Die Ausbreitungspfade und die strukturelle Veränderung von quasi geostrophischen Rossby-Wellenpaketen werden mittels der WKB-Methode untersucht. Es wird angenommen, daß die Wellenpakete an einem in Ost-West-Richtung verlaufenden festen Rand reflektiert werden können. Die Dynamik der Rossby-Wellenpakete wird auf der ß-Ebene aber auch auf der sogenannten d-Oberfiäche - wo auch die zweite Ableitung des Coriolis-Parameters eine Rolle spielt - studiert. Es wird gezeigt, daß die Wellenpakete unter bestimmten Umständen große Entfernungen in zonaler Richtung entlang der Küste zurücklegen können und damit die Strömung weit stromab beeinflussen. Die Wellenpakete sind dabei zwischen dem reflektierenden Rand und einer Umkehrbreite gefangen im Unterschied zu freien Rossbywellen in der Atmosphäre, die zwischen zwei Umkehrbreiten gefangen werden können. Es zeigt sich, daß der d-Term keine besonders wichtige Rolle für die Ausbreitung der Rossby-Wellenpakete spielt, am wichtigsten ist er noch bei der Dynamik von Wellen mit negativer Phasengeschwindigkeit. Es wird vorgeschlagen, daß ein selektiver Rossby-Wellenleiter wie er hier diskutiert wird eine Rolle in der Dynamik des Antarktik-Zirkumpolarstromes spielt. / We study the propagation and the structural change of quasi geostrophic Rossby wave packets by means of a WKB-method. Our approach involves the introduction of a rigid boundary, where the wave packets can be refiected elastically. We study Rossby wave packet dynamics at high latitudes on a modified ß-plane, where the second derivative of the Coriolis parameter with respect to latitude is taken into account (d-term). We show that under certain conditions synoptic-scale wave packets can propagate far distances along an east-west oriented \'coast\' and may affect the fiow far downstream of the source region. In contrast to free propagating Rossby wave packets ( e.g. in the atmosphere), which can be trapped between two turning latitudes, the wave packets considered here are trapped between a turning latitude and the reflecting boundary. lt turns out that the 6-term is most important for wave packets with negative phase speeds. Finally, we suggest that such a selective Rossby waveguide may play a role in the dynamics of the Antarctic Circumpolar Current.

We study the unique phenomena which occur in certain systems characterized by the crossing or avoided crossing of two electronic eigenvalues. First, an example problem will be investigated for a given Hamiltonian resulting in a codimension 1 crossing by implementing results by Hagedorn from 1994. Then we perturb the Hamiltonian to study the system for the corresponding avoided crossing by implementing results by Hagedorn and Joye from 1998. The results from these demonstrate the behavior which occurs at a codimension 1 crossing and avoided crossing and illustrates the differences. These solutions may also be used in further studies with Herman-Kluk propagation and more. Secondly, we study codimension 2 crossings by considering a more general type of wave packet. We focus on the case of Schrödinger equation but our methods are general enough to be adapted to other systems with the geometric conditions therein. The motivation comes from the construction of surface hopping algorithms giving an approximation of the solution of a system of Schrödinger equations coupled by a potential admitting a conical intersection, in the spirit of Herman-Kluk approximation (in close relation with frozen/thawed approximations). Our main Theorem gives explicit transition formulas for the profiles when passing through a conical crossing point, including precise computation of the transformation of the phase and its proof is based on a normal form approach. / Doctor of Philosophy / We study energies of molecular systems in which special circumstances occur. In particular, when these energies intersect, or come close to intersecting. These phenomena give rise to unique physics which allows special reactions to occur and are thus of interest to study. We study one example of a more specific type of energy level crossing and avoided crossing, and then consider another type of crossing in a more general setting. We find solutions for these systems to draw our results from.

