No description available.

A phenomenological study is made of several aspects of the standard model (and beyond) in the context of collider physics. These calculations are performed in the framework of Quantum Chromodynamics (QCD) and the standard Elec-troweak theory in an attempt to understand the underlying gauge theory more fully. In chapter 2, a precision QCD and electroweak calculation is performed to predict the high transverse-momentum distribution of the intermediate vector bosons produced in pṕ collisions. Calculated cross-sections are compared with data from the CERN collider and predictions are made for the Tevatron, LHC and SSC. Theoretical uncertainties, due to scale and structure function ambiguities, are estimated. In chapter 3, the equivalent photon approximation (or EPA) is studied at high energies to determine the accuracy of the approximation. An exact calculation of the process e + q → e + q + γ is performed and compared with an approximate calculation of the process γ+q → γ+q , where the initial-state photon is produced (using the EPA) from an initial-state electron. The test is carried out for the cases where the final-state electron are tagged and untagged. At high energies, the approximation is accurate to within 10%. In chapter 4, deep inelastic Compton scattering is investigated at energies of the HERA ep collider. A study of the production rate is made to determine the feasibility of measurement at HERA and it is clear that for pT < 50 GeV/c the cross-section will be measurable. In addition, studies are made to determine the efficiency of this process as a probe of the proton structure functions. The cross-section is only weakly dependent on the structure functions. In chapter 5, the production of charged Higgs scalars is considered at hadron colliders. The fully inclusive cross-section for charged Higgs scalars is calculated and compared with the associated W boson cross-section. The generic process g+b →b+t + t, which may proceed through an intermediate charged Higgs (or W) or through QCD processes, is studied and the Higgs cross-sections are compared with the W and QCD cross-sections.

Heavy quark decays provide a very advantageous investigation to test the Standard Model (SM). Recently, promising experiments with b quark, as well as the analysis of the huge data sets produced at the Large Hadron Collider(LHC) experiment, have led to an increasing study and sensitive measurements of relative b quark decays. In this thesis, a preliminary study is presented for the first time observation of the B+ → ψ(2S)φK+ with a statistical significance above 5 standard deviations using proton-proton collisions at √s = 8 TeV collected with CMS detector at LHC. The data sample, selected on the basis of the dimuon decay mode of the ψ(2S), corresponds to an integrated luminosity of 19.6 fb−1. A total of 140±15 B+ → ψ(2S)φK+ events have been observed. The branching fraction of B+ → ψ(2S)φK+ is measured relative to B+ → ψ(2S)K+, whose absolute branching fraction (BF) is known. The ratio is converted to an absolute branching fraction of B+ → ψ(2S)φK+, including systematics which is determined to be (4.0 ± 0.4(stat) ± 0.6(syst) ± 0.1(BR)) × 10−6, where the third uncertainty is due to imprecise knowledge of BF. The upper limit of the fraction of B+ → ψ(2S)(non−φ)K+ component in the selected B+ → ψ(2S)K+K−K+ channel is found to be 26% at 95% confidence level.

The Standard Model of particle physics describes all known elementary particles and their interactions. Despite its great experimental success, we know that the Standard Model is not a complete description of Nature and therefore new phenomena should be observed at higher energies. In the coming years the Large Hadron Collider will test the Standard Model by colliding protons with center of mass energies of up to 14 TeV providing some of the most stringent tests on the Standard Model. Experimental searches for Dark Matter provide a complementary program to test physics at the weak scale. In the near future new experimental data coming from direct detection experiments, and from satellites and telescopes will drastically improve our sensitivity to weak scale dark matter. This could lead to the first direct observation of dark matter, and thus of physics beyond the Standard Model. In this thesis I propose different extensions of the Standard Model and discuss their experimental consequences. I first discuss models for Axigluons, which are spin one particles in the adjoint representation of the SU(3) color gauge group. These models were motivated by the measurement of higher than predicted forward-backward asymmetry in top quark pair production at the Tevatron. I study different scenarios for Axigluon models that can explain the Tevatron result and explore their signatures at the Large Hadron Collider. Second I discuss the implications of ultraviolet scale invariance for the Standard Model, which has been advocated as a solution to the hierarchy problem. I show that in order to solve the hierarchy problem with scale invariance, new physics is required not far from the weak scale. In the last part of this thesis I propose a new model for dark matter, in which dark matter is charged under a hidden non-Abelian gauge group. This leads to modifications in the sensitivity of the usual experimental searches for dark matter in addition to distinct signatures in the Cosmic Microwave Background and in Large Scale Structure data.

