Tunneling phenomenon has been studied since the time of Sir Isaac Newton. In the case of neutron tunneling phenomenon, it is the quantum mechanics wave-particle duality which manifests itself. In this case, particularly, the neutron wave-packet under total reflection condition suffers the so-called frustrated total reflection as known in standard optics. More accurately, this tunneling phenomenon shows itself via sharp dips in the plateau of total reflection. The prerequisite to observe such quantum mechanics phenomenon lies within a thin film Fabry-Perot resonator configuration. This thin film Fabry-Perot resonator geometry consists of two reflecting mirrors separated by a transparent material from a neutron optics viewpoint. In view of the specific neutron scattering properties related to the spin of the neutron wave-packet. As a direct proof, isotopic nickel based thin films Fabry-Perot resonator have been fabricated by depositing thin film of nickel by ion beam sputtering. The vacuum chamber was pumped down to the pressure of 10-8 mbar and deposition was performed at pressure of 2x10-4 mbar. The deposition rate was kept at 1.5 nm / minute and thickness layers were monitored by a calibrated quartz microbalance. Unpolarized neutron reflectometry measurements were carried out at the ORPHEE reactor using the time-of-flight EROS reflectometer. The incidence neutron wavelength varied between 3 – 25 Å. The grazing angle and angular resolution were of the order of 0.8˚ and 0.05 respectively. The software program, a Matlab routine for the simulation of specular X-ray and neutron reflectivity data with matrix technique, was employed to simulate the phenomenon and thereafter the experimentally obtained data and calculated (theoretical) data were compared. From the analysis of the comparison, a conclusion was drawn about the agreement between experimental data and theoretical data. The tunneling phenomenon has been observed in nanostructured isotopic nickel based thin film Fabry-Perot resonator. It manifested itself by the existence of dips, tunneling resonances, in the total reflection plateau due to quasi-bound states in the isotopic nickel based thin film Fabry-Perot resonator. In total, there were 7 tunneling resonances. The full widths at half maximum of these dips were found to decrease with increasing momentum wave vector transfer (Q) and this correlated to the neutron lifetime in the nanostructured isotopic nickel based thin film Fabry-Perot resonator. / Physics / M. Sc. (Physics)

[pt] Nesta dissertação foram discutidos os resultados obtidos com um interferômetro Fabry-Perot intrínseco (FPI) a fibra óptica, para sensoriamento de deformação longitudinal, temperatura e campo magnético. O FPI foi construído através da emenda de uma fibra capilar entre dois pedaços de fibra padrão de telecomunicação, formando uma cavidade de ar retangular. Esta cavidade, quando atua como um sensor de deformação longitudinal, possui uma sensibilidade nove vezes maior que uma típica rede de Bragg (FBG). Porém, quando atua como sensor de temperatura, a sensibilidade é bem menor que a de uma rede de Bragg, tornando-se bastante útil para diversas aplicações. O sensor de campo magnético foi construído através da colagem da cavidade de ar num material magnetostrictivo, para que este convertesse as mudanças causadas em seu comprimento, devido à aplicação do campo magnético, em deformação longitudinal. Este sensor apresentou uma sensibilidade ao campo magnético quatro vezes maior do que quando o mesmo é construído com uma rede de Bragg. / [en] This thesis discusses the results obtained with an intrinsic Fabry-Perot interferometer (FPI) fiber, for sensing longitudinal strain, temperature and magnetic field. The FPI was constructed by splicing a capillary fiber between two pieces of standard telecommunication fiber, forming a rectangular air cavity. This cavity, when acting as a longitudinal deformation sensor has a sensitivity nine times greater than a typical Bragg grating (FBG). However, when it acts as a temperature sensor, the sensitivity is much smaller than a Bragg grating, making it useful for various applications. The magnetic field sensor was built placing the air cavity on a magnetostrictive material, so that it converted the changes brought in its length due to the application of the magnetic field in longitudinal deformation. The sensor showed a sensitivity to the magnetic field four times higher than when it is built with a Bragg grating.

