Deformation of Gabor systems

We introduce a new notion for the deformation of Gabor systems. Such deformations are in general nonlinear and, in particular, include the standard jitter error and linear deformations of phase space. With this new notion we prove a strong deformation result for Gabor frames and Gabor Riesz sequences that covers the known perturbation and deformation results. Our proof of the deformation theorem requires a new characterization of Gabor frames and Gabor Riesz sequences. It is in the style of Beurling's characterization of sets of sampling for bandlimited functions and extends significantly the known characterization of Gabor frames 'without inequalities' from lattices to non-uniform sets.

Minimum-uncertaity states and pseudoclassical dynamics. II

The set of initial conditions for which the pseudoclassical evolution algorithm (and minimality conservation) is verified for Hamiltonians of degrees N (N>2) is explicitly determined through a class of restrictions for the corresponding classical trajectories, and it is proved to be at most denumerable. Thus these algorithms are verified if and only if the system is quadratic except for a set of measure zero. The possibility of time-dependent a-equivalence classes is studied and its physical interpretation is presented. The implied equivalence of the pseudoclassical and Ehrenfest algorithms and their relationship with minimality conservation is discussed in detail. Also, the explicit derivation of the general unitary operator which linearly transforms minimum-uncertainty states leads to the derivation, among others, of operators with a general geometrical interpretation in phase space, such as rotations (parity, Fourier).

Excitation modes of vortices in submicron magnetic disks

Classical and quantum theory of spin waves in the vortex state of a mesoscopic submicron magnetic disk have been developed with account of the finite mass density of the vortex. Oscillations of the vortex core resemble oscillations of a charged string in a potential well in the presence of the magnetic field. A conventional gyrotropic frequency appears as a gap in the spectrum of spin waves of the vortex. The mass of the vortex has been computed, and the result agrees with experimental findings. The finite vortex mass generates a high-frequency branch of spin waves. The effects of an external magnetic field and dissipation have been addressed.

Implementação computacional do modelo carga-fluxo de carga-fluxo de dipolo para cálculo e interpretação das intensidades do espectro infravermelho

The first computational implementation that automates the procedures involved in the calculation of infrared intensities using the charge-charge flux-dipole flux model is presented. The atomic charges and dipoles from the Quantum Theory of Atoms in Molecules (QTAIM) model was programmed for Morphy98, Gaussian98 and Gaussian03 programs outputs, but for the ChelpG parameters only the Gaussian programs are supported. Results of illustrative but new calculations for the water, ammonia and methane molecules at the MP2/6-311++G(3d,3p) theoretical level, using the ChelpG and QTAIM/Morphy charges and dipoles are presented. These results showed excellent agreement with analytical results obtained directly at the MP2/6-311++G(3d,3p) level of theory.

A topologia molecular QTAIM e a descrição mecânico-quântica de ligações de hidrogênio e ligações de di-hidrogênio

Hydrogen bonds formed through the interaction between a high electronic density center (lone electron pairs, π or pseudo-π bonds) and proton donors cause important electronic and vibrational phenomena in many systems. However, it was demonstrated that proton donors interact with hydrides, such as alkali and alkaline earth metals (BeH2, MgH2, LiH and NaH), what yields a new type of interaction so-called dihydrogen bonds. The characterization of these interactions has been performed at light of the Quantum Theory of Atoms in Molecules (QTAIM), by which the electronic densities ρ are quantified and the intermolecular regions are characterized as closed-shell interactions through the analysis of the Laplacian field ∇2ρ.

O ESTADO DA ARTE DA LIGAÇÃO DE HIDROGÊNIO

Along the historical background of science, the hydrogen bond became widely known as the universal interaction, thus playing a key role in many molecular processes. Through the available theoretical approaches, many of these processes can be unveiled on the basis of the molecular parameters of the subject intermolecular system, such as the variation of bond length and mainly the frequency shift observed in the proton donor. Supported by the natural bond analysis (NBO) with the quantification of the hybridization contributions, the structural deformations and vibrational effects cited above are also attributed to the outcome of the intermolecular interaction strength, which consequently can be estimated by means of the quantum theory of atoms in molecules (QTAIM) as well as evaluated by the symmetry-adapted perturbation theory (SAPT). Moreover, to identify the preferential interaction sites for proton donors and acceptors, the molecular electrostatic potential (MEP) is useful in this regard.