Orientador: Stefano de Leo / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Matematica, Estatistica e Computação Científica / Made available in DSpace on 2018-08-15T11:34:18Z (GMT). No. of bitstreams: 1 Silva_KeniaCristinaPereira_M.pdf: 5917573 bytes, checksum: 689b0e6d7c10b6ea1e4524486138cc7e (MD5) Previous issue date: 2010 / Resumo: O objetivo principal deste trabalho é estudar a equação de Schrödinger para um potencial quaterniônico tipo barreira. A solução analítica encontrada permite comparar qualitativamente as diferenças entre a mecânica quântica complexa e a mecânica quântica quaterniônica. Antes de apresentar a solução analítica da barreira, para um melhor entendimento da motivação que leva ao estudo de uma mecânica quântica quaterniônica, será analisado em detalhes (ondas planas e pacotes de onda) o potencial tipo degrau / Abstract: The main objective of this research is to study the Schrödinger equation for a quaternionic potential barrier. The analytical solution found allow us to compare qualitatively the differences between the complex quantum mechanics and the quaternionic quantum mechanics. Before presenting the barrier analytical solution, to a better understanding of the motivation that leads us to the study of quaternionic quantum mechanics, the potencial step will be discussed in detail (plane waves and wave packets) / Mestrado / Fisica-Matematica / Mestre em Matemática Aplicada

Orientadores: Stefano De Leo, Marcelo Moraes Guzzo / Dissertação (mestrado) - Universidade Estadual de Campinas, Instituto de Física Gleb Wataghin / Made available in DSpace on 2018-08-23T16:45:38Z (GMT). No. of bitstreams: 1 Maia_GabrielGulak_M.pdf: 1857100 bytes, checksum: 8af9898714b92a166704c01eafe1b9fa (MD5) Previous issue date: 2013 / Resumo: A interação de elétrons com barreiras de potencial é um problema bem conhecido da teoria quântica não-relativística de Schrödinger. O tratamento intrinsecamente relativístico do sistema, entretanto, por meio da teoria de Dirac, nos revela diferentes aspectos não fornecidos pela teoria precedente. Por exemplo, uma vez que a equação de Dirac contém naturalmente os graus de liberdade de spin, quatro coeficientes são necessários para descrever o processo e assim o fenômeno da inversão de spin, também chamado spin flip, surge. Com o objetivo de introduzir o formalismo teórico e a notação sobre a qual se sustenta este trabalho, o primeiro capítulo é dedicado a uma breve revisão da equação de Dirac, discutindo-se as propriedades de suas matrizes, a equação de continuidade e obtendo-se suas soluções livres. No capítulo 2 o sistema de interesse, a interação planar de partículas de Dirac com barreiras de potencial eletrostático, é apresentado e são destacados os aspectos que o diferenciam de seu equivalente não-relativístico. São definidos os potenciais escalar e eletrostático e as zonas cinemáticas estabelecidas para os casos unidimensional e bidimensional. O terceiro capítulo é reservado à obtenção dos coeficientes de reflexão e transmissão com e sem spin flip para partículas de Dirac difundindo planarmente através de uma barreira quadrada de potencial eletrostático. Este objetivo é alcançado através de dois métodos distintos de interpretações complementares: O método de degraus e o cálculo de barreira. Coeficientes não-nulos são obtidos para todos os casos, exceto para a transmissão através da barreira com inversão de spin, contrastando com o fato de que todos os degraus componentes da barreira apresentam coeficientes associados diferentes de zero. No quarto capítulo analisa-se o spin das partículas incidentes e o efeito da barreira sobre o spin das partículas refletidas. Ainda que o limite para baixas velocidades seja sempre 1/2, como esperado, em regimes relativísticos encontra-se uma dependência do valor médio deste operador com a energia e o ângulo de incidência no potencial. No quinto capítulo o formalismo de pacote de ondas é desenvolvido e a coerência dos pacotes em relação 'a barreira de potencial investigada, mostrando que a probabilidade de transmissão torna-se constante conforme a largura da barreira aumenta, o que caracteriza o regime incoerente de partículas. Ao fim do capítulo são derivadas as expressões para o spin incidente, refletido e transmitido nesse formalismo. Por fim, o sexto capítulo é reservado ao estudo introdutório do valor médio de autoestados do operador de spin através do formalismo desenvolvido no capítulo anterior como