Relação de dispersão é outro nome para a função Hamiltoniana, cujo conhecimento especica completamente a dinâmica de um sistema no formalismo da mecânica classica. Sua escolha está intimamente vinculada às simetrias do sistema e, no contexto cosmologico aqui apresentado, com as simetrias locais obedecidas pelas leis fsicas. Mais ainda, a contribuição da materia na dinâmica cosmologica reflete a escolha do grupo local de simetrias das leis fsicas. Por outro lado, o problema fundamental da cosmologia pode ser definido como a construção de um modelo de evolução temporal de estados que, sob as hipoteses mais simples sobre estados iniciais (digamos, que demande a menor quantidade de informação possível para serem enunciadas), prediga o estado atual observado. O paradigma inacionario é atualmente a ideia que melhor cumpre esta denição, uma vez que prediz que uma grande variedade de condições iniciais leva a aspectos fundamentais do universo observado. Contudo, os mecanismos usuais de realização da inflação sofrem de problemas conceituais. O ponto de vista deste trabalho e que a realização convencional da inflação, isto é, atraves dos campos escalares minimamente acoplados, é a formulação localmente relativisticamente invariante da inflação. A maneira de incluir quebras e deformações da estrutura de simetrias locais na cosmologia é não única e está associado ao chamado problema trans Planckiano da inflação. Analogamente, a motivação conceitual para incluir esse tipo de modicação tampouco é unica. Dependendo do esquema de realização, a versão localmente não relativstica da mesma pode apresentar graves diculdades de conciliação com observações atuais, ou apresentar vantagens conceituais em relacão ao modelo padrão de inflacão, enquanto em conformidade com observações cosmológicas. Da maneira como foi posto o problema fundamental da cosmologia, a escolha das simetrias locais influi na regra de evolução dos estados. O conceito de simetrias encontra sua formulação independente de teorias físicas no formalismo da teoria de grupos, mas consideraremos uma extensão da ideia, de aplicabilidade mais geral, a teoria das algebras de Hopf que, de certo modo, trata das simetrias de estruturas algebricas. Esta extensão é útil inclusive no trato de simetrias dos espacos não comutativos, uma das principais propostas fsicas que em última analise afeta a estrutura de simetrias locais do espaco-tempo. A expressão simetrias locais, por si só, não diz muito sem a consideração de regras de realização. Essas regras dependem da estrutura matematica das observaveis da teoria. Sob hipoteses muito gerais, que não especicam uma teoria em particular, é possível mostrar, não como um teorema matematico formal, mas como uma hipotese tecnicamente bem motivada, que existem apenas dois tipos de teorias fsicas: as classicas e as quânticas. Trabalharemos sob essas hipoteses, as quais se formulam algebricamente assumindo a estrutura de C*-álgebra para as observaveis físicas, outra motivação para o uso das álgebras de Hopf para descrição das simetrias da natureza. / Dispersion relation is another name for the Hamiltonian function whose knowledge completely specifies the dynamics in the formalism of classical mechanics. Its choice is intimately related to the symmetries of the system, and, in the cosmological context here exposed, with the local space-time symmetries obeyed by physical laws. For the other side, the fundamental problem of cosmology can be defined as a construction of a time evolution model of states which, under simplest possible hypothesis concerning initial conditions (say, which demands the minimal amount of information to be specified), predicts the present observed state. The inflationary paradigm is currently the idea which better accomplishes this definition, since it predicts that a great variety of initial conditions lead to essential aspects of observed universe. The usual mechanisms of inflation suffer, however, with conceptual problems. The point of view of this work is that the usual realization of inflation based on weakly coupled scalar fields is the local relativistic invariant realization. The way of including breaks and deformations of the local space-time symmetries is not unique and it is associated to the so called Trans-Planckian problem of inflation. Analogously, the motivation to include this kind of modification is neither unique. Depending of the scheme of realization, the locally non-relativistic version may lead