994 resultados para LARGE HADRON COLLIDER


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Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

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We present a study of eeγ and μμγ events using 1109 (1009) pb-1 of data in the electron (muon) channel, respectively. These data were collected with the DØ detector at the Fermilab Tevatron p over(p, ̄) collider at sqrt(s) = 1.96   TeV. Having observed 453 (515) candidates in the eeγ (μμγ) final state, we measure the Zγ production cross section for a photon with transverse energy ET > 7   GeV, separation between the photon and leptons Δ Rℓ γ > 0.7, and invariant mass of the di-lepton pair Mℓ ℓ > 30   GeV / c2, to be 4.96 ± 0.30 (stat . + syst .) ± 0.30 (lumi .)   pb, in agreement with the Standard Model prediction of 4.74 ± 0.22   pb. This is the most precise Zγ cross section measurement at a hadron collider. We set limits on anomalous trilinear Zγγ and ZZγ gauge boson couplings of - 0.085 < h30 γ < 0.084, - 0.0053 < h40 γ < 0.0054 and - 0.083 < h30 Z < 0.082, - 0.0053 < h40 Z < 0.0054 at the 95% C.L. for the form-factor scale Λ = 1.2   TeV.

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A measurement of the forward-backward asymmetry (AFB) of Drell-Yan lepton pairs in pp collisions at s=7TeV is presented. The data sample, collected with the CMS detector, corresponds to an integrated luminosity of 5fb-1. The asymmetry is measured as a function of dilepton mass and rapidity in the dielectron and dimuon channels. Combined results from the two channels are presented, and are compared with the standard model predictions. The AFB measurement in the dimuon channel and the combination of the two channels are the first such results obtained at a hadron collider. The measured asymmetries are consistent with the standard model predictions. © 2012 CERN.

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Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

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Conselho Nacional de Desenvolvimento Científico e Tecnológico (CNPq)

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Questa tesi si propone di investigare l'origine di effetti non gaussiani nella distribuzione del segnale del rivelatore Time of Flight (TOF) dell'esperimento A Large Ion Collider Experiment (ALICE). Con la presa dati iniziata nel 2009 si è infatti osservata un'asimmetria nel segnale la cui origine è ancora oggetto di studio. L'analisi svolta mostra come essa sia dovuta a motivi strumentali piuttosto che fenomenologici e permette quindi di correggere in parte questa anomalia migliorando la risoluzione del rivelatore. ALICE è uno dei quattro esperimenti allestiti lungo l'anello del LHC e ha come obiettivo principale verificare l'esistenza di prove sperimentali che confermino l'esistenza di un nuovo stadio della materia, il cosiddetto Quark Gluon Plasma (QGP). Secondo la Cromodinamica Quantistica (QCD), la teoria che descrive l'interazione forte, caratteristica fondamentale di quark e gluoni è il loro confinamento all'interno di adroni. Studi recenti nell'ambito della QCD non-perturbativa hanno tuttavia dimostrato che in condizioni estreme di densità di materia adronica e temperatura sarebbe possibile un'inversione di tendenza nell'andamento della costante di accoppiamento forte. Le condizioni necessarie alla formazione del QGP sono ben riproducibili nelle collisioni ad energie ultrarelativistiche tra ioni pesanti, come quelle che sono state prodotte a LHC negli ultimi due anni, fra ioni di piombo con energie del centro di massa pari a 2.76 TeV per coppia di nucleoni. L'esperimento ALICE si propone di studiarne i prodotti e poiché la molteplicità di particelle che si generano nell'urto e considerevole, e necessario un sistema di rivelazione che permetta l'identificazione di particelle cariche su un grande angolo solido e in un ampio intervallo di impulsi. Il TOF, utilizzando un particolare rivelatore a gas detto Multigap Resistive Plate Chamber (MRPC), svolge brillantemente questo compito permettendo di raggiungere una risoluzione temporale inferiore ai 100 ps.

