The standard model of particle physics can excellently describe the vast majorityof data of particle physics experiments. However, in its simplest form, it cannot account for the fact that the neutrinos are massive particles and lepton flavorsmixed, as required by the observation of neutrino oscillations. Hence, the standardmodel must be extended in order to account for these observations, opening up thepossibility to explore new and interesting physical phenomena. There are numerous models proposed to accommodate massive neutrinos. Thesimplest of these are able to describe the observations using only a small numberof effective parameters. Furthermore, neutrinos are the only known existing particleswhich have the potential of being their own antiparticles, a possibility that isactively being investigated through experiments on neutrinoless double beta decay.In this thesis, we analyse these simple models using Bayesian inference and constraintsfrom neutrino-related experiments, and we also investigate the potential offuture experiments on neutrinoless double beta decay to probe other kinds of newphysics. In addition, more elaborate theoretical models of neutrino masses have beenproposed, with the seesaw models being a particularly popular group of models inwhich new heavy particles generate neutrino masses. We study low-scale seesawmodels, in particular the resulting energy-scale dependence of the neutrino parameters,which incorporate new particles with masses within the reach of current andfuture experiments, such as the LHC. / Standardmodellen för partikelfysik beskriver den stora majoriteten data från partikelfysikexperimentutmärkt. Den kan emellertid inte i sin enklaste form beskrivadet faktum att neutriner är massiva partiklar och leptonsmakerna är blandande,vilket krävs enligt observationerna av neutrinooscillationer. Därför måste standardmodellenutökas för att ta hänsyn till detta, vilket öppnar upp möjligheten att utforska nya och intressanta fysikaliska fenomen. Det finns många föreslagna modeller för massiva neutriner. De enklaste av dessakan beskriva observationerna med endast ett fåtal effektiva parametrar. Dessutom är neutriner de enda kända befintliga partiklar som har potentialen att vara sinaegna antipartiklar, en möjlighet som aktivt undersöks genom experiment på neutrinolöst dubbelt betasönderfall. I denna avhandling analyserar vi dessa enkla modellermed Bayesisk inferens och begränsningar från neutrinorelaterade experiment och undersöker även potentialen för framtida experiment på neutrinolöst dubbelt betasönderfall att bergänsa andra typer av ny fysik. Även mer avancerade teoretiska modeller för neutrinomassor har föreslagits, med seesawmodeller som en särskilt populär grupp av modeller där nya tunga partiklargenererar neutrinomassor. Vi studerar seesawmodeller vid låga energier, i synnerhetneutrinoparametrarnas resulterande energiberoende, vilka inkluderar nya partiklarmed massor inom räckh°all för nuvarande och framtida experiment såsom LHC. / <p>QC 20130830</p>

[pt] Atualmente podemos determinar com grande precisão os parâmetros das massas e misturas dos neutrinos. Porém, mesmo que no futuro as incertezas sobres as medidas destes parâmetros sejam reduzidas considerablemente, talvez algumas questões ainda continuem em aberto, como por exemplo, o valor absoluto da massa dos neutrinos, a hierarquia de massa e também determinar se os neutrinos são de Majorana ou Dirac, e se forem de Majorana, então quais seriam os valores das fases de CP? Nesta tese, nós abordamos parte destas questões estudando a detetabilidade da fase CP de Majorana através das medidas de massa dos neutrinos, que são extraídas de experimentos de decaimento beta, duplo decaimento beta sem neutrinos e observações cosmológicas. Para quantificar a sensibilidade dos experimentos à fase de Majorana, além de usar os gráficos convencionais das regiões permitidas, usamos a função de exclusão, definida como uma fração no espaço de parâmentros CP, que é excluída quando um conjunto de parâmetros de entrada é fornecido. A sensibilidade dos experimentos é considerada quando variamos as incertezas desde o valor mais pessimista até o valor mais optimista e também incluímos o erro experimental devido à matriz de elementos nucleares. Com esta análise, encontramos que a fase de Majorana, denotada como a21, pode ser restringida ao ser excluído o espaço de parâmentros entre um 10 por cento e até 50 por cento, com um nível de confiança de 3o, isto se consideramos que a massa do neutino mais leve é 0.1eV. Também são tratados aspectos característicos da sensibilidade à fase a21, como por exemplo, a dependência à outra fase de Majorana a31. Para finalizar, nós estudamos o caso de se na atualidade, a incerteza do elemento de matriz nuclear pode ser limitado usando as medidas dos mesmos experimentos. / [en] Nowdays we are in a precision epoch where is possible to get accurately the parameters that involve the neutrino physics, however, even that in the future the uncertainties on those parameters will decrease enormously, perhaps still will continue some open question, for instance, what is the absolute mass of neutrinos? What is the hierarchy of the masses? Are the neutrinos Majorana or Dirac? And if they were Majorana, what would be the value of the CP phases? In this work, we studying the detectability of the CP phase through experiments of neutrino beta decay, neutrinoless double beta decay and cosmology. In order to quantify the sensitivity to the Majorana phase we use the CP exlusion fraction, it is a fraction of region of the CP phase, that is excluded for a given set of assumed input parameters. The experiments sensitivity is account when it is varied since the pessimistic to optimistic one, assumptions of the experimental erros, the uncertainty of nuclear matrix elements and all the scenarios are considering with the Normal and Inverted hierarchies. We find that a Majorana phase, the called a21 can be constrained strongly by excluded 10 − 50 per cent of phase space at 3o CL for the lowest neutrino mass of 0.1 eV. The characteristic features of the sensitivity to a21, such as dependences on the other phase a31 are addressed. We also arise the question of whether the uncertainties of nuclear matrix elements could be constrined be consistancy of such measurements.