L’équipe Physique des Galaxies du Laboratoire d’Astrophysique de Marseille a développé un nouveau type d'interféromètre de Fabry-Perot, équipé de trois actionneurs piézoélectriques amplifiés et de trois capteurs capacitifs permettant le contrôle de l'espacement et du parallélisme des lames de verres de l'ordre de 200 µm avec une précision de positionnement du nm.L'objectif visé de ce manuscrit, composé de 3 parties, est le pilotage de cet interféromètre. La première partie, composée des chapitres 1 et 2, présente les généralités sur l'interférométrie de Fabry-Perot puis décrit les instruments 3DNTT et BTFI où seront installés l'interféromètre de nouvelle génération et son contrôleur associé. La conception et la réalisation d'un amplificateur hybride en vue de la réduction des non-linéarités des actionneurs piézoélectriques mettent fin à cette partie.La deuxième partie, chapitres 3 et 4, décrit le développement et la réalisation du contrôleur. Pour cela, une démarche basée sur le concept du Co-design a été adoptée.Le contrôleur ainsi réalisé est composé d'une carte de développement Microzed dont le cœur est un système sur puce de la série Zynq 7000 EPP et d'une carte d'interfaçage comportant des convertisseurs 3 ADC et 3 DAC et des circuits d'alimentation. La troisième et dernière partie, chapitres 5 et 6, traite de la modélisation d'état de l’interféromètre de Fabry-Perot et de son contrôle : un contrôle classique basé sur la régulation PID et un contrôle robuste et optimal basé sur le filtrage de KALMAN. Cette dernière partie conclut sur les perspectives pouvant découler des contributions de ce travail sur le contrôle et la commande Fabry-Perot. / The Physics of Galaxies Team of Laboratoire d'Astrophysique de Marseille (LAM) has developed a new type of Fabry-Perot, with three amplified piezoelectric actuators and three capacitive sensors to control the spacing and parallelism of mirror plates of approximately 200 µm with a positioning accuracy of 3 nm.The purpose of this manuscript, consisting of 3 parts is the control of this interferometer.The first part, consisting of Chapters 1 and 2 presents the general interferometry Fabry-Perot and then describes 3DNTT and BTFI instruments which will be installed the next generation interferometer and its associated controller. The design and implementation of a hybrid amplifier to reduce non-linearities of the piezoelectric actuators (hysteresis and creep) end this first part.The second part, Chapters 3 and 4, describes the development and implementation of the controller.For this, an approach based on codesign concept was adopted. The thus achieved controller consists of a Microzed development board whose heart is a system on chip of the 7000 series Zynq EPP (FPGA + Dual-Core ARM Cortex A9) and an interface card with converters (3 ADC and 3 DAC) and power supply circuits.For the finalization of the controller, two steps are necessary: hardware design in Xilinx Vivado and software design in Xilinx SDK.The third and final section, chapters 5 and 6 deals with the Fabry-Perot space-state modeling and its control: a classic control based on PID control and a robust and optimal control based on KALMAN filtering. This last part concludes the outlook may result from contributions of this work on the monitoring and control of the Fabry-Perot.

