Search results for "Polar"

showing 10 items of 3817 documents

Measurement of the polarization of $$\Lambda ^0 , \overline \Lambda ^0 , \Sigma ^ + $$ and ?? produced in a ?? beam of 330 GeV/c

1995

The polarization of Lambda0 , AntiLambda0 , Sigma+ and Xi- inclusively produced in Sigma- induced interactions at 330 GeV has been measured in the experiment WA89 at CERN. This is the first measurement of polarization of baryons produced by a hyperon beam. No polarization of AntiLambda is observed, as was also the case in proton beam data. At transverse momenta of about 1~GeV/c Lambda0 and Sigma+ show little polarization, significantly lower than in the proton beam data, while Xi- have a polarization comparable to the polarization of Lambda0 produced in proton beams. The polarization of Lambda0, AntiLambda0, Sigma+ and Xi- inclusively produced in Sigma- induced interactions at 330 GeV has b…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderHigh Energy Physics::PhenomenologyNuclear TheoryHyperonLambdaPolarization (waves)OmegaNuclear physicsBaryonNuclear fusionPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear ExperimentBeam (structure)Particle Physics - Experiment
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Polarimetry on dense samples of spin-polarized 3He by magnetostatic detection

1997

Abstract A very sensitive low-field fluxgate magnetometer is used to detect the static magnetic field produced by dense samples of spin-polarized 3He gas contained in spherical glass cells at pressures around several bars. The 3He nuclear polarization can be extracted with high precision ΔP P by utilizing magnetostatic detection in combination with adiabatic fast-passage spin reversal. The polarization losses can be kept well below 0.1% thus making this type of polarimetry almost non-destructive. More simply even, P can be measured with reduced accuracy by the change of field when the cell is removed from the fluxgate. In this case the accuracy is limited to about 10% due to the uncertainti…

PhysicsNuclear and High Energy PhysicsMagnetometerbusiness.industryPolarimetryPolarization (waves)MagnetostaticsMolecular physicsFluxgate compasslaw.inventionOpticslawAdiabatic processbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Sweeping the Space of Admissible Quark Mass Matrices

2002

We propose a new and efficient method of reconstructing quark mass matrices from their eigenvalues and a complete set of mixing observables. By a combination of the principle of NNI (nearest neighbour interaction) bases which are known to cover the general case, and of the polar decomposition theorem that allows to convert arbitrary nonsingular matrices to triangular form, we achieve a parameterization where the remaining freedom is reduced to one complex parameter. While this parameter runs through the domain bounded by a circle with radius R determined by the up-quark masses around the origin in the complex plane one sweeps the space of all mass matrices compatible with the given set of d…

PhysicsNuclear and High Energy PhysicsMathematical analysisPolar decompositionFOS: Physical sciencesSpace (mathematics)Domain (mathematical analysis)High Energy Physics - PhenomenologyClassical mechanicsHigh Energy Physics - Phenomenology (hep-ph)Cover (topology)Mixing (mathematics)Bounded functionComplex planeEigenvalues and eigenvectors
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Many-body approach to the inclusive (e,e ') reaction from the quasielastic to the Delta excitation region

1997

We have performed a many body calculation of the inclusive (e,e') cross section which runs over the three traditional regions at intermediate energies: the quasielastic peak, the dip region and the delta region. The longitudinal and transverse response functions in the quasielastic peak have also been evaluated. Traditional effects like polarization, meson exchange currents, final state interaction and delta renormalization in the nuclear medium have been included. Meson exchange currents are generated from a model of pion electroproduction on the nucleon which reproduces accurately the experimental data. The inclusive cross section accounts for 1N,2N,3N mechanisms of virtual photon absorpt…

PhysicsNuclear and High Energy PhysicsMesonNuclear TheoryNuclear TheoryVirtual particleFísicaPolarization (waves)RenormalizationNuclear physicsTransverse planePionNucleonNuclear ExperimentExcitation
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Polarizability effects in electronic and muonic atoms

1983

TheS state polarizability shifts are derived from the virtual forward Compton scattering in the unretarded dipole approximation. In the non-relativistic limit ω N /2m≪1, the shift is proportional to the photonuclear sum rule σ−3/2, while in the relativistic limit ω N /2m≫1 it is proportional to a logarithmically weighted σ−2 sum rule. In both cases, the characteristic momentum transfer is (2mω N )1/2. The non-locality from the intermediate lepton propagation removes the divergence typical of the static limit. Explicit formulas for the shifts are given for both the relativistic and non-relativistic limits.

