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Quantenmechanik im Kalten Krieg : David Bohm und Richard Feynman.Forstner, Christian. January 2007 (has links)
Zugl.: Regensburg, Univ., Diss., 2007.
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Quantenmechanik im Kalten Krieg : David Bohm und Richard FeynmanForstner, Christian January 2007 (has links)
Zugl.: Regensburg, Univ., Diss., 2007
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Path Integrals and Quantum Mechanics / Banintegraler och KvantmekanikSandström, Martin January 2015 (has links)
In this thesis we are investigating a different formalism of non-relativistic quantum mechanics called the path integral formalism. It is a generalization of the classical least action principle. The introduction to this subject begins with the construction of the path integral in terms of the idea of probability amplitudes whose absolute square gives the probability of finding a system in a particular state. Then we show that if the Lagrangian is a quadratic form one needs only to calculate the classical action besides from a time-dependent normalization constant to find the explicit expression of the path integral. We look in to the subject of two kinds of slit-experiments: The square slit, the single- and the double-Gaussian slit. Also, the propagator for constrained paths is calculated and applied to the Aharonov-Bohm effect, which shows that the vector potential defined in classical electrodynamics have a physical meaning in quantum mechanics. It is also shown that the path integral formulation is equivalent to the Schrödinger description of quantum mechanics, by deriving the Schrödinger equation from the path integral. Further applications of the path integral are discussed. / I detta fördjupningsarbete undersöker vi en annan formalism av icke-relativistisk kvantmekanik kallad banintegral formalismen. Det är en generalisering av den klassiska verkansprincipen. Introduktionen till detta ämne börjar med konstruktionen av banintegralen i termer av sannolikhetsamplituder vars absolutbelopp i kvadrat ger sannolikheten av att finna ett system i ett särskilt tillstånd. Sedan visar vi att om Lagrangianen är av kvadratisk form så krävs endast en beräkning av den klassiska verkan förutom en tidsberoende normaliseringskonstant för att finna ett uttryck för banintegralen. Vi ser på två olika typer av spaltproblem: Den kantinga spalten, enkel- och dubbel Gaussisk spalt. Vi beräknar dessutom propagatorn för banor med restriktioner och applicerar detta på Aharonov-Bohm effekten, som visar att den klassiska vektorpotentialen som definierad i klassisk elektrodynamik har en fysikalisk mening i kvantmekaniken. Vi visar också ekvivalensen av banintegralformalismen med Schrödingerekvationen genom att härleda Schrödingerekvationen från banintegralen. Andra applikationer av banintegralen diskuteras.
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Algebraic structures in the light of the implicate orderMonk, Nicholas Alexander M. January 1994 (has links)
No description available.
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Non-dynamical quantum trajectoriesCoffey, Timothy Michael, 1970- 11 February 2011 (has links)
Commonly held opinion is that particle trajectory descriptions are incompatible with quantum mechanics. Louis de Broglie (1926) first proposed a way to include trajectories in quantum mechanics, but the idea was abandoned until David Bohm (1952) re-invented and improved the theory. Bohm interprets the particle trajectories as physically real; for example, an electron actually is a particle moving on a well defined trajectory with a position and momentum at all times. By design, Bohm's trajectories never make predictions that differ from standard quantum mechanics, and their existence cannot be experimentally verified.
Three new methods to obtain Bohm's particle trajectories are presented. The methods are non-dynamical, and utilize none of Bohm's equations of motion; in fact, two of the methods have no equations for a particle's trajectory. Instead, all three methods use only the evolving probability density ρ=ψ*ψ to extract the trajectories. The first two methods rest upon probability conservation and density sampling, while the third method employs the informational or geometrical construction of centroidal Voronoi tessellations. In one-dimension all three methods are proved to be equivalent to Bohm's particle trajectories. For higher dimensional configuration spaces, the first two methods can be used in limited situations, but the last method can be applied in all cases. Typically, the resulting higher dimensional non-dynamical trajectories are also identical to Bohm.
Together the three methods point to a new interpretation of Bohm's particle trajectories, namely, the Bohm trajectories are simply a kinematic portrayal of the evolution of the probability density. In addition, the new methods can be used to measure Schrödinger's wave function and Planck's constant. / text
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Electron states in low dimensional structuresTan, Weichao January 1995 (has links)
No description available.
