Search results for "VIOLATION"

showing 10 items of 540 documents

Building the full Pontecorvo-Maki-Nakagawa-Sakata matrix from six independent Majorana-type phases

2009

In the framework of three light Majorana neutrinos, we show how to reconstruct, through the use of 3 x 3 unitarity, the full PMNS matrix from six independent Majorana-type phases. In particular, we express the strength of Dirac-type CP violation in terms of these Majorana-type phases by writing the area of the unitarity triangles in terms of these phases. We also study how these six Majorana phases appear in CP-odd weak-basis invariants as well as in leptonic asymmetries relevant for flavored leptogenesis.

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsmedia_common.quotation_subjectHigh Energy Physics::Phenomenology01 natural sciencesAsymmetryPhysics::History of PhysicsMassless particleMAJORANADouble beta decayLeptogenesis0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsParticle Physics - Phenomenologymedia_common
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Measurement ofCPobservables inB±→DCPK±decays and constraints on the CKM angleγ

2010

Using the entire sample of 467×10^6 Υ(4S)→BB[overbar] decays collected with the BABAR detector at the PEP-II asymmetric-energy B factory at the SLAC National Accelerator Laboratory, we perform an analysis of B^± → DK^± decays, using decay modes in which the neutral D meson decays to either CP-eigenstates or non-CP-eigenstates. We measure the partial decay rate charge asymmetries for CP-even and CP-odd D final states to be A_(CP+) = 0.25±0.06±0.02 and A_(CP-) = -0.09±0.07±0.02, respectively, where the first error is the statistical and the second is the systematic uncertainty. The parameter A_(CP+) is different from zero with a significance of 3.6 standard deviations, constituting evidence f…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityMeson010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrix01 natural sciencesB-factoryNuclear physicsParticle decay0103 physical sciencesD mesonCP violationB meson010306 general physicsPhysical Review D
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T Violation and CPT Tests in Neutral-Meson Systems

2014

The review covers transitions between M0 and M0bar in all four systems M0 = K0, D0, B0 and Bs. These systems are ideal laboratories for studying the discrete symmetries T and CPT. The properties of time reversal T are discussed in classical and quantum mechanics. T violation in K0 K0bar transitions has been observed in 1970 independent of assuming CPT symmetry by using the Bell-steinberger unitarity relation. Improvements of this observation are reviewed including the latest results in 2013. They show with high significance that CP violation in K0 K0bar transitions is only T violation without any CPT violation. Transitions in the other three systems do not show CP violation so far and there…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityMesonCPT symmetryFOS: Physical sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Homogeneous spaceBibliographyCP violationIdeal (ring theory)Neutrino oscillation
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Unitarity Triangles and the Search for New Physics

2002

Assuming that the Kobayashi-Maskawa mechanism gives the dominant contribution to CP violation at low energies, we propose a novel way of testing the flavour sector of the Standard Model which has the potencial for discovering New Physics. Using 3 x 3 unitarity of the V_{CKM} matrix and choosing a complete set of rephasing invariant phases, we derive a set of exact relations in terms of measurable quantities, namely moduli of V_{CKM} and arguments of rephasing invariant quartets. These tests complement the usual analysis in the \rho, \eta plane and, if there is New Physics, may reveal its source.

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarityPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesInvariant (physics)ModuliHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::Experiment
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Low energy neutrino factory for large theta(13)

2007

If the value of {theta}{sub 13} is within the reach of the upcoming generation of long-baseline experiments, T2K and NOvA, they show that a low-energy neutrino factory, with peak energy in the few GeV range, would provide a sensitive tool to explore CP-violation and the neutrino mass hierarchy. They consider baselines with typical length 1000-1500 km. The unique performance of the low energy neutrino factory is due to the rich neutrino oscillation pattern at energies between 1 and 4 GeV at baselines {Omicron}(1000) km. They perform both a semi-analytical study of the sensitivities and a numerical analysis to explore how well this setup can measure {theta}{sub 13}, CP-violation, and determin…

PhysicsNuclear and High Energy PhysicsParticle physicsbiologyFísicaOmicronbiology.organism_classificationNuclear physicsLow energyNeutrino detectorCP violationNeutrino FactoryInvariant massHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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Isospin dependence of the three-nucleon force

2004

We classify $A$--nucleon forces according to their isospin dependence and discuss the most general isospin structure of the three--nucleon force. We derive the leading and subleading isospin--breaking corrections to the three--nucleon force using the framework of chiral effective field theory.

