O Modelo Padrão das partículas elementares descreve com sucesso as interações eletrofracas e fortes, mostrando-se consistente com os dados experimentais disponíveis. Entretanto, há diversas questões que não são respondidas pelo mesmo, entre elas, o problema da hierarquia de gauge e o problema associado à origem das massas dos férmions. Ambos podem ser solucionados de forma natural em teorias com uma dimensão extra curva. No entanto, essas teorias violam sabor em primeira ordem de teoria de perturbações e são não renormalizáveis. Nesta dissertação utilizamos técnicas de desconstrução dimensional para resolver os problemas da hierarquia de gauge e da hierarquia de massas dos férmions com mínima violação de sabor em um modelo puramente quadridimensional. / The Standard Model of elementary particles describes the electroweak and strong interactions, and its predictions have successfully matched existing experimental data. However, there are some issues that are not addressed by this model, such as the gauge hierarchy problem and the origin of fermion masses. Both problems can be solved naturally using Warped Extra Dimensions. On the other hand, these theories are flavor-violating in tree level and are non-renormalizable. In this dissertation we apply dimensional deconstruction techniques to solve the gauge hierarchy problem and the fermion masses hierarchy problem achieving minimal flavor violation in a purely four-dimensional model

O Modelo Padrão das partículas elementares descreve com sucesso as interações eletrofracas e fortes, mostrando-se consistente com os dados experimentais disponíveis. Entretanto, há diversas questões que não são respondidas pelo mesmo, entre elas, o problema da hierarquia de gauge e o problema associado à origem das massas dos férmions. Ambos podem ser solucionados de forma natural em teorias com uma dimensão extra curva. No entanto, essas teorias violam sabor em primeira ordem de teoria de perturbações e são não renormalizáveis. Nesta dissertação utilizamos técnicas de desconstrução dimensional para resolver os problemas da hierarquia de gauge e da hierarquia de massas dos férmions com mínima violação de sabor em um modelo puramente quadridimensional. / The Standard Model of elementary particles describes the electroweak and strong interactions, and its predictions have successfully matched existing experimental data. However, there are some issues that are not addressed by this model, such as the gauge hierarchy problem and the origin of fermion masses. Both problems can be solved naturally using Warped Extra Dimensions. On the other hand, these theories are flavor-violating in tree level and are non-renormalizable. In this dissertation we apply dimensional deconstruction techniques to solve the gauge hierarchy problem and the fermion masses hierarchy problem achieving minimal flavor violation in a purely four-dimensional model

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Enquanto todos os modelos com neutrinos massivos de Majorana levam ao mesmo operador efetivo de dimensão d = 5, que não conserva número leptônico, os operadores de dimensão d = 6, obtidos a baixas energias, conservam número leptônico e são diferentes dependendo do modelo de alta energia da nova física. Derivamos os operadores de dimensão d = 6 que são característicos de modelos Seesaw genéricos, no qual a massa do neutrino resulta do intercâmbio de campos pesados que podem ser tanto singletos fermiônicos, tripletos fermiônicos ou tripletos escalares. Os operadores resultantes podem conduzir a efeitos observáveis no futuro próximo, se os coeficientes dos operadores de dimensão d = 5 e d = 6 são desacoplados. Neste trabalho apresentamos o modelo violação mínima de sabor no contexto do modelo seesaw tipo III, no qual é possível obter tal desacoplamento. Isto permite reconstruir a estrutura de sabor a partir dos valores das massas dos neutrino leves e dos parâmetros de mistura, mesmo na presença de fases de violação CP. / While all models of Majorana neutrino masses lead to the same dimension five effective operator, which does not conserve lepton number, the dimension six operators induced at low energies conserve lepton number and differ depending on the high energy model of new physics. We derive the low-energy dimension six operators which are characteristic of generic Seesaw models, in which neutrino masses result from the exchange of heavy fields which may be either fermionic singlets, fermionic triplets or scalar triplets. The resulting operators may lead to effects observable in the near future, if the coefficients of the dimension five and six operators are decoupled. In this work we present the model of minimal avor violation in the context of the type III seesaw model, in which it is possible to obtain the decoupling mentioned before. This allows to reconstruct the avour structure of the model from the values of the light neutrino masses and mixing parameters, even in the presence of CP-violating phases.

