Search results for "annihilation"

showing 10 items of 1016 documents

Normal and transverse single tau polarization at the Z-peak

1994

Abstract We study normal (to the collision plane) and transverse (within the collision plane) single-τ polarization in τ pairs produced in e + e − unpolarized collisions at the Z -resonance. The transverse polarization component is sensitive to the anomalous weak-magnetic moment, whereas the normal polarization component is sensitive to a CP-violating weak-electric dipole moment. We show how these components of the single τ polarization are accessible from the angular distribution of its decay products. We define a CP violating asymmetry of the τ decay products which, with 10 7 Z ′s produced, provides a sensitivity of 2.3 × 10 −18 e ·cm for the weak-electric dipole moment.

PhysicsNuclear and High Energy PhysicsElectron–positron annihilationmedia_common.quotation_subjectTransition dipole momentFísicaObservablePolarization (waves)AsymmetryNuclear physicsTransverse planeDipoleCP violationAtomic physicsParticle Physics - Phenomenologymedia_commonPhysics Letters B
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Constraints on anomalous QGC's in $e^{+}e^{-}$ interactions from 183 to 209 GeV

2004

The acoplanar photon pairs produced in the reaction e+ e- --> nu nubar gamma gamma are analysed in the 700 inverse nanobarns of data collected by the ALEPH detector at centre-of-mass energies between 183 and 209 GeV. No deviation from the Standard Model predictions is seen in any of the distributions examined. The resulting 95% C.L. limits set on the anomalous QGC's, az_0, az_c, aw_0 and aw_c, are -0.012 GeV**-2 < az_0/Lambda**2 < +0.019 GeV**-2, -0.041 GeV**-2 < az_c/Lambda**2 < +0.044 GeV**-2, -0.060 GeV**-2 < aw_0/Lambda**2 < +0.055 GeV**-2, -0.099 GeV**-2 < aw_c/Lambda**2 < +0.093 GeV**-2, where Lambda is the energy scale of the new Physics responsible for the anomalous couplings.

PhysicsNuclear and High Energy PhysicsGAUGE BOSON COUPLINGS010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaElectron–positron annihilationLEPLambdaFINAL-STATES01 natural sciencesHIGGSStandard ModelENERGYNuclear physicsCOLLIDERSLIMITS0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentNuclear Experiment010306 general physicsParticle Physics - ExperimentQUARTIC COUPLINGS
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Measurement of triple gauge-boson couplings at 172 GeV

1998

The triple gauge-boson couplings, αWΦ, αW and αBΦ, have been measured using 34 semileptonically and 54 hadronically decaying W+W- candidate events. The events were selected in the data recorded during 1996 with the ALEPH detector at 172 GeV, corresponding to an integrated luminosity of 10.65 pb-1. The triple gauge-boson couplings have been measured using optimal observables constructed from kinematic information of W+W- events. The results are in agreement with the Standard Model expectation.

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsAlephLuminosity (scattering theory)010308 nuclear & particles physicsElectron–positron annihilationDetectorHigh Energy Physics::PhenomenologyObservable01 natural sciencesStandard ModelALEPH ExperimentNuclear physics[PHYS.PHYS.PHYS-INS-DET] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]0103 physical sciencesHigh Energy Physics::Experiment[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsALEPH experimentParticle Physics - Experiment
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Set of sum rules for anomalous gauge boson couplings

1999

The dependence of the differential cross-section for on-shell W-pair production on the anomalous trilinear gauge couplings invariant under C and P is examined. It is shown that the contributions of the anomalous magnetic moments of the W boson due to the photon and the Z can be individually projected out by means of two appropriately constructed polynomials. The remaining four anomalous couplings are shown to satisfy a set of model-independent sum rules. Specific models which predict special relations among the anomalous couplings are then studied; in particular, the composite model of Brodsky and Hiller, and the linear and non-linear effective Lagrangian approaches. The relations predicted…

PhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsPhotonElectron–positron annihilationForm factor (quantum field theory)FOS: Physical sciencesFísicaGauge (firearms)Theoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)BibliographySum rule in quantum mechanicsInvariant (mathematics)Particle Physics - Phenomenology
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Positron implantation profiles in layered samples

2009

The paper presents theoretical and experimental studies of the positron implantation profiles in layered samples. The Monte Carlo simulations performed using the GEANT4 toolkit reveal accumulation of positrons in the denser layer embedded between two less dense layers. That effect is significant not only for low energy positrons at slow monoenergetic positron beams but also for high energy positrons which are emitted from radioactive nuclei in conventional experiments. Measurements of the positron implantation profile into the samples which consist of silver and aluminium foils of different thickness show profile features which correspond well with those simulated by the GEANT4 toolkit for …

PhysicsNuclear and High Energy PhysicsHigh energyAstrophysics::High Energy Astrophysical PhenomenaPositron Lifetime SpectroscopyPhysics::Medical PhysicsMonte Carlo methodchemistry.chemical_elementLow energyPositronchemistryAluminiumPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAtomic physicsInstrumentationLayer (electronics)Positron annihilationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Measurement of the branching fraction for D0 → K-π+

