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Excitation résonante de boîtes quantiques pour la génération d'états non-classiques de la lumière / Resonant excitation of quantum dots for the generation of non classical state of lightMonniello, Leonard 19 January 2015 (has links)
Les développements en information quantique nécessitent le contrôle et la manipulation d'états quantiques. Parmi les systèmes en physique du solide, les boîtes quantiques semiconductrices sont de bons candidats pour réaliser des bits quantiques. La taille nanométrique de ces objets conduit à un confinement spatial à trois dimensions des porteurs : le spectre d'énergie est discret comme celui d'un atome. Ces objets sont étudiés pour leurs propriétés optiques, et notamment pour l'émission de photons uniques et indiscernables, qui sont des états quantiques de la lumière. Le travail de cette thèse consiste à étudier des boîtes quantiques uniques d'InAs/GaAs excitées à la résonance de leur transition optique, à l'aide d'impulsions lumineuses picosecondes. Grâce à une géométrie unidimensionnelle en guide d'onde, il est possible de s'affranchir de la lumière diffusée du laser d'excitation, et d'observer la luminescence résonante des boîtes. On atteint alors le régime d'oscillations de Rabi qui permet d'inscrire dans la boîte une superposition cohérente du système à deux niveaux, c'est un bit quantique. Cependant, le couplage entre la boîte et son environnement modifie les propriétés de cohérence des boîtes quantiques, limitant la possibilité de réaliser des opérations sur les qubits. Deux phénomènes principaux de décohérence ont été modélisés : l'interaction avec les phonons longitudinaux acoustiques de la matrice environnante de la boîte et le couplage avec le mode électromagnétique. Nous avons enfin étudié la statistique d'émission de photons des boîtes quantiques, et nous montrons qu'elles constituent de bonnes sources de photons uniques indiscernables, à la demande. / Developments in quantum information require controlling and manipulating quantum bits. Among solid state emitters, semiconductor quantum dots seem promising to realize quantum bits. First, the nanometric size of those structures leads to the confinement of the carriers in the three directions of space, so that their energy spectrum becomes atom-like. Furthermore, they can easily be integrated into electronic and optic devices. Such structures are studied for their optical properties, especially the emission of single and indistinguishable photons, which are quantum states of light. In the present work InAs/GaAs quantum dots have been studied under resonant excitation with picosecond laser pulses. One-dimensional waveguiding geometry has been used to suppress the scattered excitation laser allowing the observation of a single dot resonant luminescence. The coupling between the laser and the dot leads to the Rabi oscillations regime which enables to address a coherent superposition of states in the two-level system, meaning a quantum bit. However, the coupling between the dot and its environment changes the coherence properties of the dots, limiting the time during which operations on the qubits are possible. Two main phenomena have been observed and studied: the interaction between the dots and the longitudinal acoustic phonons of the GaAs matrix and the coupling with the electromagnetic mode. Finally, the photon emission statistics of the quantum dots have been studied, showing that quantum dots are on demand good emitters of indistinguishable single photons.
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Resonant Excitation Of Ions In Paul Trap Mass SpectrometerSarurkar, Vikram A 06 1900 (has links)
A Paul trap mass spectrometer has a three-electrode geometry mass analyzer consisting of two identical end cap electrodes and a ring electrode. Traditionally, the two end cap electrodes are electrically grounded and an RF potential is applied to the central ring electrode to generate the "trapping field". Ions of the analyte sample are formed in situ by electron bombardment and mass analysis of the fragment ions is performed by mass selectively destabilizing the ions from the trap. The inhornogeneities present in the trapping field (introduced either by misalignment of the trap geometry or by applying a dipolar auxiliary excitation across the end cap electrodes) give rise to various interesting phenomena including, resonance ejection of the trapped ions This thesis is concerned with taking a look into the experimental aspects associated with resonance ejection of ions caused by the dipolar excitation Additionally, u also reports the work undertaken to develop necessary instrumentation for resonant excitation experiments and my contribution to operational>zc the Paul trap mass spectrometer fabricated in the laboratory. The thesis is divided into 5 chapters.
Chapter 1 is an introductory chapter. After discussing the conditions for stability of the trapped ions, it goes on to present a brief survey of a variety of applications in literature, which have used resonant excitation. Towards the end, the motivation of the present effort and the scope of work in the thesis have been spelt out. This includes (a) redesign of the ion detector electronics, (b) design of an auxiliary excitation generator, and (c) studies on resonance ejection.
