This study investigates six theoretical approaches offered as solutions to the paradox of the heap (sorites paradox), a logic puzzle dating back to the ancient Greek philosopher Eubulides. Those considered are: Incoherence Theory, Epistemic Theory, Supervaluation Theory, Many-Valued Logic, Fuzzy Logic, and Non-Classical Semantics. After critically examining all of these, it is concluded that none of the attempts to explain the sorites are fully adequate, and the paradox remains unresolved. / Philosophy / M.A. (Philosophy)

We study the low-temperature physics arising in models of a strongly correlated, tunnel-coupled double quantum dot (DQD), particularly the two-impurity Anderson model (2AIM) and the two-impurity Kondo model (2IKM), employing a combination of physical arguments and the Numerical Renormalisation Group. These models exhibit a rich range of Kondo physics. In the regime with essentially one electron on each dot, there is a competition between the Kondo effect and the interdot exchange interaction. This competition gives rise to a quantum phase transition (QPT) between local singlet and Kondo singlet phases in the 2IKM, which becomes a continuous crossover in the 2AIM as a result of the interlead charge transfer present. The 2IKM is known to exhibit two-channel Kondo (2CK) physics at the QPT, and we investigate whether this is also the case for the 2AIM at the crossover. We find that while in principle 2CK physics can be observed in the 2AIM, extremely low temperatures are required, such that it is unlikely that 2CK physics will be observed in an experimental DQD system in the near future. We have studied the effect of a magnetic field on the 2AIM and the 2IKM, finding that both the zero-field QPT in the 2IKM and the zero-field crossover in the 2AIM, persist to finite field. This presents the possibility of observing 2CK physics in an experimental DQD at finite field, but we find that the temperatures required to do so are extremely low. We show that longer even-numbered chains of spins also exhibit QPTs at finite field, and argue that a 2N-spin chain should undergo N QPTs as field is increased (starting deep in the local singlet phase at zero field). We have also carried out a joint theoretical-experimental study of a carbon nanotube based DQD, in collaboration with Dr. Mark Buitelaar et al. The agreement between experimental and theoretical results is good, and the experiments are able to access the crossover present in the 2AIM at finite field. Furthermore, the experiments show the wide range of physics exhibited by DQD systems, and illustrate the utility of such systems in probing correlated electron physics.

<p>Atomic physics plays an important role in determining the evolution stages in a wide range of laboratory and cosmic plasmas. Therefore, the main contribution to our ability to model, infer and control plasma sources is the knowledge of underlying atomic processes. Of particular importance are reliable low temperature dielectronic recombination (DR) rate coefficients.</p><p>This thesis provides systematically calculated DR rate coefficients of lithium-like beryllium and sodium ions via ∆n = 0 doubly excited resonant states. The calculations are based on complex-scaled relativistic many-body perturbation theory in an all-order formulation within the single- and double-excitation coupled-cluster scheme, including radiative corrections.</p><p>Comparison of DR resonance parameters (energy levels, autoionization widths, radiative transition probabilities and strengths) between our theoretical predictions and the heavy-ion storage rings experiments (CRYRING-Stockholm and TSRHeidelberg) shows good agreement.</p><p>The intruder state problem is a principal obstacle for general application of the coupled-cluster formalism on doubly excited states. Thus, we have developed a technique designed to avoid the intruder state problem. It is based on a convenient partitioning of the Hilbert space and reformulation of the conventional set of pairequations. The general aspects of this development are discussed, and the effectiveness of its numerical implementation (within the non-relativistic framework) is selectively illustrated on autoionizing doubly excited states of helium.</p>

No description available.

