This thesis presents a search for neutral bosons, such as new Higgs and Z' bosons, predicted by theories extending the Standard Model of particle physics. The search is performed in the di-tau analysis channel, where both tau leptons decay hadronically. Promising candidates of such theories are the Minimal Supersymmetric Standard Model (MSSM) and the non-universal G(221) model, which predict large couplings to tau leptons in large regions of their parameter space. Proton–proton collisions produced by the Large Hadron Collider (LHC) at a center-of-mass energy of 13 TeV, recorded with the ATLAS detector in 2015 and 2016, are analyzed for this search. The data correspond to an integrated luminosity of 36.1 fb^-1. This search relies on sophisticated algorithms for the reconstruction of hadronic tau decays from their decay products. This thesis presents a novel approach employing multivariate techniques to significantly improve existing algorithms, which became the default for reconstruction of hadronic tau decays in ATLAS since 2017. Additionally, the new method can provide useful information for subsequent tau identification algorithms. The MSSM extends the Higgs sector of the Standard Model by four additional Higgs bosons. Of particular interest for this thesis are the neutral CP-even H and CP-odd A bosons. The search for these bosons is performed in the mass range of 0.2 TeV to 2.25 TeV in two orthogonal categories depending on the number of identified b-quarks, each preferring one of the two considered production modes via gluon–gluon fusion or b-associated production. The data are in good agreement with the Standard Model prediction. Upper limits are set on the cross-section times branching fraction using a confidence level (CL) of 95 % independently for both production modes. Most stringent observed limits are found for a resonance mass of 1.5 TeV to be 4.94 fb and 3.65 fb for gluon–gluon fusion and b-associated production, respectively. The results are further interpreted in the hMSSM, mhmax and mhmod scenarios. Observed upper limits in the hMSSM scenario on tanβ are found to be between 4.6 at mA = 0.25 TeV and 41.4 at mA = 1.5 TeV. The search for additional Z' bosons is performed independently on the number of identified b-quarks in the mass range of 0.2 TeV to 4 TeV. As for the search for additional Higgs bosons no significant hint for new physics has been observed. 95 % CL observed upper limits are set on the cross-section times branching fraction for Z' bosons in the Sequential Standard Model (SSM) benchmark scenario between 20.5 pb at mZ' = 0.2 TeV and 7.74 fb at mZ' = 1.75 TeV. The observed upper limit for the highest considered mass of mZ' = 4 TeV is found to be 16 fb. Z' bosons in the SSM and the non-universal G(221) model are excluded at 95 % CL for masses below 2353 GeV and 2232 GeV, respectively.

<p>The CERN Large Hadron Collider (LHC) offers a unique opportunity to test the Standard Model of particle physics. The Standard Model predicts the existence of a Higgs boson and provides accurate estimates for the strength of the interactions of the Higgs boson with other particles. After the discovery of the Higgs boson, the measurement of its properties, such as its couplings to other particles, is of paramount importance. </p> <p>The projects described in this thesis explore different aspects of one of such measurements – the search for the Higgs boson decay into a pair of muons (H→<em>μμ</em>), conducted by the CMS experiment at the LHC. This decay plays an important role in elementary particle physics, as it provides a direct way to measure the coupling of the Higgs boson to the muon. The first evidence of the H→<em>μμ</em> decay was reported in 2020 as a result of an elaborate statistical analysis of the dataset collected by the CMS experiment during Run 2 of the LHC (2016–2018). The observed (expected) upper limit on the signal strength modifier for this decay at 95% confidence level was found to be 1.93 (0.81), constituting the most precise measurement to date. </p> <p>The details of this analysis, along with studies to establish possible directions for the development of the next iteration of  the H→<em>μμ</em> analysis using Run 3 data, are discussed in this thesis. In addition, a novel machine learning-based algorithm for the muon high level trigger is presented, which ultimately improves the data-taking efficiency of the CMS experiment, and hence, helps to increase the sensitivity of future H→<em>μμ</em> searches. Finally, projections of the H→<em>μμ</em> search sensitivity to the data-taking conditions at the High-Luminosity Large Hadron Collider are presented, estimating the achievable precision for future measurements of the Higgs boson properties.</p>

