The XX century witnessed the quantum and relativistic revolutions in physics. The development of these two theories, namely, Quantum Mechanics and Relativity, was the inception of many crucial discoveries and technological advances. Among them, one stands out due to its uniqueness, the neutrino discovery. However, several neutrino properties are still obscure. Neutrinos are the only fundamental particles whose nature is currently unknown. Such fermions can either be different from their antiparticles, i.e., Dirac fermions, or be their own antiparticles, that is, Majorana fermions. On the other hand, the smallness of neutrino masses is a problem seemingly related to the neutrino nature; thus, as essential task consists in addressing the phenomenologically viable models in both cases. Furthermore, it is important to search for other physical process in which the neutrino nature may manifest through different experimental signatures. A rather difficult but promising method corresponds to the detection of the cosmic neutrino background, viz. neutrinos which are relics from the Big Bang. Previous works have shown that detection rates for Dirac and Majorana neutrinos can give different results. Nevertheless, this distinction was obtained considering the Standard Model framework only. Therefore, it is important to understand the consequences of having Non-Standard Interactions contributing to the detection of neutrinos from the cosmic background. Another remarkable relic predicted by Cosmology is the unidentified Dark Matter, composing ~25% of the Universe. All searches regarding the Weakly Interacting Massive Particle, one of the principal candidates for Dark Matter, have given negative results; this has compelled experiments to increase their sensitivity. Notwithstanding, neutrinos may stand in the way of such experimental searches given that they may constitute an irreducible background. In this thesis, we will address these three different phenomena, neutrino mass models, detection of the cosmic neutrino background and the neutrino background in Dark Matter searches, by considering the different characteristics in each case. In the study of neutrino mass models, we will consider models for both Majorana and Dirac neutrinos; specifically, we will probe the neutrinophilic two-Higgs-doublet model. Regarding the detection of relic neutrinos, we will analyse the consequences of the existence of the beyond Standard Model physics in the capture rate by tritium. Finally, we will scrutinize the impact of neutrinos in Direct Detection WIMP searches, by considering Standard Model plus additional interactions in the form of simplified models. / Ao longo do século XX testemunhamos as revoluções quântica e relativista que aconteceram na Física. O desenvolvimento da Mecânica quântica e da teoria da relatividade foi o prelúdio de inúmeras descobertas e avanços tecnológicos fundamentais; em particular, a descoberta dos neutrinos. No entanto, a sua total compreensão ainda é um mistério para a física de partículas. Entendidos como partículas fermiônicas fundamentais, os neutrinos possuem sua natureza desconhecida. Podendo ser diferentes de suas antipartículas, denominadas férmions de Dirac, ou também podendo ser as suas próprias antipartícula, sendo conhecidas como férmions de Majorana. Por outro lado, o valor de sua massa continua sendo um problema em aberto, supostamente relacionado à sua natureza. Portanto, é importante estudarmos modelos fenomenológicos viáveis para as duas naturezas possíves dos neutrinos. Além disso, é necessário procurar outros processos físicos cujos resultados experimentais sejam distintos de acordo com a natureza do neutrino. Um método bastante difícil, mas promissor, corresponde à detecção do fundo de neutrinos cósmicos, isto é, os neutrinos relíquia do Big Bang. Análises prévias mostraram que as taxas de detecção para neutrinos de Dirac e de Majorana resultam em valores distintos. Porém, este resultado foi obtido supondo como base o Modelo Padrão; assim, é crucial entender as possíveis consequências da existência de interações desconhecidas na detecção dos neutrinos da radiação cósmica de fundo. Outra relíquia notável prevista pela Cosmologia é a desconhecida Matéria Escura, que compõe ~25% do Universo. Todas as buscas por WIMPs (do inglês Weakly Interactive Massive Particles), um dos principais candidatos a Matéria Escura, tem dado resultados negativos. Isto tem forçado a criação de experimentos cada vez mais sensíveis. Contudo, os neutrinos poderão ser um obstáculo nessas buscas experimentais, pois estes convertir-se-ão em um fundo irredutível. Na presente tese, abordaremos estes três fenômenos diferentes, modelos de massa para os neutrinos, a detecção do fundo de neutrinos cósmicos e o fundo de neutrinos em experimentos de detecção direta de Matéria Escura, considerando as distintas características em cada caso. No estudo dos modelos de massa para os neutrinos consideraremos modelos para neutrinos de Majorana e Dirac; exploraremos modelos neutrinofílicos com dois dubletos de Higgs. Enquanto à detecção dos neutrinos relíquia, analisaremos as consequências da presença de física além do Modelo Padrão na taxa de captura pelo trítio. Finalmente, examinaremos o impacto dos neutrinos em experimentos de detecção direta de WIMPs, supondo as interações do Modelo Padrão junto com interações adicionais na forma de modelos simplificados.

