Search results for "Radius"

showing 10 items of 708 documents

Shape coexistence in Au 187 studied by laser spectroscopy

2020

Hyperfine-structure parameters and isotope shift of the 9/2$^−$ isomeric state in $^{187}$Au relative to $^{197}$Au for the 267.6-nm atomic transition have been measured for the first time using the in-source resonance-ionization spectroscopy technique. The magnetic dipole moment and change in the mean-square charge radius for this 9/2$^−$ isomer have been deduced. The observed large isomer shift relative to the 1/2$^+$ ground state in $^{187}$Au confirms the occurrence of the shape coexistence in $^{187}$Au proposed earlier from the analysis of the nuclear spectroscopic data and particle plus triaxial rotor calculations. The analysis of the magnetic moment supports the previously proposed …

PhysicsMagnetic momentIsotope010308 nuclear & particles physicsNuclear structure01 natural sciences7. Clean energyCharge radius0103 physical sciencesPhysics::Atomic and Molecular ClustersParticleDeformation (engineering)Atomic physics010306 general physicsGround stateSpectroscopyPhysical Review C
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Hyperfine and Isotope Shift Measurements Far off Stability by Optical Pumping

1977

In this talk I will review optical pumping (OP) experiments performed by our group to ISOLDE, CERN, in a series of Hg isotopes spanning from mass number 181 to 205 (first results in refs. [1] and [2], final in refs. [3] and [4]. I will then discuss what impact these measurements had on nuclear structure research far off stability and how the results of the latter are retroacting again on the optical work. In particular they ask for isotope shifts (IS) of light even Hg isotopes which we are prepared to measure by laser spectroscopy. Further I would like to communicate briefly first results of optical pumping experiments on “exotic” Rb and Cs isotopes. Finally I will discuss plans for laser s…

PhysicsMass numberOptical pumpingNuclear magnetic resonanceLarge Hadron ColliderIsotopeCharge radiusNuclear structureAtomic physicsSpectroscopyHyperfine structure
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Conductivity reconstructions using real data from a new planar electrical impedance tomography device

2013

Abstract In this paper, we present results of reconstructions using real data from a new planar electrical impedance tomography device developed at the Institut fur Physik, Johannes Gutenberg Universitat, Mainz, Germany. The prototype consists of a planar sensing head of circular geometry, and it was designed mainly for breast cancer detection. There are 12 large outer electrodes arranged on a ring of radius  cm where the external currents are injected, and a set of 54 point-like high-impedance inner electrodes where the induced voltages are measured. Two direct (i.e. non-iterative) reconstruction algorithms are considered: one is based on a discrete resistor model, and the other one is an …

PhysicsMathematical optimizationbusiness.industryApplied MathematicsGeneral EngineeringRadiusConductivityIntegral equationComputer Science Applicationslaw.inventionPlanarOpticslawElectrodeResistorbusinessElectrical impedance tomographyVoltageInverse Problems in Science and Engineering
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Charge radii of odd-A 191–211Po isotopes

2013

Isotope shifts have been measured for the odd-A polonium isotopes 191–211Po and changes in the nuclear mean square charge radii δr2 have been deduced. The measurements were performed at CERN-ISOLDE using the in-source resonance-ionization spectroscopy technique. The combined analysis of these data and our recent results for even-A polonium isotopes indicates an onset of deformation already at 197,198Po, when going away from stability. This is significantly earlier than was suggested by previous theoretical and experimental studies of the polonium isotopes. Moreover and in contrast to the mercury isotopes, where a strong odd–even staggering of the charge radii of the ground states was observ…

PhysicsMean squareNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsShape coexistencechemistry.chemical_elementMercury IsotopesCharge (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIsotopes of nitrogenNuclear physicsIsotope shiftchemistry0103 physical sciencesNeutronPhysics::Atomic PhysicsAtomic physicsNuclear charge radiusNuclear Experiment010306 general physicsSpectroscopyPoloniumPhysics Letters B
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Theory of the n = 2 levels in muonic helium-3 ions

2017

The present knowledge of Lamb shift, fine-, and hyperfine structure of the 2S and 2P states in muonic helium-3 ions is reviewed in anticipation of the results of a first measurement of several 2S → 2P transition frequencies in the muonic helium-3 ion, μ3He+. This ion is the bound state of a single negative muon μ- and a bare helium-3 nucleus (helion), 3He++. A term-by-term comparison of all available sources, including new, updated, and so far unpublished calculations, reveals reliable values and uncertainties of the QED and nuclear structure-dependent contributions to the Lamb shift and the hyperfine splitting. These values are essential for the determination of the helion rms charge radiu…

