Search results for "LESS"

showing 10 items of 2452 documents

Study of the decayDs+→K+K−e+νe

2008

Using 214fb-1 of data recorded by the BABAR detector at the PEPII electron-positron collider, we study the decay Ds+→K+K-e+νe. Except for a small S-wave contribution, the events with K+K- masses in the range 1.01-1.03GeV/c2 correspond to mesons. For Ds+→ e+νe decays, we measure the relative normalization of the Lorentz invariant form factors at q2=0, rV=V(0)/A1(0)=1.849±0.060±0.095, r2=A2(0)/A1(0)=0.763±0. 071±0.065 and the pole mass of the axial-vector form factors mA=(2.28-0.18+0.23±0.18)GeV/c2. Within the same K+K- mass range, we also measure the relative branching fraction B(Ds+→K+K-e+νe)/B(Ds+→K+K- π+)=0.558±0.007±0.016, from which we obtain the total branching fraction B(Ds+→ e+νe)=(2…

PhysicsNuclear and High Energy PhysicsParticle physicsAntiparticleMeson010308 nuclear & particles physicsBranching fractionElectron–positron annihilationHadron01 natural sciencesParticle decayTheoretical physicsPair production0103 physical sciences010306 general physicsDimensionless quantityPhysical Review D
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Constraining Nonstandard Neutrino-Electron Interactions

2007

We present a detailed analysis on nonstandard neutrino interactions (NSI) with electrons including all muon and electron (anti)-neutrino data from existing accelerators and reactors, in conjunction with the ``neutrino counting'' data (e- e+ -> nu nu gamma) from the four LEP collaborations. First we perform a one-parameter-at-a-time analysis, showing how most constraints improve with respect to previous results reported in the literature. We also present more robust results where the NSI parameters are allowed to vary freely in the analysis. We show the importance of combining LEP data with the other experiments in removing degeneracies in the global analysis constraining flavor-conservin…

PhysicsNuclear and High Energy PhysicsParticle physicsAntiparticleMuonElectron–positron annihilationFísicaFOS: Physical sciencesElementary particleMassless particleNuclear physicsParticle decayHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoLepton
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Resonant conversion of massless neutrinos in supernovae

1996

It has been noted for a long time that, in some circumstances, {\sl massless} neutrinos may be {\sl mixed} in the leptonic charged current. Conventional neutrino oscillation searches in vacuum are insensitive to this mixing. We discuss the effects of resonant massless-neutrino conversions in the dense medium of a supernova. In particular, we show how the detected $\bar\nu_e$ energy spectra from SN1987a and the supernova $r$-process nucleosynthesis may be used to provide very stringent constraints on the mixing of {\sl massless} neutrinos.

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaAstrophysics (astro-ph)High Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstrophysicsNuclear physicsMassless particleSupernovaHigh Energy Physics - PhenomenologyGeneral Relativity and Quantum CosmologyHigh Energy Physics - Phenomenology (hep-ph)NucleosynthesisHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMixing (physics)Charged currentEnergy (signal processing)
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Interplay between collective effects and non-standard interactions of supernova neutrinos

2009

We consider the effect of nonstandard neutrino interactions (NSI, for short) on the propagation of neutrinos through the supernova (SN) envelope within a three-neutrino framework and taking into account the presence of a neutrino background. We find that for given NSI parameters, with strength generically denoted by epsilon(ij), neutrino evolution exhibits a significant time dependence. For vertical bar epsilon(tau tau)vertical bar greater than or similar to 10(-3) the neutrino survival probability may become sensitive to the V-23 octant and the sign of epsilon(tau tau). In particular, if epsilon(tau tau) greater than or similar to 10(-2) an internal I-resonance may arise independently of t…

PhysicsNuclear and High Energy PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesElementary particleFermionMassless particleSupernovaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutrino detectorAstrophysics - Solar and Stellar AstrophysicsHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationSolar and Stellar Astrophysics (astro-ph.SR)Lepton
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On dynamical gluon mass generation

2007

The effective gluon propagator constructed with the pinch technique is governed by a Schwinger-Dyson equation with special structure and gauge properties, that can be deduced from the correspondence with the background field method. Most importantly the non-perturbative gluon self-energy is transverse order-by-order in the dressed loop expansion, and separately for gluonic and ghost contributions, a property which allows for a meanigfull truncation. A linearized version of the truncated Schwinger-Dyson equation is derived, using a vertex that satisfies the required Ward identity and contains massless poles. The resulting integral equation, subject to a properly regularized constraint, is so…

PhysicsNuclear and High Energy PhysicsParticle physicsBackground field methodHigh Energy Physics::LatticeMass generationHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesPropagatorIntegral equationGluonVertex (geometry)Massless particleHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PinchMathematical physics
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Current cosmological bounds on neutrino masses and relativistic relics