Neutrino telescopes such as IceCube monitor for low-energy neutrinos O(10 MeV) produced in nuclear processes during core-collapse in supernovae. The detection horizon to the neutrino burst is 50 kpc, the distance to the Magellanic Clouds. However, this limits the number of supernovae accessible through low-energy neutrino detection, as the Galactic rate is only <img src="http://www.diva-portal.org/cgi-bin/mimetex.cgi?%5Csim" data-classname="equation" data-title="" />2 per century. Some models predict the production of high-energy O(&gt;GeV) neutrinos through acceleration mechanisms, such as the ejecta colliding with the circumstellar material or relativistic jets in the stellar envelope. This thesis examines how these high-energy neutrinos could be exploited with neutrino telescopes like IceCube to extend the detection horizon to core-collapse supernovae past the Magellanic clouds. To examine the detection horizon for IceCube, we use two data samples, one utilizing muon tracks which provide good sensitivity in the northern sky, and the other all flavor starting events, which provide good sensitivity in the southern sky. We demonstrate that extending the reach past 50 kpc and well into the 10s of Mpc is possible, where the expected rate is more than two core-collapse supernovae per year.

The IceCube Neutrino Observatory has sensitivity to MeV electron antineutrinos from core-collapse supernovae through an excess of the detection rate over the background. Wavelength-shifting sensors have the potential to greatly increase photon collection making it a promising candidate for improving the measurement of the supernova neutrino light curve in IceCube-Gen2. For high-energy neutrino reconstruction, the competing effect of increased photon collection and the broader time distribution necessitate detailed simulations to determine the impact. In this thesis, we investigate the sensitivity gain caused by wavelength shifters in a future IceCube-Gen2 detector regarding the detection of faint modulations of the supernova neutrino lightcurve. Furthermore, we lay the groundwork for a future high-energy reconstruction through the implementation and integration of wavelength-shifting sensors into the IceCube simulation framework.

The search for the neutrinoless double beta (0nbb) decay is one of the most active fields in modern particle physics. This process is not allowed within the Standard Model and its observation would imply lepton number violation and would lead to the Majorana nature of neutrinos. The experimentally observed quantity is the half-life of the decay, which can be connected to the effective Majorana neutrino mass via nuclear matrix elements. The latter can only be determined theoretically and are currently affected by large uncertainties. To reduce these uncertainties one can investigate the well established two-neutrino double beta (2nbb) decay into the ground and excited states of the daughter isotope. These similar processes are allowed within the Standard Model. In this dissertation, the search for 2nbb decays into excited states is performed in Pd-110, Pd-102 and Ge-76. Three gamma spectroscopy setups at the Felsenkeller (Germany), HADES (Belgium) and LNGS (Italy) underground laboratories are used to search for the transitions in Pd-110 and Pd-102. No signal is observed leading to lower half-live bounds (90% C.I.) of 2.9e20 yr, 3.9e20 yr and 2.9e20 yr for the 0/2nbb 2p1, 0p1 and 2p2 transitions in Pd-110 and 7.9e18 yr, 9.2e18 yr and 1.5e19 yr for the 0/2nbb 2p1, 0p1 and 2p2 transitions in Pd-102, respectively. This is a factor of 1.3 to 3 improvement compared to previous limits. The data of Phase I (Nov 2011 - May 2013) of the 0nbb decay experiment GERDA at LNGS is used to search for excited state transitions in Ge-76. The analysis is based on coincidences between two detectors and finds no signal. Lower half-life limits (90 % C.L.) of 1.6e23 yr, 3.7e23 yr and 2.3e23 yr are obtained for the 2nbb 2p1, 0p1 and 2p2 transitions, respectively. These limits are more than two orders of magnitude larger than previous ones and could exclude many old matrix element calculations. In addition to the excited state searches, important measurements and improvements for GERDA Phase II upgrades are performed within this dissertation. 