to serious difficulties in conciliation with observations, or to conceptual advantages over standard formulations while in accordance with observational data. In the way that was proposed the fundamental problem of cosmology, the choice of local symmetries affects the rule of evolution of states. The concept of symmetry finds its formulation independently of physical theories in the group theory formalism, but we will consider an extension of the idea, with wider applicability, the theory of Hopf algebras, which is about symmetries of algebraic structures. That extension is also useful to deal with symmetries of non-commutative spaces, one of the main physical proposals that affects the structure of space-time symmetries. The expression, local symmetries, by itself, does not say too much without considering realization rules. Those rules depend on mathematical structure of observables in the theory. Under very general hypothesis that do not specify a particular theory, it is possible to show, not as a formal mathematical theorem, but as a technically well motivated hypothesis, that only two types of physical theories do exist: The classical ones and the quantum ones. We are going to work under those hypothesis, which can be algebraically formulated assuming a C*-algebra structure for physical observables, another motivation for the use of algebraic structures like Hopf algebras for the description of nature\'s symmetries

Cette thèse présente quelques résultats de la théorie des probabilités quantiques et de l’analyse harmonique à valeurs operateurs. La thèse est composée des trois parties.Dans la première partie, on démontre la décomposition atomique des espaces de Hardy de martingales non commutatives. On identifie aussi les interpolés complexes et réels entre les versions conditionnelles des espaces de Hardy et BMO de martingales non commutatives.La seconde partie est consacrée à l’étude des espaces de Hardy à valeurs opérateursvia la méthode d’ondellettes. Cette approche est similaire à celle du cas des martingales non commutatives. On démontre que ces espaces de Hardy sont équivalents à ceux étudiés par Tao Mei. Par conséquent, on donne une base explicite complètement inconditionnelle pour l’espace de Hardy H1(R), muni d’une structure d’espace d’opérateurs naturelle. La troisième partie porte sur l’analyse harmonique sur le tore quantique. On établit les inégalités maximales pour diverses moyennes de sommation des séries de Fourier définies sur le tore quantique et obtient les théorèmes de convergence ponctuelle correspondant. En particulier, on obtient un analogue non commutative du théorème classique de Stein sur les moyennes de Bochner-Riesz. Ensuite, on démontre que les multiplicateurs de Fourier complètement bornés sur le tore quantique coïncident à ceux définis sur le tore classique. Finalement, on présente la théorie des espaces de Hardy et montre que ces espaces possèdent les propriétés des espaces de Hardy usuels. En particulier, on établit la dualité entre H1 et BMO. / This thesis presents some results in quantum probability and operator-valued harmonicanalysis. The main results obtained in the thesis are contained in the following three parts:In first part, we prove the atomic decomposition for the Hardy spaces h1 and H1 of noncommutative martingales. We also establish that interpolation results on the conditionedHardy spaces of noncommutative martingales. The second part is devoted to studying operator-valued Hardy spaces via Meyer’s wavelet method. It turns out that this way of approaching these spaces is parallel to that in the noncommutative martingale case. We also show that these Hardy spaces coincide with those introduced and studied by Tao Mei in [52]. As a consequence, we give an explicit completely unconditional base for Hardy spaces H1(R) equipped with a natural operator space structure. The third part deals with with harmonic analysis on quantum tori. We first establish the maximal inequalities for several means of Fourier series defined on quantum tori and obtain the corresponding pointwise convergence theorems. In particular, we prove the noncommutative analogue of the classical Stein theorem on Bochner-Riesz means. Then we prove that Lp completely bounded Fourier multipliers on quantum tori coincide with those on classical tori with equal cb-norms. Finally, we present the H1-BMO and Littlewood- Paley theories associated with the circular Poisson semigroup over quantum tori.

