Search results for "Charge radius"

showing 10 items of 92 documents

Nuclear charge radii of potassium isotopes beyond N=28

2014

We report on the measurement of optical isotope shifts for 38, 39, 42, 44, 46–51 K relative to 47 K from which changes in the nuclear mean square charge radii across the N = 28 shell closure are deduced. The investigation was carried out by bunched-beam collinear laser spectroscopy at the CERN-ISOLDE radioactive ion-beam facility. Mean square charge radii are now known from 37K to 51K, covering all ν f7/2-shell as well as all νp3/2-shell nuclei. These measurements, in conjunction with those of Ca, Cr, Mn and Fe, provide a first insight into the Z dependence of the evolution of nuclear size above the shell closure at N = 28

Mean squareNuclear and High Energy PhysicsPotassiumCollinear laser spectroscopyNuclear TheoryShell (structure)FOS: Physical scienceschemistry.chemical_elementEffective nuclear chargeNuclear Physics - ExperimentNuclear Experiment (nucl-ex)SpectroscopyNuclear ExperimentNuclear ExperimentPhysicsIsotopeCharge (physics)Physique atomique et nucléaireIsotope shiftchemistryIsotopes of potassiumPotassiumPhysics::Accelerator PhysicsAtomic physicsPräzisionsexperimente - Abteilung BlaumNuclear charge radius
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Nuclear moments of strongly deformed strontium isotopes

1990

Nuclear spins, moments and mean square charge radii of78–100Sr have been obtained by fast ion-beam collinear laserspectroscopy. The experiments performed at ISOLDE have been extended to include99Sr, measured by a non-optical detection scheme with a two-step optical pumping sequence. The results for the strongly deformed isotopes are discussed in the frame of the particle-plus-deformed core model.

Mean squareNuclear and High Energy PhysicsStrontiumSpinsIsotopeChemistrychemistry.chemical_elementCharge (physics)Condensed Matter PhysicsAtomic and Molecular Physics and OpticsIsotopes of strontiumOptical pumpingCharge radiusPhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentHyperfine Interactions
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Theory of the Lamb Shift and fine structure in muonic 4He ions and the muonic 3He– 4He Isotope Shift

2018

Abstract We provide an up to date summary of the theory contributions to the 2S → 2P Lamb shift and the fine structure of the 2P state in the muonic helium ion ( μ 4 He ) + . This summary serves as the basis for the extraction of the alpha particle charge radius from the muonic helium Lamb shift measurements at the Paul Scherrer Institute, Switzerland. Individual theory contributions needed for a charge radius extraction are compared and compiled into a consistent summary. The influence of the alpha particle charge distribution on the elastic two-photon exchange is studied to take into account possible model-dependencies of the energy levels on the electric form factor of the nucleus. We al…

Muonic atoms/ionsHelium; Isotope shift; Nuclear structures; Fine structure; Lamb shift; Muonic atoms; Muonic ionsGeneral Physics and Astronomy7. Clean energy01 natural sciencesHeliumIonLamb shiftCharge radius0103 physical sciencesPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsNuclear structureSDG 7 - Affordable and Clean Energy010306 general physicsExotic atomPhysics/dk/atira/pure/sustainabledevelopmentgoals/affordable_and_clean_energy010308 nuclear & particles physicsElectric form factorCharge densityAlpha particleLamb shiftIsotope shiftDeuteriumFine structureAtomic physics
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How to measure nuclear ground-state properties in simple systems such as 11Li or U91+?

2008

Abstract Atomic spectroscopy yields key information on properties of ground and isomeric states via a determination of the hyperfine structure and isotope shift. In order to deduce precise nuclear moments and charge radii, the electromagnetic fields produced by the electrons at the site of the nucleus must be known with high accuracy. This is presently possible only for simple systems with very few electrons. This contribution describes two scenarios for such experiments: the determination of the charge radius of the neutron-rich isotopes 8,9Li and of the halo nucleus 11Li at the on-line isotope separators at GSI and TRIUMF and the Highly charged Ion TRAP (HITRAP) facility which is under co…

Nuclear and High Energy PhysicsChemistryNuclear TheoryHighly charged ionHalo nucleusElectronAtomic spectroscopyIonNuclear physicsCharge radiusPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentGround stateInstrumentationHyperfine structureNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Determination of the isotope shift in theD 1 line between197Au and195Au

1983

The isotope shift between197Au (stable) and195Au (T 1/2=183 d) was determined by resonance fluorescence and polarization spectroscopy in the 6s2 S 1/2 -6p 2 P 1/2, λ =267.6nm line. The result is δν195, 197=-2.9(2) GHz corresponding to a change of the mean-square charge radius by δ〈r 2〉195, 197=0.063(9) fm2. The sample was confined to a resonance cell heated to temperatures of up to 1500°C.