La désintégration $B_{ (s)}$ → τμ est supprimée dans le SM, où le nombre leptonique est conservé. Son observation serait donc une preuve non ambiguë de la physique au-delà du SM. Des résultats récents [1,2] ont ravivé l'intérêt pour la recherche de tels processus [3]. Cette thèse présente la recherche des désintégrations $B_{ (s)}$→ τμ dans l'expérience LHCb, l'une des 4 grandes expériences menées au Large Hadron Collider (LHC) du CERN.Le lepton τ se désintègre avant d'atteindre le détecteur LHCb et est reconstruit en utilisant le canal τ → πππν. Le neutrino provenant de la désintégration du τ échappe à la détection. Une technique de reconstruction spécifique est utilisée pour déduire l'énergie du neutrino et donc la masse invariante du méson B qui s'est désintégré.Afin de séparer le signal du bruit de fond, une sélection hors ligne composée de différentes étapes est appliquée. Des techniques d'analyse multivariées, telles que les arbres de décision boostés (BDT), sont utilisées pendant le processus de sélection.La stratégie d'analyse est complétée par un ajustement simultané à la distribution de masse invariante des mésons B dans différentes régions d'un BDT final. Selon les prédictions du SM, aucun événement de signal n'est attendu. Dans ce cas, la méthode CLs sera utilisée pour extraire les limites supérieures des rapports de branchement BR($B_{ (s)}$→ τμ).[1] Test of lepton universality using $B^+$→$K^+$$l ^+$$l ^-$ decaysPhys. Rev. Lett. 113, 151601 (2014)[2] Measurement of the ratio of branching fractions BR(B → D*τ ν)/BR(B → D*μν)Phys. Rev. Lett. 115 (2015) 111803[3] Lepton Flavour Violation in B Decays ? Phys. Rev. Lett. 114, 091801 (2015) / The decay $B_{ (s)}$→τμ is suppressed in the SM, in which lepton flavour is conserved. Its observation would therefore be an unambiguous evidence of physics beyond the SM. Recent results [1,2] revived the interest for the search of such processes [3]. This thesis presents the search for the $B_{ (s)}$→τμ decays within the LHCb experiment, one of the 4 large experiments operated at the CERN Large Hadron Collider (LHC).The τ lepton decays before reaching the LHCb detector and is reconstructed using the τ→πππν channel. The neutrino from the τ decay escapes detection. A specific reconstruction technique is used in order to infer the energy of the ν and thus the invariant mass of the decaying B meson. This way, the complete kinematics of the process can be solved up to a two fold ambiguity.In order to disentangle signal from background, an offline selection consisting of different steps is applied. Data driven and multivariate analysis techniques, such as Boosted Decision Trees (BDT), are used during the selection process. The analysis strategy is completed by a simultaneous fit to the B meson invariant mass distribution over the different bins of a final BDT. According to the SM expectations, no signal events should be observed. In this case, the CLs method will be used to extract the upper limits on the branching fractions.[1] Test of lepton universality using $B^+$→$K^+$$l ^+$$l ^-$ decaysPhys. Rev. Lett. 113, 151601 (2014)[2] Measurement of the ratio of branching fractions BR(B → D*τ ν)/BR(B → D*μν)Phys. Rev. Lett. 115 (2015) 111803[3] Lepton Flavour Violation in B Decays ? Phys. Rev. Lett. 114, 091801 (2015)