primeira mostra das possibilidades de trabalhos futuros. Mostrado que se o bispinor incidente não for um autoestado do Hamiltoniano de Dirac uma dependência temporal é verificada no valor médio / Abstract: The interaction of electrons with potential barriers is a well-known problem of the Schr¨odinger¿s non-relativistic quantum theory. The intrinsically relativistic treatment of the problem, however, through the Dirac¿s theory, reveals us different aspects, do not provided by the preceding theory. For instance, since the Dirac equation naturally contains the spinorial degree of freedom, four coefficients are needed in order to describe the process and so the spin flip phenomenon emerges. To introduce the theoretical formalism and the notation upon which this work is sustained, the first chapter is devoted to a short review of the Dirac equation, discussing the properties of its matrices, the continuity equation and obtaining its free solutions. Chapter 2 presents the system of interest, the planar interaction of Dirac particles with electrostatic potential barriers. It also highlights the aspects that differentiate this system from its non-relativistic analogue. The scalar and electrostatic potentials are defined and the kinematic zones established for the one-dimensional and the two-dimensional cases. The third chapter is reserved for obtaining the spin flip and spin conserving transmission and reflection coefficients for Dirac particles diffusing two-dimensionally through a square electrostatic potential barrier. This goal is achieved by means of two distinct methods of complementary interpretations: The barrier calculation and the steps calculation. Non-zero coefficients are obtained in all the cases except for the spin flip transmission, contrasting with the fact that no coefficient of the individual steps that compose the barrier is null. In the fourth chapter the incident particles¿ spin is analysed as well as the effect of the barrier on the spin of the reflected particles. As expected the low velocities limits gives us a spin value of 1/2 but in relativistic regime there is a dependence of the spin with the energy and the incidence angle into the potential. In the fifth chapter the wave packet formalism is developed and the packets¿ coherence is investigated, showing that the transmission probability becomes constant as the barrier width becomes greater, characterizing the incoherence of the particle limit. At the end of the chapter the expressions for the incident, reflected and transmitted spin in the new formalism are derived. Finally, the sixth chapter is reserved to the introductory study of mean values of the spin operator eigenstates through the formalism developed in the previous chapter as an example of possibilities for future investigations. It is shown that if the incident bispinor is not a Dirac Hamiltonian eigenstate there is a time dependence in the expected value. Key-words: Relativistic Quantum Mechanics, potential barriers, wave-packets / Mestrado / Física / Mestre em Física

Les résultats présentés dans cette thèse concernent l'étude, dans la limite semi-classique, de systèmes d'équations de Schrödinger non-linéaires couplées. Selon le potentiel considéré, le système peut, ou non, présenterun couplage linéaire, en plus de celui induit par le terme non-linéaire. Dans ce manuscrit, c'est la propagation d'états cohérents -états localisés dans l'espace des phases, et que l'on va faire vivre dans un niveau d'énergie donné - qui va nous intéresser.Dans le cadre linéaire, plusieurs situations ont été étudiées, certaines préservant l'adiabaticité,et d'autres la brisant, faisant apparaître des transitions entre les niveaux d'énergie.Le rôle de la non-linéarité et l'interaction de ses effets avec un éventuel couplage linéaire sur ces phénomènes est une questionimportante pour comprendre des systèmes qui entrent en jeu dans des problèmes très actuels en physique quantique.Dans un premier temps, le potentiel pris en compte aura des valeurs propres bien séparées par un trou spectral,et nous montrerons un théorème adiabatique pour une non-linéarité qui présente un exposant critique pour le paramètre semi-classique devant la non-linéarité. Un point de vue équivalent est de considérer des données petites de l'ordre d'une puissance positive du paramètre semi-classique.Il s'agit d'un résultat analogue à celui de Carles et Fermanian-Kammerer mais dans un cadre sur-critique L^2.Dans