In the past decades, the miniaturization in optics led to new devices with structural sizes in the range of the light wavelength, where the photonic modes are con- fined and the number of states is limited. In the smallest microcavities, i.e. micrometer sized optical resonators, the propagation of only one mode is permitted that is simultaneously amplified internally. This particularly strong enhancement of the electric field is directly related to the quality factor of the cavity. By introducing an optical dipole into a high-Q microcavity, the spontaneous emission is amplified at the cavity mode frequency enabling stimulated emission in an inverted system. Although some of theses cavity e®ects can only be understood by quantum elec- trodynamic theory, most mechanisms are accessible by classical and semi-classical approaches. In this thesis, one-dimensional planar microcavities with quality factors up to 4500 have been fabricated by physical vapor deposition of dielectric thin films and organic active materials. A new cavity design based on anisotropic dielectric mirrors grown by oblique angle deposition microcavities with two energetically shifted orthogonally polarized modes is presented. The application of these anisotropic structures for terahertz di®erence signal generation is demonstrated in spectrally and time resolved transmission experiments, where optical beats with repetition rates in the terahertz range are observed. Optically pumped organic vertical cavity surface emitting lasers (VCSELs) have been realized by applying an organic solid state laser compound and high reflectance distributed Bragg reflectors. These lasers combine a very low laser threshold with small beam divergence and good stability. A transfer of the anisotropic design towards an organic VCSEL results in the generation of two perpendicularly polarized laser modes with a splitting adjustable by the fabrication conditions. The observation of an oscillation of two laser modes in a photomixing experiment proves a phase coupling mechanism. This demonstrates the potential of the anisotropic cavity design for a passive or active component in a terahertz radiation source or frequency generator. Furthermore, microcavities with two and three coupled resonators are investigated. By the application of time-resolved transmission experiments, spatial oscil- lations of the internal electric field - photonic Bloch oscillations - are successfully demonstrated. In combination with the anisotropic microcavities, this is a second concept for the modulation of transmitted light with terahertz frequencies. All experiments are accompanied by numerical or analytical models. Transmission experiments of continuously incident light and single laser pulses are compared with transfer matrix simulations and Fourier transform based approaches. For the modeling of emission experiments, a plane wave expansion method is successfully used. For the analysis of the organic VCSEL dynamics, we apply a set of rate equations that explains the gain switching process.

Realising Si-based electrically driven light emitters in a process technology compatible with mainstream microelectronics CMOS technology is key requirement for the implementation of low-cost Si-based optoelectronics and thus one of the big challenges of semiconductor technology. This work has focused on the development of microcavity enhanced silicon LEDs (MCLEDs), including their design, fabrication, and experimental as well as theoretical analysis. As a light emitting layer the abrupt pn-junction of a Si diode was used, which was fabricated by ion implantation of boron into n-type silicon. Such forward biased pn-junctions exhibit room-temperature EL at a wavelength of 1138 nm with a reasonably high power efficiency of 0.1%. Two MCLEDs emitting light at the resonant wavelength about 1150 nm were demonstrated: a) 1-lambda MCLED with the resonator formed by 90 nm thin metallic CoSi2 mirror at the bottom and semitransparent distributed Bragg reflector (DBR) on the top; b) 5.5-lambda MCLED with the resonator formed by high reflecting DBR at the bottom and semitransparent top DBR. Using the appoach of the 5.5-lambda MCLED with two DBRs the extraction efficiency is enhanced by about 65% compared to the silicon bulk pn-junction diode.

