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Simulation of the upgraded Phase-1 Trigger Readout Electronics of the Liquid-Argon Calorimeter of the ATLAS Detector at the LHCGrohs, Johannes Philipp 10 May 2016 (has links) (PDF)
In the context of an intensive upgrade plan for the Large Hadron Collider (LHC) in order to provide proton beams of increased luminosity, a revision of the data readout electronics of the Liquid-Argon-Calorimeter of the ATLAS detector is scheduled. This is required to retain the efficiency of the trigger at increased event rates despite its fixed bandwidth. The focus lies on the early digitization and finer segmentation of the data provided to the trigger. Furthermore, there is the possibility to implement new energy reconstruction algorithms which are adapted to the specific requirements of the trigger. In order to constitute crucial design decisions, such as the digitization scale or the choice of digital signal processing algorithms, comprehensive simulations are required. High trigger efficiencies are decisive at it for the successful continuation of the measurements of rare StandardModel processes as well as for a high sensitivity to new physics beyond the established theories. It can be shown that a significantly improved resolution of the missing transverse energy calculated by the trigger is achievable due to the revised segmentation of the data. Various energy reconstruction algorithms are investigated in detail. It can be concluded that these will facilitate reliable trigger decisions for all expected working conditions and for the whole possible energy range.
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Etude des performances d'étiquetage des B et analyse du canal HW dans l'expérience ATLAS. / B-TAGGING performance studies and HW analysis in the Atlas experimentBai, Yu 29 May 2012 (has links)
Les études de physique conduites à l'echelle du TEV, comme la recherche du boson de Higgs et de nouvelles particules, par exemple dans le cadre du modèle de super-symétrie, ou encore les études du quark top, succitent un interêt croissant maintenant que cette échelle est accessible. Dans ces analyses, il est souvent nécessaire d'identifier les jets issues de quark b de ceux provenant de quarks légers, de gluons ou d'autres types de bruit de fond. Par exemple, dans le cadre de la recherche du boson de Higgs leger, le Higgs est attendu de se désintégrer principalement en bb^_ les études de canaux impliquant la e e b; e production de quark top ont souvent des jets de quarks b dans leurs état finaux et du fait de la désintégration dominante du quark top en bW ; dans beaucoup d'analyse, les processus impliquant un quark top sont un bruit de fond et l'identification des jets de b fournie un excellent moyen, appelé b-jet veto, de les rejeter. Cette identification des jets de b est appellé b-tagging. Les études effectuées dans l'expérience ATLAS sur les performances du b-tagging, sa mise en route et son optimisation, sont présentées et developées dans cette thèse. / Physics studies at the TeV scale, such as searches for Higgs and new particles, for example from super-symmetry, as well as top quark studies are drawing special interest in experimental particle physics now that this scale is reachable. In these analyses, it is often necessary to identify jets from b quark out of jets from light quarks or gluons and other backgrounds. For exam- ple, in the low mass Higgs boson search, the Higgs is expected to dominantly decays into bb^_, studies involving top quark production have always b-jets in b; their final states due to dominant top decay into bW; for many analysis, top processes are a background and the b jets identification provides an excellent method to reject them using a so-called b jet veto. This b jets identification is called b-tagging. The studies done, within the ATLAS experiment, on the b-tagging performances, its commissioning and optimization, are presented and developed in this thesis.