un deuxième temps, nous considèrerons, pour le cas unidimensionnel, un potentiel explicite de taille 2 X 2,qui présente un croisement évité :les deux valeurs propres sont séparées par un paramètre delta - paramètre adiabatique -qui va tendre vers zéro lorsque le paramètre semi-classique va tendre vers zéro. Nous montrerons alors que des transitions entre les modes ont lieu.Il s'agit ici d'une version non-linéaire des travaux d'Hagedorn et Joyeoù une telle transition est démontrée pour des systèmes linéaires. / This thesis is devoted to the study of coupled nonlinear Schrödinger equations in the semi-classical limit.Depending on the potential we consider, the system can present a linear coupling, in addition to the nonlinear one.We will focus on the propagation of coherent states that will be polarized along a given eigenvector of the potential.In the linear setting, several situations have been analyzed; some of them lead to adiabatic theorems whereas the others implytransitions between energy levels. When one adds a nonlinearity, understanding nonlinear effects onthe propagation and the competition between them and the linear coupling becomes a very interesting issue.We first consider a potential with eigenvalues that present a spectral gap and will prove an adiabatic theoremfor a critical nonlinearity in the semi-classical sense. This is a L^2-supercritical result,similar to the one proved by Carles and Fermanian-Kammerer for the one-dimensional case, which is L^2-subcritical.The second part of the thesis deals with an explicit 2 X 2 potential that presents an avoided crossing point :the minimal gap between its eigenvalues becomes smaller as the semiclassical parameter tends to zero. We will prove that this system exhibits transitions between the modes. This result is a nonlinear version of the study performed by Hagedorn and Joye in the linear case.

Large amplitude internal solitary waves in the coastal ocean are commonly modelled with the Korteweg-de Vries (KdV) equation or a closely related evolution equation. The characteristic feature of these models is the solitary wave solution, and it is well documented that these provide the basic paradigm for the interpretation of oceanic observations. However, often internal waves in the ocean survive for several inertial periods, and in that case, the KdV equation is supplemented with a linear non-local term representing the effects of background rotation, commonly called the Ostrovsky equation. This equation does not support solitary wave solutions, and instead a solitary-like initial condition collapses due to radiation of inertia-gravity waves, with instead the long-time outcome typically being an unsteady nonlinear wave packet. The KdV equation and the Ostrovsky equation are formulated on the assumption that only a single vertical mode is used. In this thesis we consider the situation when two vertical modes are used, due to a near-resonance between their respective linear long wave phase speeds. This phenomenon can be described by a pair of coupled Ostrovsky equations, which is derived asymptotically from the full set of Euler equations and solved numerically using a pseudo-spectral method. The derivation of a system of coupled Ostrovsky equations is an important extension of coupled KdV equations on the one hand, and a single Ostrovsky equation on the other hand. The analytic structure and dynamical behaviour of the system have been elucidated in two main cases. The first case is when there is no background shear flow, while the second case is when the background state contains current shear, and both cases lead to new solution types with rich dynamical behaviour. We demonstrate that solitary-like initial conditions typically collapse into two unsteady nonlinear wave packets, propagating with distinct speeds corresponding to the extremum value in the group velocities. However, a background shear flow allows for several types of dynamical behaviour, supporting both unsteady and steady nonlinear wave packets, propagating with the speeds which can be predicted from the linear dispersion relation. In addition, in some cases secondary wave packets are formed associated with certain resonances which also can be identified from the linear dispersion relation. Finally, as a by-product of this study it was shown that a background shear flow can lead to the anomalous version of the single Ostrovsky equation, which supports a steady wave packet.