PhysicsNuclear and High Energy PhysicsMomentum transferCompton scatteringFísicaElementary particleDiscrete dipole approximationPolarizabilityQuantum electrodynamicsQuantum mechanicsSum rule in quantum mechanicsLimit (mathematics)Nuclear PhysicsLeptonZeitschrift f�r Physik A Atoms and Nuclei
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Ab initio calculation of nuclear structure corrections in muonic atoms

2018

The measurement of the Lamb shift in muonic hydrogen and the subsequent emergence of the proton-radius puzzle have motivated an experimental campaign devoted to measuring the Lamb shift in other light muonic atoms, such as muonic deuterium and helium. For these systems it has been shown that two-photon exchange nuclear structure corrections are the largest source of uncertainty and consequently the bottleneck for exploiting the experimental precision to extract the nuclear charge radius. Utilizing techniques and methods developed to study electromagnetic reactions in light nuclei, recent calculations of nuclear structure corrections to the muonic Lamb shift have reached unprecedented precis…

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsAtomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesEffective nuclear charge3. Good healthLamb shiftPhysics - Atomic PhysicsNuclear physicsNuclear Theory (nucl-th)DeuteriumCharge radius0103 physical sciencesEffective field theoryPhysics::Atomic and Molecular ClustersVacuum polarizationSum rule in quantum mechanicsPhysics::Atomic Physics010306 general physicsExotic atom
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General Multipole Expansion of Polarization Observables in Deuteron Electrodisintegration

2002

Formal expressions are derived for the multipole expansion of the structure functions of a general polarization observable of exclusive electrodisintegration of the deuteron using a longitudinally polarized beam and/or an oriented target. This allows one to exhibit explicitly the angular dependence of the structure functions by expanding them in terms of the small rotation matrices $d^j_{m'm}(\theta)$, whose coefficients are given in terms of the electromagnetic multipole matrix elements. Furthermore, explicit expressions for the coefficients of the angular distributions of the differential cross section including multipoles up to $L_{max}=3$ are listed in tabular form.

PhysicsNuclear and High Energy PhysicsNuclear Theory010308 nuclear & particles physicsPolarization observablesHadronFOS: Physical sciencesObservableRotation matrixPolarization (waves)01 natural sciencesNuclear Theory (nucl-th)DeuteriumQuantum electrodynamics0103 physical sciencesNuclear fusion010306 general physicsMultipole expansion
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A Ramsey apparatus for the measurement of the incoherent neutron scattering length of the deuteron

2008

Abstract A Ramsey apparatus for cold, polarised neutrons is described, which enables us to measure neutron precession angles with an absolute accuracy of about 1 ∘ . This is necessary to perform a planned high-accuracy measurement of the incoherent neutron scattering length b i , d of the deuteron. The performance of the apparatus is demonstrated in systematic stability measurements as well as in two selected examples using samples containing polarised nuclear spins.

PhysicsNuclear and High Energy PhysicsNuclear TheoryDynamic nuclear polarisationNeutron scatteringSmall-angle neutron scatteringInelastic neutron scatteringNeutron time-of-flight scatteringNeutron spin echoNuclear physicsQuasielastic neutron scatteringNeutronNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The role of the neutron electric form factor ind(e, e? N)N including polarization observables

1988

The influence of the neutron electric form factor on various observables in two-body break-up of deuterons by electrons such as differential cross section, beam, target and beam-target asymmetries and outgoing nucleon polarization as well is investigated for different kinematic regions. The electron-deuteron vector asymmetryAedV and the outgoing nucleon polarization component P′x(n) are the most promising observables in and off the quasi-free region for a determination ofGEn. Also the single polarization observablesAdT and Py0(p) and the double polarization observable P′z(n) show significant influences fromGEn.

PhysicsNuclear and High Energy PhysicsNuclear TheoryElectric form factorObservableElectronPolarization (waves)Nuclear physicsDeuteriumNuclear fusionNeutronAtomic physicsNuclear ExperimentNucleonZeitschrift f�r Physik A Atomic Nuclei
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One-quasiparticle States in the Nuclear Energy Density Functional Theory

2009

We study one-quasiproton excitations in the rare-earth region in the framework of the nuclear Density Functional Theory in the Skyrme-Hartree-Fock-Bogoliubov variant. The blocking prescription is implemented exactly, with the time-odd mean field fully taken into account. The equal filling approximation is compared with the exact blocking procedure. We show that both procedures are strictly equivalent when the time-odd channel is neglected, and discuss how nuclear alignment properties affect the time-odd fields. The impact of time-odd fields on calculated one-quasiproton bandhead energies is found to be rather small, of the order of 100-200 keV; hence, the equal filling approximation is suff…

PhysicsNuclear and High Energy PhysicsNuclear TheoryEnergy density functionalNuclear TheoryFOS: Physical sciencesNuclear matterPolarization (waves)Nuclear Theory (nucl-th)Mean field theoryQuantum mechanicsQuantum electrodynamicsQuasiparticleFunctional theoryNuclear theoryNuclear density
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