Search results for "annihilation"

showing 10 items of 1016 documents

Characterization of non-polar ZnO layers with positron annihilation spectroscopy

2008

We applied positron annihilation spectroscopy to study the effect of growth polarity on the vacancy defects in ZnO grown by metal-organic vapor phase deposition on sapphire. Both c-plane and a-plane ZnO layers were measured, and Zn vacancies were identified as the dominant defects detected by positrons. The results are qualitatively similar to those of earlier experiments in GaN. The Zn vacancy concentration decreases in c-plane ZnO by almost one order of magnitude (from high 10 cm−3 to low 10 cm−3) when the layer thickness is increased from 0.5 to 2 μm. Interestingly, in a-plane ZnO the Zn vacancy concentration is constant at a level of about 2×10 cm−3 in all the samples with thicknesses v…

PositronMaterials scienceVacancy defectAnnihilation radiationSapphireAnalytical chemistryGeneral Physics and AstronomyAnisotropyDeposition (law)Positron annihilation spectroscopyDoppler broadening
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Positron Annihilation in Medical Substances of Insulin

2005

Positrons lifetimes were measured in medical substances of insulin (human and animal), differing as far as the degree of purity and time of their activity in the organism are concerned. In all of the cases the spectrum of positron lifetime was distributed into three components, with the long-life component ranging from 1.8 to 2.08 ns and the intensity taking on values from 18 to 24%. Making use of Tao–Eldrup model, the average radius of the free volume, in which o-Ps annihilated, and the degree of filling in the volume were determined. It was found that the value of the long-life component for human insulin is higher than that of animal insulin. Moreover, the value of this component clearly…

PositronNuclear magnetic resonanceVolume (thermodynamics)Component (thermodynamics)ChemistryInsulinmedicine.medical_treatmentmedicineHuman insulinGeneral Physics and AstronomyIntensity (physics)Degree (temperature)Positron annihilationActa Physica Polonica A
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Measurement of proton electromagnetic form factors in the time-like region using initial state radiation at BESIII

2021

Physics letters / B 817, 136328 (2021). doi:10.1016/j.physletb.2021.136328

Protonannihilation [electron positron]01 natural sciencesform factor [electron]High Energy Physics - ExperimentSubatomär fysikHigh Energy Physics - Experiment (hep-ex)BESIII; Electromagnetic form factors; Initial state radiation; ProtonSubatomic Physicsangular distributionNuclear ExperimentPhysicsPhysicsForm factor (quantum field theory)initial-state interaction [radiation]Beijing Stormagnetic [form factor]ratio [form factor]electron positron --> p anti-pcolliding beams [electron positron]ProtonInitial State Radiationpair production [p]electromagnetic [form factor]Born approximationNuclear and High Energy Physicsdata analysis methodQC1-999FOS: Physical sciencesRadiation5303.773-4.600 GeV-cmsNONuclear physicsCross section (physics)Angular distributionElectromagnetic form factors0103 physical sciencesform factor [p]tree approximationddc:530010306 general physicsinitial stateBES010308 nuclear & particles physicshelicity [p]BESIIIState (functional analysis)(p anti-p) [mass spectrum]Electromagnetic form FactorsHigh Energy Physics::Experimentproduction [threshold]Initial state radiationexperimental results
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Deformed quons and bi-coherent states

2017

We discuss how a q-mutation relation can be deformed replacing a pair of conjugate operators with two other and unrelated operators, as it is done in the construction of pseudo-fermions, pseudo-bosons and truncated pseudo-bosons. This deformation involves interesting mathematical problems and suggests possible applications to pseudo-hermitian quantum mechanics. We construct bi-coherent states associated to $\D$-pseudo-quons, and we show that they share many of their properties with ordinary coherent states. In particular, we find conditions for these states to exist, to be eigenstates of suitable annihilation operators and to give rise to a resolution of the identity. Two examples are discu…

Pseudo-bosonComputer Science::Machine LearningSimilarity (geometry)Mathematical problemGeneral MathematicsFOS: Physical sciencesGeneral Physics and AstronomyComputer Science::Digital Libraries01 natural sciencesPhysics and Astronomy (all)Statistics::Machine LearningTheoretical physicsIdentity (mathematics)Engineering (all)Quon0103 physical sciencesMathematics (all)0101 mathematics010306 general physicsSettore MAT/07 - Fisica MatematicaEigenvalues and eigenvectorsMathematical PhysicsPhysicsQuantum PhysicsAnnihilation010102 general mathematicsGeneral EngineeringMathematical Physics (math-ph)Bounded functionComputer Science::Mathematical SoftwareCoherent statesQuantum Physics (quant-ph)Coherent stateResolution (algebra)
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Pseudo-Bosons from Landau Levels

2010

We construct examples of pseudo-bosons in two dimensions arising from the Hamiltonian for the Landau levels. We also prove a no-go result showing that non-linear combinations of bosonic creation and annihilation operators cannot give rise to pseudo-bosons.

Pseudo-bosonFOS: Physical sciencesnon-hermitian HamiltoniansTheoretical physicssymbols.namesakeQuantum mechanicsSettore MAT/07 - Fisica MatematicaMathematical PhysicsBosonPhysicsCondensed Matter::Quantum GasesQuantum Physicslcsh:MathematicsHigh Energy Physics::PhenomenologyCreation and annihilation operatorsAnalysiLandau quantizationMathematical Physics (math-ph)lcsh:QA1-939Non-hermitian HamiltonianLandau theorysymbolspseudo-bosonsGeometry and TopologyHamiltonian (quantum mechanics)Quantum Physics (quant-ph)Analysis
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Construction of pseudo-bosons systems

2010

In a recent paper we have considered an explicit model of a PT-symmetric system based on a modification of the canonical commutation relation. We have introduced the so-called {\em pseudo-bosons}, and the role of Riesz bases in this context has been analyzed in detail. In this paper we consider a general construction of pseudo-bosons based on an explicit {coordinate-representation}, extending what is usually done in ordinary supersymmetric quantum mechanics. We also discuss an example arising from a linear modification of standard creation and annihilation operators, and we analyze its connection with coherent states.