Das Standardmodell einer zusätzlichen sequentiellen Fermiongeneration (SM4) war 2012 auf Basis eines Fits an elektroschwache Präzisionsobservable und die Higgs-Signalstärken mit einer Signifikanz von 5.3 sigma ausgeschlossen worden. Komplementär dazu wurden in der vorliegenden Arbeit Fits des SM4 an eine Kombination eines typischen Satzes von Flavour-Observablen mit den Ergebnissen des zuvor durchgeführten Elektroschwachen Präzisionsfits durchgeführt. Im SM3-Kontext extrahierte Größen wurden gemäß ihrer Bedeutung im SM4 reinterpretiert und die angepassten theoretischen Ausdrücke angegeben. Die resultierenden Einschränkungen der CKM-Matrix des SM4, ihrer potentiell CP-verletzenden Phasen sowie der Masse des up-type-Quarks der 4. Generation t'' werden angegeben. Zum Vergleich des SM4 mit dem SM3 werden die erreichten chi^2-Werte genutzt. chi^2=15.53 im SM4 und 9.56 im SM3 passen fast vollkommen zu einer gleich guten Beschreibung der Experimente durch beide Modelle, wobei das SM3 aber sechs Freiheitsgrade mehr besitzt. Außerdem wurden die Vorhersagen des SM3 und des SM4 für die Dimyon-Ladungsasymmetrie ASL mit experimentellen Werten verglichen. Die Vorhersage des SM3 ist ca. 2 sigma vom experimentellen Wert entfernt, die des SM4 ca. 3 sigma.\par Die Ergebnisse deuten nicht darauf hin, dass die Signifikanz des 2012 erreichten Ausschlusses des SM4 durch die Hinzunahme von Flavour-Observablen zu den damals verwendeten elektroschwachen Präzisionsobservablen und Higgs-Querschnitten bedeutend verringert würde.\par Es konnte jedoch keine genaue quantitative Aussage über die Auswirkungen der Flavourobservablen auf diese Signifikanz getroffen werden, weil das Programm CKMfitter likelihood-ratio-Berechnung nur durchführen kann, wenn sich eines der untersuchten Modelle durch Fixierung von Parametern aus dem anderen ergibt (nested models), was hier nicht der Fall ist. / The Standard Model extended by an additional sequential generation of Dirac fermions (SM4) was excluded with a significance of 5.3 sigma in 2012. This was achieved in a combined fit of the SM4 to Electroweak Precision Observables and signal strengths of the Higgs boson. This thesis complements this excludion by a fit of the SM4 to a typical set of Flavour physics observables and the results of the previously performed Electroweak Precision fit. Quantities extracted in an SM3 framework are reinterpreted in SM4 terms and the adapted theoretical expressions are given. The resultant constraints on the SM4''s CKM matrix, its potentially CP-violating phases and the mass of the new up-type quark t'' are given. To compare the relative performance of the SM4 and the SM3, this work uses the chi^2 values achieved in the fit. The values of 15.53 for the SM4 and 9.56 for the SM4 are almost perfectly consistent with both models describing the experimental data equally well with the SM3 having six degrees of freedom more. The dimuon charge asymmetry ASL was not used as a fit input because the interpretation of its measurement was subject to debate at the time when the fits were produced, but its prediction in the fit was used as an additional test of the SM4. The SM3''s prediction differs from the experimental values by about 2 sigma, and the SM4''s prediction by about 3 sigma. \par In summary, these results do not suggest that any significant reduction of the 5.3 sigma exclusion could be achieved by combining the Electroweak Precision Observables and Higgs inputs with Flavour physics data. However, the exact effect of the Flavour physics input on the significance of the SM4''s exclusion cannot be given at this point because the CKMfitter software is currently not able to perform a statistically stringent likelihood comparison of non-nested models.