[pt] No presente trabalho, demonstramos o uso de fibras de cristais fotônicos (PCF) em diferentes configurações para sensoriamento. Investigamos o uso de fibras PCF com alta birrefringência para sensoriamento de pressão hidrostática e deformação, explorando a baixa dependência térmica. Onde a interferência entre os modos que se propagam em uma fibra birrefringente é analisada. Monitoramos o deslocamento do padrão de interferência do espectro de reflexão, com a variação da pressão ou deformação aplicada à fibra. Demonstramos uma técnica de criar cavidades Fabry-Perot dentro de uma fibra óptica, bem como uma técnica para controlar seu comprimento, e consequentemente, o período das franjas no padrão de interferência no espectro de reflexão. O interferômetro Fabry-Perot (FPI) investigado, possuí um altíssimo contraste nas franjas do padrão de interferência, acima dos 30 dB, sendo no momento, o recorde para o valor do contraste das franjas para FPI silica-ar. O dispositivo foi investigado quanto à resposta a deformação. Um robusto encapsulamento foi feito, possibilitando investigar a resposta do dispositivo à vibração externa. Um estudo da relação da sensibilidade com o comprimento do FPI é também investigado. Construímos um outro interferômetro a partir de um pedaço de fibra PCF e de duas regiões de colapso de suas micro-estruturas. Estas regiões permitem a excitação e recombinação dos modos da fibra. Um dos modos que participa da interferência, é o modo de casca da fibra PCF, o qual é sensível a mudança de índice de refração do meio. O dispositivo apresenta contraste acima dos 40 dB, e é investigado quanto à resposta as mudanças de índices de refração do meio externo em contato com a fibra. Com a mesma montagem, funcionalizamos um pedaço de 2,0 cm de PCF para monitoramento de respiração humana. A partir disso, desenvolvemos um dispositivo capaz de monitorar a respiração do ser humano. / [en] In this work, we have demonstrated the use of Photonic Crystal Fiber (PCF), in different configurations, for sensing applications. The high birefringence and low temperature dependence characteristics of the PCF were explored for sensing hydrostatic pressure and deformation in a reflection configuration. Sensing was based on the analysis of the interference patterns between the modes that propagate in the birefringent fiber under the variation of pressure and deformation applied to the fiber. We have also demonstrated a technique to manufacture a Fabry-Perot Interferometer (FPI) cavity within an optical fiber with control of the cavity length and thus the control of the period of the fringes in the interference pattern. The Fabry-Perot Interferometer investigated presented a very high fringe contrast, above 30 dB, and showed a record value of the contrast of the fringes for FPI silica-air. The FPI device integrated within the fiber was tested as a strain sensor and also as a device to monitor vibration. A study of the relative sensitivity of the length of the FPI was also investigated. Another interferometer was built from a piece of standard fiber and a PCF with two regions of collapsed microstructures. These regions allowed the excitation and recombination of the fiber modes. This device was tested as a refractive index sensor, presenting a fringe contrast above 40 dB. An application of this device was the development of a humid sensor to monitor human breathing.

Fabry-Perot interferometer (FPI) devices are designed based on the electro-optic (EO) activities of nonlinear optical (NLO) polymer materials for tunable optical filters (TOFs) and spatial light modulators (SLMs). The performance of the EO polymer based FPI devices is theoretically modeled with first order approximation on the FPI cavity interface phase dispersion. NLO materials including TCBD coupled hybrid sol-gel, AJL8/amorphous polycarbonate (APC), and AJLS102/APC are incorporated in FPI structures with distributed Bragg reflector mirrors and transparent conducting oxide electrodes for TOFs. High finesse (over 200), low drive voltage (10 dB isolation ratio with 5 V), and fast settling time (about sub-millisecond) are achieved. The physical origin of the large tunabilities is explored and the contributions from EO effect and inverse piezoelectric effect are analyzed. EO polymer SWOHF3ME/APC is employed in FPI devices with simplified structures for SLMs. Modulation beyond megahertz level is achieved with constant modulation ratio from DC frequency to high operation speed. The operation speed can be potentially over gigahertz with improved device and drive circuit design. When the EO polymer based SLM is configured to work at near the resonance band of the NLO material, the spectral tunability is increased due to resonance enhanced EO activity and the SLM performance is significantly improved. The EO polymer based FPI devices can be further optimized and are promising candidates for many optoelectronic applications.