Submitted by Renata Lopes (renatasil82@gmail.com) on 2017-10-11T14:36:57Z No. of bitstreams: 1 rafaelleitefernandes.pdf: 279997 bytes, checksum: 10717a2d36ac106c7c879c22dcad130e (MD5) / Approved for entry into archive by Adriana Oliveira (adriana.oliveira@ufjf.edu.br) on 2017-10-16T13:49:39Z (GMT) No. of bitstreams: 1 rafaelleitefernandes.pdf: 279997 bytes, checksum: 10717a2d36ac106c7c879c22dcad130e (MD5) / Made available in DSpace on 2017-10-16T13:49:39Z (GMT). No. of bitstreams: 1 rafaelleitefernandes.pdf: 279997 bytes, checksum: 10717a2d36ac106c7c879c22dcad130e (MD5) Previous issue date: 2017-03-08 / CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / Neste trabalho vamos analisar as contribuições da não-comutatividade nos modelos eletrodinâmicos de Proca e Podolsky. O modelo de Proca não-comutativo (NC) é originalmente não invariante perante transformações de calibre. Neste trabalho obteremos, através do método chamado "gauge unfixing" (GU), uma hamiltoniana invariante por transformações de calibre. Em seguida, vamos estudar a versão NC do modelo eletro-dinâmico de Podolsky. Utilizando o produto Moyal e o mapeamento de Seiberg-Witten, encontraremos uma lagrangeana para o modelo de Podolsky no espaço-tempo NC e, a partir daí, analisaremos as contribuições da não-comutatividade para tal modelo. O primeiro aspecto importante é a invariância de calibre. O modelo de Podolsky é originalmente invariante de calibre porém, no espaço-tempo NC, a lagrangeana não é invariante perante as mesmas tranformações. Utilizando o método de Noether, encontraremos uma ação dual invariante de calibre e as simetrias serão calculadas. Em seguida é feita a quantização do modelo de Podolsky NC através de dois métodos, o método de Dirac e o método de Faddev-Jackiw. Uma comparação será feita entre os dois métodos. / In this work we will analyse the contributions of non-commutative (NC) to the Proca electrodynamics and also Podolsky's electrodynamics. The NC Proca model is originally not gauge invariant. Here we find, through the gauge unfixing method, a gauge invariant Hamiltonian. With respect to the Podolsky model, we used de Moyal product and the Seiberg-Witten map to analyze the NC contributions to this model. The first important aspect is the gauge invariance. The Podolky model is originally gauge invariant, however, in NC space the Lagrangian in not gauge invariant through the same transformations. Using the Noether method, we find a dual action gauge invariant and we calculate the symmetries. Then, we make the quantization for the NC Podolsky model through two formalism: the Dirac and the Faddev-Jackiw. A comparison is make between this two methods.

Cette thèse s'intéresse à des familles de fonctions zêta spectrales (séries de Dirichlet) qui peuvent être associées à certaines algèbres d'opérateurs sur des espaces de Hilbert. Dans ce mémoire, la principale question étudiée sur ces fonctions zêta est l'existence d'un prolongement méromorphe à partir d'un demi-plan ouvert du plan complexe au plan complexe tout entier. Généralisant une idée de Nigel Higson, on propose dans la partie I, une méthode pour prouver l'existence de ce prolongement méromorphe pour certains fonction zêta spectrales. Cette méthode s’effectue dans le cadre d'algèbres d'opérateurs différentiels généralisés et elle s'appuie sur une suite de réduction. Le théorème principal donne, sous certaines conditions, l'existence d'un prolongement méromorphe, une localisation des pôles dans les supports de suites arithmétiques et une borne supérieure pour l'ordre de ces pôles. Dans la partie II, on reformule la méthode de la partie I dans le contexte et avec le vocabulaire des triplets spectraux de Connes et Moscovici. Dans la troisième partie, on donne une application pour des fonctions zêta associées à des opérateurs de type Laplace sur des variétés lisses, compactes et sans bord. Cet exemple a été initialement traité par Nigel Higson avec cette approche en 2006. Une deuxième application traite de fonctions zêta associées au tore non commutatif. Dans la partie IV, on utilise le calcul pseudodifférentiel associé à des algèbres de Lie nilpotentes et développé par Dominique Manchon, pour construire de nouveaux triplets spectraux. Dans la partie V se trouve la principale application de la méthode exposée dans ce mémoire. On prouve l'existence du prolongement méromorphe pour des fonctions zêta provenant de représentations de Kirillov d'une classe d'algèbre de Lie nilpotentes. / The thesis is about a families of zeta functions (Dirichlet series) that may be associated to certain algebras of Hilbert space operators. In this thesis, the main question in studying these zeta functions is to establish their meromorphic continuation from a half-plane in the complex plane to the full plane.Following an idea of Nigel Higson, we develop, in part I, a method for proving the existence of a meromorphic continuation for some spectral zeta functions. The method is based on algebras of generalized differential operators. The more important tool is the reduction sequence. The main theorem states, under some conditions, the existence of a meromorphic continuation, a localization of the poles in supports of arithmetic sequences and an upper bound of their order. A formulation of the method into the framework of Connes and Moscovici, the regular spectral triples, setting in part II. In the third part, we give an application for zeta functions associate to a Laplace-type operator on a smooth, closed manifold. This example was initially treated in this way by Nigel Higson in 2006. We give another application for zeta functions associate to the noncommutative torus. In part IV, using the work of Dominique Manchon on algebras of pseudodifferential operators associated to unitary representations of nilpotent Lie group, we construct new spectral triples. In part V, set the main application of the method. We applicate the reduction method for some algebras of generalized differential operators, arising from a Kirillov representation of a class of nilpotent Lie algebras.