Le Modèle Standard de la physique des particules prédit l’existence d’un boson scalaire massif, appelé boson de Higgs dans la littérature, comme résultant d’un mécanisme de brisure spontanée de symétrie, qui permettrait de générer la masse des particules. Le boson de Higgs, dont la masse est inconnue théoriquement, est recherché expérimentalement depuis plusieurs décennies. L’expérience ATLAS, au collisionneur LHC, a aussi entrepris cette recherche, depuis le début des collisions de protons à haute énergie en 2010. Un des canaux de désintégrations les plus intéressants à étudier dans cet environnement est le canal en deux photons, car l’état final peut être intégralement reconstruit avec une grande précision. La réponse en énergie des photons est un point crucial dans la recherche du boson de Higgs, car une résonance fine émergeant d’un bruit de fond important est attendue. Dans cette thèse une étude approfondie de la réponse en énergie des photons en utilisant le calorimètre électromagnétique d’ATLAS a été faite. Ces études ont permis de mieux comprendre la résolution et l’échelle d’énergie des photons, et donc d’améliorer la sensibilité de l’analyse d’une part et de mieux estimer les incertitudes expérimentales sur la position du signal d’autre part. Le canal en deux photons a eu un rôle prépondérant dans la découverte d’une nouvelle particule compatible avec le boson de Higgs en Juillet 2012 par les expériences ATLAS et CMS. En utilisant ce canal ainsi que la meilleure compréhension de la réponse en énergie acquise au cours de cette thèse, une mesure de la masse du boson est proposée avec les données collectées durant les années 2011 et 2012 avec une énergie de centre de masse de 7 TeV et 8 TeV.Une masse de 126.8 +/- 0.2 (stat) +/- 0.7 (syst) GeV/c2 est trouvée. L’étalonnage de la mesure de l’énergie des photons avec le calorimètre électromagnétique est la plus grande source d’incertitude sur cette mesure. Une stratégie pour réduire cette erreur systématique sur la masse est discutée. / The Standard Model of the particle physics predicts the existence of a massive scalar boson, usually referred to as Higgs boson in the literature, as resulting from the Spontaneous Symmetry Breaking mechanism, needed to generate the mass of the particles. The Higgs boson whose mass is theoretically undetermined, is experimentally looked for since half a century by various experiments. This is the case of the ATLAS experiment at LHC which started taking data from high energy collisions in 2010. One of the most important decay channel in the LHC environment is the diphoton channel, because the final state can be completely reconstructed with high precision. The photon energy response is a key point in this analysis, as the signal would appear as a narrow resonance over a large background. In this thesis, a detailed study of the photon energy response, using the ATLAS electromagnetic calorimeter has been performed. This study has provided a better understanding of the photon energy resolution and scale, thus enabling an improvement of the sensitivity of the diphoton analysis as well as a precise determination of the systematic uncertainties on the peak position. The diphoton decay channel had a prominent role in the discovery of a new particle compatible with the Standard Model Higgs boson by the ATLAS and CMS experiments, that occurred in July 2012. Using this channel as well as the better understanding of the photon energy response, a measurement of the mass of this particle is proposed in this thesis, with the data collected in 2011 and 2012 at a center-of-mass energy of 7 TeV and 8 TeV. A mass of 126.8 +/- 0.2 (stat) +\- 0.7 (syst) GeV/c2 is found. The calibration of the photon energy measurement with the calorimeter is the source of the largest systematic uncertainty on this measurement. Strategies to reduce this systematic error are discussed.