30 new BEGe detectors are characterized for their surface and active volume properties which is an essential ingredient for all future physics analyses in GERDA. These precision measurements reduce the systematic uncertainty of the active volume to a subdominant level. In extension to this, a new model for simulating pulse shapes of n+ electrode surface events is developed. With this model it is demonstrated that the dominant background of K-42 on the detector surfaces can be suppressed by a factor of 145 with an A/E pulse shape cut in Phase II. A further suppression of background is obtained by a liquid argon scintillation light veto. With newly developed Monte Carlo simulations, including the optical scintillation photons, it is demonstrated that Tl-208 in the detectors holders can be suppressed by a factor of 134. K-42 homogeneously distributed in the LAr can be suppressed with this veto in combination with pulse shape cuts by a factor of 170 for BEGe detectors. The characterization measurements and the developed simulation tools presented within this dissertation will help to enhance the sensitivity for all 0/2nbb decay modes and will allow to construct an improved background model in GERDA Phase II. / Die Suche nach dem neutrinolosen Doppelbetazerfall (0nbb) ist eines der aktivsten Felder der modernen Teilchenphysik. Der Zerfall setzt die Verletzung der Leptonenzahl voraus und hätte die Majorananatur des Neutrinos zur Folge. Die durch eine Beobachtung bestimmbare Halbwertszeit des Zerfalls ermöglicht, über ein nukleares Matrixelement, Zugang zur effektiven Majorananeutrinomasse. Die größten Unsicherheiten gehen dabei auf das Matrixelement zurück, welches nur durch verschiedene, teilweise stark voneinander abweichende theoretische Modelle zugänglich ist. Eine Möglichkeit diese Unsicherheiten zu reduzieren bieten genaue Studien des im Standardmodel erlaubten neutrinobegleiteten Doppelbetazerfalls (2nbb) in angeregte Zustände des Tochterkerns. In dieser Dissertation wird der 2nbb-Zerfall der Nuklide Pd-110, Pd-102 und Ge-76 in angeregte Zustände untersucht. Die Untersuchungen von Pd-110 und Pd-102 wurden in drei umfangreichen Gammaspektroskopie-Experimenten in den Untergrundlaboren Felsenkeller (Deutschland), HADES (Belgien) und LNGS (Italien) durchgefürt. Es wurde kein Signal beobachtet und damit die weltweit besten unteren Grenzen für die Halbwertszeit dieser Zerfälle festgesetzt: 2,9e20 yr, 3,9e20 yr und 2,9e20 yr für die 0/2nbb 2p1, 0p1 und 2p2 Übergänge in Pd-110 and 7,9e18 yr, 9,2e18 yr und 1,5e19 yr für die 0/2nbb 2p1, 0p1 und 2p2 Übergänge in Pd-102 (90% C.I.). Dies ist eine 1,3 bis 3-fache Verbesserung gegenüber den vorher bekannten Grenzen. Die Untersuchung des 2nbb-Zerfalls in Ge-76 basiert auf Daten aus Phase I (Nov. 2011 - Mai 2013) des 0nbb-Zerfall Experiments GERDA. Mit der auf koinzidenten Ereignissen basierten Analyse konnte kein Signal beobachtet werden und folgende untere Grenzen für die Halbwertszeit der 2nbb 2p1, 0p1 und 2p2 Übergänge wurden festgelegt: 1,6e23 yr, 3,7e23 yr und 2,3e23 (90% C.L.). Diese 100-fache Verbesserung gegenüber den bisher bekannten Grenzen widerlegt eine Vielzahl älterer, zur Verfügung stehender Matrixelemente. Zusätzlich wurden im Rahmen dieser Dissertation für die Erweiterungen des GERDA Experiments zur Phase II wichtige Messungen durchgeführt und Verbesserungen entwickelt. 30 neu produzierte BEGe Detektoren wurden hinsichtlich ihrer Oberflächeneigenschaften sowie ihrer aktiven Volumina charakterisiert. Diese Präzisisionsmessungen sind für alle zukünftigen Analysen in GERDA notwendig und erlauben die entsprechenden systematischen Unsicherheiten auf ein subdominantes Niveau zu reduzieren. Erweiternd wurde ein neues Model zur Beschreibung der n+ Elektrode entwickelt, welches erstmals erlaubt die Pulsform von Oberflächeninteraktionen zu simulieren. Mithilfe dieses Models konnte demonstriert werden, dass der in Oberflächeninteraktionen begründete und in GERDA dominante Messuntergrund von K-42 auf der Detektoroberfläche durch Pulsformanalyse um das 145-fache unterdrückt werden kann. Eine weitere Untergrundreduzierung wird durch ein Flüssigargon Szintillationsveto erreicht. Im Rahmen dieser Arbeit wurden vorhandene Monte Carlo Simulationen um den Transport von optischen Photonen erweitert und die 134-fache Unterdrückung des Tl-208 Untergrundes demonstriert. Die Ergebnisse dieser Arbeit helfen eine deutliche Sensitivitätsverbesserung für die zuküntige Suche nach dem 0/2nbb-Zerfall zu erzielen und erlauben die Erstellung eines präziseren Untergrundmodels in GERDA Phase II.