It is argued that the geometric dual of a noncommutative operator algebra represents a notion of quantum state space which differs from existing notions by representing observables as maps from states to outcomes rather than from states to distributions on outcomes. A program of solving for an explicitly geometric manifestation of quantum state space by adapting the spectral presheaf, a construction meant to analyze contextuality in quantum mechanics, to derive simple reconstructions of noncommutative topological tools from their topological prototypes is presented. We associate to each unital C*-algebra A a geometric object--a diagram of topological spaces representing quotient spaces of the noncommutative space underlying A—meant to serve the role of a generalized Gel'fand spectrum. After showing that any functor F from compact Hausdorff spaces to a suitable target category C can be applied directly to these geometric objects to automatically yield an extension F^∼ which acts on all unital C*-algebras, we compare a novel formulation of the operator K₀ functor to the extension K^∼ of the topological K-functor. We then conjecture that the extension of the functor assigning a topological space its topological lattice assigns a unital C*-algebra the topological lattice of its primary ideal spectrum and prove the von Neumann algebraic analogue of this conjecture.

Die Arbeit beschäftigt sich mit zwei Themen: den nichtkommutativen Yang-Mills-Theorien und der AdS/CFT-Korrespondenz. Im ersten Teil wird eine teilweise Aufsummation der theta-entwickelten Störungstheorie untersucht. Letztere stellt einen Weg dar, nichtkommutative Yang-Mills-Theorien mit beliebigen Eichgruppen G als Störungsentwicklung im Nichtkommutativitätsparameter theta zu definieren. Es wird gezeigt, daß man im Fall, daß G eine echte Untergruppe von U(N) ist, die ungleich einer U(M) ist (M / This thesis addresses two topics: noncommutative Yang-Mills theories and the AdS/CFT correspondence. In the first part we study a partial summation of the theta-expanded perturbation theory. The latter allows one to define noncommutative Yang-Mills theories with arbitrary gauge groups G as a perturbation expansion in the noncommutativity parameter theta. We show that for G being a subset of U(N) but not equal to U(M), M

Le but de cette thèse est d’étudier l’analyse sur les espaces hpc(Rd,M), la version locale des espaces de Hardy à valeurs opératorielles construits par Tao Mei. Les espaces de Hardy locaux à valeurs opératorielles sont définis par les g-fonctions de Littlewood-Paley tronquées et les fonctions intégrables de Lusin tronquées associées au noyau de Poisson. Nous développons la théorie de Calderón-Zygmund sur hpc(Rd,M); nous étudions la dualité hpcbmocq et l’interpolation. D’après ces résultats, nous obtenons la caractérisation générale de hpc(Rd,M) en remplaçant le noyau de Poisson par des fonctions tests raisonnables. Ceci joue un rôle important dans la décomposition atomique lisse de h1c(Rd,M). En même temps, nous étudions aussi les espaces de Triebel-Lizorkin inhomogènes à valeurs opératorielles Fpα,c(Rd,M). Comme dans le cas classique, ces espaces sont connectés avec des espaces de Hardy locaux à valeurs opératorielles par les potentiels de Bessel. Grâce à l’aide de la théorie de Calderón-Zygmund, nous obtenons les caractérisations de type LittlewoodPaley et de type Lusin par des noyaux plus généraux. Ces caractérisations nous permettent d’étudier différentes propriétés de Fpα,c(Rd,M), en particulier, la décomposition atomique lisse. Ceci est une extension et une amélioration de la décomposition atomique précédente de h1c(Rd,M). Comme une application importante de cette décomposition atomique lisse, nous montrons la bornitude d’opérateurs pseudo-différentiels avec les symboles réguliers à valeurs opératorielles sur des espaces de Triebel-Lizorkin Fpα,c(Rd,M), pour α ∈ R et 1 ≤ p ≤ ∞. Finalement, grâce à la transférence, nous obtenons aussi la Fpα,c-bornitude d’opérateurs pseudo-différentiels sur les tores quantiques / This thesis is devoted to the study of the analysis on the spaces hpc(Rd,M), the local version of operator-valued Hardy spaces studied by Tao Mei. The operator-valued local Hardy spaces are defined by the truncated Littlewood-Paley g-functions and the truncated Lusin square functions associated to the Poisson kernel. We develop the Calderón-Zygmund theory on hpc(Rd,M), and study the hpc-bmocq duality and the interpolation. Based on these results, we obtain general characterization of hpc(Rd,M) which states that the Poisson kernel can be replaced by any reasonable test function. This characterization plays an important role in the smooth atomic decomposition of h1c(Rd,M). We also investigate the operator-valued inhomogeneous Triebel-Lizorkin spaces Fpα,c(Rd,M). Like in the classical case, these spaces are connected with the operator-valued local Hardy spaces via Bessel potentials. Then by the aid of the Calderón-Zygmund theory, we obtain the Littlewood-Paley type and the Lusin type characterizations of Fpα,c(Rd,M) by more general kernels. These characterizations allow us to study various properties of Fpα,c(Rd,M), in particular, the smooth atomic decomposition. This is an extension and an improvement of the previous atomic decomposition of h1c(Rd,M). As an important application of this smooth atomic decomposition, we show the boundedness of pseudo-differential operators with regular operator-valued symbols on Triebel-Lizorkin spaces Fpα,c(Rd,M), for α ∈ R and 1 ≤ p ≤ ∞. Finally, by virtue of transference, we obtain the Fpα,c-boundedness of pseudo-differential operators on quantum tori