A produção de J/, e 0 em colisões p+p a uma energia no referencial do centro de massa (ps) de 200 GeV foi estudada no Experimento PHENIX no RHIC. A amostra de dados coletada durante o período de aquisição de 2006 permitiu não somente a determinação das seções de choque absolutas, mas também o estudo da polarização de J/, através de seu decaimento no canal de dieltrons em região de rapidez central. As medidas incluem a dependência com o momento transverso e são comparadas com aquelas de outros experimentos em diferentes intervalos de rapidez e energias de colisão, e com previsões teóricas. A medida da polarização de J/, deve trazer limitações aos mecanismos de formação de charmonium e a medida de feed-down de J/, s provenientes de ´ é de importância para o entendimento da produção prompt de J/, assim como para a supressão observada em colisões A+A no RHIC. / The production of J/´psi´e ´psi´collisions at the nucleon center of mass energy ´(s pot.1/2)´ have been studied in the PHENIX Experiment at RHIC. The sample collected during the 2006 data taking period allowed not only the determination of absolute cross sections but also the study of J= polarization through its decays into the dielectron channel at mid rapidity. The measurements include transverse momentum dependence and are compared to that of other experiments in different rapidity ranges and collision energies and to theoretical model predictions. The J= polarization results should provide a constraint on charmonium formation mechanisms and the measurement of the feed down of 0 to J= is of importance for understanding prompt J= production as well as the suppression observed in A+A collisions at RHIC.

Dans les études présentées ici, seules les données collectées par le détecteur ATLAS sont analysées. La première partie du document décrit en détails le contexte théorique sous-jacent à ces études, ainsi que lecolllisioneur LHC et l'expérience ATLAS. Le LHC étant un collisionneur hadronique, l'identification et la reconstruction des leptons est cruciale pour les mesures précises de section efficaces des processus du Modèle Standard, ou la recherche de nouvelle physique. C'est pourquoi la deuxième partie du document est dédiée aux mesures de performances : mesures in situ des efficacités de reconstruction et d'identification des électrons. La recherche de nouvelle physique est présentée dans la troisième partie du document. Cette étude a été réalisée dans le canal incluant deux leptons de même charge et de l'énergie transverse manquante. Les résultats inclus ont été obtenus avec un ensemble de données collectées à $sqrt s$ = 8 TeV correspondant à une luminosité intégrée de L = 20 fb$^{-1}$, ainsi que les premières données collectées avec $sqrt s$ = 13 TeV. L'état final constitué d'une paire de leptons de même charge et de jets permet également la mesure directe du couplage de Yukawa pour le quark top, à l'aide du processus $ppto tbar tH$. Ce couplage est le plus élevé dans le Modèle Standard et associe les deux particules élémentaires les plus lourdes prédites par la théorie, le quark top et le boson de Higgs. Dans la quatrième partie de ce document, une étude complète de la sensibilité pouvant être atteinte avec une énergie de $sqrt s$ = 13TeV et une luminosité intégrée de 100 fb$^{-1}$ of data, est présentée pour le canal incluant deux leptons de même charge. / For the presented studies only the data recorded with the ATLAS detector is analyzed. The theoretical framework, the LHC collider and the ATLAS experiment are given in the first part of this thesis.At hadron colliders, the lepton identification and reconstruction are crucial for precise SM cross sections and coupling measurements or for new physics searches. Therefore, the second part of my thesis is dedicated to performance studies : in-situ measurements of electron identification and reconstruction efficiencies. The search for new physics is presented in the third part of the thesis. For these studies the channel with two same~- sign leptons and missing transverse energy is considered. The results are obtained with $L$~=~20 fb$^{-1}$ of data recorded at $sqrt s$ = 8 TeV and with the very first data at $sqrt s$ = 13 TeV. At the end of Run-1 no significant excess in data over the Standard Model prediction is observed and stringent limits on the supersymmetric particle masses are set. With the two same - sign leptons and jets final state it is also possible to measure directly the top quark Yukawa coupling using the ttbar + $H$ channel. This coupling is the largest in the Standard Model and it connects two of the heaviest particles predicted by the Standard Model, the top quark and the Higgs boson. In the fourth part of this thesis, a complete optimization is performed to reach the highest sensitivity for this signal in the two same~- sign leptons channel at $sqrt s$ = 13 TeV with 100 fb$^{-1}$ of data, corresponding to the end of Run-2.

