Search results for "viola"

showing 10 items of 697 documents

The Neutral K Meson System

2003

After the observation of direct CP violation in the neutral kaon system in 1988, it became clear that the Kobayashi-Maskawa mechanism of weak quark mixing was the most likely and most natural candidate for explaining this phenomenon. It seemed natural, therefore, that the same mechanism would also produce observable CP-violating effects in other neutral meson systems. The B0 system is the evident candidate for observing CP violation in another physical system described in this chapter.

PhysicsQuarkParticle physicsMesonHigh Energy Physics::PhenomenologyEta mesonPhysical systemBaBar experimentCP violationHigh Energy Physics::ExperimentObservableMixing (physics)
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Jarlskog-like invariants for theories with scalars and fermions

1994

Within the framework of theories where both scalars and fermions are present, we develop a systematic prescription for the construction of CP-violating quantities that are invariant under basis transformations of those matter fields. In theories with Spontaneous Symmetry Breaking, the analysis involves the vevs' transformation properties under a scalar basis change, with a considerable simplification of the study of CP violation in the scalar sector. These techniques are then applied in detail to the two Higgs-doublet model with quarks. It is shown that there are new invariants involving scalar-fermion interactions, besides those already derived in previous analyses for the fermion-gauge an…

PhysicsQuarkParticle physicsSpontaneous symmetry breakingHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaElementary particleFermionTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationSymmetry breakingInvariant (mathematics)
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CP Properties of Higgs Boson Interactions with Top Quarks in the tt¯H and tH Processes Using H→γγ with the ATLAS Detector

2020

A study of the charge conjugation and parity (CP) properties of the interaction between the Higgs boson and top quarks is presented. Higgs bosons are identified via the diphoton decay channel (H→γγ), and their production in association with a top quark pair (tt[over ¯]H) or single top quark (tH) is studied. The analysis uses 139  fb^{-1} of proton-proton collision data recorded at a center-of-mass energy of sqrt[s]=13  TeV with the ATLAS detector at the Large Hadron Collider. Assuming a CP-even coupling, the tt[over ¯]H process is observed with a significance of 5.2 standard deviations. The measured cross section times H→γγ branching ratio is 1.64_{-0.36}^{+0.38}(stat)_{-0.14}^{+0.17}(sys) …

PhysicsQuarkTop quarkParticle physicsLarge Hadron ColliderBranching fractionGeneral Physics and AstronomyParity (physics)7. Clean energy01 natural sciences0103 physical sciencesHiggs bosonCP violationHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsBosonPhysical Review Letters
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Impact of New Physics on CP-Asymmetries at Long Baselines

2018

We study the impact of new physics on CP-asymmetries using different oscillation channels at long baseline experiments.

PhysicsSterile neutrinoParticle physicsOscillationPhysics beyond the Standard ModelCP violationBaseline (configuration management)Neutrino oscillation
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Improved measurement of the CKM angleγinB∓→D(*)K(*)∓decays with a Dalitz plot analysis ofDdecays toKS0π+π−andKS0K+K−

2008

We report on an improved measurement of the Cabibbo-Kobayashi-Maskawa CP-violating phase {gamma} through a Dalitz plot analysis of neutral D meson decays to K{sub s}{sup 0}{pi}{sup +}{pi}{sup -} and K{sub s}{sup 0}K{sup +}K{sup -} produced in the processes B{sup {-+}} {yields} DK{sup {-+}}, B{sup {-+}} {yields} D* K{sup {-+}} with D* {yields} D{pi}{sup 0}, D{gamma}, and B{sup {-+}} {yields} DK*{sup {-+}} with K8{sup {-+}} {yields} K{sub S}{sup 0}{pi}{sup {-+}}. Using a sample of 383 million B{bar B} pairs collected by the BABAR detector, we measure {gamma} = (76 {+-} 22 {+-} 5{+-} 5){sup o} (mod 180{sup o}), where the first error is statistical, the second is the experimental systematic unc…

PhysicsSystematic errorNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectron–positron annihilationDalitz plot01 natural sciencesCrystallographyParticle decayTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesD mesonPiCP violation010306 general physicsBar (unit)Physical Review D
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Measurement of Top Quark Polarization in Top-Antitop Events from Proton-Proton Collisions ats=7  TeVUsing the ATLAS Detector

2013

This Letter presents measurements of the polarization of the top quark in top-antitop quark pair events, using 4: 7 fb(-1) of proton-proton collision data recorded with the ATLAS detector at the La ...