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L'esperimento LHCb è stato progettato per eseguire misure di altissima precisione nel settore della fisica dei quark pesanti al Large Hadron Collidere del CERN. Sfruttando l'alta sezione d'urto di produzione di charm nelle interazioni protone-protone ad LHC e utilizzando la statistica raccolta durante il RUN-1, corrispondente ad una luminosità integrata di 3 fb{-1}, l'esperimento LHCb ha realizzato le misure più precise al mondo in questo settore. In particolare i decadimenti del mesone D0 in due corpi carichi senza leptoni nello stato finale hanno permesso di realizzare misure di violazione di CP} che raggiungono precisioni inferiori al 0.1 %. Da pochi mesi LHCb ha iniziato la seconda fase di presa dati, chiamata RUN-2, raccogliendo dati dalle interazioni protone-protone ad una energia nel centro di massa di sqrt{s}=13 TeV, superiore a quella del RUN-1. Le misure attuali di violazione di CP nel settore del charm, sono consistenti con l'ipotesi di non violazione. Il Modello Standard, pur con grandi incertezze teoriche, prevede una violazione di CP molto piccola, pertanto per verificare o meno l'esistenza di taleviolazione, sarà necessario sfruttare al massimo la statistica che verrà raccolta durante il RUN-2, ottimizzando gli algoritmi di selezione dei canali di interesse. In questa tesi verrà presentata uno studio preliminare che ha lo scopo di ottimizzare, mediante una tecnica di analisi multivariata, la selezione dei decadimenti D^*pm-> D0(K+K-)pi_s^pm e D^*pm}-> D0(pi+pi-)pi_s^pm} in previsione della prossima presa dati.

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Dr. Gates traces the history of physics leading to the hunt for the Higgs particle and confirmation of its existence in March 2013.

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We analyze transverse thrust in the framework of Soft Collinear Effective Theory and obtain a factorized expression for the cross section that permits resummation of terms enhanced in the dijet limit to arbitrary accuracy. The factorization theorem for this hadron-collider event-shape variable involves collinear emissions at different virtualities and suffers from a collinear anomaly. We compute all its ingredients at the one-loop order, and show that the two-loop input for next-to-next-to-leading logarithmic accuracy can be extracted numerically, from existing fixed-order codes.

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If magnetism is universal in nature, magnetic materials are ubiquitous. A life without magnetism is unthinkable and a day without the influence of a magnetic material is unimaginable. They find innumerable applications in the form of many passive and active devices namely, compass, electric motor, generator, microphone, loud speaker, maglev train, magnetic resonance imaging, data recording and reading, hadron collider etc. The list is endless. Such is the influence of magnetism and magnetic materials in ones day to day life. With the advent of nanoscience and nanotechnology, along with the emergence of new areas/fields such as spintronics, multiferroics and magnetic refrigeration, the importance of magnetism is ever increasing and attracting the attention of researchers worldwide. The search for a fluid which exhibits magnetism has been on for quite some time. However nature has not bestowed us with a magnetic fluid and hence it has been the dream of many researchers to synthesize a magnetic fluid which is thought to revolutionize many applications based on magnetism. The discovery of a magnetic fluid by Jacob Rabinow in the year 1952 paved the way for a new branch of Physics/Engineering which later became magnetic fluids. This gave birth to a new class of material called magnetorheological materials. Magnetorheological materials are considered superior to electrorheological materials in that magnetorheology is a contactless operation and often inexpensive.Most of the studies in the past on magnetorheological materials were based on magnetic fluids. Recently the focus has been on the solid state analogue of magnetic fluids which are called Magnetorheological Elastomers (MREs). The very word magnetorheological elastomer implies that the rheological properties of these materials can be altered by the influence of an external applied magnetic field and this process is reversible. If the application of an external magnetic field modifies the viscosity of a magnetic fluid, the effect of external magnetic stimuli on a magnetorheological elastomer is in the modification of its stiffness. They are reversible too. Magnetorheological materials exhibit variable stiffness and find applications in adaptive structures of aerospace, automotive civil and electrical engineering applications. The major advantage of MRE is that the particles are not able to settle with time and hence there is no need of a vessel to hold it. The possibility of hazardous waste leakage is no more with a solid MRE. Moreover, the particles in a solid MRE will not affect the performance and durability of the equipment. Usually MR solids work only in the pre yield region while MR fluids, typically work in the post yield state. The application of an external magnetic field modifies the stiffness constant, shear modulus and loss modulus which are complex quantities. In viscoelastic materials a part of the input energy is stored and released during each cycle and a part is dissipated as heat. The storage modulus G′ represents the capacity of the material to store energy of deformation, which contribute to material stiffness. The loss modulusG′′ represents the ability of the material to dissipate the energy of deformation. Such materials can find applications in the form of adaptive vibration absorbers (ATVAs), stiffness tunable mounts and variable impedance surfaces. MREs are an important material for automobile giants and became the focus of this research for eventual automatic vibration control, sound isolation, brakes, clutches and suspension systems

