Search results for "Bay"

showing 10 items of 1187 documents

An improved determination of the width of the top quark

2012

We present an improved determination of the total width of the top quark, $\Gamma_t$, using 5.4 fb$^{-1}$ of integrated luminosity collected by the D0 Collaboration at the Tevatron $p\bar{p}$ Collider. The total width $\Gamma_t$ is extracted from the partial decay width $\Gamma(t\to Wb)$ and the branching fraction $\mathcal{B}(t\to Wb)$. $\Gamma(t\to Wb)$ is obtained from the $t$-channel single top quark production cross section and $\mathcal{B}(t\to Wb)$ is measured in $t\bar{t}$ events. For a top mass of $172.5\;\rm GeV$, the resulting width is $\Gamma_t = 2.00^{+0.47}_{-0.43}$ GeV. This translates to a top-quark lifetime of $\tau_t = (3.29^{+0.90}_{-0.63})\times10^{-25}$ s. We also extra…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsTop quarkUnitarity010308 nuclear & particles physicsBranching fractionCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFOS: Physical sciencesLambda01 natural sciences7. Clean energyBottom quarkHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Experimental High Energy Physics0103 physical sciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSING[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Production (computer science)High Energy Physics::Experiment010306 general physics
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High scale mixing relations as a natural explanation for large neutrino mixing

2015

The origin of small mixing among the quarks and a large mixing among the neutrinos has been an open question in particle physics. In order to answer this question, we postulate general relations among the quarks and the leptonic mixing angles at a high scale, which could be the scale of Grand Unified Theories. The central idea of these relations is that the quark and the leptonic mixing angles can be unified at some high scale either due to some quark-lepton symmetry or some other underlying mechanism and as a consequence, the mixing angles of the leptonic sector are proportional to that of the quark sector. We investigate the phenomenology of the possible relations where the leptonic mixin…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsUnification010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstronomy and AstrophysicsNew Physics ; GUT ; CKM Matrix01 natural sciencesAtomic and Molecular Physics and OpticsHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesGrand Unified TheoryHigh Energy Physics::ExperimentNeutrino010306 general physicsPhenomenology (particle physics)International Journal of Modern Physics A
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Tree-level flavor-changing neutral currents in theBsystem: FromCPasymmetries to rare decays

2001

corresponding to 0.59 ≤ sin(2�) ≤ 0.82, which is cer- tainly outside the 1� Babar range but not outside the world average. This potential discrepancy is at the ori- gin of several papers (6) studying the implications of a small aJ/ in the search of new physics. In this paper, we analyze the implications of this situ- ation for a realistic model, obtained with the only addi- tion of an isosinglet down vector-like quark (7) to the SM spectrum. This model naturally arises, for instance, as the low-energy limit of an E6 grand unified theory. At a more phenomenological level, models with isosinglet quarks provide the simplest self-consistent framework to study deviations of 3 ×3 unitarity of the…

QuarkPhysicsNuclear and High Energy PhysicsParticle physicsUnitarityCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelGrand Unified TheoryB mesonQuarkoniumStandard ModelPhysical Review D
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Weak Mixing, CP Violation and Rare Decays

1989

This review summarizes experimental information on weak couplings of quark flavours from weak decays and weak production of heavy flavours and the relation of the observed direct CP violation to a non-trivial phase in the quark mixing matrix. The interest in this field is twofold: on the one side, we can measure precisely the parameters of the standard model in its own framework; on the other side, any inconsistency amongst these measurements or evidence for any process forbidden in the standard model will lead beyond that model.

QuarkPhysicsParticle physicsField (physics)Cabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyPhase (waves)CP violationHigh Energy Physics::ExperimentMeasure (mathematics)Mixing (physics)Standard Model
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Soft SUSY breaking grand unification: Leptons vs quarks on the flavor playground

2007

We systematically analyze the correlations between the various leptonic and hadronic flavor violating processes arising in SUSY Grand Unified Theories. Using the GUT-symmetric relations between the soft SUSY breaking parameters, we assess the impact of hadronic and leptonic flavor observables on the SUSY sources of flavor violation.