Nuclear and High Energy PhysicsMaterials scienceIsotopeResonance fluorescenceCharge radiusAnalytical chemistryNuclear fusionPolarization (waves)SpectroscopyD-1Zeitschrift f�r Physik A Atoms and Nuclei
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The subtraction contribution to the muonic-hydrogen Lamb shift: a point for lattice QCD calculations of the polarizability effect

2020

The proton-polarizability contribution to the muonic-hydrogen Lamb shift is a major source of theoretical uncertainty in the extraction of the proton charge radius. An empirical evaluation of this effect, based on the proton structure functions, requires a systematically improvable calculation of the "subtraction function", possibly using lattice QCD. We consider a different subtraction point, with the aim of accessing the subtraction function directly in lattice calculations. A useful feature of this subtraction point is that the corresponding contribution of the structure functions to the Lamb shift is suppressed. The whole effect is dominated by the subtraction contribution, calculable o…

Nuclear and High Energy PhysicsNuclear TheoryAtomic Physics (physics.atom-ph)FOS: Physical sciences01 natural sciencesPhysics - Atomic PhysicsNuclear Theory (nucl-th)High Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Charge radiusPolarizabilityLattice (order)0103 physical sciencesPhysics::Atomic Physics010306 general physicsExotic atomPhysics010308 nuclear & particles physicsStructure functionHigh Energy Physics - Lattice (hep-lat)SubtractionLattice QCD3. Good healthLamb shiftHigh Energy Physics - PhenomenologyQuantum electrodynamics
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Charge radii and neutron correlations in helium halo Nuclei

2011

Within the complex-energy configuration interaction framework, we study correlations of valence neutrons to explain the behavior of charge radii in the neutron halo nuclei $^{6,8}$He. We find that the experimentally observed decrease of the charge radius between $^6$He and $^8$He is caused by a subtle interplay between three effects: dineutron correlations, a spin-orbit contribution to the charge radius, and a core swelling effect. We demonstrate that two-neutron angular correlations in the $2^+_1$ resonance of $^6$He differ markedly from the ground-state correlations in $^{6,8}$He.

Nuclear and High Energy PhysicsNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryFOS: Physical scienceschemistry.chemical_element01 natural sciencesNuclear Theory (nucl-th)Charge radius0103 physical sciencesNeutronNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentHeliumPhysicsValence (chemistry)ta114010308 nuclear & particles physicsCharge densityRadiusConfiguration interactionchemistryHaloAtomic physicsPhysical Review C
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Charge radii of neon isotopes across the sd neutron shell

2011

We report on the changes in mean square charge radii of unstable neon nuclei relative to the stable Ne-20, based on the measurement of optical isotope shifts. The studies were carried out using collinear laser spectroscopy on a fast beam of neutral neon atoms. High sensitivity on short-lived isotopes was achieved thanks to nonoptical detection based on optical pumping and state-selective collisional ionization, which was complemented by an accurate determination of the beam kinetic energy. The new results provide information on the structural changes in the sequence of neon isotopes all across the neutron sd shell, ranging from the proton drip line nucleus and halo candidate Ne-17 up to the…

Nuclear and High Energy PhysicsProtonNuclear Theoryquadrupole collectivitychemistry.chemical_elementXXargon isotopesNeonCharge radiusrich nucleiNeutronPhysics::Atomic PhysicsNuclear Experimentcluster statesMagic number (physics)Physicslaser-spectroscopy measurementssodium isotopesIsland of inversionintruder configurationsmean-field theorychemistryIsotopes of neonlight-nucleiAtomic physicsmass shiftNucleon
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Constraints to new physics models for the proton charge radius puzzle from the decayK+→μ++ν+e−+e+

2014

A possible explanation for the discrepancy between electronic and muonic hydrogen measurements of the proton charge radius are new, lepton-universality violating interactions. Several new couplings and particles have been suggested that account for this discrepancy. At present, these explanations are poorly constrained. Experiments such as the upcoming kaon decay experiment at JPARC may constrain or eliminate some explanations by sensitivity to the decay channel $K^+ \rightarrow \mu^+ +\nu + e^- + e^+$. We calculate the predicted contributions of the various explanations to this channel. The predicted signals, if present, should be large enough to be resolved in the experiment.

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle physicsProtonCharge radiusPhysics beyond the Standard ModelHigh Energy Physics::ExperimentExotic atomPhysical Review D
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Nuclear Radii and Moments of Unstable Isotopes

1989

The development of on-line mass separators, which provide long chains of isotopes extending far off stability, immediately raised the question of how to gain access to the basic nuclear ground-state properties of these exotic nuclei—their spins, moments, radii, and masses. In general, the amount of radioactive material produced at these facilities is too small to form beams or targets for any kind of scattering or nuclear-reaction experiment. On the other hand, the traditional spectroscopic methods, namely, atomic, nuclear, and mass spectroscopy, have turned out to be very suitable for this application since they are easily adapted to the special on-line conditions.

Nuclear physicsSpinsIsotopeCharge radiusChemistryScatteringRadioactive wasteCharge (physics)Atomic physicsNuclear ExperimentSpectroscopyHyperfine structure
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