Quantum PhysicsComputer sciencequantum mechanicsCreation and annihilation operatorsFOS: Physical sciencesStatistical and Nonlinear PhysicsContext (language use)Mathematical Physics (math-ph)pseudo-bosonConnection (mathematics)Canonical commutation relationAlgebraCoherent statesSupersymmetric quantum mechanicsQuantum statistical mechanicsRepresentation (mathematics)Quantum Physics (quant-ph)Settore MAT/07 - Fisica MatematicaMathematical Physics
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Study of thee+e−→K+K−reaction in the energy range from 2.6 to 8.0 GeV

2015

The e^+e^− → K^+K^− cross section and charged-kaon electromagnetic form factor are measured in the e^+e^− center-of-mass energy range (E) from 2.6 to 8.0 GeV using the initial-state radiation technique with an undetected photon. The study is performed using 469  fb^(−1) of data collected with the BABAR detector at the PEP-II2 e^+e^− collider at center-of-mass energies near 10.6 GeV. The form factor is found to decrease with energy faster than 1/E^2 and approaches the asymptotic QCD prediction. Production of the K^+K^− final state through the J/ψ and ψ(2S) intermediate states is observed. The results for the kaon form factor are used together with data from other experiments to perform a mod…

Quantum chromodynamicsNuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsAmplitudePhotonPair productionMesonElectron–positron annihilationHigh Energy Physics::ExperimentRadiation7. Clean energyPhysical Review D
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Observation of an Anomalous Line Shape of theη′π+π−Mass Spectrum near thepp¯Mass Threshold inJ/ψ→γη′π+π−

2016

Using 1.09 x 10(9) J/psi events collected by the BESIII experiment in 2012, we study the J / psi -> gamma eta'pi(+)pi(-) process and observe a significant abrupt change in the slope of the eta'pi(+)pi(-) invariant mass distribution at the proton-antiproton (p (p) over bar) mass threshold. We use two models to characterize the eta'pi(+)pi(-) line shape around 1.85 GeV/c(2): one that explicitly incorporates the opening of a decay threshold in the mass spectrum (Flatte formula), and another that is the coherent sum of two resonant amplitudes. Both fits show almost equally good agreement with data, and suggest the existence of either a broad state around 1.85 GeV/c(2) with strong couplings to t…

Quantum chromodynamicsPhysics010308 nuclear & particles physicsGlueballElectron–positron annihilationGeneral Physics and Astronomy01 natural sciencesNuclear physicsAmplitude0103 physical sciencesBound statePiMass spectrumHigh Energy Physics::ExperimentInvariant mass010306 general physicsPhysical Review Letters
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Measurement of the Absolute Branching Fraction of Ds+→τ+ντ via τ+→e+νeν¯τ

2021

Using a dataset of 6.32  fb^{-1} of e^{+}e^{-} annihilation data collected with the BESIII detector at center-of-mass energies between 4178 and 4226 MeV, we have measured the absolute branching fraction of the leptonic decay D_{s}^{+}→τ^{+}ν_{τ} via τ^{+}→e^{+}ν_{e}ν[over ¯]_{τ}, and find B_{D_{s}^{+}→τ^{+}ν_{τ}}=(5.27±0.10±0.12)×10^{-2}, where the first uncertainty is statistical and the second is systematic. The precision is improved by a factor of 2 compared to the previous best measurement. Combining with f_{D_{s}^{+}} from lattice quantum chromodynamics calculations or the |V_{cs}| from the CKMfitter group, we extract |V_{cs}|=0.978±0.009±0.012 and f_{D_{s}^{+}}=(251.1±2.4±3.0)  MeV, r…

Quantum chromodynamicsPhysicsCrystallographyAnnihilation010308 nuclear & particles physicsBranching fraction0103 physical sciencesLattice (group)General Physics and Astronomy010306 general physics01 natural sciencesLeptonStandard ModelPhysical Review Letters
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A measurement of the QCD colour factors and a limit on the light gluino

1997

Using data collected from 1992 to 1995 with the ALEPH detector at LEP, a measurement of the colour factor ratios C-A/C-F and T-F/C-F and the strong coupling constant = C-F alpha(s), (M-Z)/(2 pi) has been performed by fitting theoretical predictions simultaneously to the measured differential two-jet rate and angular distributions in four-jet events. The result is found to be in excellent agreement with QCD. C-A/C-F = 2.20 +/- 0.09 (stat) +/- 0.13 (syst), T-F/C-F = 0.29 +/- 0.05 (stat) +/- 0.06 (syst). Fixing C-A/C-F and T-F/C-F to the QCD values permits a determination of alpha(s) (M-Z) and n(f), the number of active flavours. With this measurement the existence of a gluino with mass below …

Quantum chromodynamicsPhysicsGluinoParticle physicsPhysics and Astronomy (miscellaneous)PhysicsElectron–positron annihilationHigh Energy Physics::PhenomenologyLower limitNuclear physicsStrong couplingHigh Energy Physics::ExperimentLimit (mathematics)Particle Physics - ExperimentParticle Physics - Phenomenology
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