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Recherche de production électrofaible supersymétrique dans des cascades de désintégration contenant un boson de Higgs avec le détecteur ATLAS au LHC / Search for electroweak production of supersymmetry in decay cascades containing a Higgs boson with the ATLAS detector at LHCUghetto, Michaël 07 November 2014 (has links)
Depuis le démarrage des collisions proton-proton au LHC en 2009, les expériences ATLAS et CMS ont collecté plus de 25/fb de données. Le boson de Higgs est une prédiction clé du Modèle Standard de la physique des particules et sa découverte en 2012 par les expériences ATLAS et CMS complète le Modèle Standard. Le Modèle Standard, bien qu'en excellent accord avec les observations faites auprès des collisioneurs, ne répond pas à de nombreuses questions~: la nature de la matière noire, de l'énergie noire... De plus, l'instabilité de la masse du Higgs sous l'effet des corrections radiatives semble indiquer la présence d'une nouvelle physique à haute énergie. Parmi les théories au-delà du Modèle Standard, les modèles supersymétriques restent encore aujourd'hui d'excellents candidats pour étendre le Modèle Standard. Durant cette thèse, qui s'est déroulée de 2011 à 2014, j'ai travaillé à la recherche de signaux supersymétriques au sein de l'expérience ATLAS. Tout d'abord au L2C à Montpellier, où nous avons co-développé une nouvelle version de SuSpect, un programme permettant de calculer le spectre de masse du MSSM. Au sein du groupe ATLAS du CPPM à Marseille, j'ai développé pour la collaboration ATLAS des outils d'identification des jets issus de l'hadronisation des quarks b basés sur des réseaux de neurones artificiels et des arbres de décisions. Ces outils ont permis d'améliorer la discrimination des différentes saveurs de jet pour les analyses de données d'ATLAS.J'ai ensuite utilisé les données enregistrées par ATLAS en 2012 pour poser des limites sur la production associée de charginos et neutralinos se désintégrant via un boson de Higgs et un boson W pour donner un lepton chargé, deux jets issus de quarks b et de l'énergie transverse manquante. / Since the start of proton-proton collisions at LHC in 2009, the ATLAS and CMS experiments have recorded more than 25/fb of data each. The Higgs boson is akey prediction of the Standard Model of particle physics and its discovery in 2012 by the ATLAS and CMS experiments complete the Standard Model.The Standard Model, despite its excellent agreement with experiments at colliders, doesn't answer to many questions~: the nature of dark matter, dark energy... Furthermore, the instability of the Higgs mass under the effect of radiative corrections seems to indicate the existence of new physics at high energy.Among the theories beyond the Standard Model, supersymmetric models are excellent candidates to extend the Standard Model. During this thesis, between 2011 and 2014, I worked on the search of supersymmetric signals with the ATLAS experiment.First at L2C in Montpellier, where we have co-develloped a new version of SuSpect, a program designed to compute the MSSM mass spectrum.In the ATLAS groupe at CPPM in Marseille, I developped for the ATLAS collaboration a serie of tools based on artificial neural networks and decision trees to identify jets coming from b-quark hadronization. This tools have improved the discimination between different jets flavors for data analysis in ATLAS.Then, I analyzed the data collected by ATLAS in 2012 to obtain limits on the associated production charginos and neutralinos decaying via a W and a Higgs boson, resulting in a final state containing a charged lepton, two b-jets and missing transverse momentum
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Measurement of the inclusive prompt photon cross section and preparation of the search of the Higgs boson decaying into two photons with the ATLAS detector at the LHC / Mesures de la section efficace de production de photons isolés et préparation de la recherche du boson de Higgs dans le canal de désintégration en deux photons avec le détecteur ATLAS au LHCAbreu Aguilar, Henso Javier 05 July 2011 (has links)
Ce travail présente les mesures de section efficace de production de photons isoles dans les collisions proton-proton avec l’expérience ATLAS au LHC, a une énergie de 7 TeV dans le centre de masse. Les résultats sont d’abord obtenus pour une luminosité intégrée de 880 nb−1, puis dans un deuxième temps pour une luminosité de 36 pb−1. Les mesures faites avec 880 nb−1 et 36 pb−1 couvrent, respectivement, les intervalles en énergie transverse 15 ≤ E < 100 GeV et 45 ≤ E < 400 GeV. Les résultats sont compares aux prédictions de la chromodynamique quantique perturbative à l’ordre NLO. Les premières études pour la recherche du Higgs dans le canal de désintégration en deux photons sont également présentées pour 38 pb−1 de données collectées par l’expérience ATLAS en 2010 (et plus récemment pour 210 pb−1 accumules en 2011). Les limites d’exclusion observées sont citées en fonction d’une masse de Higgs se situant dans l’intervalle 110-140 GeV. / This work presents the measurements with the ATLAS experiment of the cross section for inclusive production of isolated prompt photons in proton-proton collisions at a centre-ofmass energy √s = 7 TeV. The first results are based on an integrated luminosity of 880 nb−1 and the later results are based on 36 pb−1, collected with the ATLAS detector at the Large Hadron Collider. The measurements performed with 880 nb−1 and 36 pb−1 cover the transverse energy range 15 ≤ E < 100 GeV and 45 ≤ E < 400 GeV, respectively.The results are compared to predictions from next-to-leading order perturbative QCD calculations. In addition, are also presented the first studies for the search for the Higgs boson in the decay channel into two photons with 38 pb−1 data collected by the ATLAS experiment in 2010 (and more recently with 210 pb−1 collected in 2011). Observed exclusion limits are quoted as a function of the Higgs mass in the range 110-140 GeV.
