Search results for "CP VIOLATION"

showing 10 items of 443 documents

Measurement of the D→K−π+ strong phase difference in ψ(3770)→D0D¯0

2014

Abstract We study D 0 D ¯ 0 pairs produced in e + e − collisions at s = 3.773 GeV using a data sample of 2.92 fb−1 collected with the BESIII detector. We measured the asymmetry A K π CP of the branching fractions of D → K − π + in CP-odd and CP-even eigenstates to be ( 12.7 ± 1.3 ± 0.7 ) × 10 − 2 . A K π CP can be used to extract the strong phase difference δ K π between the doubly Cabibbo-suppressed process D ¯ 0 → K − π + and the Cabibbo-favored process D 0 → K − π + . Using world-average values of external parameters, we obtain cos δ K π = 1.02 ± 0.11 ± 0.06 ± 0.01 . Here, the first and second uncertainties are statistical and systematic, respectively, while the third uncertainty arises …

Phase differencePhysicsNuclear and High Energy Physicsmedia_common.quotation_subjectElectron–positron annihilationQuantum mechanicsAnalytical chemistryPiCP violation7. Clean energyAsymmetrymedia_commonPhysics Letters B
researchProduct

Mixing asymmetries inBmeson systems, the D0 like-sign dimuon asymmetry, and generic new physics

2015

The measurement of a large like-sign dimuon asymmetry $A^b_{SL}$ by the D0 experiment at the Tevatron departs noticeably from Standard Model expectations and it may be interpreted as a hint of physics beyond the Standard Model contributing to $\Delta B\neq 0$ transitions. In this work we analyse how the natural suppression of $A^b_{SL}$ in the SM can be circumvented by New Physics. We consider generic Standard Model extensions where the charged current mixing matrix is enlarged with respect to the usual $3\times 3$ unitary Cabibbo-Kobayashi-Maskawa matrix, and show how, within this framework, a significant enhancement over Standard Model expectations for $A^b_{SL}$ is easily reachable throu…

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard Modelmedia_common.quotation_subjectTevatronFísicaFOS: Physical sciencesAsymmetryHigh Energy Physics - Experiment3. Good healthStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)CP violationB mesonCharged currentMixing (physics)media_commonPhysical Review D
researchProduct

Measuring the leptonic CP phase in neutrino oscillations with nonunitary mixing

2017

Non-unitary neutrino mixing implies an extra CP violating phase that can fake the leptonic Dirac CP phase $\delta_{CP}$ of the simplest three-neutrino mixing benchmark scheme. This would hinder the possibility of probing for CP violation in accelerator-type experiments. We take T2K and T2HK as examples to demonstrate the degeneracy between the "standard" (or "unitary") and "non-unitary" CP phases. We find, under the assumption of non-unitary mixing, that their CP sensitivities severely deteriorate. Fortunately, the TNT2K proposal of supplementing T2(H)K with a $\mu$DAR source for better measurement of $\delta_{CP}$ can partially break the CP degeneracy by probing both $\cos \delta_{CP}$ and…

PhysicsParticle physicsUnitarity010308 nuclear & particles physicsFOS: Physical sciencesUnitary state01 natural sciencesPartícules (Física nuclear)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Violació CP (Física nuclear)0103 physical sciencesCP violationStatistical analysisNeutrino010306 general physicsDegeneracy (mathematics)Neutrino oscillation
researchProduct

Impact of CP-violation on neutrino lepton number asymmetries revisited

2017

We revisit the effect of the (Dirac) CP-violating phase on neutrino lepton number asymmetries in both mass- and flavor-basis. We found that, even if there are sizable effects on muon- and tau-neutrino asymmetries, the effect on the asymmetry of electron-neutrinos is at most similar to the upper bound set by BBN for initial neutrino degeneracy parameters smaller than order unity. We also found that, for the asymmetries in mass-basis, the changes caused by CP-violation is of sub-\% level which is unlikely to be accesible neither in the current nor in the forthcoming experiments.

Particle physicsNuclear and High Energy PhysicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Physics::Instrumentation and Detectorsmedia_common.quotation_subjectFOS: Physical sciences01 natural sciencesAsymmetryNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNeutrino oscillationmedia_commonPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyLepton numberlcsh:QC1-999Massless particleHigh Energy Physics - PhenomenologyCP violationHigh Energy Physics::ExperimentNeutrinolcsh:PhysicsLeptonAstrophysics - Cosmology and Nongalactic Astrophysics
researchProduct

Neutrino oscillations and new physics

2005

I discuss the theoretical background and the status of neutrino oscillation parameters from the current worlds' global data sample and latest flux calculations. I give their allowed ranges, best fit values and discuss the small parameters and sin2theta13, which characterize CP violation in neutrino oscillations. I mention the significance of neutrinoless double beta decay and current expectations in view of oscillation results.