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Contribution à l'analyse de la dynamique quantique dans des systèmes de Hall en présence d'un flux Aharonov-Bohm dépendant du temps / Contributions to the analysis of the quantum dynamics of Hall systems with time dependant Aharonov-Bohm fluxMeresse, Cédric 25 November 2010 (has links)
Nous nous intéressons à la dynamique dans les systèmes de Hall en présence d'un flux Aharonov-Bohm dépendant du temps. Nous présenterons deux théorèmes adiabatiques applicable à ces modèles ainsi qu'un résultat sur l'existence d'une constante de mouvement non-trivial. On utilisera un algorithme de diagonalisation partielle. / We will ahve interest in the quantum dynamics in Hall systems with time dependent Aharonov-Bohm flux. We will present two adiabatic theorems which can applied to these models and a quantitive result on the existence of a non-trivial constant of motion. To prove this result, we will use a partial diagonalization algorithm
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The Aharonov-Bohm effect and resonant scattering in graphene / Aharonov-Bohm-Effekt und resonante Streuung in GraphenSchelter, Jörg January 2012 (has links) (PDF)
In this thesis, the electronic transport properties of mesoscopic condensed matter systems based on graphene are investigated by means of numerical as well as analytical methods. In particular, it is analyzed how the concepts of quantum interference and disorder, which are essential to mesoscopic devices in general, are affected by the unique electronic and transport properties of the graphene material system. We consider the famous Aharonov–Bohm effect in ring-shaped transport geometries, and, besides providing an overview over the recent developments on the subject, we study the signatures of fundamental phenomena such as Klein tunneling and specular Andreev reflection, which are specific to graphene, in the magnetoconductance oscillations. To this end, we introduce and utilize a variant of the well-known recursive Green’s function technique, which is an efficient numerical method for the calculation of transport observables in effectively non-interacting open quantum systems in the framework of a tight binding model. This technique is also applied to study the effects of a specific kind of disorder, namely short-range resonant scatterers, such as strongly bound adatoms or molecules, that can be modeled as vacancies in the graphene lattice. This numerical analysis of the conductance in the presence of resonant scatterers in graphene leads to a non-trivial classification of impurity sites in the graphene lattice and is further substantiated by an independent analytical treatment in the framework of the Dirac equation. The present thesis further contains a formal introduction to the topic of non-equilibrium quantum transport as appropriate for the development of the numerical technique mentioned above, a general introduction to the physics of graphene with a focus on the particular phenomena investigated in this work, and a conclusion where the obtained results are summarized and open questions as well as potential future developments are highlighted. / In dieser Arbeit werden die elektronischen Transporteigenschaften von Graphen-basierten mesoskopischen Festkörpersystemen mittels numerischer und analytischer Methoden untersucht. Im Besonderen wird analysiert, wie Konzepte von Quanteninterferenz und Unordnung, die eine wesentliche Rolle für mesoskopische Systeme spielen, durch die einzigartigen elektronischen und Transporteigenschaften von Graphen beeinflusst werden. Wir betrachten den berühmten Aharonov-Bohm-Effekt in ringförmigen Transportgeometrien, geben einen Überblick über die Entwicklung dieses Themas in den letzten Jahren und befassen uns mit den charakteristischen Merkmalen, die fundamentale Phänomene wie Klein-Tunneln und gerichtete Andreev-Reflexion, welche spezifisch für Graphen sind, in den Magnetooszillationen der elektrischen Leitfähigkeit aufweisen. Dazu führen wir eine Variante der Methode der rekursiven Greenschen Funktionen ein, die ein effizientes numerisches Verfahren zur Berechnung von Transportobservablen in effektiv nicht-wechselwirkenden, offenen Quantensystemen im Rahmen eines „tight binding“-Modells darstellt. Diese Methode wird desweiteren zur Erforschung eines speziellen Typs von Unordnung herangezogen, nämlich kurzreichweitiger, resonanter Streuzentren wie stark gebundene Adatome oder Moleküle, die als Fehlstellen in der Graphen-Gitterstruktur modelliert werden können. Diese numerische Analyse der elektrischen Leitfähigkeit bei Anwesenheit resonanter Streuzentren in Graphen führt zu einer nicht-trivialen Klassifizierung von Fremdatom-Gitterplätzen innerhalb des Graphen-Gitters und wird durch eine unabhängige analytische Behandlung im Rahmen der Dirac-Gleichung bekräftigt. Die vorliegende Arbeit enthält weiterhin eine formale Einführung in das Thema des Nichtgleichgewichts-Quantentransports, wie es für die Entwicklung der genannten numerischen Methode dienlich ist, eine allgemeine Einführung in die Physik von Graphen mit Fokus auf die speziellen Aspekte, die in dieser Arbeit untersucht werden, sowie eine abschließende Darstellung, in der die erhaltenen Ergebnisse zusammengefasst und offene Fragen sowie mögliche zukünftige Entwicklungen hervorgehoben werden.
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An analysis of spin correlations in <sup>12</sup>C(d,<sup>2</sup>He)<sup>12</sup>B to test the Bell and Wigner inequalities : a tale of two protonsPolachic, Christopher John Arthur 05 February 2003
Arising out of the EPR debate, the Bell and Wigner inequalities of quantum theory are experimentally testable relations which address the question of quantum completeness. This thesis provides feasibility results for a fermionic test of the Bell inequality, and the first known attempt to investigate the completeness question through the Wigner relation. Such a test is made possible by the production of an entangled p-p singlet at the KVI research facility in Groningen, the Netherlands, through the reactions 12C(d,2He)12B and p(d,2He)n. The p-p spin-correlations are analyzable via the KVI's 2-pi polarimeter acceptance, which eliminates loopholes common to previous experiments. The results distinguish between a hidden variables and quantum mechanical description of the universe. Also presented is a critique of the GHZ argument against the existence of local hidden variables.
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An analysis of spin correlations in <sup>12</sup>C(d,<sup>2</sup>He)<sup>12</sup>B to test the Bell and Wigner inequalities : a tale of two protonsPolachic, Christopher John Arthur 05 February 2003 (has links)
Arising out of the EPR debate, the Bell and Wigner inequalities of quantum theory are experimentally testable relations which address the question of quantum completeness. This thesis provides feasibility results for a fermionic test of the Bell inequality, and the first known attempt to investigate the completeness question through the Wigner relation. Such a test is made possible by the production of an entangled p-p singlet at the KVI research facility in Groningen, the Netherlands, through the reactions 12C(d,2He)12B and p(d,2He)n. The p-p spin-correlations are analyzable via the KVI's 2-pi polarimeter acceptance, which eliminates loopholes common to previous experiments. The results distinguish between a hidden variables and quantum mechanical description of the universe. Also presented is a critique of the GHZ argument against the existence of local hidden variables.
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