Search results for "DECAY"

showing 10 items of 2087 documents

Search for Dimuon Decays of a Light Scalar Boson in Radiative Transitions Υ→γA0

2009

We search for evidence of a light scalar boson in the radiative decays of the {Upsilon}(2S) and {Upsilon}(3S) resonances: {Upsilon}(2S, 3S) {yields} {gamma}A{sup 0}, A{sup 0} {yields} {mu}{sup +}{mu}{sup -}. Such a particle appears in extensions of the Standaard Model, where a light CP-odd Higgs boson naturally couples strongly to b-quarks. We find no evidence for such processes in the mass range 0.212 {<=} m{sub A{sup 0}} {<=} 9.3 GeV in the samples of 99 x 10{sup 6} {Upsilon}(2S) and 122 x 10{sup 6} {Upsilon}(3S) decays collected by the BABAR detector at the PEP-II B-factory and set stringent upper limits on the effective coupling of the b quark to the A{sup 0}. We also limit the dimuon b…

PhysicsParticle physicsMuonMeson010308 nuclear & particles physicsBranching fractionParticle physicsGeneral Physics and AstronomyElementary particleBABAR detectorScalar bosonCoupling (probability)01 natural sciencesHEPParticle decayBaBar0103 physical sciencesFísica de partículesExperiments010306 general physicsBoson
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Flavor Changing Yukawa Coupling in the Standard Model and Muon Polarization in KL-->mumu¯

1986

The muon longitudinal polarization P/sub L/ in K/sub L/..--> mu..mu-bar decay is investigated in the standard model. The induced s-bardH vertex responsible for P/sub L/ turns out to be unexpectedly ''large.'' The measurement of P/sub L/ above approx.10/sup -3/ will, therefore, be a signal of the existence of a rather light Higgs boson (M/sub H/< or approx. =10 GeV). It is also shown that the mechanism of gauge-dependence cancellation between Higgs-boson-exchange and box diagrams works even in the standard model.

PhysicsParticle physicsMuonQuark modelHigh Energy Physics::PhenomenologyYukawa potentialGeneral Physics and AstronomyFísicaElementary particleParticle decayPair productionHiggs bosonHigh Energy Physics::ExperimentBoson
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Supersymmetric majoron signatures and solar neutrino oscillations

1988

Spontaneous R-parity breaking in supergravity solves the solar neutrino problem through matter-enhanced neutrino oscillations. The model may be tested in collider experiments and through ``dynamical'' effects associated with the existence of a weakly interacting majoron. Apart from astrophysical effects, majoron emission can produce observable changes in \ensuremath{\mu} and \ensuremath{\tau} decay spectra for parameter values that substantially reduce the solar neutrino flux. A signature of the model is the possible observation of the decay \ensuremath{\mu}\ensuremath{\rightarrow}e+majoron.

PhysicsParticle physicsMuonSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyGeneral Physics and AstronomySolar neutrino problemPartícules (Física nuclear)Nuclear physicsParticle decayHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLeptonMajoron
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Search for heavy neutrinos in \(\pi ^{ + } \to \mu ^{ + }\nu \) decay and status of lepton universality test in the PIENU experiment

2019

International audience; In the present work of the PIENU experiment, heavy neutrinos were sought in pion decays \(\pi ^{ + } \to \mu ^{ + }\nu \). No evidence for extra peak was found in the muon kinetic energy spectrum and 90% confidence level upper limits were set on the neutrino mixing matrix \(|U_{\mu i}|^{2}\) in the mass range of 15.7 to 33.8 MeV/c^2, improving an order of magnitude over previous experiments. Current status of lepton universality test is also reported.

PhysicsParticle physicsMuonpi+ --> muon+ neutrinopi: decayneutrino: heavy: search forUniversality (philosophy)Pontecorvo–Maki–Nakagawa–Sakata matrixkineticenergy spectrumKinetic energyPion[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentNeutrinoneutrino: mixingOrder of magnitudeParticle Physics - ExperimentLeptonexperimental resultslepton: universality
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THE X(3872) AND OTHER X,Y,Z RESONANCES AS HIDDEN CHARM MESON-MESON MOLECULES

2011

We report on some ideas concerning the nature of the X(3872) resonance and the need for approximately equal charged and neutral components of $D \bar{D}^* +cc$. Then we discuss how some hidden charm states are obtained from the interaction between vector mesons with charm and can be associated to some of the charmonium-like X,Y,Z states. Finally we discuss how the nature of these states could be investigated through different types of radiative decay.

PhysicsParticle physicsNuclear TheoryMesonHigh Energy Physics::PhenomenologyRadiative decayFOS: Physical sciencesResonanceVector meson dominanceNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)MoleculeHigh Energy Physics::ExperimentCharm (quantum number)Nuclear theoryX(3872)International Journal of Modern Physics: Conference Series
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Microscopic calculations of isospin-breaking corrections to superallowed beta-decay

2011

The superallowed beta-decay rates that provide stringent constraints on physics beyond the Standard Model of particle physics are affected by nuclear structure effects through isospin-breaking corrections. The self-consistent isospin- and angular-momentum-projected nuclear density functional theory is used for the first time to compute those corrections for a number of Fermi transitions in nuclei from A=10 to A=74. The resulting leading element of the CKM matrix, |V_{ud}|= 0.97447(23), agrees well with the recent result by Towner and Hardy [Phys. Rev. C {\bf 77}, 025501 (2008)].