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Asymétrie de charge et mesures angulaires des bosons W dans l'expérience ATLAS auprès du LHC / Charge asymmetry and W boson angular measurement in the ATLAS experiment at the LHCBlanchard, Jean-Baptiste 12 September 2011 (has links)
Le LHC est un collisionneur de protons, situé 100 mètres sous la frontière franco-suisse, conçu pour fonctionner à sqrt(s) = 14 TeV. Les premières collisions à sqrt(s) = 7 TeV ont eu lieu au début de l'année 2010, ouvrant la chasse aux nouvelles particules telles le boson de Higgs, les partenaires supersymétriques... Ces premières données ont permis aussi de faire des mesures de précisions afin de vérifier le fonctionnement du détecteur et de contraindre certains paramètre du Modèle Standard. C'est dans ce cadre que s'inscrit cette thèse. Le travail présenté dans ce manuscrit s'articule en deux parties distinctes dont le but est de contraindre d'éventuels biais et sources d'erreurs systématiques pour permettre une première mesure précise de la masse du boson W au LHC. D'un point de vue technique, une analyse consistant à étudier les variations de température de l'argon liquide, dans lequel sont immergés les calorimètres a été menée afin de comprendre leur origine et de limiter leur contribution à l'incertitude sur l'échelle d'énergie des électrons. D'autre part, le travail a été focalisé sur les effets de polarisation, en développant et proposant trois mesures originales : la quantification de leur influence sur la détermination directe de MW au LHC, les mesures de fractions d'hélicité dans les données 2010 et une mesure de l'asymétrie de charge permettant de découpler les effets de PDFs des effets de polarisation, appliquée aux données 2010. / The LHC is a proton collider, buried 100 meters below the franco-swiss border, built to work at sqrt(s) = 14 TeV. First collisions at sqrt(s) = 7 TeV occurred in the beginning of 2010, starting officially new particles hunting, like Higgs boson, supersymmetric partner... First data have also been used to do precision measurements in order to check detector performances and constrain many Standard Model parameters. The latter will be the main topic of this thesis.The work presented within this manuscript can be split in two different parts aiming to a common goal: reduce possible bias and systematic errors to provide a first precise W boson mass measurement at the LHC. On a technical aspect, an analysis has been done on the liquid argon that lies within calorimeter's cryostat, in order to understand temperature fluctuation and quantify its effect on the electron energy scale. On the other hand, attention has been focused on polarization effects, by developping and proposing three new measurements: quantification of their influence on MW measurement at the LHC, helicity fractions measurement in 2010 data and a charge asymmetry measurement that decouples PDF and polarization effects, on 2010 data.