We present in this thesis a detailed analysis of Higgs boson interactions at future colliders. In particular we examine, in a model independent way, the sensitivity of an Linear Collider in probing the interaction of Higgs boson with a pair of vector bosons with/without the use of polarized initial beams and/or the information on final state fermion polarization. We devise several observables which have definite transformation properties under discrete symmetry operations to constrain the different anomalous parts of the Higgs boson interactions having the same transformation properties. We also investigate effects of initial state radiation (ISR) and beamstrahlung on probes of anomalous Higgs boson couplings at higher center of mass energies. We begin the first chapter with an introduction of the Standard Model (SM) of particle physics. We mainly focus on the Higgs sector of the SM. In this chapter we review the electroweak (EW) symmetry breaking mechanism, viz. the Higgs mechanism, responsible for generating masses of all the particles in the SM. We briefly summarize the high precision tests of the SM. We discuss constraints on the mass of the SM Higgs boson derived from theoretical considerations such as stability of the electroweak vacuum, unitarity in scattering amplitudes, perturbativity of the Higgs self-coupling and no fine-tuning in the radiative corrections in the Higgs sector. Next we present the experimental bounds on the mass of the SM Higgs boson obtained from the direct searches of the Higgs boson at LEP and from the electroweak high precision measurements. We then discuss the importance of a general model independent approach to study properties of the Higgs boson and to verify the uniqueness of the SM. In the context of low energy effective theory, this analysis can be made by using the effective Lagrangian that contains higher dimensional operators. We conclude this chapter giving examples of dimension-6 operators which can contribute to the anomalous Higgs boson interactions that we analyze in this thesis. Second chapter contains the dominant Higgs boson production processes at an collider.In a model independent analysis we consider the effects of the most general ¯ (V = W Z) vertex, consistent with Lorentz invariance, for the process where f is any light fermion. This vertex also includes the possibility of CP violation and can be written as: where ki denote the momenta of the two W’s (Z’s), ǫναβis the antisymmetric tensor with ǫ0123 = 1. Previous studies showed that the squared matrix element of the process e+e−ZH does not include all the anomalous parts of a general ZZH vertex. Also it is obvious that one cannot analyse anomalous WWH couplings using this process. Hence we consider the full process e+e−ffH to probe all the anomalous parts of the VVH vertex. We devise a general and very elegant procedure to probe these couplings at an e+e−collider. We construct various combinations by taking dot and scalar triple product of momenta of initial and final state particles. These combinations have definite transformation properties under CP and naive time reversal (T˜)transformations. Hence the corresponding observables constructed using expectation value of sign of these combinations can probe a specific part of the anomalous VVH couplings whose coefficient in the effective Lagrangian has same transformation properties. We investigate the possible sensitivity to which the anomalous VVH couplings can be probed at a Linear Collider using these observables in the process e+e−ffH for unpolarized beams [1, 2]. We consider the case of a Linear Collider, operating at center of mass energy of 500 GeV, with an integrated luminosityof 500 fb−1 and assume a Higgs boson of mass 120 GeV. We impose various kinematical cuts on different final state particles to reduce backgrounds ¯and consider the events where H decays into bb with branching ratio 0.68. We can enhance or suppress the effect of the s-channel, Z-exchange diagram by imposing cut on the ¯invariant mass of the ff system. We use b-tagging efficiency to be 70%; a value expected to be possible in the collider environment. We first consider asymmetries involving either the polar or azimuthal angular distributions. Then we combine these informations to construct combined polar-azimuthal asymmetries in order to enhance the sensitivity. We obtain strong constraints on most of the anomalous parts of the ZZH vertex using cross section and these asymmetries. The process e+eν¯ −νH has two missing ν’s in the final state. Hence their momenta are not available to construct any observables. Therefore, direct probes for T˜-odd WWH couplings viz. ℑ(bW), ℜ(˜bW), cannot be constructed and only weak, indirect bounds are possible. Further, without using polarized beams the contamination from the ZZH vertex cannot be eliminated in the determination of WWH couplings. In the third chapter we analyze use of linearly polarized e+/e−beams and/or information on final state lepton polarization in probingthe interaction of the Higgs boson with a pair of vector bosons[3, 4]. We make several combinations of different particle momenta and spins. We then define observables as expectation values of signs of these combinations for longitudinally polarized beams and/or for production of final state τ’s with a definite helicity state. Use of polarization allows us