QuarkPhysicsParticle physicsNuclear and High Energy PhysicsAnomalous magnetic dipole momentCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesSupersymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Grand Unified TheoryCentre for High Energy PhysicsSoft SUSY breakingHigh Energy Physics::ExperimentMinimal Supersymmetric Standard ModelLepton
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Physical constraints on a class of two-Higgs doublet models with FCNC at tree level

2014

We analyse the constraints and some of the phenomenological implications of a class of two Higgs doublet models where there are flavour-changing neutral currents (FCNC) at tree level but the potentially dangerous FCNC couplings are suppressed by small entries of the CKM matrix V. This class of models have the remarkable feature that, as a result of a discrete symmetry of the Lagrangian, the FCNC couplings are entirely fixed in the quark sector by V and the ratio v 2/v 1 of the vevs of the neutral Higgs. The discrete symmetry is extended to the leptonic sector, so that there are FCNC in the leptonic sector with their flavour structure fixed by the leptonic mixing matrix. We analyse a large n…

QuarkPhysicsParticle physicsNuclear and High Energy PhysicsHiggs PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyStructure (category theory)FísicaFOS: Physical sciencesHigh Energy Physics - ExperimentMatrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Higgs Physics; Beyond Standard ModelBeyond Standard ModelHiggs bosonHigh Energy Physics::ExperimentTree (set theory)Mixing (physics)Discrete symmetryJournal of High Energy Physics
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A solution to the strong CP problem transforming the theta angle to the KM CP-violating phase

2010

It is shown that in the scheme with a rotating fermion mass matrix (i.e. one with a scale-dependent orientation in generation space) suggested earlier for explaining fermion mixing and mass hierarchy, the theta angle term in the QCD action of topological origin can be eliminated by chiral transformations, while giving still nonzero masses to all quarks. Instead, the effects of such transformations get transmitted by the rotation to the CKM matrix as the KM phase giving, for theta of order unity, a Jarlskog invariant typically of order 10(-5), as experimentally observed. Strong and weak CP violations appear then as just two facets of the same phenomenon.

QuarkPhysicsQuantum chromodynamicsHigh Energy Physics - TheoryNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics - Theory (hep-th)CP violationStrong CP problemInvariant (mathematics)Mixing (physics)
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Kl3Semileptonic Form Factor from (2+1)-Flavor Lattice QCD

2008

We present the first results for the ${K}_{l3}$ form factor from simulations with $2+1$ flavors of dynamical domain wall quarks. Combining our result, namely, ${f}_{+}(0)=0.964(5)$ with the latest experimental results for ${K}_{l3}$ decays leads to $|{V}_{us}|=0.2249(14)$, reducing the uncertaintity in this important parameter. For the $O({p}^{6})$ term in the chiral expansion we obtain $\ensuremath{\Delta}f=\ensuremath{-}0.013(5)$.

QuarkPhysicsQuantum chromodynamicsParticle physics010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixLattice field theoryForm factor (quantum field theory)General Physics and AstronomyLattice QCD01 natural sciencesDomain wall (magnetism)Lattice gauge theory0103 physical sciences010306 general physicsPhysical Review Letters
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Weak Mixing, CP Violation and the Standard Model

1990

These lectures summarize experimental information on weak couplings of quark flavours from weak decays and weak production of heavy flavours and the relation of the observed direct CP violation to a non-trivial phase in the quark mixing matrix. The interest in this field is twofold: on the one side, we can measure precisely the parameters of the standard model in its own framework; on the other side, any inconsistency amongst these measurements or evidence for any process forbidden in the standard model will lead beyond that model. The outline of these lectures is the following: 1. Weak Mixing of Quarks 1.1 Kobayashi-Maskawa-Matrix 1.2 Experimental Constraints on the KM Matrix 1.3 Allowed R…

QuarkPhysicsTop quarkParticle physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyCP violationPenguin diagramHigh Energy Physics::ExperimentPhenomenology (particle physics)Bottom quark
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Precision Measurement of the RatioB(t→Wb)/B(t→Wq)and Extraction ofVtb

2011

We present a measurement of the ratio of top quark branching fractions R = B(t -> Wb)/B(t -> Wq), where q can be a d, s or b quark, in the lepton+jets and dilepton ttbar final states. The measurement uses data from 5.4 fb-1 of ppbar collisions collected with the D0 detector at the Fermilab Tevatron Collider. We measure R = 0.90 +/- 0.04, and we extract the CKM matrix element |Vtb| as |Vtb| = 0.95 +/- 0.02, assuming unitarity of the 3x3 CKM matrix.

QuarkPhysicsTop quarkParticle physicsUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixBranching fractionHigh Energy Physics::PhenomenologyTevatronGeneral Physics and Astronomy7. Clean energy01 natural sciencesBottom quarkNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentFermilab010306 general physicsPhysical Review Letters
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