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Measurement of the Brout-Englert-Higgs boson couplings in its diphoton decay channel with the ATLAS detector at the LHC / Mesure des couplages du boson de Brout-Englert-Higgs se désintégrant en deux photons par l'expérience ATLAS au LHCScifo, Estelle 11 July 2014 (has links)
Après la découverte du boson de Higgs par les expériences ATLAS et CMS au LHC, annoncée le 4 juillet 2012 au CERN, l'heure est maintenant à la mesure des propriétés de cette nouvelle particule pour vérifier sa compatibilité avec le boson scalaire prédit par le Modèle Standard. Son couplage aux autres particules est une mesure importante car toute déviation par rapport à la valeur prédite par la théorie peut être le signe d'une nouvelle physique, au-delà du Modèle Standard. Cette thèse présente la mesure des couplages du boson de Higgs dans son mode de désintégration en deux photons, utilisant l'ensemble des données collectées en 2011 (4.5 fb^{-1} à 7 TeV) et 2012 (20.3 fb^{-1} à 8 TeV) par le détecteur ATLAS. Les événements sont classifiés en fonction des objets produits en association avec le Higgs : deux jets pour la production VBF, lepton et énergie transverse manquante pour le higgsstrahlung (WH et ZH) et jets de b pour le ttH, les événements restants étant produits majoritairement par le processus de production dominant ggH. L'impact de la modélisation du moment transverse du Higgs, dans son mode de production par fusion de gluons, est aussi estimé. Les derniers développements théoriques dans ce domaine permettent d'atteindre une précision à l'ordre NNLO+NNLL (QCD), avec la prise en compte de l'effet des masses finies des quarks top et bottom dans la boucle jusqu'à l'ordre NLO+NLL, implémentée dans le programme HRes. Une méthode de pondération est dérivée pour prendre en compte ces dernières avancées, en prenant en compte la corrélation avec le nombre de jets. Les résultats finaux sont en bon accord avec les prédictions du Modèle Standard, en prenant en compte les barres d'erreur. A la masse mesurée par la combinaison des canaux diphoton et quatre leptons dans ATLAS, mH = 125.4 +/- 0.4 GeV, la section efficace totale ramenée à celle attendue par le Modèle Standard est : mu = 1.17^{+0.28}_{-0.25} = 1.17 +/- 0.23(stat) ^{+0.10}_{-0.08}(syst) ^{+0.12}_{-0.08}(théorie) et le rapport du nombre d'événements mesurés pour chaque mode de production à celui prédit par le Modèle Standard est : mu_ggH = 1.32 +/- 0.32(stat.) ^{+0.13}_{-0.09}(syst.) ^{+0.19}_{-0.11}(théorie) ; mu_VBF = 0.8 +/- 0.7(stat.) ^{+0.2}_{-0.1}(syst.) ^{+0.2}_{-0.3}(théorie) ; mu_WH = 1.0 +/- 1.5(stat.) ^{+0.3}_{-0.1}(syst.) ^{+0.2}_{-0.1}(théorie) ; mu_ZH = 0.1 ^{+3.6}_{-0.1}(stat.) ^{+0.7}_{-0.0}(syst.) ^{+0.1}_{-0.0}(théorie) ; mu_ttH = 1.6 ^{+2.6}_{-1.8}(stat.) ^{+0.6}_{-0.4}(syst.} ^{+0.5}_{-0.2}(théorie) / After the Higgs boson discovery in the first LHC data, the focus is now on its properties measurement. Among these properties, its couplings are of particular importance since any deviation from the expected value can be an indication of new physics, beyond the Standard Model. This thesis is oriented towards the Higgs couplings measurements with the ATLAS experiment, using the diphoton decay channel. Selected diphoton events are classified into different categories to disentangle the five Higgs production modes by tagging the objects produced in association with the Higgs boson: two jets for the VBF production mode, lepton and missing transverse energy for the higgsstrahlung (WH and ZH), b-jets for ttH, the remaining events being mostly produced via the dominant production mode ggH. The impact of the Higgs pT modelling in the ggH production mode is also investigated. Theoretical developments provide predictions of the pT shape at NNLO+NNLL accuracy, including top and bottom mass effects in the loop up to NLO+NLL, implemented in the HRes program. A reweighting technique to take into account these latest theoretical improvements is derived, taking into consideration the correlation with the