Cette thèse de doctorat décrit la recherche de la production du boson de Higgs associée à une paire de quarks tops (tt̅H) dans un ensemble de données de collisions proton-proton à une énergie de centre de masse de √s = 13 TeV et avec une luminosité intégrée de 36,1 fb⁻¹, enregistrée par le détecteur ATLAS en 2015 et 2016. Sept états finaux, correspondants à différentes désintégrations du boson de Higgs, sont optimisés pour une meilleure séparation du signal par rapport au bruit de fond. Un excès d’événements par rapport au bruit de fond MS est observé avec une signification de 4,1 écarts types, tandis que 2,8 sont attendus. En combinaison avec des résultats de recherches avec d’autres canaux de désintégration du boson de Higgs, la production de tt̅H a été découverte par le détecteur ATLAS en utilisant jusqu’à 79,8 fb⁻¹ de données de collisions à √s = 7, 8 et 13 TeV.Les courants neutres, qui changent de saveur dans la désintégration du quark top en un boson de Higgs et un quark léger (t → Hq), sont fortement supprimés dans le MS. Des nouveaux modèles physiques peuvent prédire un rapport d’embranchement de t → Hc de 0,15%. La recherche de ces désintégrations, avec un état final à deux ou trois leptons, n’observe aucun signal. Une limite supérieure sur le ratio d’embranchement de t → Hc (t → Hu) avec un niveau de confiance de 95% est observé à 0,16% (0,19%) avec une limite attendue de 0,15% (0,15%).Pour contourner la limitation du nombre insuffisant des collisions, le LHC et ses expériences prévoient un plan de mise à niveau ambitieux. Un système de démonstration est en service depuis 2015 et ses performances étudiées avec des données de calibrations et de collisions. / This doctoral thesis describes the search for the associated Higgs boson production with a pair of top quarks (tt̅H) in a dataset of proton-proton collisions at a center-of-mass energy of √s = 13 TeV and with an integrated luminosity of 36.1 fb⁻¹, recorded by the ATLAS detector in 2015 and 2016. Seven final states, associated to different Higgs boson decay, are optimised to get the best signal to background separation. An excess of events over the SM background is observed with a significance of 4.1 standard deviations, while 2.8 are expected. In combination with search results obtained for other Higgs boson decay channels, the tt̅H production has been discovered with the ATLAS detector using up to 79.8 fb⁻¹ of collision data at √s = 7, 8 and 13 TeV.Flavour-changing neutral currents in top quark decays into a Higgs boson and a light up-type quark (t → Hq) are strongly suppressed in the SM. New physics models can predict a t → Hc decay branching ratio of 0.15%. The search for these decays in final states with two or three leptons observes no signal. An upper limit on the t → Hc (t → Hu) decay branching ratio at a 95% confidence level is set at 0.16% (0.19%) with an expected limit of 0.15% (0.15%).To bypass the limitation of an insufficient amount of collision data, the LHC and its experiments foresee an ambitious upgrade plan. The current ATLAS Liquid Argon Calorimeter readout will be replaced to get an increased granularity to improve the trigger selectivity and avoid bandwidth saturation at high luminosity. A demonstrator system has been operated since 2015 and its performance studied with calibration and collision data.