Le théorème de l'indice d'Atiyah et Singer, démontré en 1963, est un résultat qui a permis de relier des thématiques mathématiques variées, allant des équations aux dérivées partielles a la topologie et la géométrie différentielle. Plus précisément, il fait le lien entre la dimension de l'espace des solutions d'une équation aux dérivées partielles elliptique et des invariants topologiques du type (co)homologie, et a des applications importantes, regroupant plusieurs théorèmes majeurs venant de divers domaines (géométrie algébrique, topologie différentielle, analyse fonctionnelle). D'un autre cote, les fonctions zêta associées à des opérateurs pseudo différentiels sur une variété riemannienne close contiennent dans leurs propriétés analytiques des informations intéressantes. On peut par exemple retrouver dans les résidus le théorème de Weyl sur l asymptotique du nombre de valeurs propres d'un laplacien, et en particulier le volume de la variété. En se plaçant dans le cadre de la géométrie différentielle non commutative développée par Connes, on peut pousser cette idée plus loin. Plus précisément, on peut obtenir, en combinant des techniques de renormalisation zêta avec la propriété d'excision en cohomologie cyclique, des théorèmes d'indice dans l'esprit de celui d'Atiyah-Singer. L'intérêt de ce point de vue réside dans sa généralisation possible à des situations géométriques plus délicates. La présente thèse établit des résultats dans cette direction / The index theorem of Atiyah and Singer, discovered in 1963, is a striking result which relates many different fields in mathematics going from the analysis of partial differential equations to differential topology and geometry. To be more precise, this theorem relates the dimension of the space of some elliptic partial differential equations and topological invariants coming from (co)homology theories, and has important applications. Many major results from different fields (algebraic topology, differential topology, functional analysis) may be seen as corollaries of this result, or obtained from techniques developed in the framework of index theory. On another side, zeta functions associated to pseudodifferential operators on a closed Riemannian manifold contain in their analytic properties many interesting informations. For instance, the Weyl theorem on the asymptotic number of eigenvalues of a Laplacian may be recovered within the residues of the zeta function. This gives in particular the volume of the manifold, which is a geometric data. Using the framework of noncommutative geometry developed by Connes, this idea may be pushed further, yielding index theorems in the spirit of the one of Atiyah Singer. The interest in this viewpoint is to be suitable for more delicate geometrical situations. The present thesis establishes results in this direction

Wir behandeln nichtkommutative Algebren über Ringen und auf algebraischen Varietäten. Im ersten Teil beschreiben wir ein Kriterium, das angibt, ob und wie weit sich eine gegebene Azumaya-Algebra über dem Funktionenkörper einer algebraischen Varietät als Garbe von Azumaya-Algebren auf die Varietät ausdehnen lässt. Außerdem untersuchen wir die lokale Struktur von Azumaya-Algebren oder allgemeiner von Maximalordnungen, die mit Hilfe des Cyclic-Covering-Tricks von Chan konstruiert werden. Mit dieser Methode lassen sich Maximalordnungen auf algebraischen Flächen konstruieren, die zudem genau über einer gewählten Kurve verzweigen. Im zweiten Teil betrachten wir die nichtassoziativen Oktavenalgebren und allgemeiner auch Kompositionsalgebren über Ringen. Dabei übertragen wir die bekannten Aussagen von Kompositionsalgebren über Körpern auf die Situation von Algebren über Ringen. Wir untersuchen Oktavenalgebren und Maximalordnungen über diskreten Bewertungsringen und verallgemeinern ein Resultat von van der Blij und Springer über die lokale Natur von Maximalordnungen über den rationalen Zahlen und über algebraischen Zahlkörpern auf den Fall von beliebigen noetherschen, ganzabgeschlossenen Integritätsbereichen. Abschließend führen wir eine Definition von Garben von Oktavenalgebren und Garben von Maximalordnungen in Oktavenalgebren über algebraischen Varietäten ein.