number of jets. Its impact on the final measurement is estimated to be of the order of a few percent. The final couplings results, measured at the Higgs mass obtained by the combination of the H->gamma gamma and H->ZZ*->4l channels in ATLAS (mH = 125.4 +/- 0.4 GeV) do not show any statistically significant deviation from the Standard Model. The observed signal strength mu = sigma^{obs} / sigma^{exp} is found to be: mu = 1.17^{+0.28}_{-0.25} = 1.17 +/- 0.23(stat) ^{+0.10}_{-0.08}(syst) ^{+0.12}_{-0.08}(theory). The ratio of the observed number of events in each production mode to the expected ones are measured at: mu_ggH = 1.32 +/- 0.32(stat.) ^{+0.13}_{-0.09}(syst.) ^{+0.19}_{-0.11}(theory) ; mu_VBF = 0.8 +/- 0.7(stat.) ^{+0.2}_{-0.1}(syst.) ^{+0.2}_{-0.3}(theory) ; mu_WH = 1.0 +/- 1.5(stat.) ^{+0.3}_{-0.1}(syst.) ^{+0.2}_{-0.1}(theory) ; mu_ZH = 0.1 ^{+3.6}_{-0.1}(stat.) ^{+0.7}_{-0.0}(syst.) ^{+0.1}_{-0.0}(theory) ; mu_ttH = 1.6 ^{+2.6}_{-1.8}(stat.) ^{+0.6}_{-0.4}(syst.} ^{+0.5}_{-0.2}(theory)
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Higgs Physics Beyond the Standard Model / Physique du Higgs au-delà du Modèle StandardQuevillon, Jérémie 19 June 2014 (has links)
Le 4 Juillet 2012, la découverte d'une nouvelle particule scalaire d'une masse de l’ordre de 125 GeV a été annoncée par les collaborations ATLAS et CMS.Une nouvelle ère s'annonce : celle au cours de laquelle il faudra déterminer précisément les propriétés de cette nouvelle particule.Cela est crucial afin d'établir si cette particule est bien la trace du mécanisme responsable de la brisure de la symétrie du secteur électro-faible. Cela permettrait aussi de repérer tout élément susceptible d'être associé à une « nouvelle physique » dans le cas où le mécanisme de brisure ferait intervenir des ingrédients autres que ceux prédits par le Modèle Standard.Dans cette thèse, nous avons essayé de comprendre et de caractériser jusqu’à quel point ce nouveau champ scalaire est le boson de Higgs prédit par le Modèle Standard. Nous avons établi les applications d'une telle découverte dans le contexte de théories supersymétriques et de modèles décrivant la matière noire.Dans une première partie consacrée au Modèle Standard de la physique des particules, nous étudions après une courte introduction au domaine, le processus de production d'une paire de bosons de Higgs au LHC. Un résultat majeur est que ce mode de production permettra de mesurer le couplage trilinéaire du Higgs qui est un paramètre essentiel à mesurer afin de reconstruire le potentiel du Higgs et donc représente la dernière vérification à effectuer pour confirmer l'origine de la brisure spontanée de la symétrie électro-faible.La deuxième partie traite des théories supersymétriques. Après une introduction au sujet, un de nos importants résultats est d'avoir fortement contraint un certain nombre de modèles supersymétriques après la découverte du boson de Higgs. Nous avons aussi introduit une nouvelle approche qui permet aux physiciens expérimentateurs de rechercher de manière efficace les bosons de Higgs supersymétriques dans les expériences actuelles et futures du LHC.La troisième partie concerne la matière noire. Nous présentons des résultats qui établis-sent d'importantes limitations sur des modèles où la matière noire interagirait avec le boson de Higgs. Nous discutons aussi de scénarios alternatifs qui font intervenir de la matière noire hors équilibre avec le bain thermique. Dans un premier temps nous dé-montrons qu'il existe un lien étroit entre la température de réchauffement de l'univers et le schéma de brisure du groupe de jauge du Modèle Standard et dans un deuxième temps nous étudions la genèse de matière noire par l'intermédiaire de nouveaux bosons Z’. / On the 4th of July 2012, the discovery of a new scalar particle with a mass of order 125 GeV was announced by the ATLAS and CMS collaborations. An important era is now opening: the precise determination of the properties of the produced particle. This is of extreme importance in order to establish that this