There exists substantial applications motivating the study of nonlinear longitudinal wave propagation in layered (or laminated) elastic waveguides, in particular within areas related to non-destructive testing, where there is a demand to understand, reinforce, and improve deformation properties of such structures. It has been shown [76] that long longitudinal waves in such structures can be accurately modelled by coupled regularised Boussinesq (cRB) equations, provided the bonding between layers is sufficiently soft. The work in this thesis firstly examines the initial-value problem (IVP) for the system of cRB equations in [76] on the infinite line, for localised or sufficiently rapidly decaying initial conditions. Using asymptotic multiple-scales expansions, a nonsecular weakly nonlinear solution of the IVP is constructed, up to the accuracy of the problem formulation. The asymptotic theory is supported with numerical simulations of the cRB equations. The weakly nonlinear solution for the equivalent IVP for a single regularised Boussinesq equation is then constructed; constituting an extension of the classical d'Alembert's formula for the leading order wave equation. The initial conditions are also extended to allow one to separately specify an O(1) and O(ε) part. Large classes of solutions are derived and several particular examples are explicitly analysed with numerical simulations. The weakly nonlinear solution is then improved by considering the IVP for a single regularised Boussinesq-type equation, in order to further develop the higher order terms in the solution. More specifically, it enables one to now correctly specify the higher order term's time dependence. Numerical simulations of the IVP are compared with several examples to justify the improvement of the solution. Finally an asymptotic procedure is developed to describe the class of radiating solitary wave solutions which exist as solutions to cRB equations under particular regimes of the parameters. The validity of the analytical solution is examined with numerical simulations of the cRB equations. Numerical simulations throughout this work are derived and implemented via developments of several finite difference schemes and pseudo-spectral methods, explained in detail in the appendices.

Dans le but de réduire le bruit de jet, source principale de nuisance sonore au décollage d'un avion, une compréhension fine des mécanismes aéroacoustiques mis en jeu est nécessaire. Les structures cohérentes de grande échelle se développant dans la couche de mélange d'un jet semblent responsables d'une part importante du bruit observé en champ lointain, surtout dans les basses fréquences. Une approche permettant d'étudier ces structures turbulentes est fournie par la théorie de stabilité, notamment au moyen des équations de stabilité parabolisées (PSE). L'étude de ces ondes d'instabilité est alors complémentaire d'autres approches (LES ou expériences), puisqu'elle permet de mettre en évidence la nature et la dynamique de ces structures, également présentes dans les résultats de simulations ou de mesures.Au cours de ces travaux de thèse, nous nous sommes intéressés aux structures cohérentes se développant dans des jets à double flux étudiés au cours du projet européen CoJeN (Coaxial Jet Noise). En particulier, nous avons exploité une base de données issues de mesures de fluctuations de pression réalisées en champ proche et en champ lointain de ces jets. Nous avons alors pu comparer les résultats de notre modélisation PSE à ces mesures en périphérie immédiate du jet, confirmant ainsi la pertinence d’un tel modèle, même dans des configurations aussi complexes. De plus, le calcul du rayonnement acoustique en champ lointain engendré par les fluctuations de pression modélisées nous a permis de faire des comparaisons directes avec les niveaux et les directivités mesurés. Nous avons ainsi pu mettre en évidence quantitativement la contribution de ces structures turbulentes de grande échelle au bruit total rayonné par le jet. / Increasingly stringent aircraft noise regulations require the development of innovative noise reduction strategies. Jet noise is a dominant acoustic component during take-off and a fine understanding of the underlying aeroacoustics mechanisms is then necessary. Large-scale coherent structures that develop in the mixing layer of jets appear to be the dominant acoustic source responsible for the lowfrequency far-field noise observed at low emission angles. A stability analysis based on the parabolized stability equations (PSE) is a suitable tool for studying these coherent structures, revealing the nature and the dynamics of the fluctuations obtained by simulations or experiments. The present work is focused on coherent structures developing in the two mixing layers of dualstream jets studied in the course of the European project CoJeN (Coaxial Jet Noise). In particular, pressure fluctuations measurements acquired in the near and far fields of two coaxial jets have been thoroughly analyzed. A direct comparison of these experimental results with linear PSE calculations has been performed in the vicinity of the jets, referred to as the linear-hydrodynamic region, confirming the relevance of the approach even in such complex industrial configurations. Furthermore, the acoustic projection to the far-field of the wavepackets issued by this model and calibrated in the near-field allows a direct comparison of the acoustic levels and directivity with far field sound measurements. A quantitative assessment of the contribution of the instability waves to the total jet noise measured has therefore been obtained.