Chapter 2 outlines the design considerations, circuit description and fabrication details for the ion detector electronics. The circuits presented in this chapter include (a) electrometer amplifier and (b) -3 kV DC supply for the electron multiplier detector. The electrometer amplifier amplifies the ion current signal from the electron multiplier detector and it needs to have a high input impedance and a high slew rate. The electron multiplier detector requires -3 kV DC power supply for operation. The -3 kV DC power supply is required to have a regulated output voltage with low ripple in the output.
Chapter 3 presents the design considerations, circuit description and fabrication details for the auxiliary excitation generator. The auxiliary excitation generator is a three channel DDS (Direct Digital Synthesis) oscillator with independent control of frequency amplitude, and phase of the output signal. Chapter 3 also discusses the micro controller based control sub-system that allows the user to set above mentioned output parameters. The control sub-system provides a user-friendly keyboard interface and 2-line alphanumeric LCD display per channel. It also provides various bus interfaces (such as I2C and SPI) to interface with DDS oscillator ICs, amplitude control DAC, and LCD displays. The chapter then goes on to describe the implementation details of the software written for the control sub-system. The hardware design is simplified by using a micro controller as heart of the control sub-system and employing the software to handle the complex functions. As an example, the design of the keyboard interface is simplified by directly connecting a matrix keyboard to the input/output port of the micro controller. The software is used to scan the keyboard, detect key press and find out the key pressed. Nonetheless, in order to meet specific performance required for the present work, the software needs to have a sense of time, be portable and scalable. Details of the "layered" architecture adopted by as to meet these specific requirements, the lower level "driver" functions implemented for various interfaces of the control sub-system, and the higher level or the "application" software, are described. The application software uses the driver functions to accomplish various tasks required to be executed by the control sub-system. Finally, the chapter presents the design consideration and fabrication details of the coupling transformer used to couple the output of the auxiliary excitation generator to the Paul trap
Chapter 4 describes the resonant excitation experiments performed as part of the present work. First of all the chapter presents the improvement in the performance of the Paul trap mass spectrometer as a result of redesigned ion detector electronics It is seen that the resolution is improved significantly due to the improved response time of the electrometer amplifier. The chapter then describes the effect of the resonant excitation on the ions and also that the frequency of the applied auxiliary excitation should be between 500 kHz to 125 kHz. Next, a number of mass spectra for different frequencies of the applied auxiliary excitation are presented. These mass spectra indicate that the resonant ejection sets in for lower masses even at lower amplitude of the auxiliary excitation where as higher amplitude is required for the resonant ejection of the higher masses. It is seen that the resonant excitation of ions improves resolution of the mass spectrum. Moreover, the auxiliary excitation results in ejection of the ions at lower amplitude of the RF voltage and thus allows extending the mass range of the mass spectrometer. We present the mass spectrum of CCI4 which is not possible to normally record in our instrument. We also present results intended to understand the relation between frequency and amplitude of the auxiliary excitation on the mass spectra of benzene. Finally, results of an interesting experiment are presented which indicates the presence of the non-linear resonance points in the Paul trap.
Chapter 5 presents the concluding remarks.
References cited in the thesis are attached in their alphabetical order at the end of the thesis.
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Integrated nano-optomechanics in photonic crystal / Nano-optomécanique intégrée dans les cristaux photoniquesZhu, Rui 16 September 2019 (has links)
Les oscillateurs de référence de haute pureté sont actuellement utilisés dans un grand nombre d’applications allant du contrôle de fréquence aux horloges pour les radars, les GPS et l’espace... Les tendances actuelles dans ce domaine requièrent des architectures miniaturisées avec la génération de signaux directement dans la gamme de fréquences d’intérêt, autour de quelques GHz. Récemment, de nouvelles architectures basées sur les principes de l’optomécanique ont vu le jour dans ce but. De tels oscillateurs optomécanique génèrent non seulement des signaux hyperfréquences directement dans la gamme de fréquences GHz avec éventuellement un faible bruit de phase, mais permettent également un degré élevé d'intégration sur puce. Ce travail de thèse s'inscrit dans cette démarche. L’oscillateur optomécanique étudié se compose de cavités à cristaux photoniques suspendues couplées à des guides d’ondes silicium sur isolant intégrés dans une architecture tridimensionnelle. Ces cavités abritent des modes optiques fortement confinés autour de 1550nm et des modes mécaniques dans le GHz. De plus, ces structures présentent un recouvrement spatial entre phonon et photon élevé. Il en résulte un couplage optomécanique amélioré. Cette force de couplage optomécanique améliorée est ici sondée optiquement sur des structures à cristaux photoniques de conception optimisée. Ces cavités sont