Search results for "Top quark condensate"

showing 10 items of 26 documents

Heavy quark impact factor and the single bottom production at the LHC

2014

Grigorios Chachamis Instituto de Fisica Corpuscular, Universitat de Valencia – Consejo Superior de Investigaciones Cientificas, Parc Cientific, E-46980 Paterna (Valencia), Spain E-mail: grigorios.chachamis@ific.uv.es Michal Deak∗ Instituto de Fisica Corpuscular, Universitat de Valencia – Consejo Superior de Investigaciones Cientificas, Parc Cientific, E-46980 Paterna (Valencia), Spain E-mail: michal.deak@ific.uv.es

Nuclear physicsQuarkPhysicsParticle physicsTop quarkLarge Hadron ColliderB mesonTop quark condensatePhenomenology (particle physics)Bottom quarkProceedings of XXI International Workshop on Deep-Inelastic Scattering and Related Subjects — PoS(DIS 2013)
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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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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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CORRELATIONS BETWEEN ε′/ε AND HEAVY TOP

1991

The paper reviews new theoretical developments for the CP-parameter ε′/ε and its intimate connection with the mass of a heavy top quark. It presents an extensive list of results and their implications for experiments.

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsGeneral Physics and AstronomyCP violationAstronomy and AstrophysicsTop quark condensateRenormalization groupBottom quarkConnection (mathematics)Modern Physics Letters A
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Top quark decay in the Aligned two-Higgs-doublet Model

2015

AbstractWe compute the one loop right and left anomalous tensor couplings (gR and gL, respectively) for the top quark, in the aligned two-Higgs-doublet model. They are the magnetic-like couplings in the most general parameterization of the tbW vertex. We find that the aligned two-Higgs doublet model, that includes as particular cases some of the most studied extensions of the Higgs sector, as Type I and II 2HDM, introduces new electroweak contributions and provides theoretical predictions that are very sensitive to both new scalar masses and the neutral scalar mixing angle. The model can account for new CP violation effects via the introduction of complex alignment parameters that have impo…

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLarge Hadron ColliderPhysics beyond the Standard ModelElectroweak interactionHigh Energy Physics::PhenomenologyTop quark condensatePartícules (Física nuclear)Two-Higgs-doublet modelsHiggs sectorTwo-Higgs-doublet modelCP violationNew physicsTop anomalous couplings
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Combination of searches for anomalous top quark couplings with 5.4 fb−1 of pp¯ collisions

2012

We present measurements of the tWb coupling form factors using information from electroweak single top quark production and from the helicity of W bosons from top quark decays in t (t) over bar events. We set upper limits on anomalous tWb coupling form factors using data collected with the DO detector at the Tevatron p (p) over bar collider corresponding to an integrated luminosity of 5.4 fb(-1).

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsLuminosity (scattering theory)010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionTevatronTop quark condensate01 natural sciencesHelicitylaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsColliderBosonPhysics Letters B
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NN Interaction in Chiral Constituent Quark Models

2003

We review the actual state in the description of the nucleon-nucleon (NN) interaction by means of chiral constituent quark models. We present a series of relevant features that are nicely explained within the quark model framework.

PhysicsParticle physicsSeries (mathematics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFlavourQuark modelConstituent quarkState (functional analysis)Top quark condensateNuclear ExperimentNuclear theory
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The non-perturbative unquenched quark model

2017

In recent years states in the quarkonium spectrum not expected in the naive quark model have appeared and created a lot of interest. In the theoretical side the study of the effect of meson-meson thresholds in the spectrum have been performed in different approximations. In a quark model framework, and in the spirit of the Cornell model, when a meson-meson threshold is included, the coupling to all the quark-antiquark states have to be considered. In practice only the closest states are included perturbatively. In this contribution we will present a framework in which we couple quark-antiquark states with meson-meson states non-perturbatively, taking into account effectively the coupling to…

PhysicsParticle physicsTop quark010308 nuclear & particles physicsHigh Energy Physics::LatticePhysicsQC1-999Quark modelNuclear TheoryHigh Energy Physics::PhenomenologyTop quark condensateQuarkonium01 natural sciencesBottom quark0103 physical sciencesB mesonHigh Energy Physics::ExperimentNon-perturbative010306 general physicsNuclear ExperimentX(3872)EPJ Web of Conferences
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