2004

We combine the most recent observations of large-scale structure (2dF and SDSS galaxy surveys) and cosmic microwave anisotropies (WMAP and ACBAR) to put constraints on flat cosmological models where the number of massive neutrinos and of massless relativistic relics are both left arbitrary. We discuss the impact of each dataset and of various priors on our bounds. For the standard case of three thermalized neutrinos, we find an upper bound on the total neutrino mass sum m_nu < 1.0 (resp. 0.6) eV (at 2sigma), using only CMB and LSS data (resp. including priors from supernovae data and the HST Key Project), a bound that is quite insensitive to the splitting of the total mass between the th…

PhysicsNuclear and High Energy PhysicsParticle physicsCosmic microwave backgroundDark matterAstrophysics (astro-ph)FOS: Physical sciencesFísicaAstrophysicsAstrophysics::Cosmology and Extragalactic AstrophysicsAstrophysicsUpper and lower boundsCMB cold spotMassless particleHigh Energy Physics - PhenomenologySupernovaHigh Energy Physics - Phenomenology (hep-ph)Observational cosmologyNeutrino
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SINGLE PHOTON DECAYS OF THE $Z^0$ AND SUSY WITH SPONTANEOUSLY BROKEN R-PARITY

1995

Spontaneous violation of R parity can induce rare single photon decays of the $Z^0$ involving the emission of (nearly) massless pseudoscalar Goldstone bosons, majorons, as well as massive CP even or CP odd spin zero bosons that arise in the electroweak breaking sector of these models. We show that the majoron emitting decays can have a sizeable branching ratio of $10^{-5}$ or so, without conflicting any experimental observation from neutrino physics or particle searches. These decays may lead to interesting structures for the single photon spectrum involving either mono chromatic photons as well as continuous spectra that grow with energy. They would easily account for an excess of single p…

PhysicsNuclear and High Energy PhysicsParticle physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryMassless particlePseudoscalarHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)R-parityGoldstone bosonHigh Energy Physics::ExperimentBosonMajoron
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Search forWWandWZResonances Decaying to Electron, MissingET, and Two Jets inpp¯Collisions ats=1.96  TeV.

2009

We present a search for WW and WZ production in final states that contain a charged lepton (electron or muon) and at least two jets, produced in {radical}(s)=1.96 TeV pp collisions at the Fermilab Tevatron, using data corresponding to 1.2 fb{sup -1} of integrated luminosity collected with the CDF II detector. Diboson production in this decay channel has yet to be observed at hadron colliders due to the large single W plus jets background. An artificial neural network has been developed to increase signal sensitivity, as compared with an event selection based on conventional cuts. We set a 95% confidence level upper limit of {sigma}{sub WW}xBR(W{yields}l{nu}{sub l},W{yields}jets)+{sigma}{sub…

PhysicsNuclear and High Energy PhysicsParticle physicsGauge bosonMuon010308 nuclear & particles physicsHadronHigh Energy Physics::PhenomenologyTevatronGeneral Physics and AstronomyElementary particleCoupling (probability)01 natural sciencesStandard ModelNuclear physicsMassless particleParticle decay0103 physical sciencesProduction (computer science)High Energy Physics::ExperimentSensitivity (control systems)010306 general physicsLeptonBosonPhysical Review Letters
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Search for squarks and gluinos using final states with jets and missing transverse momentum with the ATLAS detector in s=7 TeV proton–proton collisio…

2011

A search for squarks and gluinos in events containing jets, missing transverse momentum and no electrons or muons is presented. The data were recorded in 2011 by the ATLAS experiment in root s = 7 TeV proton-proton collisions at the Large Hadron Collider. No excess above the Standard Model background expectation is observed in 1.04 fb(-1) of data. Gluino and squark masses below 700 GeV and 875 GeV respectively are excluded at the 95% confidence level in simplified models containing only squarks of the first two generations, a gluino octet and a massless neutralino. The exclusion limit increases to 1075 GeV for squarks and gluinos of equal mass. In MSUGRA/CMSSM models with tan beta = 10, A(0…

PhysicsNuclear and High Energy PhysicsParticle physicsGluinoLarge Hadron ColliderMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyATLAS experimentSupersymmetry01 natural sciencesStandard ModelNuclear physicsMassless particlemedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesNeutralinomedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsMinimal Supersymmetric Standard ModelPhysics Letters B
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Thermal leptogenesis in a 5D split fermion scenario with bulk neutrinos

2009

We study the thermal leptogenesis in a hybrid model, which combines the so called split fermion model and the bulk neutrino model defined in five dimensional spacetime. This model predicts the existence of a heavy neutrino pair nearly degenerate in mass, whose decays might generate a CP violation large enough for creating the baryon asymmetry of the universe through leptogenesis. We investigate numerically the constraints this sets on the parameters of the model such as the size of the compactified fifth dimension.

PhysicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermionBaryonMassless particleHigh Energy Physics - PhenomenologyBaryon asymmetryHigh Energy Physics - Phenomenology (hep-ph)LeptogenesisCP violationHigh Energy Physics::ExperimentNeutrinoLepton
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