La notion de symétrie de jauge est au coeur de notre compréhension de l'interaction électrofaible et permet d'expliquer l'ensemble des observations expérimentales actuelles. Pourtant, l'incompatibilité intrinsèque entre l'invariance de jauge et la masse des particules nécessite d'introduire une nouvelle particule, le boson de Higgs, toujours non observée à ce jour. Cette thèse présente l'analyse de 7.3/fb de collisions protons-antiprotons à sqrt{s} = 1.96 TeV enregistrées par le détecteur D0 au Tevatron en vue de la recherche du boson de Higgs dans l'état final mu+tau. Cette analyse vient compléter les canaux principaux dimuons, électron-muon et diélectrons en exploitant également la désintégration H -> WW -> lvlv, majoritaire dans la fenêtre de masse accessible au Tevatron. L'état final contenant un lepton tau, leur identification parmi les jets a été améliorée d'environ 15% grâce au développement de plusieurs idées : l'ajustement des paramètres du réseau de neurones d'identification, la prise en compte de certaines dépendances cinématiques des performances de l'algorithme, l'exploitation du temps de vie du lepton tau et une étude exhaustive visant à inclure la mesure du détecteur de pieds de gerbe dans le processus d'identification. Dans un second temps, la recherche du boson de Higgs dans l'état final mu+tau étant dominée par le bruit de fond W+jets (où un jet est faussement identifié comme un lepton tau), une méthode a été élaborée pour obtenir une modélisation convenable de ce bruit de fond, non fournie par la simulation par défaut. Cette méthode est basée, entre autres, sur l'étude de la corrélation de charge entre le muon et le candidat tau qui permet de mesurer ce bruit de fond dans les données en excluant la région du signal. Ensuite, l'exploitation des cinématiques et/ou topologies différentes du signal et du bruit de fond a permis d'optimiser cette recherche atteignant alors une sensibilité attendue (observée) de 7.8 (6.6) fois le Modèle Standard pour une masse de 165 GeV/c2. Enfin, l'interprétation de l'analyse dans un scénario à quatre familles de fermions a été effectuée. Pour la première fois, cette analyse est incluse dans les combinaisons D0 et Tevatron présentées à Moriond EW et EPS 2011. / The gauge symmetry is the heart of our understanding of the electroweak interaction and describes all the current experimental results. However, the intrinsic incompatibility between the gauge invariance and the mass of particles leads to the introduction of a new particle, the Higgs boson, for which we have no experimental evidence as of today. This thesis describes the Higgs boson search in the mu+tau final state in 7.3/fb of protons-antiprotons collisions at sqrt{s} = 1.96 TeV collected by the D0 detector at the Tevatron. This analysis completes the golden channels (dimuons, electron-muon, dielectrons) exploiting the decay chain H-> WW ->lvlv, which is the main Higgs boson decay mode in the mass window accessible to the Tevatron. Since the final state includes a tau lepton, work was done to improve their identification among jets. An increase of 15% was achieved thanks to the the following : changing tuning parameters for the tau identification neural network, use of the kinematical dependence of the algorithm performances, incorporation of the tau lepton life time information and full study of the additionnal information coming from the central preshower measurements. Then, since the dominant background of the mu+tau Higgs boson search is W+jets (where one jet fakes a tau), a method was developed to obtain good modeling of this background, not provided by the default simulation. This method is based, among other things, on the charge correlation between the muon and the tau candidate which allows for calibration of this background in the data excluding the signal region. Finally, all the kinematic and/or topological differences between the signal and the background were exploited to optimize this search, reaching an (observed) expected sensitivity of 7.8 (6.6) times the Standard Model for mH = 165 GeV/c2. In addition, this result was also interpreted in a fourth fermion generation scenario. For the first time, this analysis is included in the D0 and Tevatron combinations, both presented at Moriond EW and EPS 2011.