La mesure récente de l'angle de mélange theta-13, à laquelle l'expérience Double Chooz contribue, a ouvert la voie aux futures expériences de la physique des neutrinos. Dans ce manuscrit, la caractérisation de certains bruits de l'expérience sont décrits. Les muons cosmiques qui s'arrêtent et se désintègrent dans le détecteur sont mal reconstruits, résultant en distorsion de la distribution temporelle des signaux laquelle peut être utilisée pour identifier ce type de fond. Les neutrons rapides créés par spallation par les muons cosmiques produisent de nombreux protons de recul qui peuvent entraîner un décalage dans la distribution temporelle des signaux et ainsi être identifiés. Ces distributions temporelles ont aussi été utilisées pour identifier la formation de l'état d'orthopositronium en observant et en mesurant un délai entre l'ionisation du positron et l'annihilation de celui-ci, pouvant permettre une séparation positron-électron. / The measurement of the theta-13 mixing angle, to which the Double Chooz experiment contributed, paves the way to future findings in neutrino physics. In this manuscript, we describe the characterization of some Double Chooz backgrounds. Cosmic muons that stop and decay in the detector are characterized by anisotropic emission of the scintillation light, causing the vertex to be poorly reconstructed. The resulting pulse shape distortion can be used to tag and remove such background. Fast spallation neutrons producing multiple recoil protons may produce a similar distortion in the pulse shape and can also be tagged. Pulse shapes are also used to identify the formation of ortho-positronium. The tagging of such electron-positron bound state is made possible by the induced distortion in the pulse shape due to the delay in the positron annihilation, and can be used for an electron-positron separation.

The search for the neutrinoless double beta (0nbb) decay is one of the most active fields in modern particle physics. This process is not allowed within the Standard Model and its observation would imply lepton number violation and would lead to the Majorana nature of neutrinos. The experimentally observed quantity is the half-life of the decay, which can be connected to the effective Majorana neutrino mass via nuclear matrix elements. The latter can only be determined theoretically and are currently affected by large uncertainties. To reduce these uncertainties one can investigate the well established two-neutrino double beta (2nbb) decay into the ground and excited states of the daughter isotope. These similar processes are allowed within the Standard Model. In this dissertation, the search for 2nbb decays into excited states is performed in Pd-110, Pd-102 and Ge-76. Three gamma spectroscopy setups at the Felsenkeller (Germany), HADES (Belgium) and LNGS (Italy) underground laboratories are used to search for the transitions in Pd-110 and Pd-102. No signal is observed leading to lower half-live bounds (90% C.I.) of 2.9e20 yr, 3.9e20 yr and 2.9e20 yr for the 0/2nbb 2p1, 0p1 and 2p2 transitions in Pd-110 and 7.9e18 yr, 9.2e18 yr and 1.5e19 yr for the 0/2nbb 2p1, 0p1 and 2p2 transitions in Pd-102, respectively. This is a factor of 1.3 to 3 improvement compared to previous limits. The data of Phase I (Nov 2011 - May 2013) of the 0nbb decay experiment GERDA at LNGS is used to search for excited state transitions in Ge-76. The analysis is based on coincidences between two detectors and finds no signal. Lower half-life limits (90 % C.L.) of 1.6e23 yr, 3.7e23 yr and 2.3e23 yr are obtained for the 2nbb 2p1, 0p1 and 2p2 transitions, respectively. These limits are more than two orders of magnitude larger than previous ones and could exclude many old matrix element calculations. In addition to the excited state searches, important measurements and improvements for GERDA Phase II upgrades are performed within this dissertation. 