PhysicsMuonNuclear TheoryAtomic Physics (physics.atom-ph)010308 nuclear & particles physicsNuclear structureFOS: Physical sciences01 natural sciencesAtomic and Molecular Physics and OpticsPhysics - Atomic PhysicsLamb shiftNuclear Theory (nucl-th)Nuclear physicsCharge radiusHelium-30103 physical sciencesAtomic PhysicsHelionPhysics::Atomic Physics010306 general physicsHyperfine structureExotic atom
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Measuring the surface thickness of the weak charge density of nuclei

2020

The present PREX-II and CREX experiments are measuring the rms radius of the weak charge density of $^{208}$Pb and $^{48}$Ca. We discuss the feasibility of a new parity violating electron scattering experiment to measure the surface thickness of the weak charge density of a heavy nucleus. Once PREX-II and CREX have constrained weak radii, an additional parity violating measurement at a momentum transfer near 0.76 fm$^{-1}$ for $^{208}$Pb or 1.28 fm$^{-1}$ for $^{48}$Ca can determine the surface thickness.

PhysicsNuclear Theory (nucl-th)Nuclear TheoryMomentum transferCharge densityFOS: Physical sciencesParity (physics)RadiusAtomic physicsNuclear Experiment (nucl-ex)Electron scatteringNuclear theoryNuclear Experiment
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Two-photon exchange on the neutron and the hyperfine splitting

2018

We calculate the contribution from the two-photon exchange on the neutron to the hyperfine splitting of S energy levels. We update the value of the neutron Zemach radius, estimate total recoil and polarizability corrections. The resulting two-photon exchange in electronic atoms exceeds by an order of magnitude the leading Zemach term and has different sign both in electronic and muonic hydrogen.

PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)FOS: Physical sciencesRadiusPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)RecoilPolarizabilityNeutronPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Atomic physicsNuclear ExperimentHyperfine structureOrder of magnitudeExotic atomSign (mathematics)Physical Review D
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Breakdown of the expansion of finite-size corrections to the hydrogen Lamb shift in moments of charge distribution

2015

We quantify a limitation in the usual accounting of the finite-size effects, where the leading $[(Z\alpha)^4]$ and subleading $[(Z\alpha)^5]$ contributions to the Lamb shift are given by the mean-square radius and the third Zemach moment of the charge distribution. In the presence of any non-smooth behaviour of the nuclear form factor at scales comparable to the inverse Bohr radius, the expansion of the Lamb shift in the moments breaks down. This is relevant for some of the explanations of the "proton size puzzle". We find, for instance, that the de R\'ujula toy model of the proton form factor does not resolve the puzzle as claimed, despite the large value of the third Zemach moment. Withou…

PhysicsNuclear TheoryProtonAtomic Physics (physics.atom-ph)Form factor (quantum field theory)Electric form factorFOS: Physical sciencesRadiusAtomic and Molecular Physics and OpticsPhysics - Atomic PhysicsLamb shiftNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Charge radiusQuantum mechanicsMoment (physics)Atomic physicsBohr radiusPhysical Review A
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Accretion-induced quasinormal mode excitation of a Schwarzschild black hole

2007

By combining the numerical solution of the nonlinear hydrodynamics equations with the solution of the linear inhomogeneous Zerilli-Moncrief and Regge-Wheeler equations we investigate the properties of the gravitational radiation emitted during the axisymmetric accretion of matter onto a Schwarzschild black hole. The matter models considered include quadrupolar dust shells and thick accretion disks, permitting us to simulate situations which may be encountered at the end stages of stellar gravitational collapse or binary neutron star merger. We focus on the interference pattern appearing in the energy spectra of the emitted gravitational waves and on the amount of excitation of the quasi-nor…

PhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaWhite holePrimordial black holeAstrophysicsCharged black holeBlack holeGeneral Relativity and Quantum CosmologyRotating black holeExtremal black holeStellar black holeSchwarzschild radiusAstrophysics::Galaxy AstrophysicsPhysical Review D
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Charge radius of the neutrino

2000

Using the pinch technique we construct at one-loop order a neutrino charge radius, which is finite, depends neither on the gauge-fixing parameter nor on the gauge-fixing scheme employed, and is process independent. This definition stems solely from an effective proper photon-neutrino one-loop vertex, with no reference to box or self-energy contributions. The role of the $\mathrm{WW}$ box in this construction is critically examined. In particular it is shown that the exclusion of the effective $\mathrm{WW}$ box from the definition of the neutrino charge radius is not a matter of convention but is in fact dynamically realized when the target fermions are right-handedly polarized. In this way …

PhysicsNuclear and High Energy PhysicsCamps de galga (Física)Background field methodElectroweak interactionFermionsymbols.namesakeTheoretical physicsCharge radiusQuantum mechanicssymbolsFeynman diagramGauge theoryCamps Teoria quàntica deNeutrinoGauge fixing
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