Search results for "positron annihilation"

showing 10 items of 757 documents

New ISR Cross Section Results onKS0KL0π0andKS0KL0π0π0From BaBar

2017

Abstract We present preliminary measurements of the cross sections for e + e − → K S 0 K L 0 π 0 and K S 0 K L 0 π 0 π 0 obtained using the technique of Initial State Radiation with 469 fb −1 of e + e − collision data collected with the BaBar detector at or near the ϒ ( 4 S ) resonance. The resonant substructure of K S 0 K L 0 π 0 is investigated, and branching fractions for the decays of the charmonium resonances J / ψ and ψ ( 2 S ) into these final states are measured.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsElectron–positron annihilation0103 physical sciencesResonanceSubstructure010306 general physics01 natural sciencesNuclear and Particle Physics Proceedings
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Search for high mass photon pairs in (f= e, μ, τ, v, q) at LEP

1993

Abstract The result of a search for high mass photon pairs from the processes e + e − → f f γγ (f = e, μ, τ, v and q) with the ALEPH detector is reported. The result for f = e , μ and τ is to be compared with the observation of 4 events by the L3 Collaboration with invariant masses, M γγ , of the two photons near 60 GeV. From a data sample approximately twice as large taken from 1990 to 1992, 6 events are found with M γγ distributed between 50 GeV and 72 GeV, while 4.9 events are expected from a QED calculation. There is no evidence for a mass peak; only one event ( μ + μ − γγ ) at M γγ = 59.4 ± 0.2 GeV is compatible with the L3 observation. In addition, for M γγ > 50 GeV, no event is found…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsHigh energyPhotonElectron–positron annihilationHigh massALEPH experimentPhysics Letters B
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Search for a light Higgs resonance in radiative decays of theϒ(1S)with a charm tag

2015

A search is presented for the decay Υ(1S)→ γA^0, A^0 → cc[bar], where A^0 is a candidate for the CP-odd Higgs boson of the next-to-minimal supersymmetric standard model. The search is based on data collected with the BABAR detector at the Υ(2S) resonance. A sample of Υ(1S) mesons is selected via the decay Υ(2S)→π + π − Υ(1S). The A^0 → cc[bar] decay is identified through the reconstruction of hadronic D^0, D^+, and D^∗ (2010)^+ meson decays. No significant signal is observed. The measured 90% confidence-level upper limits on the product branching fraction B(Υ(1S) → γA^0 ) × B(A^0 → cc[bar] ) range from 7.4×10^(−5) to 2.4×10^(−3) for A^0 masses from 4.00 to 8.95  GeV/c^2 and 9.10 to 9.25  Ge…

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsPionMesonBranching fractionElectron–positron annihilationHadronHiggs bosonResonanceMinimal Supersymmetric Standard ModelPhysical Review D
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Observation ofe+e−→ηJ/ψat center-of-mass energys=4.009  GeV

2012

Using a 478 pb(-1) data sample collected with the BESIII detector operating at the Beijing Electron Positron Collider storage ring at a center-of-mass energy of root s = 4.009 GeV, the production of e(+)e(-) -> eta J/psi is observed for the first time with a statistical significance of greater than 10 sigma. The Born cross section is measured to be (32.1 +/- 2.8 +/- 1.3) pb, where the first error is statistical and the second systematic. Assuming the eta J/psi signal is from a hadronic transition of the psi(4040), the fractional transition rate is determined to be B(psi(4040) -> eta J/psi) = (5.2 +/- 0.5 +/- 0.2 +/- 0.5) x 10(-3), where the first, second, and third errors are statistical, s…

Nuclear physicsPhysicsNuclear and High Energy PhysicsPositronAnnihilationlawElectron–positron annihilationHadronHigh Energy Physics::ExperimentCenter of massColliderEnergy (signal processing)law.inventionPhysical Review D
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Measurement of the B0→D*−π+π−π+ branching fraction

2016

Using a sample of (470.9 +- 2.8) x 10^6 BB-bar pairs, we measure the decay branching fraction B(B^0 -> D^*- pi^+ pi^- pi^+) = (7.26 +- 0.11 +- 0.31) x 10^-3, where the first uncertainty is statistical and the second is systematic. Our measurement will be helpful in studies of lepton universality by measuring B(B^0 -> D^*- tau^+ nu_tau) using tau^+ -> pi^+ pi^- pi^+ nu-bar_tau decays, normalized to B(B^0 -> D^*- pi^+ pi^- pi^+.

