Search results for "atomic mass"

showing 10 items of 103 documents

Superconducting Solenoid System with Adjustable Shielding Factor for Precision Measurements of the Properties of the Antiproton

2019

Physical review applied 12(4), 044012 (2019). doi:10.1103/PhysRevApplied.12.044012

MAGNETIC-MOMENTSpeichertechnik - Abteilung BlaumPenning trapNuclear engineeringGeneral Physics and Astronomy02 engineering and technologyPROTON53001 natural sciencesNoise (electronics)Physics AppliedTrap (computing)External magnetic field0103 physical sciencesPENNING TRAP TECHNIQUEFACILITYddc:530Physics::Atomic PhysicsSolenoidsDetectors and Experimental TechniquesNuclear Experiment010306 general physicsSuperconductivityPhysicsScience & TechnologyLarge Hadron ColliderPhysics021001 nanoscience & nanotechnologyMagnetic fieldElectromagnetic coilAntiprotonPhysical SciencesMagnetic momentsElectromagnetic shieldingPhysics::Accelerator PhysicsCharge-to-mass ratiosDewey Decimal Classification::500 | Naturwissenschaften::530 | PhysikATOMIC MASSPARTICLE0210 nano-technologyMASS MEASUREMENTSPhysical Review Applied
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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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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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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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Precision Measurements of Atomic Masses Using Highly Charged Ions and Atomic Clusters

1992

A high precision Penning trap will be connected to the beam of highly charged ions from the electron beam ion source CRYSIS at the Manne Siegbahn Institute for Physics (MSI) in Stockholm. The first series of experiments aim at accurate mass measurements by exploiting the increase of the cyclotron frequency with the charge state of the trapped ion. Using charged states of about 50 it should be possible to achieve relative mass accuracies for mass doublets better than 10-9. For this high accuracy a Penning trap with low imperfections is needed, as well as a sophisticated beam handling and retardation system for controlled injection of the ions into the trap. In order to minimize the effect of…

Mass numberPhysicslawCyclotronCluster (physics)Atomic physicsPenning trapIon sourceAtomic massBeam (structure)Ionlaw.invention
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Raman studies of isotope effects in Si and GaAs

1999

Abstract We have measured by Raman scattering changes of the optic phonon energy and line width in Si and GaAs with isotopic composition. The phonon energies of isotopically pure samples show the expected dependence on the average atomic mass in Si and the reduced mass in GaAs, respectively, as well as small anharmonic contributions. In isotopically disordered samples we find frequency shifts of 1.15(20) cm−1 for 28Si0.530Si0.5 and 0.31(20) cm−1 for the TO phonon of natGaAs, induced by mass disorder which also contributes to the line broadening. We give theoretical estimates of these effects.

Materials sciencePhononAnharmonicityReduced massCondensed Matter::Mesoscopic Systems and Quantum Hall EffectCondensed Matter PhysicsAtomic massElectronic Optical and Magnetic Materialssymbols.namesakeKinetic isotope effectsymbolsElectrical and Electronic EngineeringAtomic physicsRaman spectroscopyRaman scatteringLine (formation)Physica B: Condensed Matter
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Accuracy tests of atomic mass measurements in a penning trap using externally produced highly charged ions

1997

The SMILETRAP experimental set-up, a Penning trap mass spectrometer for highly charged ions, is described. Capture and observation of cyclotron frequencies of externally produced highly charged ions is demonstrated. Mass measurements utilizing different charge states and species to verify the consistency of the measurements are presented. A relative uncertainty <3 10−9 is attained in comparisons between highly charged 12C, 14N, 16O, 20Ne and singly charged H, H2 and H3 ions. The current limitations and future developments are discussed.

Materials sciencelawCyclotronIon trapAtomic physicsCondensed Matter PhysicsPenning trapMass spectrometryMathematical PhysicsAtomic and Molecular Physics and OpticsAtomic masslaw.inventionIonPhysica Scripta
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Precision mass measurements on neutron-rich rare-earth isotopes at JYFLTRAP - reduced neutron pairing and implications for the $r$-process calculatio…

2018

The rare-earth peak in the $r$-process abundance pattern depends sensitively on both the astrophysical conditions and subtle changes in nuclear structure in the region. This work takes an important step elucidating the nuclear structure and reducing the uncertainties in $r$-process calculations via precise atomic mass measurements at the JYFLTRAP double Penning trap. $^{158}$Nd, $^{160}$Pm, $^{162}$Sm, and $^{164-166}$Gd have been measured for the first time and the precisions for $^{156}$Nd, $^{158}$Pm, $^{162,163}$Eu, $^{163}$Gd, and $^{164}$Tb have been improved considerably. Nuclear structure has been probed via two-neutron separation energies $S_{2n}$ and neutron pairing energy metrics…

Nuclear TheoryastrofysiikkaRare earthnuclear astrophysicsGeneral Physics and AstronomyFOS: Physical sciences7. Clean energy01 natural sciencesbinding energy and massesNuclear Theory (nucl-th)0103 physical sciencesNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentSolar and Stellar Astrophysics (astro-ph.SR)PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)Isotopeta114010308 nuclear & particles physicsNuclear structureharvinaiset maametallitPenning trapAtomic mass3. Good healthAstrophysics - Solar and Stellar Astrophysics13. Climate actionPairingr-processAtomic physicsydinfysiikkaAstrophysics - High Energy Astrophysical Phenomena
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Mass measurement of cooled neutron-deficient bismuth projectile fragments with time-resolved Schottky mass spectrometry at the FRS-ESR facility

2005

Masses of 582 neutron-deficient nuclides ($30\leq{Z}\leq{85}$) were measured with time-resolved Schottky mass spectrometry at the FRS-ESR facility at GSI, 117 were used for calibration. The masses of 71 nuclides were obtained for the first time. A typical mass accuracy of 30 $\mu$u was achieved. These data have entered the latest atomic mass evaluation. The mass determination of about 140 additional nuclides was possible via known energies ($Q$-values) of $\alpha-$, $\beta-$, or proton decays. The obtained results are compared with the results of other measurements.

Nuclear and High Energy PhysicsA=79–207ProtonAtomic massesNuclear Theorychemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometry01 natural sciences7. Clean energyBismuthmassesNuclear physicsZ=30–850103 physical sciencesNeutronNuclide010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsTime-resolved Schottky mass spectrometrySchottky diodeAtomic massMasschemistrymeasured
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Towards higher accuracy with the ISOLTRAP mass spectrometer

1996

To now the masses of more than hundred unstable isotopes have been determined with the ISOLTRAP mass spectrometer installed at ISOLDE/CERN. Typically a resolving power of mΔm ≈ 1 × 106 was used and the mass determinations were assigned an accuracy of δmm ≈ 1 × 10−7. We show that with improvements to ISOLTRAP and refinements of the experimental technique an accuracy of δmm ≈ 3 × 10−8 can be obtained.

Nuclear and High Energy PhysicsLarge Hadron ColliderIsotope010308 nuclear & particles physicsChemistry[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trapMass spectrometry01 natural sciencesISOLTRAPAtomic massNuclear physics0103 physical sciencesAtomic physics010306 general physicsInstrumentation
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