Search results for "Antiparticle"

showing 10 items of 69 documents

Event Excess in the MiniBooNE Search forν¯μ→ν¯eOscillations

2010

The MiniBooNE experiment at Fermilab reports results from a search for {nu}{sub {mu}{yields}{nu}e} oscillations, using a data sample corresponding to 5.66x10{sup 20} protons on target. An excess of 20.9{+-}14.0 events is observed in the energy range 475<E{sub {nu}}{sup QE}<1250 MeV, which, when constrained by the observed {nu}{sub {mu}} events, has a probability for consistency with the background-only hypothesis of 0.5%. On the other hand, fitting for {nu}{sub {mu}{yields}{nu}e} oscillations, the best-fit point has a {chi}{sup 2} probability of 8.7%. The data are consistent with {nu}{sub {mu}{yields}{nu}e} oscillations in the 0.1 to 1.0 eV{sup 2} {Delta}m{sup 2} range and with the evidence…

Nuclear physicsMiniBooNEPhysicsParticle physicsAntiparticleAntimatterGeneral Physics and AstronomyNeutrinoNeutrino oscillationParticle identificationEnergy (signal processing)LeptonPhysical Review Letters
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A test of charge-parity-time invariance at the atto-electronvolt scale

2017

We developed a novel fast measurement procedure for cyclotron frequency comparisons of two individual particles in a Penning trap, which enabled us to compare the charge-to-mass ratio of the proton and the antiproton with a fractional precision of 69 parts per trillion. To date this is the most precise test of charge-parity-time invariance using baryons. Our measurements were performed at cyclotron frequencies of about 30 MHz, which means that charge-parity-time symmetry holds at the atto-electronvolt scale.

Nuclear physicsPhysicsBaryonAntiparticleScale (ratio)Physics in GeneralAntimatterElectronvoltPräzisionsexperimente - Abteilung BlaumParity (mathematics)NucleonNuclear ExperimentAtto-
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Estimates of the Nuclear Time Delay in Dissipative U + U and U + Cm Collisions Derived from the Shape of Positron andδ-Ray Spectra

1983

Positron and delta-ray spectra have been measured in coincidence with quasielastic scattered particles and fission fragments from the bombardment of Pd, U, and Cm targets with U beams of energies between 5.9 and 8.4 MeV/u. For collisions leading to a fission reaction, the atomic positron and delta-ray spectra fall off more steeply at high energies than expected from calculations based on pure Rutherford trajectories. A quantitative analysis of this effect is in accord with a nuclear contact time of about 10/sup -21/ s.

Nuclear reactionElastic scatteringPhysicsAntiparticleFissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGeneral Physics and AstronomyNuclear physicssymbols.namesakePositronNuclear fissionAntimattersymbolsPhysics::Accelerator PhysicsRutherford scatteringAtomic physicsNuclear ExperimentPhysical Review Letters
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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
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Polarization analysis of $\bar{p}$ produced in pA collisions

2019

A quite simple procedure for the generation of a polarized antiproton beam could be worked out if antiprotons are produced with some polarization. In order to investigate this possibility measurements of the polarization of produced antiprotons have been started at a CERN/PS test beam. The polarization will be determined from the asymmetry of the elastic antiproton scattering at a liquid hydrogen target in the CNI region for which the analyzing power is well known. The data are under analysis and an additional measurement is done in 2018. Details on the experiment and the ongoing data analysis will be given.

PhysicsAntiparticle010308 nuclear & particles physicsPhysicsQC1-999Polarization (waves)01 natural sciences7. Clean energyNuclear physicsAntiproton beamAntiproton0103 physical sciencesPhysics::Accelerator Physicsddc:530High Energy Physics::ExperimentPhysics::Atomic Physics010306 general physicsAntihydrogenNuclear Experiment
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Status of the analysis for the search of polarization in the antiproton production process

2016

The P-349 experiment aims to test whether for antiprotons the production process itself can be a source of polarization in view of the preparation of a polarized antiproton beam. In this article we present the details of performed measurements and report on the status of the ongoing analysis.

PhysicsAntiparticle010308 nuclear & particles physicsPhysicsQC1-999Polarization (waves)01 natural sciencesEngineering physicsNuclear physicsSubatomär fysikAntiproton beamAntiprotonAntimatter0103 physical sciencesSubatomic PhysicsPhysics::Accelerator PhysicsNuclear Physics - Experimentddc:530010306 general physicsEPJ Web of Conferences
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Positron annihilation studies of binary Ni-based alloys

1987

Positron annihilation studies of Ni–1 at. % X (X = Pb, In and Zn) alloys have been performed. The experimentally observed changes in the parameters connecting the shape of angular correlation curve with the kind and concentration of crystal lattice defects are correlated with the values of the vacancy-solute binding energy calculated from the vacancy model of melting.

PhysicsAntiparticleAnnihilationBinding energyGeneral ChemistryCrystal structureCondensed Matter PhysicsCrystallographic defectCondensed Matter::Materials SciencePositronVacancy defectAntimatterGeneral Materials ScienceAtomic physicsCrystal Research and Technology
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Nonlinear density dependence of the positron decay rate in helium

1980

The decay rate of thermalized positrons in helium is calculated as a function of the fluid density, incorporating the multiple scattering of the positron off the atoms. The obtained nonlinearity agrees with experimental data outside the self-trapping region.

PhysicsAntiparticleAnnihilationScatteringchemistry.chemical_elementPositronchemistryAntimatterPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPhysics::Atomic PhysicsPositron emissionAtomic physicsHeliumLeptonPhysical Review A
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Accelerator testing of the general antiparticle spectrometer; a novel approach to indirect dark matter detection

2005

We report on recent accelerator testing of a prototype general antiparticle spectrometer (GAPS). GAPS is a novel approach for indirect dark matter searches that exploits the antideuterons produced in neutralino-neutralino annihilations. GAPS captures these antideuterons into a target with the subsequent formation of exotic atoms. These exotic atoms decay with the emission of X-rays of precisely defined energy and a correlated pion signature from nuclear annihilation. This signature uniquely characterizes the antideuterons. Preliminary analysis of data from a prototype GAPS in an antiproton beam at the KEK accelerator in Japan has confirmed the multi-X-ray/pion star topology and indicated X-…

PhysicsAntiparticleAnnihilationSpectrometerAstrophysics (astro-ph)Dark matterFOS: Physical sciencesAstronomy and AstrophysicsAstrophysicsAstrophysicsPreliminary analysisNuclear physicsAntiproton beamPionHigh Energy Physics::ExperimentNuclear ExperimentExotic atomJournal of Cosmology and Astroparticle Physics
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New determination of the electron's mass.

2001

A new independent value for the electron's mass in units of the atomic mass unit is presented, ${m}_{e}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}0.0005485799092(4)\mathrm{u}$. The value is obtained from our recent measurement of the $g$ factor of the electron in ${}^{12}{\mathrm{C}}^{5+}$ in combination with the most recent quantum electrodynamical (QED) predictions. In the QED corrections, terms of order ${\ensuremath{\alpha}}^{2}$ were included by a perturbation expansion in $Z\ensuremath{\alpha}$. Our total precision is three times better than that of the accepted value for the electron's mass.

PhysicsAntiparticleAtomic mass constantLandé g-factorElectron rest massGeneral Physics and AstronomyOrder (ring theory)Elementary particleAtomic mass unitAtomic physicsHyperfine structurePhysical review letters
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