No presente trabalho, investigamos algumas propriedades e aplicações para imagens de diferença de polarização (PDI\'s) propondo dois sistemas de aquisição destas imagens como alternativas à arquitetura proposta por Tyo (1996). O primeiro sistema aqui abordado faz uso de duas câmeras e dois polarizadores para a obtenção de PDI\'s. A redundância, em termos de elementos de aquisição de imagens, visa suprir uma deficiência do sistema supracitado, qual seja a sua impossibilidade de operar em tempo real. O segundo projeto propõe a utilização de filtros polarizadores baseados em implementações de estruturas Fabry-Perot utilizando-se filmes finos birrefringentes de TiOx, como elemento principal de um dispositivo que possa ser produzido na forma de um microssistema integrado de aquisição de imagens completamente compatível com as tecnologias de produção CMOS disponíveis hoje em dia. Dadas as possibilidades envolvendo esse último projeto, definimos como objetivo principal deste trabalho a obtenção de filtros polarizadores baseados em tecnologia de filmes finos birrefringentes, que foram obtidos por deposição física num equipamento de Sputtering DC. Na etapa de análise dos dados, foram feitas caracterizações ópticas (espectrofotometria) e RBS tanto dos filtros finais quanto dos filmes de TiOx, que foram ensaiados previamente para a extração de parâmetros necessários para o projeto dos filtros de interferência. Conclui-se o trabalho comprovando a possibilidade de se obter filtros polarizadores que possam ser utilizados em sistemas integrados de aquisição de imagens, mas ressalva-se que o equipamento de Sputtering DC empregado não é o ideal para essa aplicação, sugerindo-se o uso de equipamentos capazes de monitorar espessura e índices de refração durante o processo de deposição dos filmes (um exemplo seria um sistema de deposição por e-beam acoplado a um elipsômetro de transmitância) / In the present work, it was investigated some properties and applications for polarization-difference images (PDI\'s), what led us to the proposition of two acquisition systems for such images as alternatives to the architecture proposed by Tyo (1996). The first system here discussed uses two cameras and two polarizers in the attainment of PDI\'s. The image elements redundancy is supposed to overcome a deficiency of the above-mentioned system that is its inability to operate in real time. The second project proposes the use of polarizing filters based on Fabry-Perot structures obtained with birefringent thin films of TiOx. Such filters are the key elements in a device that can be implemented as an integrated microsystem, fully compatible with the CMOS production technologies, available nowadays. Given the possibilities associated with this last project, it was defined as the main goal of this work, the attainment of polarizing filters based on birefringent thin films technology, physically deposited by a DC Sputtering equipment. During the phase of data analysis, it was carried out optical characterizations (spectrofotometry) as well as RBS analysis, both for the filters itself and for the TiOx films, that were previously investigated in order to determine the required parameters for the design of the interference filters. This work is concluded by proving the possibility of using polarizing filters in integrated image acquisition systems, but a remark ismade stating that the employed equipment is not the ideal one for such applications and it is suggested the use of deposition set up capable to monitor thickness and refractive indexes during the run (an example would be an e-beam equipment connected to a transmittance ellipsometer).

No presente trabalho, investigamos algumas propriedades e aplicações para imagens de diferença de polarização (PDI\'s) propondo dois sistemas de aquisição destas imagens como alternativas à arquitetura proposta por Tyo (1996). O primeiro sistema aqui abordado faz uso de duas câmeras e dois polarizadores para a obtenção de PDI\'s. A redundância, em termos de elementos de aquisição de imagens, visa suprir uma deficiência do sistema supracitado, qual seja a sua impossibilidade de operar em tempo real. O segundo projeto propõe a utilização de filtros polarizadores baseados em implementações de estruturas Fabry-Perot utilizando-se filmes finos birrefringentes de TiOx, como elemento principal de um dispositivo que possa ser produzido na forma de um microssistema integrado de aquisição de imagens completamente compatível com as tecnologias de produção CMOS disponíveis hoje em dia. Dadas as possibilidades envolvendo esse último projeto, definimos como objetivo principal deste trabalho a obtenção de filtros polarizadores baseados em tecnologia de filmes finos birrefringentes, que