Search results for "magnetic dipole moment"

showing 10 items of 117 documents

Evolution of nuclear structure in neutron-rich odd-Zn isotopes and isomers

2017

Collinear laser spectroscopy was performed on Zn (Z=30) isotopes at ISOLDE, CERN. The study of hyperfine spectra of nuclei across the Zn isotopic chain, N=33–49, allowed the measurement of nuclear spins for the ground and isomeric states in odd-A neutron-rich nuclei up to N=50. Exactly one long-lived (&

Nuclear and High Energy Physicsshell closureShell closureNuclear TheoryLasermagnetic dipole moment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesQuadrupole momentMagnetic dipole momentNaturvetenskap0103 physical sciencesPhysics::Atomic and Molecular ClustersDalton Nuclear InstituteNuclear Physics - Experimentddc:530NeutronPhysics::Atomic Physics010306 general physicsNuclear ExperimentHyperfine structurePhysicsValence (chemistry)quadrupole momentMagnetic moment010308 nuclear & particles physicsNuclear structurePhysique atomique et nucléairelcsh:QC1-999laserZincResearchInstitutes_Networks_Beacons/dalton_nuclear_instituteZinc ; Magnetic dipole moment ; Quadrupole moment ; Laser ; Shell closureQuadrupoleNuclear magnetic momentPräzisionsexperimente - Abteilung BlaumAtomic physicsNatural SciencesMagnetic dipolelcsh:Physics
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Final report on the CERN muon storage ring including the anomalous magnetic moment and the electric dipole moment of the muon, and a direct test of r…

1978

Abstract A comprehensive description of the muon storage ring and its operation is given, and the final results of the experiment are presented and discussed. The anomalous magnetic moments of positive and negative muons are found to be aμ+ = 1165911(11) × 10−9 and aμ− = 1165937(12) × 10−9 giving an average value for muons of aμ = 1165924(8.5) × 10−9. The electric dipole moments were also measured with the results Dμ+= (8.6 ± 4.5) × 10−9e · cm and Dμ− = (0.8 ± 4.3) × 10−19e · cm. Under the assumption of the CPT theorem these yield a weighted average of Dμ = (3.7 ± 3.4) × 10−19e · cm. Finally the time transformation of special relativity is shown to be valid to (0.8 ± 0.7) × 10−3 at γ ≅ 29.3…

Nuclear physicsPhysicsNuclear and High Energy PhysicsDipoleElectric dipole momentParticle physicsMuonMagnetic momentAnomalous magnetic dipole momentCPT symmetryTime dilationParticle Physics - ExperimentStorage ringNuclear Physics B
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HADRONIC CROSS SECTION MEASUREMENT AT BES-III

2014

Measurements of the R ratio are closely related to two pre quantities, the anomalous magnetic moment of the muon (g - 2), and the value of the electromagnetic fine structure constant [Formula: see text]. Hadronic contributions to both quantities can be derived via dispersion integrals, using experimental R data as input. For the phenomenological evaluations of these contributions, different energy ranges of hadronic cross section data are required. At BES-III, Initial State Radiation (ISR) from an existing Ψ(3770) dataset will be used for measurements of hadronic cross sections below [Formula: see text], while for higher energies a dedicated energy scan program will be performed up to [For…

Nuclear physicsPhysicsParticle physicsCross section (physics)MuonAnomalous magnetic dipole momentHadronDispersion (optics)High Energy Physics::ExperimentFine-structure constantRadiationEnergy (signal processing)International Journal of Modern Physics: Conference Series
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Leptons and QCD

2015

Three important QCD-related aspects of the τ and μ dynamics are reviewed: the determination of the strong coupling from the hadronic tau decay width, leading to the updated value αs(mτ2)=0.331±0.013; the measurement of |Vus| through the Cabibbo-suppressed decays of the τ, and the Standard Model prediction for the muon anomalous magnetic moment.

Nuclear physicsQuantum chromodynamicsPhysicsNuclear and High Energy PhysicsParticle physicsMuonAnomalous magnetic dipole momentHigh Energy Physics::PhenomenologyHadronStrong couplingHigh Energy Physics::ExperimentLeptonStandard ModelNuclear and Particle Physics Proceedings
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Real and Virtual Compton Scattering (experiments)

1999

This paper deals with Real and Virtual Compton Scattering off the proton at threshold and the way to deduce information about the nucleon polarizabilities.

Nuclear physicsScattering cross-sectionPhysicsAnomalous magnetic dipole momentProtonAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryPhysics::Atomic and Molecular ClustersCompton scatteringNuclear ExperimentNucleon
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Developments in the position-space approach to the HLbL contribution to the muon $g-2$ on the lattice

2019

The measurement of the anomalous magnetic moment of the muon and its prediction allow for a high-precision test of the Standard Model (SM). In this proceedings article we present ongoing work combining lattice QCD and continuum QED in order to determine an important SM contribution to the magnetic moment, the hadronic light-by-light contribution. We compute the quark-connected contribution in the Mainz position-space approach and investigate the long-distance part of our data using calculations of the $\pi^0$-pole and charged pion loop contributions.