réalisées dans des matériaux semi-conducteurs III-V dont la piézoélectricité nous permet d'intégrer des outils supplémentaires pour sonder et contrôler les vibrations mécaniques via un pilotage capacitif, piézoélectrique ou acoustique. Ce contrôle total des modes mécaniques et de l’interaction optomécanique ouvre la voie à la mise en œuvre de circuits intégrés pour le verrouillage par injection et des boucles de rétroaction permettant de réduire le bruit de phase de l’oscillateur. / High purity reference oscillators are currently used in a wide variety of frequency control and timing applications including radar, GPS, space... Current trends in such fields call for miniaturized architectures with direct signal generation in the frequency range of interest, around few GHz. Recently, novel optomechanically-enhanced architectures have emerged with this purpose. Such optomechanically-driven oscillators not only generate microwave signals directly in the GHz frequency range with possibly low phase noise but also are amenable to a high degree of integration on single chip settings. This PhD work falls within this scope. The optomechanically-driven oscillator under study consists of suspended photonic crystal cavities coupled to integrated silicon-on-insulator waveguides in a three-dimensional architecture. These cavities harbor highly-confined optical modes around 1,55 µm and mechanical modes in the GHz and most importantly, feature a high phonon-photon spatial overlap, all resulting in an enhanced optomechanical coupling. This enhanced optomechanical coupling strength is here probed optically on photonic crystal structures with optimized design. These cavities are hosted in III-V semiconductor materials whose piezoelectricity enable us to integrate additional tools for probing and controlling mechanical vibrations via capacitive, piezoelectric or acoustic driving. This full control over the mechanical modes and optomechanical interaction, paves the way towards the implementation of integrated injection locking circuits of feedback loops for reducing the phase noise of the oscillator.
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Low Energy X-ray Radiosensitization Activated with High-Z ElementsLim, Sara Gail Ng January 2014 (has links)
No description available.
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Indiscernabilité des photons émis par une boîte quantique semiconductrice sous excitation résonnante continue / Indistinguishability of the photons emitted by a semiconductor quantum dot under continuous-wave resonant excitationProux, Raphaël 26 November 2015 (has links)
Les boîtes quantiques sont des sources de photons uniques prometteuses pour les réseaux d’information quantique, qui peuvent être intégrées dans des circuits photoniques et s’appuyer sur des technologies de semi-conducteur éprouvées. Dans ce contexte, ce travail se concentre sur les propriétés d’indiscernabilité des photons émis par une boîte quantique semiconductrice sous excitation résonnante. Nous utilisons une configuration particulière où les boîtes sont insérées dans une microcavité planaire permettant de s’affranchir du fond de diffusion parasite du laser d’excitation et d’améliorer la collection du signal d’émission. Nous pouvons ainsi explorer un régime de très basse puissance, où les photons d’excitation sont diffusés élastiquement sur la transition fondamentale de la boîte quantique (régime de diffusion Rayleigh résonnante). Dans ce régime, la cohérence du laser d’excitation est transmise aux photons émis, faisant des boîtes quantiques une source de photons uniques avec une cohérence extrêmement longue.Les propriétés d’indiscernabilité sont étudiées en utilisant les interférences à deux photons (coalescence) dans un interféromètre de Hong–Ou–Mandel. Une étude expérimentale complète de l’indiscernabilité est présentée en fonction de la puissance d’excitation ainsi que du temps de cohérence du laser d’excitation. Elle montre en particulier l’effet de la diffusion élastique dans la limite de basse puissance d’excitation. Il apparaît qu’une nouvelle caractéristique quantitative doit être introduite afin d’estimer l’indiscernabilité en tant que phénomène temporel, un aspect particulièrement important lorsque les émetteurs sont des sources continues de photons. / Quantum dots are good candidates as single photon emitters for quantum information networks, facilitating their integration in photonic circuits based on well known semiconductor technology. In this context, this work focuses on the indistinguishability of the photons emitted by semiconductor quantum dots excited resonantly. We use a peculiar configuration where the quantumdots are embedded in a planar microcavity, allowing for better excitation and collection efficiencies. We are then able to investigate very low excitation power regimes, where the photons are elastically scattered by the fundamental transition of the quantum dot (Resonant Rayleigh Scattering). In this regime, the coherence of the excitation laser is imprinted on the emitted photons, making the quantum dot a source of single photons with a very long coherence.The indistinguishability is investigated by using a Hong–Ou–Mandel interferometer to perform two-photon interference. We carry out a comprehensive experimental study of the excitation power dependence of the indistinguishability as well as its dependence on the excitation laser coherence, which shows the important role of elastic scattering in the low excitation power limit. It appears that a new figure of merit needs to be introduced to assess the indistinguishability as a temporal phenomenon, an aspect which is particularly relevant when dealing with continuous-wave excitation.
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