foram obtidos por deposição física num equipamento de Sputtering DC. Na etapa de análise dos dados, foram feitas caracterizações ópticas (espectrofotometria) e RBS tanto dos filtros finais quanto dos filmes de TiOx, que foram ensaiados previamente para a extração de parâmetros necessários para o projeto dos filtros de interferência. Conclui-se o trabalho comprovando a possibilidade de se obter filtros polarizadores que possam ser utilizados em sistemas integrados de aquisição de imagens, mas ressalva-se que o equipamento de Sputtering DC empregado não é o ideal para essa aplicação, sugerindo-se o uso de equipamentos capazes de monitorar espessura e índices de refração durante o processo de deposição dos filmes (um exemplo seria um sistema de deposição por e-beam acoplado a um elipsômetro de transmitância) / In the present work, it was investigated some properties and applications for polarization-difference images (PDI\'s), what led us to the proposition of two acquisition systems for such images as alternatives to the architecture proposed by Tyo (1996). The first system here discussed uses two cameras and two polarizers in the attainment of PDI\'s. The image elements redundancy is supposed to overcome a deficiency of the above-mentioned system that is its inability to operate in real time. The second project proposes the use of polarizing filters based on Fabry-Perot structures obtained with birefringent thin films of TiOx. Such filters are the key elements in a device that can be implemented as an integrated microsystem, fully compatible with the CMOS production technologies, available nowadays. Given the possibilities associated with this last project, it was defined as the main goal of this work, the attainment of polarizing filters based on birefringent thin films technology, physically deposited by a DC Sputtering equipment. During the phase of data analysis, it was carried out optical characterizations (spectrofotometry) as well as RBS analysis, both for the filters itself and for the TiOx films, that were previously investigated in order to determine the required parameters for the design of the interference filters. This work is concluded by proving the possibility of using polarizing filters in integrated image acquisition systems, but a remark ismade stating that the employed equipment is not the ideal one for such applications and it is suggested the use of deposition set up capable to monitor thickness and refractive indexes during the run (an example would be an e-beam equipment connected to a transmittance ellipsometer).

Le comportement d'un empilement multicouche interférentiel soumis à une sollicitation extérieure, de type thermique ou mécanique, est devenu un point critique, au regard des exigences de stabilité de plus en plus sévères exprimées aujourd'hui sur les performances des empilements. Afin de prédire de manière rigoureuse et précise l'évolution de ces performances optiques sous sollicitation, quelle que soit la formule de l'empilement, il est nécessaire de connaître les variations de l'indice de réfraction n et de l'épaisseur e de chaque couche, de chaque matériau, de l'empilement. Cela implique la connaissance des paramètres permettant de décrire ces variations, à savoir le coefficient d'expansion thermique a, le coefficient de Poisson n, le coefficient de dépendance de l'indice de réfraction avec la température b, et enfin les coefficients élasto-optiques p11 et p12. Cependant, si l'effet global d'une sollicitation est mesurable sur un empilement complet, ces coefficients sont quasi inconnus au niveau d'une couche mince individuelle tant le même effet devient faible sur une couche de quelques centaines de nanomètres d'épaisseur. Pour mesurer ces paramètres à ce niveau élémentaire, nous présentons une méthode optique basée sur l'utilisation d'un interféromètre de Fabry-Perot comportant une couche du matériau à caractériser, soumis à un échelon de température. L'étude se scinde selon deux axes. Le premier, purement optique, s'intéresse particulièrement au principe de la mesure et à la stabilité de la méthode face aux erreurs et aux bruits de mesures. Le second, purement mécanique, montre comment s'affranchir des inévitables déformations mécaniques des lames de l'interféromètre soumis à la sollicitation thermique, ce qui est indispensable pour parvenir à la mesure des coefficients recherchés. La réunion de ces deux axes a permis de finaliser la méthode de mesure et de concevoir puis réaliser un banc expérimental ayant une résolution en longueur d'onde inférieure au picomètre, dédié à l'extraction de ces paramètres avec la précision requise. Nous en présentons les premiers résultats expérimentaux dédiés à montrer la faisabilité de la mesure.