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We study the pair production of neutral Higgs bosons through gluon fusion at hadron colliders in the framework of the minimal supersymmetric standard model. We present analytical expressions for the relevant amplitudes, including both quark and squark loop contributions, and allowing for mixing between the superpartners of left- and right-handed quarks. Squark loop contributions can increase the cross section for the production of two CP-even Higgs bosons by more than two orders of magnitude, if the relevant trilinear soft breaking parameter is large and the mass of the lighter squark eigenstate is not too far above its current lower bound. In the region of large tan β, neutral Higgs boson pair production might even be observable in the 4b final state during the next run of the Fermilab Tevatron collider. ©1999 The American Physical Society.

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In this thesis we investigate the phenomenology of supersymmetric particles at hadron colliders beyond next-to-leading order (NLO) in perturbation theory. We discuss the foundations of Soft-Collinear Effective Theory (SCET) and, in particular, we explicitly construct the SCET Lagrangian for QCD. As an example, we discuss factorization and resummation for the Drell-Yan process in SCET. We use techniques from SCET to improve existing calculations of the production cross sections for slepton-pair production and top-squark-pair production at hadron colliders. As a first application, we implement soft-gluon resummation at next-to-next-to-next-to-leading logarithmic order (NNNLL) for slepton-pair production in the minimal supersymmetric extension of the Standard Model (MSSM). This approach resums large logarithmic corrections arising from the dynamical enhancement of the partonic threshold region caused by steeply falling parton luminosities. We evaluate the resummed invariant-mass distribution and total cross section for slepton-pair production at the Tevatron and LHC and we match these results, in the threshold region, onto NLO fixed-order calculations. As a second application we present the most precise predictions available for top-squark-pair production total cross sections at the LHC. These results are based on approximate NNLO formulas in fixed-order perturbation theory, which completely determine the coefficients multiplying the singular plus distributions. The analysis of the threshold region is carried out in pair invariant mass (PIM) kinematics and in single-particle inclusive (1PI) kinematics. We then match our results in the threshold region onto the exact fixed-order NLO results and perform a detailed numerical analysis of the total cross section.

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A search for new physics using three-lepton (trilepton) data collected with the CDF II detector and corresponding to an integrated luminosity of 976 pb-1 is presented. The standard model predicts a low rate of trilepton events, which makes some supersymmetric processes, such as chargino-neutralino production, measurable in this channel. The mu+mu+l signature is investigated, where l is an electron or a muon, with the additional requirement of large missing transverse energy. In this analysis, the lepton transverse momenta with respect to the beam direction (pT) are as low as 5 GeV/c, a selection that improves the sensitivity to particles which are light as well as to ones which result in leptonically decaying tau leptons. At the same time, this low-p_T selection presents additional challenges due to the non-negligible heavy-quark background at low lepton momenta. This background is measured with an innovative technique using experimental data. Several dimuon and trilepton control regions are investigated, and good agreement between experimental results and standard-model predictions is observed. In the signal region, we observe one three-muon event and expect 0.4+/-0.1 mu+mu+l events

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We reconstruct B+/- -> D K+/- decays in a data sample collected by the CDF II detector at the Tevatron collider corresponding to 1 fb-1 of integrated luminosity. We select decay modes where the D meson decays to either K- pi+ (flavor eigenstate) or K- K+, pi- pi+ (CP-even eigenstates), and measure the direct CP asymmetry A_CP+ = 0.39 +/- 0.17(stat) +/- 0.04(syst), and the double ratio of CP-even to flavor eigenstate branching fractions R_CP+ = 1.30 +/- 0.24(stat) +/- 0.12(syst). These measurements will improve the determination of the CKM angle gamma. They are performed here for the first time using data from hadron collisions.