to devise more observables as compared to the unpolarized case. We list the observables for which use of polarization affords a distinct gain in sensitivity. In our analysis we divide the total luminosity of 500 fb−1 equally among different polarization states of initial state e−/e+ and take the values 80% and 60% for e−/e+ respectively, foreseen at the ILC. We construct numerical combinations of various linearly polarized cross sections to enhance the contribution of ℜ(bZ) while getting rid of ΔaZand vice versa. It is necessary to construct such combinations of cross section as ℜ(bZ), ΔaZhave same CP and T˜transformation properties and hence there are no asymmetries that can be constructed to probe them individually. With these combinations it is possible to probe both these CP-and T˜-even couplings cleanly, using linearly polarized beams. We find that longitudinal beam polarization can improve the sensitivity to CP-odd ZZH couplings viz. ℜ(˜bZ), ℑ(˜bZ), by a factor of about 6 −7. We also construct observables for final state τ’s with definite helicity. We make a plausible assumption that it should be possible to isolate events with τ’s in definite helicity state with an efficiency of 40%. With this assumption we demonstrate that the use of final state τ polarization can improve the sensitivity to the CP-even and T˜-odd ZZH coupling (ℑ(bZ)) by a factor of about 3. Moreover use of final state τ-polarization measurement along with linearly polarized beams can improve the sensitivity for one of the CP-odd ZZH couplings (ℜ(˜bZ))bya factor of about 2.Use of longitudinally polarized beams can also help to reduce the contamination in the measurement of the WWH couplings coming from the ZZH vertex contribution. We also perform χ2-analysis using the observables for different polarizations. The cross section of the t–channel diagram increases with increasing center of mass energy. Therefore, off hand it may look like that going to higher energy can increase the sensitivity to WWH couplings. Hence in this chapter we further investigate possible gain in sensitivity going to higher center of mass energies[3, 4]. We use the same observables constructed with unpolarized beams and consider various center of mass energies ranging from 300 GeV to 3 TeV. We find that it is possible to increase the bZ)byabouta factor 2 1 TeVas compared to the case of 500 GeV. In this analysis we include the effects of initial state radiation (ISR) and beamstrahlung. Both the ISR and beamstrahlung =500 GeV, the ISR can affect cross sections for s–channel processes by 10−15%.However, we observe that the effects of ISR and beamstrahlung change both the SM and anomalous contributions more beneficial for the study of anomalous V V H couplings. In the last chapter we investigate the role of transversely polarized beams to constrain the anomalous V V H couplings[5]. Using transverse spin direction of e±it is possible to devise observables which are nonzero only for transversely polarized beams. Use of transverse beam polarization allows construction of completely independent probes of both the CP-and T˜-even anomalous ZZH couplings (ΔaZ, ℜ(bZ)), leading to independent determination of all the anomalous parts of the ZZH vertex. In addition the use of transverse beam polarization can also add to the sensitivity for one of the CP-odd ZZH couplings viz. ℜ(˜bZ). Measurement of final state τ-polarization with transversely polarized beams can in fact also offer improvement on the sensitivity for ℑ(bZ) which is even under CP-and odd under T˜-transformation. Use of transverse beam polarization cannot improve the bounds on the anomalous WWH couplings as the squared matrix element of the t– channel WW–fusion diagram does not have any transverse beam polarization dependent term. A summary of the results obtained in this thesis is follows. We have developed a general procedure to construct observables with specific CP and T˜transformation properties to probe various anomalous couplings of the Higgs boson to a pair of vector bosons (V = W/Z) at an e+/e−Linear Collider. We investigate probes of these couplings in the process e+e−ffH. This process gives access to those anomalous couplings which cannot be probed using angular distribution of the Z boson in the process e+eZH. We showed that it would be possible to obtain stringent bounds on some of the parts of the anomalous ZZH vertex even without using polarized beams and/or information on polarization of final state particles. Use of longitudinal beam polarization and/or final state τ polarization can significantly enhance the sensitivity in probing most of the anomalous parts of a general ZZH vertex. Use of longitudinal beam polarization also reduces the contamination from the ZZH couplings in the determination of the ˜T-even anomalous WWH couplings (ℜ(bW), ℑ(˜bW)). However, two missing neutrinos in the final state do not allow any direct probe of the T˜-odd WWH couplings (ℑ(bW), ℜ(˜bW)).We find that use of transverse polarization of the beams is essential to construct independent probes of the two anomalous ZZH couplings, which are even under CP and T˜transformations, viz.ΔaZand ℜ(bZ).We observed that there will be no significant gain 500 GeV), but with polarized beams is preferable from the point of view of studying anomalous V V H coupling. (For mathematical equations pl see the pdf file.)