30 new BEGe detectors are characterized for their surface and active volume properties which is an essential ingredient for all future physics analyses in GERDA. These precision measurements reduce the systematic uncertainty of the active volume to a subdominant level. In extension to this, a new model for simulating pulse shapes of n+ electrode surface events is developed. With this model it is demonstrated that the dominant background of K-42 on the detector surfaces can be suppressed by a factor of 145 with an A/E pulse shape cut in Phase II. A further suppression of background is obtained by a liquid argon scintillation light veto. With newly developed Monte Carlo simulations, including the optical scintillation photons, it is demonstrated that Tl-208 in the detectors holders can be suppressed by a factor of 134. K-42 homogeneously distributed in the LAr can be suppressed with this veto in combination with pulse shape cuts by a factor of 170 for BEGe detectors. The characterization measurements and the developed simulation tools presented within this dissertation will help to enhance the sensitivity for all 0/2nbb decay modes and will allow to construct an improved background model in GERDA Phase II. / Die Suche nach dem neutrinolosen Doppelbetazerfall (0nbb) ist eines der aktivsten Felder der modernen Teilchenphysik. Der Zerfall setzt die Verletzung der Leptonenzahl voraus und hätte die Majorananatur des Neutrinos zur Folge. Die durch eine Beobachtung bestimmbare Halbwertszeit des Zerfalls ermöglicht, über ein nukleares Matrixelement, Zugang zur effektiven Majorananeutrinomasse. Die größten Unsicherheiten gehen dabei auf das Matrixelement zurück, welches nur durch verschiedene, teilweise stark voneinander abweichende theoretische Modelle zugänglich ist. Eine Möglichkeit diese Unsicherheiten zu reduzieren bieten genaue Studien des im Standardmodel erlaubten neutrinobegleiteten Doppelbetazerfalls (2nbb) in angeregte Zustände des Tochterkerns. In dieser Dissertation wird der 2nbb-Zerfall der Nuklide Pd-110, Pd-102 und Ge-76 in angeregte Zustände untersucht. Die Untersuchungen von Pd-110 und Pd-102 wurden in drei umfangreichen Gammaspektroskopie-Experimenten in den Untergrundlaboren Felsenkeller (Deutschland), HADES (Belgien) und LNGS (Italien) durchgefürt. Es wurde kein Signal beobachtet und damit die weltweit besten unteren Grenzen für die Halbwertszeit dieser Zerfälle festgesetzt: 2,9e20 yr, 3,9e20 yr und 2,9e20 yr für die 0/2nbb 2p1, 0p1 und 2p2 Übergänge in Pd-110 and 7,9e18 yr, 9,2e18 yr und 1,5e19 yr für die 0/2nbb 2p1, 0p1 und 2p2 Übergänge in Pd-102 (90% C.I.). Dies ist eine 1,3 bis 3-fache Verbesserung gegenüber den vorher bekannten Grenzen. Die Untersuchung des 2nbb-Zerfalls in Ge-76 basiert auf Daten aus Phase I (Nov. 2011 - Mai 2013) des 0nbb-Zerfall Experiments GERDA. Mit der auf koinzidenten Ereignissen basierten Analyse konnte kein Signal beobachtet werden und folgende untere Grenzen für die Halbwertszeit der 2nbb 2p1, 0p1 und 2p2 Übergänge wurden festgelegt: 1,6e23 yr, 3,7e23 yr und 2,3e23 (90% C.L.). Diese 100-fache Verbesserung gegenüber den bisher bekannten Grenzen widerlegt eine Vielzahl älterer, zur Verfügung stehender Matrixelemente. Zusätzlich wurden im Rahmen dieser Dissertation für die Erweiterungen des GERDA Experiments zur Phase II wichtige Messungen durchgeführt und Verbesserungen entwickelt. 30 neu produzierte BEGe Detektoren wurden hinsichtlich ihrer Oberflächeneigenschaften sowie ihrer aktiven Volumina charakterisiert. Diese Präzisisionsmessungen sind für alle zukünftigen Analysen in GERDA notwendig und erlauben die entsprechenden systematischen Unsicherheiten auf ein subdominantes Niveau zu reduzieren. Erweiternd wurde ein neues Model zur Beschreibung der n+ Elektrode entwickelt, welches erstmals erlaubt die Pulsform von Oberflächeninteraktionen zu simulieren. Mithilfe dieses Models konnte demonstriert werden, dass der in Oberflächeninteraktionen begründete und in GERDA dominante Messuntergrund von K-42 auf der Detektoroberfläche durch Pulsformanalyse um das 145-fache unterdrückt werden kann. Eine weitere Untergrundreduzierung wird durch ein Flüssigargon Szintillationsveto erreicht. Im Rahmen dieser Arbeit wurden vorhandene Monte Carlo Simulationen um den Transport von optischen Photonen erweitert und die 134-fache Unterdrückung des Tl-208 Untergrundes demonstriert. Die Ergebnisse dieser Arbeit helfen eine deutliche Sensitivitätsverbesserung für die zuküntige Suche nach dem 0/2nbb-Zerfall zu erzielen und erlauben die Erstellung eines präziseren Untergrundmodels in GERDA Phase II.