The solutions and tunneling properties for a linear potential and an inverted harmonic oscillator in an infinite well

In this work we look at two different 1-dimensional quantum systems. The potentials for these systems are a linear potential in an infinite well and an inverted harmonic oscillator in an infinite well. We will solve the Schrödinger equation for both of these systems and get the energy eigenvalues and eigenfunctions. The solutions are obtained by using the boundary conditions and numerical methods. The motivation for our study comes from experimental background. For the linear potential we have two different boundary conditions. The first one is the so called normal boundary condition in which the wave function goes to zero on the edge of the well. The second condition is called derivative boundary condition in which the derivative of the wave function goes to zero on the edge of the well. The actual solutions are Airy functions. In the case of the inverted oscillator the solutions are parabolic cylinder functions and they are solved only using the normal boundary condition. Both of the potentials are compared with the particle in a box solutions. We will also present figures and tables from which we can see how the solutions look like. The similarities and differences with the particle in a box solution are also shown visually. The figures and calculations are done using mathematical software. We will also compare the linear potential to a case where the infinite wall is only on the left side. For this case we will also show graphical information of the different properties. With the inverted harmonic oscillator we will take a closer look at the quantum mechanical tunneling. We present some of the history of the quantum tunneling theory, its developers and finally we show the Feynman path integral theory. This theory enables us to get the instanton solutions. The instanton solutions are a way to look at the tunneling properties of the quantum system. The results are compared with the solutions of the double-well potential which is very similar to our case as a quantum system. The solutions are obtained using the same methods which makes the comparison relatively easy. All in all we consider and go through some of the stages of the quantum theory. We also look at the different ways to interpret the theory. We also present the special functions that are needed in our solutions, and look at the properties and different relations to other special functions. It is essential to notice that it is possible to use different mathematical formalisms to get the desired result. The quantum theory has been built for over one hundred years and it has different approaches. Different aspects make it possible to look at different things.

The solutions and tunneling properties for a linear potential and an inverted harmonic oscillator in an infinite well

In this work we look at two different 1-dimensional quantum systems. The potentials for these systems are a linear potential in an infinite well and an inverted harmonic oscillator in an infinite well. We will solve the Schrödinger equation for both of these systems and get the energy eigenvalues and eigenfunctions. The solutions are obtained by using the boundary conditions and numerical methods. The motivation for our study comes from experimental background. For the linear potential we have two different boundary conditions. The first one is the so called normal boundary condition in which the wave function goes to zero on the edge of the well. The second condition is called derivative boundary condition in which the derivative of the wave function goes to zero on the edge of the well. The actual solutions are Airy functions. In the case of the inverted oscillator the solutions are parabolic cylinder functions and they are solved only using the normal boundary condition. Both of the potentials are compared with the particle in a box solutions. We will also present figures and tables from which we can see how the solutions look like. The similarities and differences with the particle in a box solution are also shown visually. The figures and calculations are done using mathematical software. We will also compare the linear potential to a case where the infinite wall is only on the left side. For this case we will also show graphical information of the different properties. With the inverted harmonic oscillator we will take a closer look at the quantum mechanical tunneling. We present some of the history of the quantum tunneling theory, its developers and finally we show the Feynman path integral theory. This theory enables us to get the instanton solutions. The instanton solutions are a way to look at the tunneling properties of the quantum system. The results are compared with the solutions of the double-well potential which is very similar to our case as a quantum system. The solutions are obtained using the same methods which makes the comparison relatively easy. All in all we consider and go through some of the stages of the quantum theory. We also look at the different ways to interpret the theory. We also present the special functions that are needed in our solutions, and look at the properties and different relations to other special functions. It is essential to notice that it is possible to use different mathematical formalisms to get the desired result. The quantum theory has been built for over one hundred years and it has different approaches. Different aspects make it possible to look at different things.

Structure and energetics of mixed 4He-3He drops

Using a finite-range density functional, we have investigated the energetics and structural features of mixed helium clusters. The possibility of doping the cluster with a molecule of sulfur hexafluoride is also considered. It is seen that the repulsion introduced by the impurity strongly modifies the properties of the smallest drops. Although only a qualitative comparison is possible, the gross features displayed by our calculations are in agreement with recent experimental findings.

Continuum bound states as surface states of a finite periodic system

We discuss the relation between continuum bound states (CBSs) localized on a defect, and surface states of a finite periodic system. We model an experiment of Capasso et al. [F. Capasso, C. Sirtori, J. Faist, D. L. Sivco, S-N. G. Chu, and A. Y. Cho, Nature (London) 358, 565 (1992)] using the transfer-matrix method. We compute the rate for intrasubband transitions from the ground state to the CBS and derive a sum rule. Finally we show how to improve the confinement of a CBS while keeping the energy fixed.