No description available.

A produção de J/, e 0 em colisões p+p a uma energia no referencial do centro de massa (ps) de 200 GeV foi estudada no Experimento PHENIX no RHIC. A amostra de dados coletada durante o período de aquisição de 2006 permitiu não somente a determinação das seções de choque absolutas, mas também o estudo da polarização de J/, através de seu decaimento no canal de dieltrons em região de rapidez central. As medidas incluem a dependência com o momento transverso e são comparadas com aquelas de outros experimentos em diferentes intervalos de rapidez e energias de colisão, e com previsões teóricas. A medida da polarização de J/, deve trazer limitações aos mecanismos de formação de charmonium e a medida de feed-down de J/, s provenientes de ´ é de importância para o entendimento da produção prompt de J/, assim como para a supressão observada em colisões A+A no RHIC. / The production of J/´psi´e ´psi´collisions at the nucleon center of mass energy ´(s pot.1/2)´ have been studied in the PHENIX Experiment at RHIC. The sample collected during the 2006 data taking period allowed not only the determination of absolute cross sections but also the study of J= polarization through its decays into the dielectron channel at mid rapidity. The measurements include transverse momentum dependence and are compared to that of other experiments in different rapidity ranges and collision energies and to theoretical model predictions. The J= polarization results should provide a constraint on charmonium formation mechanisms and the measurement of the feed down of 0 to J= is of importance for understanding prompt J= production as well as the suppression observed in A+A collisions at RHIC.

No description available.