particle is indeed the relic of the mechanism responsible for the electroweak symmetry breaking and to pin down effects of new physics if additional ingredients beyond those of the Standard Model are involved in the symmetry breaking mechanism. In this thesis we have tried to understand and characterize to which extent this new scalar field is the Standard Model Higgs Boson and set the implications of this discovery in the context of Supersymmetric theories and dark matter models.In a first part devoted to the Standard Model of particle physics, we discuss the Higgs pair production processes at the LHC and the main output of our results is that they al-low for the determination of the trilinear Higgs self-coupling which represents a first important step towards the reconstruction of the Higgs potential and thus the final verifica-tion of the Higgs mechanism as the origin of electroweak symmetry breaking.The second part is about Supersymmetric theories. After a review of the topics one of our result is to set strong restrictions on Supersymmetric models after the Higgs discov-ery. We also introduce a new approach which would allow experimentalists to efficiently look for supersymmetric heavy Higgs bosons at current and next LHC runs.The third part concerns dark matter. We present results which give strong constraints on Higgs-portal models. We finally discuss alternative non-thermal dark matter scenario. Firstly, we demonstrate that there exists a tight link between the reheating temperature and the scheme of the Standard Model gauge group breaking and secondly we study the genesis of dark matter by a Z’ portal.
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Event-by-event Hydrodynamics for LHC / Hidrodinâmica Evento-por-evento para o LHCMachado, Meera Vieira 06 August 2015 (has links)
We perform an event-by-event hydrodynamic analysis for Pb-Pb collisions at the incident energy of sqrt(sNN) = 2.76TeV, also studying the effects of two equations of state under the same initial conditions and freeze-out scenario: one characterized by a critical point and the other based on Lattice QCD (Quantum Chromodynamics) calculations. The observables of interest are particle spectra in terms of pseudorapidity and transverse momentum, as well as flow harmonics, which are coefficients that carry information on the initial anisotropies of the system throughout its evolution. Those are computed and compared with experimental Large Hadron Collider (LHC) data. There are slight differences in the results for each equation of state, caused by their distinct features. Lastly, the LHC-based calculations are compared with previous works related to the Relativistic Heavy-Ion Collider (RHIC) experimental data. The main techniques of the latter are performed in this work, which results in differences between some aspects in the outcome for each collision type, from initial energy distributions to freeze-out temperatures. / É feita uma análise de hidrodinâmica evento-por-evento para colisões de Pb-Pb à energia incidente de sqrt(sNN) = 2.76TeV. Estudamos os efeitos de duas equações de estado sob as mesmas condições iniciais e desacoplamento: uma é caracterizada por um ponto crítico e a outra é baseada em cálculos de Lattice QCD (Cromodinâmica Quântica). Os observáveis de interesse são os espectros de partículas em termos da pseudo rapidez e momento transversal, assim como os coeficientes harmônicos de Fourier que, por sua vez, carregam as anisotropias iniciais do sistema durante toda a sua evolução. Tais observáveis são calculados e comparados com dados experimentais do Large Hadron Collider (LHC). Por fim, os cálculos baseados em parâmetros referentes às energias do LHC são comparados com trabalhos anteriores feitos com base em dados experimentais do Relativistic Heavy-Ion Collider (RHIC). Os principais métodos usados no caso anterior são aplicados a este trabalho, o que resulta em algumas diferenças entre os resultados dos dois tipos de colisão, desde a distribuição de energia inicial a temperaturas de freeze-out.