Submitted by Renata Lopes (renatasil82@gmail.com) on 2016-12-22T13:25:11Z No. of bitstreams: 1 vahidnikoofard.pdf: 794368 bytes, checksum: 26feb8d15d2757f79f8d7dfb69b610c2 (MD5) / Approved for entry into archive by Diamantino Mayra (mayra.diamantino@ufjf.edu.br) on 2017-01-31T10:20:21Z (GMT) No. of bitstreams: 1 vahidnikoofard.pdf: 794368 bytes, checksum: 26feb8d15d2757f79f8d7dfb69b610c2 (MD5) / Made available in DSpace on 2017-01-31T10:20:21Z (GMT). No. of bitstreams: 1 vahidnikoofard.pdf: 794368 bytes, checksum: 26feb8d15d2757f79f8d7dfb69b610c2 (MD5) Previous issue date: 2015-06-30 / CAPES - Coordenação de Aperfeiçoamento de Pessoal de Nível Superior / Esta tese é composta por assuntos distintos entre si de teorias quânticas de campos onde alguns deles são descritos em espaços não-comutativos (NC). Em primeiro lugar, analisamos a dinâmica de uma partícula livre sobre uma 2-esfera e através da dinâmica das suas equações de movimento, obtivemos as perturbações NCs neste espaço de fase. Este modelo sugere uma origem para o Zitterbewegung do elétron. Depois disso, consideramos umaversãoNCdasegundaleideNewtonparaestemodelo, quefoiobtidocomestecenário geométrico aplicado a este modelo. Em seguida, discutimos um formalismo alternativo relacionado à não-comutatividade chamado DFR onde o parâmetro NC é considerado uma coordenada e demonstramos exatamente que ela tem obrigatoriamente um momento conjugado neste espaço de fase DFR, diferentemente do que alguns autores da atual literatura sobre DFR afirmam. No próximo assunto, usando o formalismo de solda que, em poucaspalavras,colocapartículascomquiralidadesopostasnomesmomultipleto,soldamos algumas versões NCs de modelos bem conhecidos como modelos de Schwinger quirais e modelos (anti) auto duais no espaço-tempo de Minkowski estendido. Em outro assunto estudado aqui, também construímos a versão NC do modelo de Jackiw-Pi com um grupo de calibre arbitrário e usamos o mapeamento bem conhecido de Seiberg-Witten para obter este modelo NC em termos de variáveis comutativos. Finalmente, utilizamos o formalismo de campos e anticampos (ou método BV) para construir a ação de Batalin-Vilkovisky (BV) do modelo Jackiw-Pi estendido e após o prEntendiocedimento de fixação de calibre chegamos a uma ação completa, pronta para quantização. / This thesis is composed of distinct aspects of quantum field theories where some of them are described in noncommutative (NC) spaces. Firstly, we have analyzed the dynamics of a free particle over a 2-sphere and through the dynamics of the equations of motion we have derived its NC perturbations in the phase-space. This model suggests an origin for Zitterbewegung feature of the electron. After that we have considered the NC version of Newton’s second law for this model, which was obtained with the geometricalscenarioappliedtothismodel. Thenwehavediscussedtheso-calledDoplicher– Fredenhagen–Roberts (DFR) alternative formalism concerning noncommutativity where the NC parameter has a coordinate role and we showed exactly that it has a conjugated momentum in the DFR phase-space, differently of what some authors of the current DFR-literature claims. In the next issue, using the soldering formalism which, in few words, put opposite chiral particles in the same multiplet, we have soldered some NC versions of well known models like the chiral Schwinger model and (anti)self dual models in the extended Minkowski spacetime. Changing the subject, we have constructed the NC spacetime version of Jackiw-Pi model with an arbitrary gauge group and we used the well known Seiberg-Witten map to obtain the NC model expressed in terms of commutative variables. Finally, we have used the field-antifield (or BV method) formalism to construct the Batalin-Vilkovisky (BV) action of the extended Jackiw-Pi model and after the gauge fixing procedure we have arrived at a quantized-ready action for this model.