PhysicsNuclear and High Energy PhysicsParticle physicsOscillationPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFluxFOS: Physical sciencesFísicaAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayCP violationHigh Energy Physics::ExperimentNeutrino oscillation
researchProduct

A measurement of the phases of the CP-violating amplitudes in K0→2π decays and a test of CPT invariance

1990

Abstract The phases of the CP-violating amplitudes in K0→π+π− and K0→2π0 decays, φ+−=46.9°±2.2° and φ00=47.1°±2.8°, have been measured in the same experiment, and a direct comparison gives the phase difference φ00−φ+−=0.2°±2.9°. This result leads to an upper limit on possible CPT violation in the K0 mass matrix, of |(m K 0 −m K 0 )/m K 0 | −18 at the 95% confidence level and is the most stringent test of the equality of particle and antiparticle masses.

Phase differencePhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsAntiparticleAmplitudeCPT symmetryCP violationLimit (mathematics)Mass matrixlcsh:Physicslcsh:QC1-999Physics Letters B
researchProduct

Study ofB−→DK−π+π−andB−→Dπ−π+π−decays and determination of the CKM angleγ

2015

We report a study of the suppressed B- -> DK-pi(+)pi(-) and favored B- -> D pi(-)pi(+)pi(-) decays, where the neutral D meson is detected through its decays to the K--/+pi(+/-) and CP -even K+K- and pi(+)pi(-) final states. The measurement is carried out using a proton-proton collision data sample collected by the LHCb experiment, corresponding to an integrated luminosity of 3.0 fb(-1). We observe the first significant signals in the CP - even final states of the D meson for both the suppressed B- -> DK-pi(+)pi(-) and favored B- -> D pi(-)pi(+)pi(-) modes, as well as in the doubly Cabibbo suppressed D -> K+pi(-) final state of the B- -> D pi(-)pi(+)pi(-) decay. Evidence for the suppressed d…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixAnalytical chemistry01 natural sciences0103 physical sciencesD mesonPiCP violation010306 general physicsConjugatePhysical Review D
researchProduct

Measurement of branching fractions in radiativeBdecays toηKγand search forBdecays toη′Kγ

2006

We present measurements of the B ->eta K gamma branching fractions and upper limits for the B ->eta K-'gamma branching fractions. For B+->eta K+gamma we also measure the time-integrated charge asymmetry. The data sample, collected with the BABAR detector at the Stanford Linear Accelerator Center, represents 232x10(6) produced B (B) over bar pairs. The results for branching fractions and upper limits at 90% confidence level in units of 10(-6) are: B(B-0 ->eta K-0 gamma)=11.3(-2.6)(+2.8)+/- 0.6, B(B+->eta K+gamma)=10.0 +/- 1.3 +/- 0.5, B(B-0 ->eta K-'(0)gamma) eta K-'(+)gamma) eta K+gamma is A(ch)=-0.09 +/- 0.12 +/- 0.01. The first errors are statistical and the second systematic.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationAnalytical chemistryBranching (polymer chemistry)01 natural sciencesParticle identificationParticle decay0103 physical sciencesRadiative transferCP violationAtomic physics010306 general physicsPhysical Review D
researchProduct

The Cabibbo angle as a universal seed for quark and lepton mixings

2015

A model-independent ansatz to describe lepton and quark mixing in a unified way is suggested based upon the Cabibbo angle. In our framework neutrinos mix in a "Bi-Large" fashion, while the charged leptons mix as the "down-type" quarks do. In addition to the standard Wolfenstein parameters (lambda, A) two other free parameters are needed to specify the physical lepton mixing matrix. Through this simple assumption one makes specific predictions for the atmospheric angle as well as leptonic CP violation in good agreement with current observations.

QuarkNuclear and High Energy PhysicsParticle physicsPMNS matrixPhysics beyond the Standard ModelPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)ddc:530Mixing (physics)PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaBi-Large mixinglcsh:QC1-999High Energy Physics - PhenomenologyCKM matrixCabibbo angleCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino mixingWolfenstein parameterlcsh:PhysicsLepton
researchProduct

CP and T violation in neutrino oscillations

2000

The conditions to induce appreciable CP-and T-odd effects in neutrino oscillations are discussed. The propagation in matter leads to fake CP-and CPT-odd asymmetries, besides a Bohm-Aharonov type modification of the interference pattern. We study the separation of fake and genuine CP violation by means of energy and distance dependence.

PhysicsHigh Energy Physics - PhenomenologyNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - Phenomenology (hep-ph)FísicaCP violationFOS: Physical sciencesHigh Energy Physics::ExperimentNeutrino oscillationAtomic and Molecular Physics and OpticsEnergy (signal processing)
researchProduct