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Produção de Mésons Vetoriais em Processos Foto-Induzidos no LHC / Vector Meson Production in Photoinduced Processes at LHCMoreira, Bruno Duarte da Silva 26 April 2017 (has links)
O advento dos colisores modernos tem proporcionado novas possibilidades de estudo em física de partículas como, por exemplo, a busca por nova física e o estudo de novos estados da matéria hadrônica. Em particular, em colisões de íons pesados em altas energias, acredita-se que um novo estado da matéria seja formado antes da colisão, o chamado condensado de vidros de cor. Tal estado seria a condição inicial de um plasma de quarks e glúons e é caracterizado por altas densidades de pártons (quarks e glúons). De fato, as equações de evolução da Cromodinâmica Quântica predizem que, para virtualidades moderadas e altas energias, os hádrons se tornam sistemas extremamente densos devido ao crescimento das distribuições de glúons nessas condições. Um crescimento indefinido das distribuições de glúons poderia levar à violação do vínculo de unitariedade. Para evitar essa violação, existe um mecanismo chamado de saturação de pártons o qual contém o crescimento das distribuições de quarks e glúons de forma a respeitar o vínculo de unitariedade. Teoricamente, no limite de altas energias, observa-se que os hádrons são populados especialmente por glúons. Experimentalmente, existem indícios da saturação em colisões ep, pp, pA e AA, contudo, isso ainda é uma questão em aberto. Portanto, no limite de altas densidades, espera- se que a física não linear, a qual leva em conta efeitos de recombinações de glúon, passe a se manifestar. Uma alternativa para o estudo da saturação em colisores hadrônicos são os processos foto-induzidos, os quais ocorrem em interações ultraperiféricas. Em uma colisão ultraperiférica entre dois hádrons, o parâmetro de impacto é maior do que a soma dos raios dos hádrons, de forma que interações fortes são suprimidas. Dessa forma os hádrons atuam como fontes de fótons (quase reais) podendo ocorrer interações fóton-hádron e fóton-fóton. Nesse trabalho estudamos a fotoprodução difrativa de mésons vetoriais em energias do LHC para colisões ultraperiféricas próton-próton, próton-núcleo e núcleo-núcleo e a produção dupla de mésons vetoriais em colisões fóton-fóton e devido ao mecanismo de duplo espalhamento fóton-p(A). Mostramos como esses processos podem ser usados para estudar a física de altas energias e os efeitos de saturação. Os efeitos de saturação em nossos cálculos são levados em conta através do formalismo de dipolo de cor, que é uma das ferramentas básicas usadas nessa tese. O tratamento de colisões ultraperiféricas hádron-hádron foi feito com a aproximação de fótons equivalentes que assim como o formalismo de dipolo, foi extensamente usada. Nossos resultados apontam que o estudo fenomenológico e experimental dos tipos de processos citados acima são factíveis e podem ser usados para vincular a dinâmica da QCD em altas energias. / The advent of the modern colliders has provided new possibilities of study in particle physics as, for example, the search for new physics and the study of new states of the hadronic matter. In particular, in high energy heavy ion collisions is expected that a new state can be formed before the collision, the so called Color Glass Condensate. This state would be the initial condition of the Quark Gluon Plasma and is characterized by high parton (quarks and gluons) densities. Indeed, the Quantum Chromodynamics evolution equations predict that, for moderate virtualities and high energies, the hadrons become extremely dense systems due to the growth of the parton distribution in these conditions. An indefinite growth of the parton distributions could lead to the violation of the unitarity bound. To avoid this violation, there is a mechanism called parton saturation which tames the growth of the parton distributions to satisfy the unitarity bound. Theoretically, in the high energy limit, one can see that the hadrons are populated mainly by gluons. Experimentally, there are indications of the saturation in ep, pp, pA and AA collisions, however, this is an open question. So, in the high density limit, we expect that the nonlinear physics, which takes into account gluon recombination effects start to manifest itself. An alternative for the study of the saturation at hadronic colliders are the photon-induced processes, which occurs in ultra-peripheral collisions. In a ultra-peripheral collision between two hadrons the impact parameter is greater than the sum of the radii of the hadrons, so the strong interaction is suppressed. Thus, the hadrons act as sources of (almost real) photons and may occur photon-hadron and photon-photon interactions. In this work we study the diffractive photoproduction of vector mesons at LHC and future colliders energies in ultra-peripheral proton-proton, proton-nucleus and nucleus-nucleus collisions and the double vector meson production in photon-photon collisions and due to the double photon-p(A) scattering mechanism. We show how these processes can be used to study the high energy physics and the saturation effects. These effects are considered in our calculations through the color dipole formalism, which is one of the basic tools used in this thesis. The treatment of the ultra-peripheral hadron-hadron collisions was done through the equivalent photon approximation that just as in the dipole formalism, was widely used. Our results point that the phenomenological and experimental studies of the processes cited above are feasible and can be used to constraint the QCD dynamics in high energies.
