qui souffre d'un important problème de sensibilité. Pour répondre à cette problématique, le paradigme actuel est d'accroitre le champ magnétique des aimants d'IRM. Ceci mène toutefois à une explosion des coûts et à des contraintes accrues vis-à-vis des patients. L'approche que nous présentons est radicalement différente~: il s'agit de travailler à champ faible. Les antennes classiques n'étant pas assez sensibles pour recueillir le signal, l'idée est d'utiliser des SQIF. Ces derniers sont une nouvelle technologie d'antennes supraconductrices ultra-sensibles basées sur les réseaux de SQUID. Le projet vise à optimiser les capteurs SQIF et à les adapter pour la première fois à la RMN afin de mesurer un signal sur un aimant à 0.2~T.Pour ce faire, nous avons développé et étudié les performances de nouvelles architectures d'antennes SQIF afin de définir la géométrie la plus adaptée à la RMN. Nous avons également cherché à mieux comprendre comment le contexte d'utilisation de ces nouvelles antennes pouvait influencer leurs performances. Le jeu d'antennes le plus performant réalisé avait un facteur de transfert de 8.4~kVperT et un seuil de détection de 190~fTperHz. Il fut également observé que la présence d'un champ magnétique pendant le refroidissement de ces capteurs supraconducteurs dégradait leur réponse, phénomène à prendre en compte en RMN.Un Démonstrateur Super-QIF intégrant un SQIF dans l'IRM à 0.2~T fut conçu en tenant compte des contraintes géométriques et de l'environnement magnétique. Après sa fabrication, la température du cryostat était de 50~K, donc suffisante pour le bon fonctionnement des SQIF. Les premiers tests ont montrés que la présence du système ne perturbait pas le signal de RMN.Le démonstrateur est toujours en cours de développement et devrait permettre de mesurer un de RMN dans les mois à venir. À long terme, ces travaux pavent la voie à des applications des SQIF en IRM à champ terrestre. / Magnetic resonance imaging (MRI) is a modality that offers good contrasts and good spatial resolution, but suffers from a significant sensitivity problem. To address this issue, the current paradigm is to increase the magnetic field of MRI magnets. However, this leads to an explosion of costs and to increased constraints on patients. The approach we present is radically different: it involves working in a weak field. As conventional antennas are not sensitive enough to collect the signal, the idea is to use SQIF. These are a new ultra sensitive superconducting antenna technology based on SQUID networks. The project aims to optimize SQIF technology and adapt it to measure an NMR signal in a 0.2~T magnet.To do this, we developed and studied the performance of new SQIF antenna architectures in order to define the geometry most suitable for NMR. We also sought to better understand how the context of use of these new antennas could influence their performance. The best performing antennas set had a transfer factor of 8.4~kVperT and a detection threshold of 190~fTperHz. It was also observed that the presence of a magnetic field during the cooling of these superconducting sensors degraded their response, a phenomenon to be accounted for in NMR.The Super-QIF Demonstrator incorporating a SQIF in the 0.2~T MRI was designed considering the geometric constraints and the magnetic environment. After its assembly, the temperature of the cryostat was 50~K, therefore sufficient for the proper operation of SQIF. The first tests showed that the system presence did not disturb the NMR signal.The demonstrator is still under development and is expected to measure an NMR signal in the forthcoming months. In the long term, this work paves the way for applications of SQIF in Earth's field MRI.

Les qubits de spin sont des candidats prometteurs pour le traitement de l’information quantique en raison de leurs longs temps de cohérence. Les deux principaux qubits présents dans un système à trois spins ont été démontré au cours des dernières années dans la boîte quantique latérale triple. Le diagramme des niveaux d’énergie de quelques électrons dans la boîte quantique triple est beaucoup plus complexe que son homologue à deux ou à une boîte. Il en résulte des possibilités de fuites hors des qubits ciblés. Dans ce mémoire, nous présenterons une nouvelles technologie pour améliorer le contrôle des états de spin et augmenter le temps de cohérence des qubits. Nous avons effectué des mesures préliminaires sur des échantillons sur lesquels a été incorporé un microaimant. Ce microaimant crée un champ magnétique non-uniforme au niveau des boîtes quantiques qui sera utilisé pour effectuer une rotation de spin et pour améliorer certains types d’oscillations. Nous avons optimisé la forme des géométries afin de créer des gradients de champ magnétique optimaux spécifiquement pour la boîte quantique triple. Différents problèmes ont été encourus et la stratégie que nous avons adoptée pour les régler sera présentée. De plus, nous avons analysé les phénomènes de fuites entre les états quantiques en étudiant la réponse d’un système à trois spins en fonction de différentes impulsions électriques. Nous présentons deux processus d’interférence jamais répertoriés entre les qubits de la boîte quantique triple. Afin d’identifier l’origine de ces interférences, nous avons utilisé leur dépendance en champ magnétique.

