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<p dir="ltr">In this article, we establish results concerning the nilpotent representation theory of groups. In particular, we utilize a theorem of Stallings to provide a general method that constructs pairs of groups that have isomorphic universal nilpotent quotients. We then prove by counterexample that absolute Galois groups of number fields are not determined by their universal nilpotent quotients. We also show that this is the case for residually nilpotent Kleinian groups and in fact, there exist non-isomorphic pairs that have arbitrarily large nilpotent genus. We additionally provide examples of non-isomorphic curves whose geometric fundamental groups have isomorphic universal nilpotent quotients and the isomorphisms are compatible with the outer Galois actions. </p>

No / This paper reports on the growth of benzamide crystals in the presence of 2'-aminoacetophenone. The resulting self-replicating intergrowth of benzamide crystals gives rise to ordered crystal aggregates in which individuals share a common c*. This behavior is interpreted using the concept of a motif capper additive which is able to halt the extension of structural motifs at the surface of a growing crystal. In this case the additive was selected to terminate the hydrogen-bonding ribbons, which extend along the b axis of the benzamide structure.

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In this thesis we investigate strongly-correlated states of ultracold bosonic atoms in rotating ring lattices and arrays of double-well potentials. In the first part of the thesis, we study the tunneling dynamics of ultracold bosons in double-well potentials. In the non-interacting limit single-particle transitions dominate, while in the interaction-dominated regime correlated tunneling of all particles prevails. At intermediate times of the many-particle flopping process correlated states occur, but the timescales of these processes increase dramatically with the number of particles. Using an array of double-well potentials, a large number of such few-particle superposition states can be produced in parallel. In the second part of the thesis, we study the effects of rotation on ultracold bosons confined to one-dimensional ring lattices. We find that at commensurate filling there exists a critical rotation frequency, at which the ground state of the weakly-interacting gas is fragmented into a macroscopic superposition of different quasi-momentum states. We demonstrate that the generation of such superposition states using slightly non-uniform ring lattices has several practical advantages. Moreover, we show that different quasi-momentum states can be distinguished in time-of-flight absorption imaging and propose to probe correlations via the many-body oscillations induced by a sudden change in the rotation frequency. Finally, we compare these macroscopic superposition states to those occurring in superconducting quantum interference devices. In the third part of the thesis, we demonstrate the creation of entangled states with ultracold bosonic atoms by dynamical manipulation of the shape of the lattice potential. To this end, we consider an optical superlattice that allows both the splitting of each site into a double-well potential and the variation of the height of the potential barrier between the sites. We show how to use this array of double-well potentials to perform entangling operations between neighboring qubits encoded on the Zeeman levels of the atoms. As one possible application, we present a method of realizing a resource state for measurement-based quantum computation via Bell-pair measurements. In the final part of the thesis, we study ultracold bosons on a two-dimensional square lattice in the presence of an effective magnetic field and point out a couple of features this system has in common with ultracold bosons in one-dimensional rotating ring lattices.

Esse trabalho visa a investigar a estrutura bi-Hamiltoniana de uma classe de sistemas dinâmicos. Depois de introduzir as ferramentas necessárias, a saber, as noções de variedade de Poisson, de grupo de PoissonLieedenetworknodiscoenoanêl,introduziremosossistemasdinâmicos relevantes nessa dissertação, chamados de reticulados de Coxeter-Toda. Esses sistemas dinâmicos, cujo espaço de fase pode ser identicado com umoportunoquocientedeumacéluladupladeCoxeter-Bruhatdogrupo linear geral, são obtidos por redução do sistema de Toda em GLn. Na parte nal do presente trabalho apresentaremos alguns resultados relacionado à um sistema dinâmico discreto chamado de aplicação do pentagrama, o qual pode ser obtido através uma oportuna discretização do sistema dinâmico de Boussinesq. / This work aims to study the bi-Hamiltonian structure of a class of dynamical systems. After introducing the relevant tools, namely the notions of Poisson manifold, Poisson-Lie group and of network dened in a disc and in an annulus, we will introduce the dynamical systems of interest for this dissertation, i.e., the Coxeter-Toda lattices. These dynamical systems, whose phase-space can be identied with a suitable quotient of a Coxeter double Bruhat cell of the general linear group, are obtained by reduction starting from the Toda ow on GLn. In the nal part of the present work will be presented some results concerning a discrete integrable system close to the so called Pentagram map, which is a discretization of the Boussinesq dynamical system..

Para um espaço localmente compacto K e um espaço de Banach X, seja C_0(K,X) o espaço das funções continuas que se anulam no infinito munido da norma do supremo. Nesta tese se provam resultados relacionados com a geometria destes espaços. / For a locally compact Hausdorff space K and a Banach spaces X, let C_0(K,X) be the Banach space of continuous functions which vanish at infinity endowed with the supremum norm. We prove some results about geometry of these spaces.

Apresentamos uma teoria para obtenção de seções de choque de espalhamento inelástico de luz via mecanismos de flutuações de densidade de carga e spin em um gás de elétrons não-uniforme formado por um sistema multi-camadas de GaAs periodicamente &#948-dopadas com concentração eletrônica relativamente alta. Os cálculos, onde estão inclusos efeitos da interação coulombiana entre os portadores, efeitos de correlação e troca dinâmicos e o acoplamento com fônons LO, foram efetuados em condições de extrema ressonância com o gap de split-off do GaAs. Em tais condições, a estrutura detalhada dos níveis de energia dos buracos de spin-split torna-se extremamente importante e é fundamental para o surgimento do espectro de partícula independente apresentado nos espectros polarizados. Este comportamento é revelado através da seção de choque de espalhamento que consiste da parte imaginária de uma função resposta constituída de um termo de caráter de partícula independente e outro de caráter coletivo. De forma a levar em conta o amortecimento das flutuações de densidade, propõe-se uma função espectral baseada na conservação da corrente local. Comparação com formas de linha experimentais disponíveis para o caso de espectros despolarizados mostram excelente concordância. No caso dos espectros polarizados a concordância se deu em nível semi-quantitativo, já que excitações de caráter coletivo obtidas experimentalmente apresentaram intensidade menor do que aquelas fornecidas pela teoria. Tal discrepância é atribuída a efeitos de desordem introduzidas no processo de dopagem e que implicam na quebra das regras de conservação de momentum. / We present a theory for the inelastic light scattering cross-section for the mechanisms of charge and spin-density fluctuations in the relatively high concentration of the non-uniform electron gas of a multi-layered &#948-doped GaAs system. The calculations are done in conditions of extreme resonance with the spin-split edge of GaAs and include the effects of Coulomb interactions between the carriers, dynamical exchange-correlations and coupling with LO phonons. In such conditions, the detailed energy level structure of the spin-split holes becomes extremely important and is responsible by the single-particle behavior presented in the polarized spectrum. This behavior revealed by the scattering cross-section derived from the imaginary part of a response function, consists of a term showing single particle character and another displaying collective character. To include the damping of the density fluctuations, a spectral function is proposed based on the foreknowledge that the local current must be conserved. Comparison with the available experimental line-shapes for the depolarized spectra show excellent agreement. In the case of polarized spectra the agreement was given in semi-quantitative terms as experimental collective excitations present less intensity than those calculated by the theory. Such difference is attributed to disorder effects produced during the doping process which results in break down of momentum conservation rules.