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Mecânica quântica não-aditiva

João Philipe Macedo Braga

Published Jan 1, 2015• 0 citations
OpenAlex

Abstract

In this thesis, we study the nonadditive quantum mechanics (NAQM), which is a theory developed from first principles in order to understand the effects of the space metric in the quantum theory. In non-Euclidean spaces, the translation of length ∆x does not necessarily take a particle from the position x to x + ∆x. The result of this translation depends on the metric. This is the starting point for the development of the NAQM. Through a redefinition of the translation operator, we obtain new commutation relations between the position operator and the momentum operator, and a Schrödinger-like equation which describes the time evolution of the state of a particle. We show that this equation, with appropriate boundary conditions, can be seen as a Sturm-Liouville problem, ensuring that the energies of the particle are real and that the eigenstates of the hamiltonian are orthonormal and form a basis in the space of the states. In spite of these modifications, we show the determinism in the time evolution, the superposition principle and the local and global probability conservation remain valid. On the other hand, we generalize the Ehrenfest theorem, showing that, for the average values of the physical quantities, the NAQM is identical to the classical mechanics in a non-inertial reference frame, and we demonstrate the existence of a nonzero minimum uncertainty for the momentum. Besides, we investigate, classically as well as quantically, the dynamical effects of the metric in the time evolution of a free particle. In order to perform the quantum simulation, we adapt the split operator technique to solve numerically the new Schrödinger equation. Lastly, we explore the possibility of mapping of several physical problems of different nature through the arising of an effective potential which appears due to a simple change of coordinates.