PhysicsTop quarkParticle physicsMuon010308 nuclear & particles physicsAtlas (topology)High Energy Physics::PhenomenologyNuclear TheoryGeneral Physics and AstronomyElectronPolarization (waves)01 natural sciencesNuclear physicsPair production0103 physical sciencesPhysics::Atomic and Molecular ClustersCP violationHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsLeptonPhysical Review Letters
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Underlying A_4 Symmetry for the Neutrino Mass Matrix and the Quark Mixing Matrix

2002

The discrete non-Abelian symmetry $A_4$, valid at some high-energy scale, naturally leads to degenerate neutrino masses, without spoiling the hierarchy of charged-lepton masses. Realistic neutrino mass splittings and mixing angles (one of which is necessarily maximal and the other large) are then induced radiatively in the context of softly broken supersymmetry. The quark mixing matrix is also calculable in a similar way. The mixing parameter $U_{e3}$ is predicted to be imaginary, leading to maximal CP violation in neutrino oscillations. Neutrinoless double beta decay and $\tau \to \mu \gamma$ should be in the experimentally accessible range.

PhysicsTribimaximal mixingParticle physicsNuclear and High Energy PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaMass matrixHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)
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Working group report: Neutrino physics

2009

This is the report of the neutrino physics working group at WHEPP-X. We summarize the problems selected and discussed at the workshop and the papers which have resulted subsequently.

Physicsline-experiment-simulatorParticle physicsGroup (mathematics)Solar neutrinooscillation experimentsGeneral Physics and AstronomyNeutrino Mass ModelsSolar neutrino problemPhysics and Astronomy(all)Oscillation ExperimentsNeutrino OscillationsNuclear physicsLeptogenesisLine-Experiment-SimulatorLeptogenesisPhysical Sciences and MathematicsMeasurements of neutrino speedNeutrinoLepton Flavour ViolationNeutrino oscillation
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Precision Measurement ofCPViolation inBS0→J/ΨK+K−Decays

2015

The time-dependent CP asymmetry in B-S(0) -> J/Psi K+K- decays is measured using pp collision data, corresponding to an integrated luminosity of 3.0 fb(-1), collected with the LHCb detector at center-of-mass energies of 7 and 8 TeV. In a sample of 96 000 B-S(0) -> J/Psi K+K- decays, the CP-violating phase phi(s) is measured, as well as the decay widths GL and GH of the light and heavy mass eigenstates of the B-s(0)-(B) over bar (0)(s) system. The values obtained are phi(s) = -0.058 +/- 0.049 +/- 0.006 rad, Gamma(s) equivalent to (Gamma(L) + Gamma(H))/2 = 0.6603 +/- 0.0027 +/- 0.0015 ps(-1), and Delta Gamma(s) equivalent to Gamma(L)-Gamma(H) = 0.0805 +/- 0.0091 +/- 0.0032 ps(-1), where the f…

Physicsmedia_common.quotation_subjectAnalytical chemistryGeneral Physics and AstronomyCP violationHigh Energy Physics::ExperimentAtomic physicsAsymmetryBar (unit)Luminositymedia_commonStandard ModelPhysical Review Letters
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New physics vs new paradigms: distinguishing CPT violation from NSI

2019

Our way of describing Nature is based on local relativistic quantum field theories, and then CPT symmetry, a natural consequence of Lorentz invariance, locality and hermiticity of the Hamiltonian, is one of the few if not the only prediction that all of them share. Therefore, testing CPT invariance does not test a particular model but the whole paradigm. Current and future long baseline experiments will assess the status of CPT in the neutrino sector at an unprecedented level and thus its distinction from similar experimental signatures arising from non-standard interactions is imperative. Whether the whole paradigm is at stake or just the standard model of neutrinos crucially depends on th…

Physics::General PhysicsPhysics and Astronomy (miscellaneous)CPT symmetryPhysics beyond the Standard ModelFOS: Physical scienceslcsh:AstrophysicsLorentz covariance01 natural sciencesPartícules (Física nuclear)High Energy Physics - Experimentsymbols.namesakeTheoretical physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)lcsh:QB460-4660103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivityQuantum field theory010306 general physicsEngineering (miscellaneous)Physics010308 nuclear & particles physicsLocalityHigh Energy Physics::PhenomenologyHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentNeutrinoHamiltonian (quantum mechanics)
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