Search results for "atomic mass"

showing 10 items of 103 documents

$Q$-value of the superallowed $\beta$ decay of 62Ga

2006

Masses of the radioactive isotopes 62Ga, 62Zn and 62Cu have been measured at the JYFLTRAP facility with a relative precision of better than 18 ppb. A Q_EC value of (9181.07 +- 0.54) keV for the superallowed decay of 62Ga is obtained from the measured cyclotron frequency ratios of 62Ga-62Zn, 62Ga-62Ni and 62Zn-62Ni ions. The resulting Ft-value supports the validity of the conserved vector current hypothesis (CVC). The mass excess values measured were (-51986.5 +-1.0) keV for 62Ga, (-61167.9 +- 0.9) keV for 62Zn and (-62787.2 +- 0.9) keV for 62Cu.

Nuclear and High Energy PhysicsMass excessQ valuePenning trapCyclotronFOS: Physical sciences27.50.+e; 23.40.-s; 24.80.+g; 21.10.Dr[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyIonlaw.inventionNuclear physicslawDouble beta decayFt value0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsRadionuclide010308 nuclear & particles physicsBeta decayQ-valueAtomic massAtomic mass
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SMILETRAP — Atomic mass measurements with ppb accuracy by using highly charged ions

1996

In the SMILETRAP facility externally produced highly charged ions are captured in a Penning trap and utilized for high precision measurements of atomic masses. Accuracy tests on a ppb level have been performed, using highly charged carbon, oxygen and neon ions. In all cases hydrogen ions served as a reference for the calibration and monitoring of the magnetic field in the trap. Deviations smaller than 3 ppb from the expected results were found in mass measurements of the16O and20Ne atomic masses. The proton atomic mass, determined from the reference measurements on hydrogen ions, is in good agreement with the accepted value [1]. A direct mass measurement on the86Kr-isotope, using trapped86K…

Nuclear and High Energy PhysicsProtonHydrogenAnalytical chemistrychemistry.chemical_elementCondensed Matter PhysicsPenning trapAtomic and Molecular Physics and OpticsAtomic massIonNeonchemistryCalibrationPhysics::Atomic PhysicsPhysical and Theoretical ChemistryAtomic physicsCarbonHyperfine Interactions
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Recent developments in Penning-trap mass spectrometry

2016

Abstract Penning-trap mass spectrometry provides atomic masses with the highest precision. At accelerator-based on-line facilities it is applied to investigate exotic radionuclides in the context of tests of fundamental symmetries, nuclear structure studies, and nuclear astrophysics research. Recent progress in slowing down radioactive ion-beams in buffer-gas cells in combination with advanced ion-manipulation techniques has paved the way to reach nuclides ever-more far from stability. In this endeavor many efforts are underway to increase the sensitivity, the efficiency, and the precision of Penning-trap mass spectrometry. In this article some recent experimental developments are addressed…

Nuclear and High Energy PhysicsRadionuclideChemistry010401 analytical chemistryContext (language use)Penning trapMass spectrometry01 natural sciencesAtomic mass0104 chemical sciencesNuclear physics0103 physical sciencesNuclear astrophysicsNuclideNuclear Experiment010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Towards Shorter-Lived Nuclides in ISOLTRAP Mass Measurements

2001

Recently, the applicability of Penning trap mass spectrometry has been extended to nuclides with a half-life of less than one second. The mass of 33Ar(T 1/2 = 174 ms) was measured using the ISOLTRAP spectrometer with an accuracy of 4.2 keV. This measurement provided a stringent test of the Isobaric Multiplet Mass Equation (IMME) at mass number A = 33 and isospin T = 3/2. The fast measurement cycle that shows the way to other measurements of very-short-lived nuclides is presented. Furthermore, the results of the IMME test are displayed.

Nuclear physicsMass numberChemistryNuclideIon trapAtomic physicsMass spectrometryPenning trapISOLTRAPAtomic massHybrid mass spectrometer
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Direct mass measurements above uranium bridge the gap to the island of stability

2010

The mass of an atom incorporates all its constituents and their interactions. The difference between the mass of an atom and the sum of its building blocks (the binding energy) is a manifestation of Einstein's famous relation E = mc(2). The binding energy determines the energy available for nuclear reactions and decays (and thus the creation of elements by stellar nucleosynthesis), and holds the key to the fundamental question of how heavy the elements can be. Superheavy elements have been observed in challenging production experiments, but our present knowledge of the binding energy of these nuclides is based only on the detection of their decay products. The reconstruction from extended d…

Nuclear physicsMass numberMultidisciplinaryMass excessAtomic mass constantIsotopeChemistryNuclideAtomic physicsNuclear ExperimentAtomic massBeta-decay stable isobarsSpontaneous fission
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A new upper limit of the electron anti neutrino rest mass from tritium β-decay

1993

Abstract A new upper limit of the electron anti neutrino rest mass has been deduced from the tritium β-decay spectrum. A source of molecular tritium has been investigated with a new solenoid retarding spectrometer. The results are m ν ϵ 2 = −38.8 ± 34.1 stat ± 15.1 syst (eV) 2 /c 4 from which we conclude m ν ϵ ≤ 7.2 eV/c 2 with 95% c.l. Our β-endpoint corresponds to a 3H-3He atomic mass difference of Δm( 3 H- 3 He) = 18590.8 ± 3 eV/c 2 (1σ) .

