Search results for "Mass number"

showing 10 items of 51 documents

Systematic approach toβand2νββdecays of massA=100–136nuclei

2015

In this work we perform a systematic study of pairs of single-$\ensuremath{\beta}$-decaying nuclei in the mass region $A=100--136$ to extract information on the effective value of the axial-vector coupling constant ${g}_{\mathrm{A}}$. As the many-body framework we use the quasiparticle random-phase approximation (QRPA) and its proton-neutron variant (pnQRPA) in single-particle valence bases with Woods-Saxon-calculated single-particle energies. It is found that, to a reasonable approximation, ${g}_{\mathrm{A}}$ is a linear function of the mass number $A$, with a slightly different parametrization below and above the mass $A=121$. Using the values of ${g}_{\mathrm{A}}$ extracted from the line…

Coupling constantPhysicsMass numberSemileptonic decayNuclear and High Energy PhysicsValence (chemistry)Excited stateQuasiparticleAtomic physicsGround statePhysical Review C
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Beam-normal single-spin asymmetry in elastic scattering of electrons from a spin-0 nucleus

2021

We study the beam-normal single-spin asymmetry (BNSSA) in high-energy elastic electron scattering from several spin-0 nuclei. Existing theoretical approaches work in the plane-wave formalism and predict the BNSSA to scale as $\ensuremath{\sim}A/Z$ with the atomic number $Z$ and nuclear mass number $A$. While this prediction holds for light and intermediate nuclei, a striking disagreement in both the sign and the magnitude of BNSSA was observed by the PREX collaboration for $^{208}\mathrm{Pb}$, coined the ``PREX puzzle.'' To shed light on this disagreement, we go beyond the plane-wave approach which neglects Coulomb distortions known to be significant for heavy nuclei. We explicitly investig…

Elastic scatteringMass numberPhysicsNuclear Theory010308 nuclear & particles physicsScatteringmedia_common.quotation_subjectFOS: Physical sciencesElectron01 natural sciencesAsymmetryNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanics0103 physical sciencesCoulombAtomic numberNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentSpin-½media_commonPhysical Review C
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High-accuracy mass measurements on neutron deficient neon isotopes

2005

International audience; The atomic masses of the short-lived nuclides 17Ne and 19Ne have been measured with the triple-trap mass spectrometer ISOLTRAP at ISOLDE/CERN. The obtained mass excess for both nuclides deviates significantly from the literature value, in the case of 17Ne about 40 keV. The mass value of 17Ne can be applied for a test of the isobaric multiplet mass equation with respect to an isospin T = 3/2 quartet. In addition, both masses can contribute to the data analysis of collinear laser-spectroscopy experiments where mean-square nuclear-charge radii are determined.

Mass excessNuclear Theorychemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyISOLTRAPNuclear physicsNeonnuclei with mass number 6 to 190103 physical sciencesNuclideneon010306 general physicsNuclear ExperimentPhysicsmass spectrometers010308 nuclear & particles physicsneutronsAtomic massMass formulaMass21.10.Dr 27.20.+n 29.30.-hIsotopes of neonchemistrynuclear massAtomic physics
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Breakdown of the Isobaric Multiplet Mass Equation atA=33,T=3/2

2001

Mass measurements on ${}^{33,34,42,43}\mathrm{Ar}$ were performed using the Penning trap mass spectrometer ISOLTRAP and a newly constructed linear Paul trap. This arrangement allowed us, for the first time, to extend Penning trap mass measurements to nuclides with half-lives below one second ( ${}^{33}\mathrm{Ar}$: ${T}_{1/2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}174\mathrm{ms}$). A mass accuracy of about ${10}^{\ensuremath{-}7}$ $(\ensuremath{\delta}m\ensuremath{\approx}4\mathrm{keV})$ was achieved for all investigated nuclides. The isobaric multiplet mass equation was checked for the $A\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}33$, $T\phantom{\rule{0ex}{0ex}}=\phantom…

Mass formulaPhysicsMass numberGeneral Physics and AstronomyIsobaric processIon trapAtomic physicsQuadratic form (statistics)Penning trapISOLTRAPMultipletPhysical Review Letters
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Mass Measurements with the CSS2 and CIME cyclotrons at GANIL

2005

Commune avec ACEN; This paper presents two original direct mass-measurement techniques developed at GANIL using the CSS2 and CIME cyclotrons as high-resolution mass spectrometers. The mass measurement with the CSS2 cyclotron is based on a time-of-flight method along the spiral trajectory of the ions inside the cyclotron. The atomic mass excesses of 68Se and 80Y recently measured with this technique are -53.958(246) MeV and -60.971(180) MeV, respectively. The new mass-measurement technique with the CIME cyclotron is based on the sweep of the acceleration radio-frequency of the cyclotron. Tests with stable beams have been performed in order to study the accuracy of this new mass-measurement m…

Mass numberChemistryCyclotron020206 networking & telecommunicationsParticle accelerator02 engineering and technologyrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryAtomic masslaw.inventionIonNuclear physicsAccelerationlaw29.20.Hm 29.30.-h 21.10.Dr 27.50.+e0202 electrical engineering electronic engineering information engineering020201 artificial intelligence & image processing
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Multiplicity dependence of light (anti-)nuclei production in p–Pb collisions at sNN=5.02 TeV