Pauli distorted double folded potential

The enhancement in the production of even-Z nuclei observed in nuclear fission has also been observed in fragments produced from heavy ion collsions. Beams of 40Ar, 40Cl, and 40Ca at 25 MeV/nucleon were impinged on 58Fe and 58Ni targets. The resulting fragments were detected using the MSU 4pi detector array, which had additional silicon detectors for better isotopic resolution. Comparison of the ratios of yields for each element showed enhancement of even-Z fragment production. The enhancement was more pronounced for reactions with a greater difference in the N/Z of the compound system. However, this effect was less for systems that were more neutron rich. The average N/Z for fragments also displayed an odd-even effect with a lower average N/Z for the even-Z fragments. This is related to the greater availability of neutron-poor isotopes for even-Z nuclei

Identität der Identität und Differenz von Raum und Zeit bei Schelling mit Blick auf die Relativitäts- und Quantentheorie

In genannter Schrift soll versucht werden, einen aus der Kantschen und Fichteschen Erkenntnistheorie erfolgenden allgemeinen Zusammenhang herzustellen zwischen dem kategorialen Denken hinsichtlich Denken und Anschauen und dem Problem von Raum und Zeit, wie es sich mit der Entwicklung der modernen Physik durch die Relativitäts- und Quantentheorie deutlich aufdrängt. Es wird gezeigt, dass F.W.J. Schelling grundlegende Lösungsansätze hierzu bereitstellt, welche auf dem Gebiet der Logik, der Epistomologie und Naturphilosophie in der Nachfolge von Kant, Fichte und Spinoza stattfinden, jedoch weit über seine Zeit hinausreichen. Diese Ansätze werden von Schelling selbst unter den Begriff einer „Identität der Identität und Differenz“ gesetzt. In der genannten Dissertation sollen Denkbewegungen dargestellt werden, die eine Anbindung der Schellingschen Naturphilosophie an die sich mit den genannten unterschiedlichen Theorien bzw. deren problematischer Vereinheitlichung beschäftigende Physik zu erreichen versuchen. Der formelle Aufbau der Arbeit gehorcht der inhaltlichen Struktur dieser Anbindungsbemühung, insofern unterstellt wird, dass diese rein nur aus einem dialektischen Denken (sowohl in der Erkenntnistheorie, als auch Naturphilosophie) heraus überhaupt erreicht werden kann. So werden sowohl die Tätigkeiten des Verstandes als die des Anschauens in ihrem Zusammenspiel, wie aber auch die Verstandes- und Anschauungstätigkeiten an sich selbst betrachtet, dialektisch vermittelt dargestellt, was innerhalb der formellen Deduktion der Kantschen Kategorien und der korrespondierenden Anschauungsformen selbst durchgeführt wird. Schellings Intention seines späteren Denkens, die philosophischen Probleme auf die Geschichtlichkeit, die Freiheit und den Erfahrungsbezug des Menschen zu beziehen, wird nicht als Gegenposition zu den frühen Ansätze der Logik und Transzendentalphilosophie gedeutet, sondern selbst als Endpunkt einer dialektischen Entwicklung des Schellingschen Denkens gefasst. Dies ergibt folgenden formellen Aufbau der Arbeit: Zunächst wird in einem einleitenden Abschnitt über die Aufgabe der Philosophie selbst und ihrer Darstellbarkeit im Zusammenhang mit der Hegel-Schelling-Kontroverse gearbeitet, um Schelling als adäquaten Bezugspunkt für unsere moderne Diskussion auf der methodischen und sprachlichen Ebene einzuführen. Im Hauptteil werden die wesentlichen Momente der für Schelling wichtigen Transzendentalphilosophie der Jahrhundertwende dargestellt, um diese dann an den späteren phänomenologisch-epistemologischen Ansätzen zu spiegeln. Von der theoretischen Seite kommend werden die Hauptmomente der praktischen Philosophie Schellings aufgezeigt, um dann den Menschen in einem dritten Schritt Symbol der Ununterschiedenheit von logischen und freien Tätigkeiten bzw. von Leib und Seele zu deuten. Diese Resultate bleiben zunächst einmal liegen, um in dem zweiten Hauptabschnitt auf grundlegende naturphilosophische Voraussetzungen und Resultate derjenigen Physik einzugehen, welche die prinzipiellen Verständnisschwierigkeiten der Physik des frühen 20. Jahrhundert in die heutige kosmologische und atomistische Diskussion mitbringt. Der dritte Hauptabschnitt stellt den Versuch dar, Schellings Naturphilosophie an symptomatische Anschauungen der Physik heranzuführen, um ihn als zeitgenössischen Kritiker einzuführen, wie aber auch als einen, der bestimmte moderne naturwissenschaftliche bzw. physikalische Resultate im Besonderen vorwegzunehmen vermochte. Die Einführung seiner Philosophie in aktuelle naturphilosophische Diskussion wird als unabdingbare Voraussetzung zu einem zukünftigen Verständnis des Natur, des Kosmos´ und des Menschen gefordert.