PhysicsParticle physicsNuclear Theoryta114Physics beyond the Standard ModelHigh Energy Physics::PhenomenologyNuclear TheoryNuclear structureGeneral Physics and AstronomyFOS: Physical sciencesNuclear matterBeta decayNuclear physicsNuclear Theory (nucl-th)Standard Model (mathematical formulation)IsospinNuclear ExperimentNuclear densityFermi Gamma-ray Space Telescope
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Measurement of the Ξ0→Λγ decay asymmetry and branching fraction

2004

In data taken with the NA48 experiment at the CERN SPS in 1999, 730 candidates of the weak radiative hyperon decay Ξ0→Λγ have been found with an estimated background of 58±8 events. From these events the Ξ0→Λγ decay asymmetry has been determined to α(Ξ0→Λγ)=-0.78±0.18stat±0.06 syst, which is the first evidence of a decay asymmetry in Ξ 0→Λγ. The branching fraction of the decay has been measured to be Br(Ξ0→Λγ)=(1.16±0.05 stat±0.06syst)×10-3. © 2004 Elsevier B.V. All rights reserved.

PhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron ColliderBranching fractionmedia_common.quotation_subjectiperoni Xi0HyperonRadiative decayNA48 experimentAsymmetryNuclear physicsdecadimenti radiativiRadiative transferiperoni Xi0; decadimenti radiativimedia_commonPhysics Letters B
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A4-based tri-bimaximal mixing within inverse and linear seesaw schemes

2009

We consider tri-bimaximal lepton mixing within low-scale seesaw schemes where light neutrino masses arise from TeV scale physics, potentially accessible at the Large Hadron Collider (LHC). Two examples are considered, based on the A4 flavor symmetry realized within the inverse or the linear seesaw mechanisms. Both are highly predictive so that in both the light neutrino sector effectively depends only on three mass parameters and one Majorana phase, with no CP violation in neutrino oscillations. We find that the linear seesaw leads to a lower bound for neutrinoless double beta decay while the inverse seesaw does not. The models also lead to potentially sizeable decay rates for lepton flavor…

PhysicsParticle physicsNuclear and High Energy PhysicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryDouble beta decayCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationLepton
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Measurement of the effective Bs0→K+K− lifetime

2012

A precise determination of the effective $B_s^0 \rightarrow K^+ K^-$ lifetime can be used to constrain contributions from physics beyond the Standard Model in the $B_s^0$ meson system. Conventional approaches select $B$ meson decay products that are significantly displaced from the $B$ meson production vertex. As a consequence, $B$ mesons with low decay times are suppressed, introducing a bias to the decay time spectrum which must be corrected. This analysis uses a technique that explicitly avoids a lifetime bias by using a neural network based trigger and event selection. Using 1.0 fb$^{-1}$ of data recorded by the LHCb experiment, the effective $B_s^0 \rightarrow K^+ K^-$ lifetime is meas…

PhysicsParticle physicsNuclear and High Energy PhysicsMeson productionMesonBranching fraction010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::Phenomenology01 natural sciencesLuminosityVertex (geometry)Nuclear physicsEvent selectionDecay time0103 physical sciencesCP violationHigh Energy Physics::Experiment010306 general physicsEnergy (signal processing)Physics Letters B
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Light vector meson production in pp collisions at s=7 TeV

2012

The ALICE experiment has measured low-mass dimuon production in pp collisions at root s = 7 TeV in the dimuon rapidity region 2.5 < y < 4. The observed dimuon mass spectrum is described as a superposition of resonance decays (eta, rho, omega, eta', phi) into muons and semi-leptonic decays of charmed mesons. The measured production cross sections for omega and phi are sigma(omega)(1 < p(t) < 5 GeV/c. 2.5 < y < 4) = 5.28 +/- 0.54(stat) +/- 0.49(syst) mb and sigma(phi)(1 < p(t) < 5 GeV/c. 2.5 < y < 4) = 0.940 +/- 0.084(stat) +/- 0.076(syst) mb. The differential cross sections d(2)sigma/dy dp(t) are extracted as a function of p(t) for omega and phi. The ratio between the rho and omega cross sec…

PhysicsParticle physicsNuclear and High Energy PhysicsMuonMeson010308 nuclear & particles physicsPhysicsHadronElementary particle01 natural sciencesOmegaNuclear physicsParticle decayLight vector meson0103 physical sciencesALICE; LHC; CERN; vector meson; pp; 7 TeVHigh Energy Physics::ExperimentRapidityVector mesonNuclear Experiment010306 general physicsPhysics Letters B
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