2020

The measurement of the deuteron and anti- deuteron production in the rapidity range −1 < y < 0 as a function of transverse momentum and event multiplicity in p–Pb collisions at √sNN= 5.02 TeV is presented. (Anti-)deuterons are identified via their specific energy loss dE/dxand via their time-of-flight. Their production in p–Pb collisions is compared to pp and Pb–Pb collisions and is discussed within the context of thermal and coalescence models. The ratio of integrated yields of deuterons to protons (d/p) shows a significant increase as a function of the charged-particle multiplicity of the event starting from values similar to those observed in pp collisions at low multiplicities and appro…

Mass numberCoalescence (physics)PhysicsNuclear and High Energy PhysicsLarge Hadron Collider010308 nuclear & particles physicsNuclear TheoryMultiplicity (mathematics)01 natural sciencesSpectral lineNuclear physicsTime of flightDeuterium0103 physical sciencesRapidityNuclear Experiment010306 general physicsPhysics Letters B
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Transport of recoil atoms in a stream of liquid-air-cooled pure helium

1974

Abstract Pure commercial helium cooled down to the temperature of liquid air (80 K) has been used for rapid transportation of recoil atoms over distances as long as 10 m. Transport efficiencies of several tens of per cent have been obtained for recoil atoms resulting from alpha decay or from decay by fission. The angle of divergence of the beam of recoil atoms at the exit of the transport capillary is measured to be (11±2)° for particles of mass number A = 211. Experimental results are discussed in terms of thermal diffusion. The elimination of carrier vapors will probably simplify the use of the helium-jet technique in on-line mass separators.

Mass numberFission productsMaterials scienceFissionchemistry.chemical_elementGeneral MedicineThermal diffusivityRecoilchemistryLiquid airPhysics::Atomic and Molecular ClustersPhysics::Atomic PhysicsAlpha decayAtomic physicsHeliumNuclear Instruments and Methods
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Simple Nuclear Structure inCd111–129from Atomic Isomer Shifts

2016

Isomer shifts have been determined in ^{111-129}Cd by high-resolution laser spectroscopy at CERN-ISOLDE. The corresponding mean square charge-radii changes, from the 1/2^{+} and the 3/2^{+} ground states to the 11/2^{-} isomers, have been found to follow a distinct parabolic dependence as a function of the atomic mass number. Since the isomers have been previously associated with simplicity due to the linear mass dependence of their quadrupole moments, the regularity of the isomer shifts suggests a higher order of symmetry affecting the ground states in addition. A comprehensive description assuming nuclear deformation is found to accurately reproduce the radii differences in conjunction wi…

Mass numberPhysics010308 nuclear & particles physicsNuclear structureGeneral Physics and AstronomyOrder (ring theory)01 natural sciencesSymmetry (physics)0103 physical sciencesQuadrupolePhysics::Atomic and Molecular ClustersDensity functional theoryAtomic physics010306 general physicsSpectroscopyLine (formation)Physical Review Letters
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Resonance Ionization Mass Spectroscopy for Trace Analysis

1990

My first lecture at this Summer School on Applied Laser Spectroscopy dealt with the determination of nuclear ground-state properties, i.e. atomic mass M, the nuclear spin I, the magnetic dipole moment μ I, the spectroscopic quadrupole moment Q, and the changes in the mean-square charge radius δ(r2) A,A´ between isotopes with mass number A and A´. These quantities can be determined for stable, long-, or short-lived isotopes by mass spectrometry and optical spectroscopy. In the latter case, the hyperfine structure (HFS) and the volume effect of the isotope shift (IS) are determined in atomic levels or optical transitions. The state of the art mainly concerning short-lived nuclei is described …

Mass numberPhysicsCharge radiusInstrumental chemistryPhysics::Atomic PhysicsAtomic physicsThermal ionization mass spectrometryNuclear ExperimentSpectroscopyMass spectrometryHyperfine structureAtomic mass
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Description of light nuclei in pionless effective field theory using the stochastic variational method

2016

We construct a coordinate-space potential based on pionless effective field theory with a Gaussian regulator. Charge-symmetry breaking is included through the Coulomb potential and through two- and three-body contact interactions. Starting with the effective field theory potential, we apply the stochastic variational method to determine the ground states of nuclei with mass number $A\leq 4$. At next-to-next-to-leading order, two out of three independent three-body parameters can be fitted to the three-body binding energies. To fix the remaining one, we look for a simultaneous description of the binding energy of $^4$He and the charge radii of $^3$He and $^4$He. We show that at the order con…

Mass numberPhysicsNuclear Theory010308 nuclear & particles physicsGaussianBinding energyOrder (ring theory)FOS: Physical sciencesCharge (physics)01 natural sciencesNuclear Theory (nucl-th)symbols.namesakeVariational methodQuantum electrodynamics0103 physical sciencesEffective field theorysymbolsElectric potential010306 general physicsMathematical physics
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