Carrier, spin, charge current, and spin current injection by one- and two-color optical schemes are investigated within 30-band k·p theory. Parameters of the band model are optimized to give full-Brillouin zone band structures for GaAs and Ge that give accurate Γ-point effective masses and gyromagnetic factors and give access to the L valley, and to the E₁ and E₁+Δ₁ critical points in the linear optical absorption. Calculations of one- and two-photon carrier and spin injection and two-color current injection are performed for excitation energies in the range of 0—4 eV in GaAs and 0—3.5 eV in Ge. Significant spin and spin current injection occurs with 30% spin polarization in GaAs and Ge at photon energy matching the E₁ critical point. Further, the anisotropy and disparity of the current injection between parallel and perpendicular linearly-polarized beam configurations are calculated. For light propagating along a <111> crystal axis, anisotropic contributions in coherent current control and two-photon spin injection give rise to normal current components and in-plane spin components. In Ge, contributions from the holes to spin, electrical current, and spin current injection are investigated. Optical orientation results in 83% spin-polarized holes at the band edge. The effects of carrier dynamics in Ge are treated within a rate-equation model. The detection of spin dynamics in a pump-probe setup is considered, and the Fermi-factor approach is justified for electrons but not for holes. Carrier and current injection are further investigated in single-layer and bilayer graphene within the tight-binding model. In single-layer graphene, the linear-circular dichroism in two-photon absorption yields an absorption coefficient that is twice as large for circularly polarized light compared to linearly polarized light. Coherent current injection is largest for co-circularly polarized beams and zero for cross-circularly polarized beams. For linearly polarized beams, the magnitude of the injected current is independent of beam polarizations. In contrast, the injected current in bilayer graphene shows disparity between parallel and perpendicular configurations of the beams. The resulting angular dependence of the current is a macroscopic, measurable consequence of interlayer coupling in the bilayer.

Carrier, spin, charge current, and spin current injection by one- and two-color optical schemes are investigated within 30-band k·p theory. Parameters of the band model are optimized to give full-Brillouin zone band structures for GaAs and Ge that give accurate Γ-point effective masses and gyromagnetic factors and give access to the L valley, and to the E₁ and E₁+Δ₁ critical points in the linear optical absorption. Calculations of one- and two-photon carrier and spin injection and two-color current injection are performed for excitation energies in the range of 0—4 eV in GaAs and 0—3.5 eV in Ge. Significant spin and spin current injection occurs with 30% spin polarization in GaAs and Ge at photon energy matching the E₁ critical point. Further, the anisotropy and disparity of the current injection between parallel and perpendicular linearly-polarized beam configurations are calculated. For light propagating along a <111> crystal axis, anisotropic contributions in coherent current control and two-photon spin injection give rise to normal current components and in-plane spin components. In Ge, contributions from the holes to spin, electrical current, and spin current injection are investigated. Optical orientation results in 83% spin-polarized holes at the band edge. The effects of carrier dynamics in Ge are treated within a rate-equation model. The detection of spin dynamics in a pump-probe setup is considered, and the Fermi-factor approach is justified for electrons but not for holes. Carrier and current injection are further investigated in single-layer and bilayer graphene within the tight-binding model. In single-layer graphene, the linear-circular dichroism in two-photon absorption yields an absorption coefficient that is twice as large for circularly polarized light compared to linearly polarized light. Coherent current injection is largest for co-circularly polarized beams and zero for cross-circularly polarized beams. For linearly polarized beams, the magnitude of the injected current is independent of beam polarizations. In contrast, the injected current in bilayer graphene shows disparity between parallel and perpendicular configurations of the beams. The resulting angular dependence of the current is a macroscopic, measurable consequence of interlayer coupling in the bilayer.

L'objectif de ce travail était d’élaborer la brique de base d'un convertisseur analogique numérique supraconducteur à architecture pipeline, fonctionnant à 30GHz de fréquence d’échantillonnage. Ce convertisseur est constitué d’un bloc de N comparateurs disposés en cascade le long d’une ligne de transmission. Chaque étage de comparaison est constitué d'un SQUID rf mutuellement couplé à un tronçon de ligne de transmission. Lorsque le signal à convertir arrive à la hauteur d'un comparateur, il génère un champ magnétique qui induit un courant dans le SQUID rf. Ce courant pourra faire commuter la jonction Josephson du SQUID rf dans certains cas, en fonction des caractéristiques internes de la jonction Josephson du SQUID et de son environnement. La commutation, qui s’accompagne de l’apparition d’une impulsion de tension quantifiée SFQ, a été étudiée de manière théorique et expérimentale en fonction des différents paramètres du problème. / Superconductive analogue to digital converters (ADC) generally have speed and power dissipation advantages which should enable their application in telecommunication, medicine, and where an analogue signal (delivered e.g. by a sensor) needs to be digitized for post-processing.We are developing a new concept of analogue to digital converter using high critical temperature (Tc=90K) superconductors and operating at 30GHz; this converter is based an original structure, the pipeline architecture. The principle is to place a cascade of N comparators along a transmission line on which propagates the up-converted analogue signal. The carrier frequency is used in this case as a sampling signal.Each comparator, made with a SQUID loop, produces one bit at the carrier frequency: it codes the input signal by generating or not an RSFQ pulse (respectively "1” or “0"), and passes the residue (attenuated signal) in the following comparator.Here, we present steps for the comparator optimisation and mask design.Besides simulation results, we present the measurements at 30GHz carrier frequency of the comparator designed at low critical temperature (LTS). Finally, we suggest other tools to develop the optimised low critical temperature converter and we proposed the concept of the comparator operating at high critical temperature (HTS).