Search results for "Condensate"

showing 10 items of 208 documents

Dynamical Symmetry Breaking in Warped Compactifications

2001

We study dynamical electroweak symmetry breaking in the Randall-Sundrum scenario. We show that one extra dimension is enough to give the correct pattern of electroweak symmetry breaking in a simple model with gauge bosons and the right-handed top quark in the bulk. The top quark mass is also in agreement with experiment. Furthermore, we propose an extended scenario with all Standard Model gauge bosons and fermions propagating in the bulk, which naturally accommodates the fermion mass hierarchies. No new fields or interactions beyond the observed in the Standard Model are required.

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonSpontaneous symmetry breakingHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesTechnicolorTop quark condensateExplicit symmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Symmetry breakingChiral symmetry breaking
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Centrality dependence of the pseudorapidity density distribution for charged particles in Pb–Pb collisions at sNN=2.76 TeV

2017

We present the charged-particle pseudorapidity density in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02\,\mathrm{Te\kern-.25exV}$ in centrality classes measured by ALICE. The measurement covers a wide pseudorapidity range from $-3.5$ to $5$, which is sufficient for reliable estimates of the total number of charged particles produced in the collisions. For the most central (0-5%) collisions we find $21\,400\pm 1\,300$ while for the most peripheral (80-90%) we find $230\pm 38$. This corresponds to an increase of $(27\pm4)\%$ over the results at $\sqrt{s_{\mathrm{NN}}}=2.76\,\mathrm{Te\kern-.25exV}$ previously reported by ALICE. The energy dependence of the total number of charged particles…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsExtrapolation01 natural sciencesCharged particleColor-glass condensateNuclear physicsPseudorapidity0103 physical sciencesQuark–gluon plasmaRapidityImpact parameterCentralityNuclear Experiment010306 general physicsNucleonGlauberScalingPhysics Letters B
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Nuclear modification of forward J/ψ production in proton-nucleus collisions at the LHC

2016

We re-evaluate the nuclear suppression of forward J/ψ production at high energy in the Color Glass Condensate framework. We use the collinear approximation for the projectile proton probed at large x and an up to date dipole cross section fitted to HERA data to describe the target in proton-proton collisions. We show that using the Glauber approach to generalize the proton dipole cross section to the case of a nucleus target leads to a nuclear modification factor much closer to LHC data than previous estimates using the same framework.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderProtonta114010308 nuclear & particles physicsProjectileNuclear TheoryHERAquarkonia01 natural sciencesColor-glass condensateCross section (physics)DipoleCGC0103 physical sciencesBKNuclear Experiment010306 general physicsGlauberInternational Conference on Hard and Electromagnetic Probes of High Energy Nuclear Collisions
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Single inclusive particle production at high energy from HERA data to proton-nucleus collisions

2013

We study single inclusive hadron production in proton-proton and proton-nucleus collisions in the CGC framework. The parameters in the calculation are determined solely by standard nuclear geometry and by electron-proton deep inelastic scattering data, which is fit using the running coupling BK equation. We show that it is possible to obtain a good fit of the HERA inclusive cross section also without an anomalous dimension in the initial condition. We argue that one must consistently use the proton transverse area as measured by a high virtuality probe in DIS also for the single inclusive cross section in proton-proton and proton-nucleus collisions. We show that this leads to a midrapidity …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderProtonta114Nuclear Theory010308 nuclear & particles physicsHadronNuclear TheoryFOS: Physical sciencesHERACoupling (probability)Deep inelastic scattering01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)Nuclear physicsCross section (physics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear Experiment
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Centrality dependence of forward J/ψ suppression in high energy proton–nucleus collisions

2015

The production of forward $J/\psi$ mesons in proton-nucleus collisions can provide important information on gluon saturation. In a previous work we studied this process in the Color Glass Condensate framework, describing the target using a dipole cross section fitted to HERA inclusive data and extrapolated to the case of a nuclear target using the optical Glauber model. In this work we study the centrality dependence of the nuclear suppression in this model and compare our results with recent LHC data for this observable.