1997

The branching fraction for D-0 --> K(-)pi(+) is measured with the statistics collected by ALEPH from 1991 to 1994. The method is based on the comparison between the rate for the reconstructed D*+ --> (D) pi(+), D-0 --> K(-)pi(+) decay chain and the rate for inclusive soft pion production at low transverse momentum with respect to the nearest jet. The result is B(D-0 --> K(-)pi(+)) = (3.90 +/- 0.09 +/- 0.12)% (C) 1997 Published by Elsevier Science B.V. RI ANTONELLI, ANTONELLA/C-6238-2011; Passalacqua, Luca/F-5127-2011; Murtas, Fabrizio/B-5729-2012; St.Denis, Richard/C-8997-2012; Sanchez, Federico/F-5809-2012; Forti, Francesco/H-3035-2011; Ferrante, Isidoro/F-1017-2012

PhysicsNuclear and High Energy PhysicsJet (fluid)010308 nuclear & particles physicsBranching fractionElectron–positron annihilationPhysics01 natural sciencesNuclear physicsALEPH ExperimentPion0103 physical sciencesTransverse momentumDecay chain010306 general physicsALEPH experiment
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Event shapes and jet rates in electron-positron annihilation at NNLO

2009

This article gives the perturbative NNLO results for the most commonly used event shape variables associated to three-jet events in electron-positron annihilation: Thrust, heavy jet mass, wide jet broadening, total jet broadening, C parameter and the Durham three-to-two jet transition variable. In addition the NNLO results for the jet rates corresponding to the Durham, Geneva, Jade-E0 and Cambridge jet algorithms are presented.

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AnnihilationElectron–positron annihilationAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesThrustHigh Energy Physics::ExperimentEvent (particle physics)
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Factorization and resummation for jet broadening

2011

Jet broadening is an event-shape variable probing the transverse momenta of particles inside jets. It has been measured precisely in e+e- annihilations and is used to extract the strong coupling constant. The factorization of the associated cross section at small values of the broadening is afflicted by a collinear anomaly. Based on an analysis of this anomaly, we present the first all-order expressions for jet-broadening distributions, which are free of large perturbative logarithms in the two-jet limit. Our formulae reproduce known results at next-to-leading logarithmic order but also extend to higher orders.

PhysicsNuclear and High Energy PhysicsJet (fluid)Particle physicsLogarithm010308 nuclear & particles physicsElectron–positron annihilationFOS: Physical sciences01 natural sciencessymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)FactorizationQuantum electrodynamics0103 physical sciencesWeierstrass factorization theoremEffective field theorysymbolsAnomaly (physics)Resummation010306 general physicsPHYSICS LETTERS B
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The ASTERIX spectrometer at LEAR

1989

The ASTERIX spectrometer has been used to study the formation and the ground state of the pp atom and exclusive final states of pp annihilation at rest in a H2 gas target at NTP, using antiprotons from the Low Energy Antiproton Ring (LEAR) at CERN. The article describes the mechanical construction of the apparatus, the trigger logic, the chamber readout, and the data acquisition system. The detector calibration and the offline processing of the 55 million reconstructed events are illustrated. An overview is given about the new physics results obtained by the experiment.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderAnnihilationSpectrometerPhysics::Instrumentation and DetectorsASTERIXNuclear physicsData acquisitionAntiprotonCalibrationDetectors and Experimental TechniquesGround stateInstrumentation
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Measurement of time dependentCPasymmetry parameters inB0meson decays toωKS0,η′K0, andπ0KS0

2009

We present measurements of the time-dependent CP-violation parameters S and C in the decays B-0 -> omega K-S(0), B-0 -> eta'K-0, reconstructed as eta'K-S(0) and eta'K-L(0), and B-0 -> pi K-0(S)0. The data sample corresponds to the full BABAR dataset of 467 x 10(6) B (B) over bar pairs produced at the PEP-II asymmetric-energy e(+)e(-) collider at the Stanford Linear Accelerator Center. The results are S-omega KS0 = 0.55(-0.29)(+0.26) +/- 0.02, C-omega KS0 = 0.52(-0.20)(+0.22) +/- 0.03, S-eta'K0 = 0.57 +/- 0.08 +/- 0.02, C-eta'K0 = 0.08 +/- 0.06 +/- 0.02, S-pi 0KS0 = 0.55 +/- 0.20 +/- 0.03, and C-pi 0KS0 = 0.13 +/- 0.13 +/- 0.03, where the first errors are statistical and the second systemati…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsBETA (programming language)Electron–positron annihilationAnalytical chemistryCenter (category theory)01 natural sciencesOmegaParticle decayPair production0103 physical sciencesCP violationAtomic physics010306 general physicscomputercomputer.programming_languagePhysical Review D
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