The vast majority of all experimental results in particle physics can be described by the Standard Model (SM) of particle physics. However, neither the existence of neutrino masses nor the mixing in the leptonic sector, which have been observed, can be described within this model. In fact, the model only describes a fraction of the known energy in the Universe. Thus, we know there must exist a theory beyond the SM. There is a plethora of possible candidates for such a model, such as supersymmetry, extra dimensional theories, and string theory. So far, there are no evidence in favor of these models. These theories often reside at high energies, and will therefore be manifest as effective theories at the low energies experienced here on Earth. A first example in extra-dimensional theories. From our four-dimensional point of view, particles which propagate through the extra dimensions will effectivel be perceived as towers of heavy particles. In this thesis we consider an extra-dimensional model with universal extra dimensions, where all SM particles are allowed to propagate through the extra dimensions. Especially, we place a bound on the range of validity for this model. We study the renormalization group running of the leptonic parameters as well as the Higgs self-coupling in this model with the neutrino masses generated by a Weinberg operator. Grand unified theories, where the gauge couplings of the SM are unified into a single oe at some high energy scale, are motivated by the electroweak unification. The unification must necessarily take place at energies many orders of magnitude greater than those that ever can be achieved on Earth. In order to make sense of the theoru, ehich is given at the grand unified scale, at the electroweak scale, the symmetry at the grand unified scale is broken down to the SM symmetry. Within these models the SM is considered as an effective field theory. We study renormalization group running of the leptonic parameters in a non-supersymmetric SO(10) model which is broken in two steps via the Pati-Salam group. Finally, the discovery of the new boson at the LHC provides a new opportunity to search for physics beyond the SM. We consider an effective model where the magnitudes of the couplings in the Higgs sector are scaled by so-called coupling scale factors. We perform Bayesian parameter inference based on the LHC data. Furthermore, we perform Bayesian model comparison, comparing models where one or several of the Higgs couplings are allowed, to the SM, where the couplings are fixed. / <p>QC 20141020</p>

L’expérience Tokai-to-Kamioka (T2K), située au Japon, étudie les oscillations des neutrinos et anti-neutrinos muoniques. Elle se donne pour objectif de mesurer les paramètres de la matrice de mélange, en particulier l’angle de mélange θ13 et la phase de violation de la symétrie CP. L’incertitude principale sur ces mesures provient de la méconnaissance des interactions des neutrinos avec les noyaux des divers matériaux composant les détecteurs. Afin de réduire ces erreurs systématiques, le détecteur WAGASCI, composé d’un réseau de barres de scintillateurs dans une cuve d’eau, a été construit et installé en 2016 sur le site de J-PARC à Tokai.Nous présentons dans cette thèse le phénomène d’oscillation des neutrinos et les effets nucléaires qui permettent de décrire les interactions entre neutrinos et noyaux. Nous illustrons également la construction du premier module WAGASCI – appelé le WaterModule – effectuée à l’automne 2015 ainsi que les études d’étalonnage de la réponse en énergie du détecteur.Les données collectées avec le WaterModule sont ensuite utilisées pour mesurer la section efficace des interactions par courant chargé des neutrinos muoniques produisant un pion dans l’état final (canal CC1π). Nous présentons ainsi les étapes menant à cette mesure : l’identification des particules, la sélection d’un échantillon d’évènements candidats puis l’étude des incertitudes statistiques et systématiques. Pour extraire la section efficace en fonction de l’angle et de l’impulsion du muon, nous utilisons une méthode statistique (unfolding) itérative pour laquelle