Particle physicsHigh Energy Physics::LatticeHadronhep-latFOS: Physical sciencesPosition and momentum space01 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)PionHigh Energy Physics - LatticeLattice (order)0103 physical sciences010306 general physicsParticle Physics - PhenomenologyPhysicsMuonMagnetic momentAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHigh Energy Physics - Lattice (hep-lat)hep-phParticle Physics - LatticeLattice QCDHigh Energy Physics - PhenomenologyHigh Energy Physics::Experiment
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Lorentz-covariant coordinate-space representation of the leading hadronic contribution to the anomalous magnetic moment of the muon

2017

We present a Lorentz-covariant, Euclidean coordinate-space expression for the hadronic vacuum polarisation, the Adler function and the leading hadronic contribution to the anomalous magnetic moment of the muon. The representation offers a lot of flexibility for an implementation in lattice QCD. We expect it to be particularly helpful for the quark-line disconnected contributions.

Particle physicsPhysics and Astronomy (miscellaneous)Lorentz transformationHigh Energy Physics::LatticeHadronFOS: Physical scienceslcsh:Astrophysics01 natural sciencessymbols.namesakeHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEuclidean geometrylcsh:QB460-466Covariant transformationlcsh:Nuclear and particle physics. Atomic energy. RadioactivityCoordinate space010306 general physicsEngineering (miscellaneous)PhysicsMuonAnomalous magnetic dipole moment010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)High Energy Physics::PhenomenologyLattice QCDHigh Energy Physics - Phenomenologysymbolslcsh:QC770-798High Energy Physics::ExperimentEuropean Physical Journal C
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Dissecting the Hadronic Contributions to (g−2)μ by Schwinger’s Sum Rule

2018

The theoretical uncertainty of $(g\ensuremath{-}2{)}_{\ensuremath{\mu}}$ is currently dominated by hadronic contributions. In order to express those in terms of directly measurable quantities, we consider a sum rule relating $g\ensuremath{-}2$ to an integral of a photoabsorption cross section. The sum rule, attributed to Schwinger, can be viewed as a combination of two older sum rules: Gerasimov-Drell-Hearn and Burkhardt-Cottingham. The Schwinger sum rule has an important feature, distinguishing it from the other two: the relation between the anomalous magnetic moment and the integral of a photoabsorption cross section is linear, rather than quadratic. The linear property makes it suitable …

PhysicsAnomalous magnetic dipole moment010308 nuclear & particles physicsNuclear TheoryHadronGeneral Physics and AstronomyOrder (ring theory)01 natural sciencesQuadratic equation0103 physical sciencesSum rule in quantum mechanicsNuclear Experiment010306 general physicsNuclear theoryMathematical physicsPhysical Review Letters
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On the magnetic dipole moment of the153Tb ground state

1981

Temperature dependence of the angular distribution anisotropy of the 212·0 keV gamma-ray following the decay of153Tb oriented in a gadolinium host was measured at temperatures from 16 to 70 mK. Magnetic dipole hyperfine splitting parameter a0 for153Tb(Gd) and magnetic dipole moment of the153Tb ground state were estimated to be ¦a0¦≧1·2×10−5 eV and ¦μ¦≧≧3·1 nuclear magnetons, respectively.

PhysicsBond dipole momentDipoleMagnetic momentCondensed matter physicsNuclear magnetic momentTransition dipole momentGeneral Physics and AstronomyElectric dipole transitionAtomic physicsElectron magnetic dipole momentMagnetic dipoleCzechoslovak Journal of Physics
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Field Dependence of the Electron Spin Relaxation in Quantum Dots

2005

Interaction of the electron spin with local elastic twists due to transverse phonons has been studied. Universal dependence of the spin relaxation rate on the strength and direction of the magnetic field has been obtained in terms of the electron gyromagnetic tensor and macroscopic elastic constants of the solid. The theory contains no unknown parameters and it can be easily tested in experiment. At high magnetic field it provides parameter-free lower bound on the electron spin relaxation in quantum dots.

PhysicsCondensed Matter - Materials ScienceCondensed matter physicsSpin polarizationStatistical Mechanics (cond-mat.stat-mech)Relaxation (NMR)General Physics and AstronomyMaterials Science (cond-mat.mtrl-sci)FOS: Physical sciences02 engineering and technologyElectronZero field splitting021001 nanoscience & nanotechnology01 natural sciences7. Clean energyElectron magnetic dipole momentSpin magnetic momentQuantum dot0103 physical sciencesSpinplasmonics010306 general physics0210 nano-technologyCondensed Matter - Statistical Mechanics
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