Šis darbas yra skirtas šiuolaikinės atomo trikdžių teorijos matematinio aparato, paremto efektinių operatorių formalizmu, plėtojimui. Darbe nuosekliai ir sistemingai, pradedant nuo pačių bendriausių principų, nagrinėjami Foko erdvės apribojimo į redukavimo grupių neredukuotinus poerdvius metodai bei pateikiama neredukuotinų tenzorinių operatorių, charakterizuojančių fizikines ir efektines sąveikas, klasifikacija bendrais ir tam tikrais atskirais atvejais. Gautos išraiškos ir iš jų išplaukiančios išvados yra grindžiamos matematine kalba. Dauguma esminių rezultatų yra suformuluoti teoremų pavidalu. Disertaciją sudaro 101 puslapis, 5 skyriai, 4 priedai, 40 lentelių ir 9 paveikslėliai. Pagrindiniai rezultatai, pateikti disertacijoje, yra publikuoti fizikos ir matematikos mokslų žurnaluose. / The principal goals of the thesis are subjected to general methods and forms of effective operators by the nowadays demands of theoretical application of many-body perturbation theory to atomic physics. The present theoretical research follows up step by step by systematic observation of various possibilities to restrict the Fock space operators to their irreducible subspaces and the classification of irreducible tensor operators which represent the physical as well as the effective interactions. To ground the results of the thesis, the symbolic preparation of obtained expressions is strictly proved mathematically. Most of the main results are listed in theorems. The doctoral dissertation contains 101 pages, 5 sections, 4 appendices, 40 tables and 9 figures. The main results described in the present dissertation have been published in journals of physical and mathematical sciences.

The principal goals of the thesis are subjected to general methods and forms of effective operators by the nowadays demands of theoretical application of many-body perturbation theory to atomic physics. The present theoretical research follows up step by step by systematic observation of various possibilities to restrict the Fock space operators to their irreducible subspaces and the classification of irreducible tensor operators which represent the physical as well as the effective interactions. To ground the results of the thesis, the symbolic preparation of obtained expressions is strictly proved mathematically. Most of the main results are listed in theorems. The doctoral dissertation contains 101 pages, 5 sections, 4 appendices, 40 tables and 9 figures. The main results described in the present dissertation have been published in journals of physical and mathematical sciences. / Šis darbas yra skirtas šiuolaikinės atomo trikdžių teorijos matematinio aparato, paremto efektinių operatorių formalizmu, plėtojimui. Darbe nuosekliai ir sistemingai, pradedant nuo pačių bendriausių principų, nagrinėjami Foko erdvės apribojimo į redukavimo grupių neredukuotinus poerdvius metodai bei pateikiama neredukuotinų tenzorinių operatorių, charakterizuojančių fizikines ir efektines sąveikas, klasifikacija bendrais ir tam tikrais atskirais atvejais. Gautos išraiškos ir iš jų išplaukiančios išvados yra grindžiamos matematine kalba. Dauguma esminių rezultatų yra suformuluoti teoremų pavidalu. Disertaciją sudaro 101 puslapis, 5 skyriai, 4 priedai, 40 lentelių ir 9 paveikslėliai. Pagrindiniai rezultatai, pateikti disertacijoje, yra publikuoti fizikos ir matematikos mokslų žurnaluose.

No description available.

This thesis deals with the recent issue of increased number of university students. It entails the problematic success on the labor market or reduction of quality of the particular studies. This research focuses not only on the Czech Republic region but also on some other chosen countries contending with the very similar issue. This thesis follows the analogous paper of Jan Keller and Lubor Tvrdý: "Vzdělanostní společnost? Chrám, výtah a pojišťovna". Classical statistical research and questionnaire survey were employed as the key methods of answering the main inquiries.

Title: Categorial methods in structure theory Author: Jakub Opršal Department / Institute: Mathematical Institute, Charles University Supervisor of the master thesis: prof. RNDr. Věra Trnková, DrSc. Abstract: In the first part of the thesis we investigate functor algebras. Initial algebras have distin- guished role in the study of these structures, and it can be constructed by certain transfinite construction, which is called initial algebra construction. Sooner this year Adámek and Trnková have prooved, that the construction stops in either at most three, or in κ steps where κ is a regular cardinal. We continue with their work, and we study the relation between the size of the algebra and the length of the convergence. We prove that the length of the convergence never exceeds the cardinality of the initial algebra. Another transfinite construction has been studied in 1980 by Kelly. He has described the construction of free algebras for a pointed functor and defined a class of well-pointed functors for which the construction is especially simple (and is in fact special case of the construction of relatively terminal coalgebra which has been recently defined by Adámek and Trnková). In the last chapter we describe all well-pointed functors in categories of sets and the dual category, and we provide list of...