un critère de convergence doit être établi ; nous présentons cette méthode ainsi qu’un moyen de construire un critère de convergence dicté par les données.Cette mesure, comme l’ensemble des mesures effectuées avec le détecteur WAGASCI, contribuera à réduire de manière significative les incertitudes systématiques de l’expérience T2K, ouvrant la voie à la mesure de la phase de violation de la symétrie CP. / The Tokai-to-Kamioka experiment (T2K), located in Japan, studies oscillations of muon neutrinos and antineutrinos. It aims to measure neutrino mixing parameters, such as the mixing angle θ13 and the CP-symmetry violating phase. The principal uncertainty on these measurements relates to the limited knowledge on neutrino-nucleus interactions on various target materials in the detectors. In order to reduce these systematic uncertainties, the WAGASCI detector – a lattice of scintillator bars in a water tank – has been built and installed in 2016 at J-PARC (Tokai, Japan).In this thesis we introduce neutrino oscillations alongside the nuclear effects required to describe how neutrinos interact with nuclei. We also show how the first WAGASCI module, the so-called WaterModule, was built in autumn 2015 in Tokai. The charge calibration of the WaterModule is also presented.The first WaterModule data are used to measure the muon neutrino charged-current cross section with one charged pion in the final state (CC1π channel). We detail the steps leading to this measurement: the particle identification; the selection of CC1π-candidate events; and the study of statistical and systematic uncertainties. To extract the double differential cross section with respect to muon momentum and angle, we use an iterative unfolding approach that requires a convergence criterion. We present this method and a way to build a data-driven convergence criterion.This measurement, as well as all coming measurements from the full WAGASCI detector, will contribute to significantly reduce the systematic errors for the T2K experiment. We will thus take a step further towards the measurement of the CP-symmetry violating phase.

We consider a simple model for invisible neutrino decay as a sub-leading effect in the standard three-flavor neutrino oscillation framework, and use the Cayley–Hamilton formalism to obtain a full set of neutrino oscillation probabilities in matter. These are given as analytical series expansions in the small parameters α ∼ O(λ^2) and s_13 ∼ O(λ), where λ ≡ 0.2 is a “book-keeping parameter” denoting the order of the expansion. We produce explicit formulas for P_eµ, P_eτ , P_µµ, P_µτ , and P_ττ to order O(λ^3), and for P_ee to order O(λ^2), all having first corrections of order O(λ^4). Moreover, we also present vacuum limits of our expressions, as well as discuss the effect of decay on unitarity. We show that all rows in the unitarity table have corrections of order O(λ^2), with the second and third rows having additional corrections of order O(1). In the limit of no decay, unitarity is restored, and we furthermore recover known results for all probabilities. / Vi betraktar en enkel modell för osynligt neutrinosönderfall som en icke-ledande effekt inom det vedertagna ramverket för oscillationer med tre neutrinosmaker och använder Cayley–Hamilton-formalismen för att erhålla en fullständig uppsättning av sannolikheter för neutrinooscillationer i materia. Dessa ges som analytiska serieutvecklingar i de små parametrarna α ∼ O(λ^2) och s_13 ∼ O(λ), där λ ≡ 0.2 är en gemensam “bokföringsparameter” som anger serieutvecklingens ordning. Vi tar fram explicita uttryck för P_eµ, P_eτ , P_µµ, P_µτ och P_ττ till ordning O(λ^3) och för P_ee till ordning O(λ^2), med första korrigeringar för alla sannolikheterna till ordning O(λ^4). Därutöver presenterar vi gränsvärden för våra uttryck i vakuum samt diskuterar sönderfallets inverkan på unitaritet. Vi finner att alla rader i unitaritetstabellen har korrigeringar till ordning O(λ^2) och därtill korrigeringar till ordning O(1) för den andra och tredje raden. I avsaknad av sönderfall återfås unitaritet och vi reproducerar dessutom kända resultatför alla sannolikheter.