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In this thesis, we study the nonadditive quantum mechanics (NAQM), which is a theory developed from first principles in order to understand the effects of the space metric in the quantum theory. In non-Euclidean spaces, the translation of length ∆x does not necessarily take a particle from the position x to x + ∆x. The result of this translation depends on the metric. This is the starting point for the development of the NAQM. Through a redefinition of the translation operator, we obtain new commutation relations between the position operator and the momentum operator, and a Schrödinger-like equation which describes the time evolution of the state of a particle. We show that this equation, with appropriate boundary conditions, can be seen as a Sturm-Liouville problem, ensuring that the energies of the particle are real and that the eigenstates of the hamiltonian are orthonormal and form a basis in the space of the states. In spite of these modifications, we show the determinism in the time evolution, the superposition principle and the local and global probability conservation remain valid. On the other hand, we generalize the Ehrenfest theorem, showing that, for the average values of the physical quantities, the NAQM is identical to the classical mechanics in a non-inertial reference frame, and we demonstrate the existence of a nonzero minimum uncertainty for the momentum. Besides, we investigate, classically as well as quantically, the dynamical effects of the metric in the time evolution of a free particle. In order to perform the quantum simulation, we adapt the split operator technique to solve numerically the new Schrödinger equation. Lastly, we explore the possibility of mapping of several physical problems of different nature through the arising of an effective potential which appears due to a simple change of coordinates.
In this work we analyze some aspects related to the introduction, in the non-relativistic quantum mechanics,of a translation operator whose action is a function of the point of application. From the introduction of this operator, we derive a modified canonical commutation relation and a modified representation for the momentum operator and we show that such changes require a restructuring of the Hilbert space. We also see that the “new” Hilbert space can be associated with the case of a particle with position dependent mass and also that of a particle moving in a curved space. Still, we compare our formalism with the formalism of von Roos, we analyze the classical limit of this formalism,we solve the problem of a particle with position-dependent mass in two dimensions and we end up analyzing some quantities of information theory for the case of a one-dimensional harmonic particle.
Following previous works by E. Prugovečki [Physica A 91A, 202 (1978) and Stochastic Quantum Mechanics and Quantum Space–time (Reidel, Dordrecht, 1986)] on common features of classical and quantum mechanics, we develop a unified mathematical framework for classical and quantum mechanics (based on L2-spaces over classical phase space), in order to investigate to what extent quantum mechanics can be obtained as a simple modification of classical mechanics (on both logical and analytical levels). To obtain this unified framework, we split quantum theory in two parts: (i) general quantum axiomatics (a system is described by a state in a Hilbert space, observables are self-adjoints operators, and so on) and (ii) quantum mechanics proper that specifies the Hilbert space as L2(Rn); the Heisenberg rule [pi,qj]=−iℏδij with p=−iℏ∇, the free Hamiltonian H=−ℏ2Δ/2m and so on. We show that general quantum axiomatics (up to a supplementary “axiom of classicity”) can be used as a nonstandard mathematical ground to formulate physical ideas and equations of ordinary classical statistical mechanics. So, the question of a “true quantization” with “ℏ” must be seen as an independent physical problem not directly related with quantum formalism. At this stage, we show that this nonstandard formulation of classical mechanics exhibits a new kind of operation that has no classical counterpart: this operation is related to the “quantization process,” and we show why quantization physically depends on group theory (the Galilei group). This analytical procedure of quantization replaces the “correspondence principle” (or canonical quantization) and allows us to map classical mechanics into quantum mechanics, giving all operators of quantum dynamics and the Schrödinger equation. The great advantage of this point of view is that quantization is based on concrete physical arguments and not derived from some “pure algebraic rule” (we exhibit also some limit of the correspondence principle). Moreover spins for particles are naturally generated, including an approximation of their interaction with magnetic fields. We also recover by this approach the semi-classical formalism developed by E. Prugovečki [Stochastic Quantum Mechanics and Quantum Space–time (Reidel, Dordrecht, 1986)].
Although gravity could not be quantized yet, there are good theoretical evidences that the unification of General Relativity and Quantum Mechanics should lead to the existence of a minimal observable length, a length scale below which the very notion of length looses meaning. Such effect proves to be worth some further analysis, for it acts as a natural regulator parameter, thus avoiding the divergences that plague Quantum Field Theories. In order to investigate some of the physical consequences of the existence of this peculiar effect, we propose to include it in the framework of Quantum Mechanics by modifying the Heisenberg algebra (i.e., the commutation relation of position and momentum operators, Xˆ and Pˆ), so that a minimum non-zero value for the uncertainty ?x emerges, which, being a limitation to the localizability of particles, acts as a minimal length. The Hilbert space of the theory must be modified accordingly. As we will see, the changes are not merely quantitative. On the contrary, our main result is that the familiar concept of “position measurement” must be reformulated, as well as other concepts related to it. We present a proposal for such reformulation.
This paper posits the existence of, and finds a candidate for, a variable change that allows quantum mechanics to be interpreted as quantum geometry. The Bohr model of the Hydrogen atom is thought of in terms of an indeterministic electron position and a deterministic metric and the motivation for this paper is to try to change variables to have a deterministic position and momentum for the electron and nucleus but with an indeterministic (quantum) metric that reproduces the physics of the Bohr model. This mapping is achieved by allowing the metric in the Hamiltonian to be different to the metric in the space-time distance element and then representing the two metrics with vierbeins and assuming they are canonically conjugate variables. Effectively, the usual Schrödinger space-time variables have been re-interpreted as four of the potentially sixteen parameters of the metric tensor vierbein in the distance element while the metric tensor vierbein in the Hamiltonian is an operator expressible as first-order derivatives in these variables or vice versa. I then argue that this reproduces observed quantum physics at the sub-atomic level by demonstrating the energy spectrum of electron orbitals is exactly the same as the usual relativistic Bohr model for the Hydrogen atom in a certain limit. Next, by introducing a single dimensionless running coupling that shows up in the analogous place as, but in addition to, Planck's constant in the commutator definition I argue that this allows massive objects to couple to the physical space-time geometry but not massless ones - no matter coupling value. This claim is based on a fit to the Schwarzschild metric with a few simple assumptions and thus obtaining an effective theory of how the quantum geometries at nearby space-time points couple to one another. This demonstrates that this coupling constant is related to Newton's gravitational constant.
This study discusses the quantum behavior of a particle, which is controlled by fluctuations in the physical space-time (ST) variables, rather than provides a novel interpretation of quantum theory. The fluctuations, i.e., inhomogeneities in a homogeneous phase ST, are prescribed by their probability. They determine the reciprocal space and correlate with the correlation entropy different from zero. Alongside with the minimum entropy, action, and the presence of the Winn-Ehrenfest adiabatic invariant (AI), the fluctuations require the Gilbert information (probabilistic) space linking the physical and the reciprocal ST. Physical quantities in the information space are represented by linear Hermitian operators, which is due to the entropy production in the presence of an AI. Evolution of a quantum system is described by the wave functions having the meaning of information concerning all virtually possible states of a quantum particle. The wave functions are the solutions to the Schrodinger equation and represent a navigation 'roadmap' for the particle to follow. A quantum system is in fact a classical Hamiltonian system in the space of coefficients of the wave function decomposition with respect to the operator eigenfunctions. It is the linearity and the Hermitian nature of the operators which determine the trajectory and the superposition principle in case of the wave behavior of fluctuations. The uncertainty principle, reflects correlation of the fluctuations and, hence, their nonlocality. This study discusses the wave function phase, the Berry phase and its relationship to quantization, discriminability of states and macroscopic quantum effects caused by localization of the particle, followed by a possible entropy change during its transition into a new thermodynamic state.