Die vorliegende Arbeit beschäftigt sich mit dem Konzept der radial nicht-oszillierenden, zeitlich stabilen ultrakurzen Bessel ähnlichen Strahlen oder "Nadelstrahlen" ("needle beams"), die zu einer Klasse von optischen hochlokalisierten Wellenpaketen generalisiert werden. Hierbei wird die Theorie über das räumlich-zeitlichen Ausbreitungsverhaltens von nicht auseinanderdriftenden Nadelstrahlen mit Pulsdauern von kleiner als 10 fs näher diskutiert. Dies wird durch eine systematische Darstellung der Methoden zur Generierung und Detektierung von lokalisierten Wellen komplettiert, die ein optischen Drehmoment tragen. Für die Erzeugung von HLWs kommen räumliche Lichtmodulatoren zum Einsatz, die ein flexibles Zuschneiden von Wellenpaketen mit der Dauer weniger Zyklen des EM-Feldes erlauben. Es wird gezeigt, dass solche optischen Pulse sich über beträchtliche Entfernungen ausbreiten, ohne dass sich dabei signifikant der Strahldurchmesser vergrößert oder der Puls zeitlich verbreitert. In variabler Weise werden verschiedene geometrische (z.B. ringförmige) Lichtverteilungen erzeugt. Anwendungspotential findet sich insbesondere in den Techniken der räumlichen Pulsformung und Diagnostik. Als besonders wichtiger Ansatz ist der Zeit-Wellenfront-Sensor zu erwähnen, welcher die nichtlineare, mehrkanalige Autokorrelation, die Wellenfrontdetektion mittels nichtdiffraktiver Teilstrahlen nach dem Shack-Hartmann-Prinzip und eine adaptive Funktionalität miteinander vorteilhaft verbindet. Das enorme Potential solcher Ansätze wird durch die hohe Genauigkeit orts-, winkel- und zeitabhängiger Rekonstruktionen der Wellenpakete nachgewiesen. Darüber hinaus ermöglicht das räumliche Kodieren und anschließende Verfolgen der Teilstrahlen eine wesentliche Verbesserung der Identifikation relevanter Parameter von Verteilungsfunktionen. Schließlich werden erste Schritte zur experimentellen Generation von optischen "light bullets" mit ganzzahligen und fraktalen orbitalen Drehmomenten präsentiert. / This thesis deals with the concept of radially non-oscillating, temporally stable ultrashort-pulsed Bessel-like beams or "needle pulses", which are an example of a highly localized wave packet (HLW). HLWs are the closest approximation of linear-optical light bullets and provide specific benefits compared to conventional Gaussian-like light bullets. The spatio-temporally nonspreading propagation behavior of few-cycle needle beams of less than 10 fs duration will be theoretically discussed in detail. An overview of the generation and detection of localized waves carrying an orbital angular momentum is also given. High fidelity spatial light modulators are used for the generation of HLWs. The flexible tailoring of few-cycle wave packets at near-infrared wavelengths is reported. It is shown that such pulses propagate over a huge depth of focus, neither significantly changing their spot size or nor the pulse duration. Variable geometrical distributions like circular disks, rings, or bars of light are shaped and exploited as building blocks for structures of higher complexity. Another section of the thesis emphasizes the numerous potential applications of related techniques for an optimized two-dimensional spatial pulse shaping and diagnostics (reduce ambiguities) based on localized waves. As a particularly important example, time-wavefront sensing is used to combine nonlinear multichannel autocorrelation with Shack-Hartmann wavefront sensing by means of localized sub-beams and adaptive functionality. The capabilities of such devices are illustrated by the results of angular and temporal mapping of few-cycle wave packets. Moreover, spatial encoding and subsequent tracking of individual sub-beams, even at incident angles of up to 50°, enables to significantly improve the spot recognition. Finally, first steps towards the generation of optical light bullets carrying integer or non-integer orbital angular momenta are presented.