Neutrinooszillationen sind das einzige Phänomen jenseits des Standardmodells, das experimentell mit hoher statistischer Signifikanz bestätigt wurde. Diese Arbeit präsentiert eine Messung der atmosphärischen Neutrinooszillationen unter Verwendung von acht Jahren an Daten, die zwischen 2011 und 2019 vom IceCube DeepCore-Detektor aufgenommen wurden. Die Ereignisauswahl wurde im Vergleich zu früheren DeepCore-Messungen verbessert, wobei ein besonderes Augenmerk auf ihre Robustheit gegenüber systematischen Unsicherheiten in den Detektoreigenschaften gelegt wurde. Die Oszillationsparameter werden über eine Maximum-Likelihood-Fit an gebinnte Daten in der gemessenen Energie und Zenitwinkel geschätzt, wobei die Erwartungswerte aus gewichteten simulierten Ereignissen abgeleitet werdem. Diese Arbeit diskutiert den Simulations- und Datenauswahlprozess sowie die statistischen Methoden, die verwendet werden, um einen genauen Erwartungswert unter variablen Detektoreigenschaften und anderen systematischen Unsicherheiten zu liefern. Die Messung wird zunächst unter Verwendung des Standardmodells der Drei-Flavor-Oszillation durchgeführt, wobei das atmosphärische Massensplitting und der Mischwinkel auf $\Delta m^2_{32} = 2.42_{-0.75}^{+0.77} \times10^{-3};\mathrm{eV}^2$ und $\sin^2\theta_{23} = 0.507_{-0.053}^{+0.050}$ geschätzt werden. Das Drei-Flavor-Modell wird dann um einen zusätzlichen Masseneigenzustand erweitert, der einem sterilen Neutrino mit Massensplitting $\Delta m^2_{41} = 1;\mathrm{eV}^2$ entspricht und mit den aktiven $\nu_\mu$- und $\nu_\tau$-Flavorzuständen mischen kann. Es wird kein signifikantes Signal eines sterilen Neutrinos beobachtet, und die Mischungsamplituden zwischen den sterilen und aktiven Zuständen werden auf $|U_{\mu 4}|^2 < 0.0534$ und $|U_{\tau 4}|^2 < 0.0574$ bei 90\% C.L. begrenzt. Diese Grenzwerte sind um den Faktor zwei bis drei strenger als das vorherige DeepCore-Ergebnis, und die Einschränkung von $|U_{\tau 4}|^2$ ist die stärkste der Welt. / Neutrino oscillations are the only phenomenon beyond the Standard Model that has been confirmed experimentally to a very high statistical significance. This work presents a measurement of atmospheric neutrino oscillations using eight years of data taken by the IceCube DeepCore detector between 2011 and 2019. The event selection has been improved over that used in previous DeepCore measurements with a particular emphasis on its robustness with respect to systematic uncertainties in the detector properties. The oscillation parameters are estimated via a maximum likelihood fit to binned data in the observed energy and zenith angle, where the expectation is derived from weighted simulated events. This work discusses the simulation and data selection process, as well as the statistical methods employed to give an accurate expectation value under variable detector properties and other systematic uncertainties. The measurement is first performed first under the standard three-flavor oscillation model, where the atmospheric mass splitting and mixing angle are estimated to be $\Delta m^2_{32} = 2.42_{-0.75}^{+0.77} \times10^{-3}\;\mathrm{eV}^2$ and $\sin^2\theta_{23} = 0.507_{-0.053}^{+0.050}$, respectively. The three-flavor model is then extended by an additional mass eigenstate corresponding to a sterile neutrino with mass splitting $\Delta m^2_{41} = 1\;\mathrm{eV}^2$ that can mix with the active $\nu_\mu$ and $\nu_\tau$ flavor states. No significant signal of a sterile neutrino is observed and the mixing amplitudes between the sterile and active states are constrained to $|U_{\mu 4}|^2 < 0.0534$ and $|U_{\tau 4}|^2 < 0.0574$ at 90\% C.L. These limits are more stringent than the previous DeepCore result by a factor between two and three and the constraint on $|U_{\tau 4}|^2$ is the strongest in the world.