Nuclear physicsPhysicsParticle physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilation0103 physical sciences010306 general physics01 natural sciencesLeptonUniversality (dynamical systems)
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Observation of the Semileptonic Decay D0→a0(980)−e+νe and Evidence for D+→a0(980)0e+νe

2018

Using an e(+)e(-) collision data sample of 2.93 fb(-1) collected at a center-of-mass energy of 3.773 GeV by the BESIII detector at BEPCII, we report the observation of D-0 -> a(0)(980)(-)e(+)nu( ...

Nuclear physicsPhysicsSemileptonic decay010308 nuclear & particles physicsElectron–positron annihilation0103 physical sciencesDetectorGeneral Physics and Astronomy010306 general physics01 natural sciencesEnergy (signal processing)Physical Review Letters
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REVIEW OF R MEASUREMENTS

2013

We review the status of R measurements in the energy range below 12 GeV, where recently a major progress has been achieved recently. These measurements are phenomenologically motivated by their impact on precision QCD and on electroweak parameters. We also report on improved results which can be expected in near future from presently running or upcoming facilities.

Nuclear physicsQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationElectroweak interactionGeneral Physics and AstronomyHigh Energy Physics::ExperimentAstronomy and AstrophysicsModern Physics Letters A
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Next-to-next-to-leading order corrections to three-jet observables in electron-positron annihilation.

2008

I report on a numerical program, which can be used to calculate any infrared safe three-jet observable in electron-positron annihilation to next-to-next-to-leading order in the strong coupling constant ${\ensuremath{\alpha}}_{s}$. The results are compared to a recent calculation by another group. Numerical differences in three color factors are discussed and explained.

Nuclear physicsQuantum chromodynamicsPhysicsRenormalizationParticle physicsColor modelAnnihilationElectron–positron annihilationGeneral Physics and AstronomyOrder (ring theory)ObservableJet (particle physics)Physical review letters
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Search for flavor-changing neutral current and lepton-flavor violating decays of D-0 -> l(+)l(-)

2004

We report on a search for the flavor-changing neutral current decays $\Dz\to e^+e^-$ and $\Dz\to\mu^+\mu^-$, and the lepton-flavor violating decay $\Dz\to e^\pm\mu^\mp$. The measurement is based on $122 {fb}^{-1}$ of data collected by the \babar detector at the PEP-II asymmetric $e^+e^-$ collider. No evidence is found for any of the decays. The upper limits on the branching fractions, at the 90 % confidence level, are $1.2\times 10^{-6}$ for $\Dz\to e^+e^-$, $1.3\times 10^{-6}$ for $\Dz\to\mu^+\mu^-$, and $8.1\times 10^{-7}$ for $\Dz\to e^\pm\mu^\mp$.

OptimizationParticle physicsLepton-flavor violating (LFV)Electron–positron annihilationBABARCharged particleGeneral Physics and Astronomy-Standard model (SM)Lambda baryon01 natural sciencesPARTICLE PHYSICS; PEP2; BABARHigh Energy Physics - ExperimentNONuclear physicsSilicon microstrip detector0103 physical sciencesPEP2010306 general physicsDETECTOR; BABAR; SLACDETECTORFlavorProbabilityPhysicsNeutral current010308 nuclear & particles physicsEnergy dissipationFlavor-changing neutral currentColliding beam acceleratorMicrostrip deviceHEPFlavor-changing neutral current (FCNC)Drift chamberPARTICLE PHYSICSHigh Energy Physics::ExperimentParticle detectorSLACLepton
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Analytical results forO(αs)radiative corrections toe+e−→tt¯↑up to a given gluon energy cut

2009

We determine the O({alpha}{sub s}) radiative corrections to polarized top quark pair production in e{sup +}e{sup -} annihilations with a specified gluon energy cut. We write down fully analytical results for the unpolarized and polarized O({alpha}{sub s}) cross sections e{sup +}e{sup -}{yields}tt(G) and e{sup +}e{sup -}{yields}tt{sup {up_arrow}}(G) including their polar orientation dependence relative to the beam direction. In the soft-gluon limit we recover the usual factorizing form known from the soft-gluon approximation. In the limit when the gluon energy cut takes its maximum value we recover the totally inclusive unpolarized and polarized cross sections calculated previously. We provi…

Orientation (vector space)PhysicsNuclear and High Energy PhysicsParticle physicsTop quarkAnnihilationPair productionElectron–positron annihilationHigh Energy Physics::PhenomenologyRadiative transferEnergy (signal processing)GluonPhysical Review D
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