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Study of the angular correlation between heavy-flavour decay electrons and charged unidentified particles in pp and p-Pb collisions with ALICE / Estudo da correlação angular entre elétrons oriundos de quarks pesados e partículas carregadas em colisões pp e p-Pb com o detector ALICEOliveira Filho, Elienos Pereira de 05 December 2014 (has links)
The aim of relativistic heavy-ion collisions is to investigate the properties of the Quark-Gluon Plasma (QGP) phase, that is achieved at high-enough temperatures and/or densities. In this context, light on heavy-ion collisions (e. g. p-Pb) are used to assess Cold Nuclear Matter effects (CNM), while elementary hadronic collisions (e. g. proton-proton) provide tests for QCD (Quantum Chromodynamics) based calculations and baseline for studies with heavy- ions. Heavy quarks, i. e. charm and beauty, are very convenient in the characterization of the QGP. They are produced via initial hard parton-parton scatterings at the early stages of the collision and, therefore, they are a self-generated probe for the system created in the reaction. In this work the angular correlation between electrons from heavy-flavour hadron decays and charged particles was studied in pp (2.76 and 7 TeV) and p-Pb (5.02 TeV) collisions at the CERN Large Hadron Collider, using the ALICE detector. The correlation strengths were evaluated as a function of multiplicity in p-Pb collisions. In pp collisions the relative beauty (and charm) contribution to the total heavy-flavour decay electron yield was estimated using the measured correlation distribution and Monte Carlo templates. / O próposito de colisões entre íons pesados relativísticos é investigar as propriedades do plasma de quarks e gluons (QGP, do inglês Quark-Gluon Plasma). A transição de fase, de um estado hadrônico para o QGP, ocorre em regimes onde a temperatura e/ou densidade atingem um valor suficientemente alto. Neste contexto, colisões entre íons pesados e leves (por exemplo, p-Pb) permitem acessar efeitos devido à matéria nuclear fria (CNM, do inglês Cold Nuclear Matter) e colisões elementares (por exemplo, próton-próton) são usadas como referência para estudos com íons pesados, além de proporcionarem testes para cálculos de QCD perturbativa. Quarks pesados, isto é charm e bottom, são ferramentes muito convenientes no estudo e caracterização do QGP. Essas partículas são produzidas através de espalhamento duro nos instantes iniciais da colisão e, portanto, elas atuam como uma sonda externa para o sistema criado na reação. Esse trabalho consiste no estudo da correlação angular entre elétrons oriundos de quarks pesados e partículas carregadas, em colisões pp (2.76 e 7 TeV) e p-Pb (5.02 TeV), no acelerador LHC (do inglês Large Hadron Collider) do CERN, usando o detector ALICE (do inglês A Large Ion Collider Experiment). A distribuição angular mencionada foi medida em função da multiplicidade do evento, no caso de colisões p-Pb. Em colisões pp, a contribuição relativa de quarks charm e bottom para o total de elétrons provenientes de quarks pesados foi estimada usando a função de correlação obtida.
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