Nuclear physicsPhysicsNuclear and High Energy PhysicsSpectrometerInvariant massTritiumLimit (mathematics)ElectronNeutrinoAtomic physicsAtomic and Molecular Physics and OpticsAtomic massNuclear Physics B - Proceedings Supplements
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Independent Isotopic Product Yields in 25 MeV and 50 MeV Charged Particle Induced Fission of 238U and 232Th

2014

Abstract Independent isotopic yields for most elements from Zn to La in 25-MeV proton-induced fission of 238U and 232Th have been determined at the IGISOL facility in the University of Jyvaskyla. In addition, isotopic yields for Zn, Ga, Rb, Sr, Zr, Pd and Xe in 50-MeV proton-induced fission of 238U and for Zn, Ga, Rb, Sr, Cd and In in 25-MeV deuterium-induced fission of 238U have been measured. The utilised technique recently developed at the University of Jyvaskyla, is based on a combination of the ion guide technique and the ability of a Penning trap to unambiguously identify the isotopes by their atomic mass. Since the yields are determined by ion counting, no prior knowledge beyond the …

Nuclear physicsPhysicsNuclear and High Energy Physicsta114IsotopeFissionProduct (mathematics)Nuclear dataPenning trapCharged particleAtomic massIonNuclear Data Sheets
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Mass measurements on stable nuclides in the rare-earth region with the Penning-trap mass spectrometer RIGA-TRAP

2011

The masses of 15 stable nuclides in the rare-earth region have been measured with the Penning-trap mass spectrometer TRIGA-TRAP. This is the first series of absolute mass measurements linking these nuclides to the atomic-mass standard $^{12}\mathrm{C}$. Previously, nuclear reaction studies almost exclusively determined the literature values of these masses in the Atomic-Mass Evaluation. The TRIGA-TRAP results show deviations on the order of 3--4 standard deviations from the latest published values of the Atomic-Mass Evaluation 2003 for some cases. However, the binding-energy differences that are important for nuclear structure studies have been confirmed and improved. The new masses are dis…

Nuclear reactionNuclear and High Energy PhysicsBinding energyRESONANCE NEUTRON-CAPTURE[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryNUCLEAR-STRUCTURE01 natural sciencesBeta-decay stable isobarsNuclear physics0103 physical sciencesNuclidePhysics::Atomic PhysicsSU(4) SYMMETRY010306 general physicsNuclear ExperimentSEPARATION ENERGIESPhysicsIsotopeCARBON CLUSTERS010308 nuclear & particles physicsCarbon-12ISOSPIN SYMMETRYRAMSEY METHODGAMMAPenning trapISOTOPESATOMIC MASS
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High-precision mass measurements of 25Al and 30P at JYFLTRAP

2016

The masses of the astrophysically relevant nuclei 25Al and 30P have been measured with a Penning trap for the first time. The mass-excess values for 25Al ( $\Delta = -8915.962(63)$ keV) and 30P ( $\Delta = -20200.854(64)$ keV) obtained with the JYFLTRAP double Penning trap mass spectrometer are in good agreement with the Atomic Mass Evaluation 2012 values but $ \approx$ 5-10 times more precise. A high precision is required for calculating resonant proton-capture rates of astrophysically important reactions 25Al (p, $ \gamma$ )26Si and 30P(p, $ \gamma$ )31S . In this work, $ Q_{(p,\gamma)} = 5513.99(13)$ keV and $ Q_{(p,\gamma)} = 6130.64(24)$ keV were obtained for 25Al and 30P , respectivel…

Nuclear reactionNuclear and High Energy PhysicsmassaspektrometriaQ valueAstrophysics::High Energy Astrophysical PhenomenaastrofysiikkaHadronatomipainot01 natural sciencesNuclear physics0103 physical sciencesNuclear astrophysicsJYFLTRAPIsotopes of siliconalumiiniNuclear Experiment010306 general physicsfosforiPhysics010308 nuclear & particles physicsatomic massPenning trapAtomic masshigh-precision mass measurementAtomic physicsydinfysiikkaRadioactive decay
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The decay energy of the pure s-process nuclide ¹²³ Te

2016

Physics letters / B 758, 407 - 411 (2016). doi:10.1016/j.physletb.2016.04.059

Penning-trap mass spectrometryPhysicsNuclear and High Energy Physics010308 nuclear & particles physicsElectron captureAtomic massesIonic bondingAstrophysicsMass spectrometry53001 natural scienceslcsh:QC1-999Atomic massNuclear physicsMassDecay energyTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesddc:530NuclidePräzisionsexperimente - Abteilung BlaumAtomic physics010306 general physicss-processlcsh:Physics
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