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Colliderta114Nuclear TheoryMeson010308 nuclear & particles physicsNuclear TheoryObservablequarkoniaHERABalitsky-Kovchegov equation01 natural sciencesColor-glass condensateGluonNuclear physicsHigh Energy Physics - PhenomenologyDipole0103 physical sciencescolor glass condensateHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsGlauberNuclear Physics A
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Small x physics and RHIC data

2010

This is a review of applications of the Color Glass Condensate to the phenomenology of relativistic heavy ion collisions. The initial stages of the collision can be understood in terms of the nonperturbatively strong nonlinear glasma color fields. We discuss how the CGC framework can and has been used to compute properties of the initial conditions of AA collisions. In particular this has led to recent progress in understanding multiparticle correlations, which can provide a directly observable signal of the properties of the initial stage of the collision process.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theoryta114010308 nuclear & particles physicsFOS: Physical sciencesGeneral Physics and AstronomyObservableCollisionDeep inelastic scattering01 natural sciencesColor-glass condensateNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesQuark–gluon plasmaBibliographyImpact parameterNuclear Experiment010306 general physicsPhenomenology (particle physics)Computer Science::DatabasesInternational Journal of Modern Physics E
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Particle production from the Color Glass Condensate: proton-nucleus collisions in light of the HERA data

2014

We compute single inclusive hadron production in proton-proton and proton-nucleus collisions consistently within the CGC framework. The parameters in the calculations are obtained from electron-proton DIS and standard nuclear geometry. We obtain a good description of the DIS data without an anomalous dimension in the initial condition of the BK evolution and get a good agreement with the available single inclusive proton-proton and proton-nucleus data.

PhysicsNuclear and High Energy PhysicsParticle physicsProtonNuclear Theoryta114HadronNuclear TheoryFOS: Physical sciencesHERA7. Clean energyColor-glass condensateNuclear physicsNuclear Theory (nucl-th)High Energy Physics - Phenomenologymedicine.anatomical_structureHigh Energy Physics - Phenomenology (hep-ph)medicineInitial value problemParticlePhysics::Accelerator PhysicsBoundary value problemNuclear ExperimentNucleus
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Electroweak and finite width corrections to top quark decays into transverse and longitudinal $ W $-bosons

2002

We calculate the electroweak and finite width corrections to the decay of an unpolarized top quark into a bottom quark and a $ W $-gauge boson where the helicities of the $ W $ are specified as longitudinal, transverse-plus and transverse-minus. Together with the $ O(\alpha_s) $ corrections these corrections may become relevant for the determination of the mass of the top quark through angular decay measurements.

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesTechnicolorTop quark condensateHelicityBottom quarkNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)W and Z bosonsHigh Energy Physics::ExperimentBoson
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IMPLICATIONS OF A LARGE $Ht \bar{t}$-COUPLING FOR THREE-BODY DECAYS OF HIGGS BOSON AND TOP QUARK

1991

The three-body decays a heavy Higgs [Formula: see text], [Formula: see text] and of a heavy top t → bW+ H are studied in the context of the Standard Model. The common feature of these decay channels is the relative big coupling constant of the Higgs particle to the top quark. Indeed within a certain range of the masses M H , mt we find that branching ratios of the order O(10-3) are possible for the decays [Formula: see text] and t → bW+ H. The decay with [Formula: see text] as a function of M H and mt is investigated below the 2mt threshold (Mtt < 2mt) and is found to have an interesting behaviour just near this threshold.

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkMesonBranching fractionGeneral Physics and AstronomyAstronomy and AstrophysicsElementary particleTop quark condensateQuarkoniumNuclear physicsParticle decayHiggs bosonModern Physics Letters A
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Measurement of the top quark mass in thelepton+jetsfinal state with the matrix element method

2006

We present a measurement of the top quark mass with the Matrix Element method in the lepton+jets final state. As the energy scale for calorimeter jets represents the dominant source of systematic uncertainty, the Matrix Element likelihood is extended by an additional parameter, which is defined as a global multiplicative factor applied to the standard energy scale. The top quark mass is obtained from a fit that yields the combined statistical and systematic jet energy scale uncertainty.

PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkScale (ratio)010308 nuclear & particles physicsTop quark condensateJet (particle physics)01 natural sciencesTransfer matrixParticle identificationNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentInvariant mass010306 general physicsLeptonPhysical Review D
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