PhysicsNuclear and High Energy PhysicsParticle physicschiral [symmetry]Weak isospinNuclear Theorynuclear forceeffective LagrangianHigh Energy Physics::PhenomenologyNuclear Theorythree-body problem [nucleon]FOS: Physical sciencesFew-body systemsdependence [isospin]Nuclear Theory (nucl-th)Quantum electrodynamicsIsospinEffective field theoryNuclear forceddc:530Symmetry breakingviolation [isospin]Quantum field theoryNucleonNuclear Experiment
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Invariants and flavour in the general Two Higgs Doublet Model

2012

The flavour structure of the general Two Higgs Doublet Model (2HDM) is analysed and a detailed study of the parameter space is presented, showing that flavour mixing in the 2HDM can be parametrized by various unitary matrices which arise from the misalignment in flavour space between pairs of various Hermitian flavour matrices which can be constructed within the model. This is entirely analogous to the generation of the CKM matrix in the Standard Model (SM). We construct weak basis invariants which can give insight into the physical implications of any flavour model, written in an arbitrary weak basis (WB) in the context of 2HDM. We apply this technique to two special cases, models with MFV…

PhysicsNuclear and High Energy PhysicsParticle physicsfísica010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFlavourFOS: Physical sciencesUnitary matrixCP-violationParameter space01 natural sciencesHermitian matrixQuark mass matricesBaryogenesisHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)Two-Higgs-doublet modelHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsParticle Physics - Phenomenology
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Summary of the Beauty '96 Conference

1996

Abstract We review a few important subjects of the Beauty '96 Conference. This includes, in particular, prospects for future experiments on CP violation in B decays.

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectBeautyCP violationInstrumentationmedia_commonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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CP violation through particle mixing and theH-Alineshape

2006

We consider the possibility of looking for CP-mixing effects in two-Higgs doublet models (and particularly in the MSSM) by studying the lineshape of the CP-even (H) and CP-odd (A) neutral scalars. In most cases H and A come quite degenerate in mass, and their s-channel production would lead to nearly overlapping resonances. CP-violating effects may connect these two Higgs bosons, giving origin to one-loop particle mixing, which, due to their mass proximity, can be resonantly enhanced. The corresponding transition amplitude contains then CP-even and CP-odd components; besides the signal of intereference between both amplitudes, leading to a CP-odd asymmetry, we propose to look for the mixing…

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectDegenerate energy levelsFísicaFOS: Physical sciencesContext (language use)AsymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeHiggs bosonCP violationMixing (physics)Bosonmedia_commonJournal of High Energy Physics
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Direct test of time reversal symmetry in the entangled neutral kaon system at a phi-factory

2013

We present a novel method to perform a direct T (time reversal) symmetry test in the neutral kaon system, independent of any CP and/or CPT symmetry tests. This is based on the comparison of suitable transition probabilities, where the required interchange of in out states for a given process is obtained exploiting the Einstein-Podolski-Rosen correlations of neutral kaon pairs produced at a phi-factory. In the time distribution between the two decays, we compare a reference transition like the one defined by the time-ordered decays (l(-), pi pi) with the T-conjugated one defined by (3 pi(0), l(+)). With the use of this and other T-conjugated comparisons, the KLOE-2 experiment at DA Phi NE co…

PhysicsNuclear and High Energy PhysicsParticle physicsphi-FactoryTime reversal violationCPT symmetryDiscrete symmetriesTime distributionQuantum entanglementdiscrete symmetries; time reversal violation; neutral kaons; phi-factory; φ-factoryNuclear physicsSymmetry testHigh Energy Physics - PhenomenologyT-symmetryViolació CP (Física nuclear)φ-factoryDirect testFactory (object-oriented programming)CP violationFísica nuclearHigh Energy Physics::ExperimentNeutral kaonsParticle Physics - Phenomenology
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