Com o rápido avanço das técnicas experimentais observado nas últimas décadas, a fabricação de sistemas nanoestruturados se tornou uma realidade. Nessa escala de grandeza, as interações entre elétrons e vibrações nucleares têm um papel importante no transporte eletrônico, podendo causar a perda de coerência de fase dos elétrons, a abertura de novos canais de condução e a supressão de canais puramente elásticos. Neste trabalho, o problema do transporte eletrônico em escala nanométrica foi tratado considerando as interações elétron-fônon, o que resultou na implementação de ferramentas computacionais para simulação realística de materiais. O transporte eletrônico foi abordado por meio do formalismo das Funções de Green Fora do Equilíbrio, onde as interações elétron-fônon foram tratadas por diferentes modelos. Para considerar o efeito dessas interações no transporte, é necessário, em princípio, incluir um termo de autoenergia de espalhamento na Hamiltoniana do sistema. Contudo, a forma exata dessa autoenergia é desconhecida e aproximações são necessárias. O primeiro efeito da interação elétron-fônon estudado foi a perda de coerência de fase, o que foi abordado pelo modelo fenomenológico das sondas de Büttiker [1]. Foram realizadas duas implementações diferentes deste modelo, a primeira na forma usual, onde se considera uma aproximação elástica para o cálculo da corrente, e a segunda por meio de uma nova proposta sem a aproximação elástica. Entretanto, como a autoenergia de interação utilizada não contém informação a respeito da estrutura dos fônons, o modelo produz somente um alargamento do canal de condutância, simulando apenas o efeito de perda de coerência de fase dos elétrons devido à interação com fônons do material. Para poder incluir as informações sobre a estrutura dos fônons, foi desenvolvido o programa PhOnonS ITeratIVE VIBRATIONS, para o cálculo das frequências e dos modos vibracionais de materiais e para calcular a matriz de acoplamento elétron-fônon, a partir de métodos de primeiros princípios. No cálculo da matriz de acoplamento elétron-fônon, além da implementação do código algumas intervenções foram realizadas no programa SIESTA [2,3] (uma implementação da Teoria do Funcional da Densidade). Outra abordagem para a interação elétron-fônon consiste em expandir a autoenergia de interação perturbativamente em diagramas de Feynman até a primeira ordem, o que é convencionalmente chamado de primeira aproximação de Born. Essa aproximação, assim como a sua versão autoconsistente, no qual uma classe mais ampla de diagramas é considerada, foram incorporadas ao programa SMEAGOL [4], um código de transporte eletrônico ab initio baseado na combinação DFT-NEGF e que utiliza como plataforma do cálculo da estrutura eletrônica o código SIESTA. Essas implementações, em conjunto com diversas mudanças realizadas no código SMEAGOL, deram origem ao programa Inelastic SMEAGOL para cálculos de transporte inelástico ab initio. Nessa busca por uma descrição mais realista dos dispositivos eletrônicos, outro aspecto que deve ser considerado é o fato de que os dispositivos muitas vezes podem alcançar escalas de comprimento da ordem de 100 nm com um grande número de defeitos aleatoriamente distribuídos, o que pode levar a um novo regime fundamental de transporte, a saber, o de localização de Anderson [5]. Neste trabalho, foi desenvolvido o programa Inelastic DISORDER, que permite calcular, por primeiros princípios, as propriedades de transporte elástico e inelástico de sistemas com dezenas de milhares de átomos com um grande número de defeitos posicionados aleatoriamente. O método combina cálculos de estrutura eletrônica via DFT com o formalismo NEGF para o transporte, onde as interações elétron-fônon são incluídas por meio de teoria de perturbação com relação à matriz de acoplamento elétron-fônon (Lowest Order Expansion). O método desenvolvido foi aplicado ao estudo de nanofitas de grafeno com impurezas hidroxílicas. Observou-se que, ao incluir a interação elétron-fônon, as propriedades de transporte sofrem mudanças significativas, indicando que estas interações podem influenciar nos efeitos de localização por desordem. [1] M. Büttiker. Phys. Rev. B 33(5), 30203026 (1986). [2] E. Artacho, D. Sánchez-Portal, P. Ordejón, A. García e J. M. Soler. Phys. Stat. Sol. (b) 215, 809817 (1999). [3] J. M. Soler, E. Artacho, J. D. Gale, A. García, J. Junquera, P. Ordejón e D. Sánchez- Portal. J. Phys. Cond. Mat. 14, 27452779 (2002). [4] A. R. Rocha, V. M. García-Suárez, S. W. Bailey, C. J. Lambert, J. Ferrer e S. Sanvito. Phys. Rev. B 73, 085414 (2006). [5] P. W. Anderson. Phys. Rev. 109, 1492 (1958). / With the fast improvement of experimental techniques over the past decades, the synthesis of nanoscale systems has become a reality. At this length scales, the interaction between electrons and ionic vibrations plays an important role in electronic transport, and may cause the loss of the electron\'s phase coherence, the opening of new conductance channels and the suppression of purely elastic ones. In this work the electronic transport problem at nanoscale was addressed considering the electron-phonon interactions, resulting on the development of computational tools for realistic simulations of materials. The electronic transport was approached with the Non-Equilibrium Green\'s Function formalism, where electron-phonon interactions were addressed by different models. To take into account the interaction\'s effects, one needs in principle to include a self-energy scattering term in the system Hamiltonian. Nevertheless, the exact form of this self-energy is unknown and approximations are required. The first effect from electron-phonon interactions dealt was the loss of phase coherence, which was approached by the Büttiker\'s probes phenomenological model [1]. Two different implementations of this model were performed, the first in the standard form, where an elastic approximation is considered in order to compute the current, and the second by a new method without the elastic approximation. However, since the interaction self-energy used doesn\'t contains any information about the phonon\'s structure, this model only produces a broadening at the conducting channels, simulating just the effect of loss of phase coherence from the electrons due to their interactions with the phonons. In order to be able to include information about the phonon\'s structure, the computational code PhOnonS ITeratIVE VIBRATIONS was developed, for calculating the frequencies and vibrational modes of the materials and to compute the electron-phonon coupling matrix, from first principles methods. In the calculation of the electron-phonon coupling matrix, besides the code implementation some changes were performed at the SIESTA program [2,3] (a Density Functional Theory implementation). Another approach for the electron-phonon interactions consists of expanding the interaction self-energy perturbatively in Feynman diagrams until the first order, what is conventionally called the first Born approximation. This approximation, together with its self-consistent version, where a wider class of diagrams are regarded, have been incorporated into the SMEAGOL program [4], an ab initio electronic transport code based on the combination DFT-NEGF which uses the SIESTA code as a platform for electronic structure calculations. The implementations, together with many changes performed on SMEAGOL code, gave rise to the Inelastic SMEAGOL program for inelastic ab initio transport calculations. In this search for a more realistic description of electronic devices, another feature that should be taken into account is the fact that these devices most often can reach the 100 nm length scale with a large number of randomly distributed defects, which can lead to a fundamentally new transport regime, namely the Anderson localization regime [5]. In this work, the program Inelastic DISORDER was developed, which allows one to compute, by first principles, the elastic and inelastic transport properties from systems with tens of thousands of atoms with a large number of randomly positioned defects. The method combines electronic structure calculations via DFT with the NEGF formalism for transport, where the electron-phonon interactions are included with perturbation theory on the electron-phonon coupling matrix (Lowest Order Expansion). The developed method was applied to the study of graphene nanoribbons with joint attachment of hydroxyl impurities. It was observed that, by including the electron-phonon interaction, the transport properties experience significant changes, indicating that these interactions can influence the effects of localization by disorder. [1] M. Büttiker. Phys. Rev. B 33(5), 30203026 (1986). [2] E. Artacho, D. Sánchez-Portal, P. Ordejón, A. García, and J. M. Soler. Phys. Stat. Sol. (b) 215, 809817 (1999). [3] J. M. Soler, E. Artacho, J. D. Gale, A. García, J. Junquera, P. Ordejón, and D. Sánchez- Portal. J. Phys. Cond. Mat. 14, 27452779 (2002). [4] A. R. Rocha, V. M. García-Suárez, S. W. Bailey, C. J. Lambert, J. Ferrer, and S. Sanvito. Phys. Rev. B 73, 085414 (2006). [5] P. W. Anderson. Phys. Rev. 109, 1492 (1958).