In the ATLAS experiment at the Large Hadron Collider (LHC) at CERN, direct searches for the elusive Higgs boson will be conducted, as well as for physics beyond the Standard Model. The charged Higgs boson (H±) is interesting both as a part of the Higgs sector, and as a clear sign of new physics. This thesis focuses on H± searches, with H± production in top-antitop pair events, and in particular the  bW± bH±, H±→τhadν, W±→qq channel. Its potential was investigated  as  part of a larger study of the expected performance of the entire ATLAS experiment. Full simulation of the ATLAS detector and trigger was used, and all dominant systematics considered. It was shown to be the most promising H± discovery channel for mH±&lt;mt. As hadronic τ decays are important for H± searches, their correct identification is critical. Possibilities of improving tau-jet identification in  pile-up and top-antitop pair events were investigated. Redundant or even performance-reducing variables in the default likelihood identification were identified, as were new variables showing discriminatory power. This allows for increased rejection of QCD jets in these environments, and higher robustness of the method. Before any physics studies, a commissioned and well-understood detector is required. The Lorentz angle of the ATLAS Semi-Conductor Tracker (SCT) barrel was measured using 2008 cosmic-ray data. It is an important observable for the performance of several detector aspects. Potential sources of systematics were investigated and evaluated. The Lorentz angle in the SCT barrel was measured as θL = 3.93 ± 0.03(stat) ± 0.10(syst) degrees, agreeing with the model prediction. The Compact Linear Collider (CLIC) is a proposed successor to the LHC. The potential for charged and heavy neutral Higgs bosons at CLIC was investigated, in terms of both discovery and precision measurement of parameters like tanβ or the Higgs masses, up to and beyond 1 TeV, which would be challenging at the LHC

The Standard Model of particle physics successfully describes present collider data. Nevertheless, theoretical and cosmological results call for its extension. A softly broken supersymmetric completion around the TeV scale solves several of the outstanding issues. Supersymmetry requires two Higgs doublets, leading to five physical Higgs states. These include a pair of charged Higgs bosons H±, which are a generic feature of theories with multiple Higgs doublets. Using results from high-energy colliders and flavour physics, constraints are derived on the charged Higgs boson mass and couplings; both for constrained scenarios in the minimal supersymmetric standard model (MSSM) with grand unification, and for general two-Higgs-doublet models. The MSSM results are compared to the projected reach for charged Higgs searches at the Large Hadron Collider (LHC). At the LHC, a light charged Higgs is accessible through top quark decay. Beyond a discovery, it is demonstrated how angular distributions sensitive to top quark spin correlations can be used to determine the structure of the H±tb coupling. The public code 2HDMC, which performs calculations in a general, CP-conserving, two-Higgs-doublet model, is introduced. In parallel to the developments at colliders, the most energetic particles ever recorded are the ultra-high-energy (UHE) cosmic rays. To gain more insight into their origin, new experiments are searching for UHE neutrinos. These searches require detectors of vast volume, which can be achieved by searching for coherent radio pulses arising from the Askaryan effect. The prospects of using a satellite orbiting the Moon to search for neutrino interactions are investigated, and a similar study for an Earth-based radio telescope is presented. In both cases, the method is found competitive for detection of the very highest energy neutrinos considered.

The Standard Model of the particle physics predicts the existence of a massive scalar boson, usually referred to as Higgs boson in the literature, as resulting from the Spontaneous Symmetry Breaking mechanism, needed to generate the mass of the particles. The Higgs boson whose mass is theoretically undetermined, is experimentally looked for since half a century by various experiments. This is the case of the ATLAS experiment at LHC which started taking data from high energy collisions in 2010. One of the most important decay channel in the LHC environment is the diphoton channel, because the final state can be completely reconstructed with high precision. The photon energy response is a key point in this analysis, as the signal would appear as a narrow resonance over a large background. In this thesis, a detailed study of the photon energy response, using the ATLAS electromagnetic calorimeter has been performed. This study has provided a better understanding of the photon energy resolution and scale, thus enabling an improvement of the sensitivity of the diphoton analysis as well as a precise determination of the systematic uncertainties on the peak position. The diphoton decay channel had a prominent role in the discovery of a new particle compatible with the Standard Model Higgs boson by the ATLAS and CMS experiments, that occurred in July 2012. Using this channel as well as the better understanding of the photon energy response, a measurement of the mass of this particle is proposed in this thesis, with the data collected in 2011 and 2012 at a center-of-mass energy of 7 TeV and 8 TeV. A mass of 126.8 +/- 0.2 (stat) +\- 0.7 (syst) GeV/c2 is found. The calibration of the photon energy measurement with the calorimeter is the source of the largest systematic uncertainty on this measurement. Strategies to reduce this systematic error are discussed.