Enquanto todos os modelos com neutrinos massivos de Majorana levam ao mesmo operador efetivo de dimensão d = 5, que não conserva número leptônico, os operadores de dimensão d = 6, obtidos a baixas energias, conservam número leptônico e são diferentes dependendo do modelo de alta energia da nova física. Derivamos os operadores de dimensão d = 6 que são característicos de modelos Seesaw genéricos, no qual a massa do neutrino resulta do intercâmbio de campos pesados que podem ser tanto singletos fermiônicos, tripletos fermiônicos ou tripletos escalares. Os operadores resultantes podem conduzir a efeitos observáveis no futuro próximo, se os coeficientes dos operadores de dimensão d = 5 e d = 6 são desacoplados. Neste trabalho apresentamos o modelo violação mínima de sabor no contexto do modelo seesaw tipo III, no qual é possível obter tal desacoplamento. Isto permite reconstruir a estrutura de sabor a partir dos valores das massas dos neutrino leves e dos parâmetros de mistura, mesmo na presença de fases de violação CP. / While all models of Majorana neutrino masses lead to the same dimension five effective operator, which does not conserve lepton number, the dimension six operators induced at low energies conserve lepton number and differ depending on the high energy model of new physics. We derive the low-energy dimension six operators which are characteristic of generic Seesaw models, in which neutrino masses result from the exchange of heavy fields which may be either fermionic singlets, fermionic triplets or scalar triplets. The resulting operators may lead to effects observable in the near future, if the coefficients of the dimension five and six operators are decoupled. In this work we present the model of minimal avor violation in the context of the type III seesaw model, in which it is possible to obtain the decoupling mentioned before. This allows to reconstruct the avour structure of the model from the values of the light neutrino masses and mixing parameters, even in the presence of CP-violating phases.

It is widely believed that the Standard Model (SM) can not be a fundamental theory of the basic interactions. Originated from this fact, many new physics models have been proposed. Among them, the two Higgs doublet model (2HDM), the SM enlarged by adding one extra scalar doublet, is considered as the simplest extension of the SM. In this work, within the framework of the model III version of the 2HDM, the exclusive decay the branching ratio is calculated and discussed in various physical regions determined by model parameters. It is observed that it is possible to reach present experimental upper limits in model Finally, the avor changing top quark decay,

The lepton flavor violating interactions are interesting in the sense that they are sensitive the physics beyond the standard model and they ensure considerable information about the restrictions of the free parameters, with the help of the possible accurate measurements. In this work, we investigate the lepton flavor violating H+ ! W+l and the lepton flavor conserving H+ ! W+l decays in the general two Higgs doublet model and we estimate decay widths of these decays. After that, we analyze lepton flavor violating decay ! i in the same model and calculate its branching ratio. We observe that the experimental results of the processes under consideration can give comprehensive information about the physics beyond the standard model and the existing free parameters.

The lepton flavor violating interactions are worthwhile to examine since they are sensitive to physics beyond the Standard Model. The simplest extension of the Standard Model promoting the lepton flavor violating interactions are the so called two Higgs doublet model which contains an additional Higgs doublet carrying the same quantum numbers as the first one. In this model, the lepton flavor violating interactions are induced by new scalar Higgs bosons, scalar h^0 and pseudo scalar A^0, and Yukawa couplings, appearing as free parameters, are determined by using the experimental data. On the other hand, the possible extra dimensions are interesting in the sense that they ensure a solution to the hierarchy and cosmological constant problems and also result in the enhancement in the physical quantities of various processes. In the present work, we predict the branching ratios of lepton flavor violating radion decays r-&gt / e^+- mu^-+, r-&gt / e^+- tau^-+ and r-&gt / mu^+- tau^-+ in the two Higgs doublet model, including a single extra dimension, in the framework of the Randall Sundrum scenario. We observed that the branching ratios of the processes we study are at most at the order of 10^-8 for the small values of radion mass and it decreases with the increasing values of the radion mass. Among the LFV decays we study, the r-&gt / mu^+- tau^-+ decay would be the most suitable one to measure its branching ratio.

<p>The ability of the Mu2e experiment to probe, or discover BSM physics in direct CLFV μ+ and π+ decay modes is estimated.</p>