Le Large Hadron Collider (LHC) au CERN (Organisation Européenne pour la Recherche Nucléaire) fonctionne depuis 2009 à la frontière franco-suisse. Cet accélérateur de particules a produit des quantités importantes de collisions proton-proton, à des énergies dans le centre de masse de 7 TeV (2010 et 2011), et 8 TeV (depuis avril 2012). L'un des buts de l'expérience Compact Muon Solenoid (CMS), qui enregistre et analyse ces collisions, est la recherche de bosons de Higgs. Dans le cadre du Modèle Standard, cette particule serait le quantum du champ de Higgs, qui permet d'expliquer le mécanisme de brisure de symétrie électrofaible. Un canal parmi les plus sensibles pour la recherche d'un boson de Higgs léger (c'est-à-dire pour des masses du boson de Higgs entre 90GeV/c2 et 150GeV/c2) au LHC est la désintégration en deux photons. En effet, la production de deux photons isolés de haute énergie dans l'état final constitue un signal clair en milieu hadronique, malgré le faible rapport d'embranchement. De plus, à ces masses, la largeur du pic en masse invariante reconstruite est dominée par la résolution du détecteur. Une compréhension fine de l'objet photon, tel que reconstruit par l'expérience, est donc un pré requis obligatoire. La première partie de mes travaux de thèse porte sur l'étude des désintégrations radiatives Z$^0 \rightarrow \mu\mu\gamma$ ces désintégrations sont la seule source de photons certifiés de haute pureté du Modèle Standard, pour laquelle l'impulsion transverse des photons est relativement proche de celle prévue pour des photons issus d'un boson de Higgs. L'étude de ces désintégrations a permis la détermination de l'échelle d'énergie différentielle des photons dans les données à 7 TeV. Elles ont également été utilisées dans les données à 8 TeV comme outil de validation des variables de forme de cluster pour les photons dans la simulation, ainsi que pour déterminer l'efficacité des critères de réjection des électrons. La deuxième partie de mes travaux de thèse traite de la recherche d'un boson de Higgs se désintégrant en deux photons. Cette recherche est effectuée en plusieurs classes d'évènements pour améliorer la sensibilité, et l'étude de cette procédure de séparation en classes est présentée. Enfin, une analyse de faisabilité de recherche d'un boson de Higgs se désintégrant en deux photons, produit lors de la désintégration d'un quark vecteur lourd à 14 TeV a été effectuée / The Large Hadron Collider (LHC) at CERN (European Organisation for Nuclear Research) has been in operation since 2009 at the border between France and Switzerland. This particle accelerator has provided a significant quantity of proton-proton collisions, at center of mass energies of 7 TeV (2010 and 2011) and 8 TeV (since April 2012). One of the purposes of the Compact Muon Solenoid (CMS) experiment, which records and analyses those collisions, is the search for Higgs bosons. In the Standard Model, this particle would be the quantum of the Higgs field, thought to explain the electroweak symmetry-breaking mechanism. One of the most sensitive channels for the search for a light Higgs boson (i.e. for masses between 90 GeV=c2 and 150 GeV=c2) at the LHC is through its decay into two photons. Indeed, the production of two highly energetic and isolated photons in the final state is a clean signal in hadronic collisions, despite the small branching ratio. Moreover, at these masses, the width of the reconstructed invariant mass peak is dominated by the detector resolution. Hence, a precise understanding of the photon object as reconstructed by the experiment is required. The first part of the work presented here is the study of radiative decays Z$^0 \rightarrow \mu\mu\gamma$ these decays are the only Standard Model source of high purity certified photons, for which the transverse momentum of the photon is relatively similar to the one of the photons coming from a Higgs boson decay. The study of these decays enables the determination of the differential photon energy scale in the 7 TeV data. These decays have also been used in the 8 TeV data as a validation tool of photon cluster shape variables in the simulation, and also as a way to determine the electron rejection criteria efficiency. The second part of the work concerns the search for a Higgs boson decaying into two photons. This search is done in several event classes in order to increase the sensitivity of the analysis, the study of the class separation procedure is presented. Finally, a benchmark study for the search for a Higgs boson decaying into two photons via vector-like top-partner decays at 14 TeV has been performed