Search results for "atomic mass"

showing 10 items of 103 documents

High-accuracy mass determination of unstable cesium and barium isotopes

1999

Direct mass measurements of short-lived Cs and Ba isotopes have been performed with the tandem Penning trap mass spectrometer ISOLTRAP installed at the on-line isotope separator ISOLDE at CERN. Typically, a mass resolving power of 600 000 and an accuracy of $\delta \mbox{m} \approx 13$ keV have been obtained. The masses of $^{123,124,126}$Ba and $^{122m}$Cs were measured for the first time. A least-squares adjustment has been performed and the experimental masses are compared with theoretical ones, particularly in the frame of a macroscopic-microscopic model.

PhysicsNuclear and High Energy PhysicsIsotope[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]010308 nuclear & particles physicschemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryPenning trap7. Clean energy01 natural sciencesISOLTRAPAtomic massNuclear physicsMasschemistryCaesium0103 physical sciencesNuclear Physics - ExperimentAtomic physicsNuclear Experiment010306 general physicsHybrid mass spectrometer
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Measurement of the Higgs boson mass from theH→γγandH→ZZ*→4ℓchannels inppcollisions at center-of-mass energies of 7 and 8 TeV with the ATLAS detector

2014

An improved measurement of the mass of the Higgs boson is derived from a combined fit to the reconstructed invariant mass spectra of the decay channels H -> gamma gamma and H -> ZZ* -> 4l. The analysis uses the pp collision data sample recorded by the ATLAS experiment at the CERN Large Hadron Collider at center-of-mass energies of 7 TeV and 8 TeV, corresponding to an integrated luminosity of 25 fb(-1). The measured value of the Higgs boson mass is m(H) = 125.36 +/- 0.37(stat) +/- 0.18 (syst) GeV. This result is based on improved energy-scale calibrations for photons, electrons, and muons as well as other analysis improvements, and supersedes the previous result from ATLAS. Upper limits on t…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderMuon010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyATLAS experiment7. Clean energy01 natural sciencesAtomic massNuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHiggs bosonHigh Energy Physics::ExperimentInvariant massCenter of mass010306 general physicsPhysical Review D
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Masses of neutron-rich Ni and Cu isotopes and the shell closure at Z = 28 , N = 40

2007

The Penning trap mass spectrometer JYFLTRAP, coupled to the Ion Guide Isotope Separator On-Line (IGISOL) facility at Jyvaskyla, was employed to measure the atomic masses of neutron-rich 70-73Ni and 73, 75Cu isotopes with a typical accuracy less than 5keV. The mass of 73Ni was measured for the first time. Comparisons with the previous data are discussed. Two-neutron separation energies show a weak subshell closure at 68 28Ni40 . A well established proton shell gap is observed at Z = 28 .

PhysicsNuclear and High Energy PhysicsProtonIsotopePenning trapMass spectrometryAtomic massIonNuclear physicsNuclear fusionNeutronPhysics::Atomic PhysicsAtomic physicsNuclear ExperimentThe European Physical Journal A
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Direct mass measurements of the heaviest elements with Penning traps

2013

Abstract Penning-trap mass spectrometry (PTMS) is a mature technique to provide atomic masses with highest precision. Applied to radionuclides it enables us to investigate their nuclear structure via binding energies and derived quantities such as nucleon separation energies. Recent progress in slowing down radioactive ion beams in buffer gas cells in combination with advanced ion-manipulation techniques has opened the door to access even the elements above fermium by PTMS. Such elements are produced in complete fusion–evaporation reactions of heavy ions with lead, bismuth, and actinide targets at very low rates. Pioneering high-precision mass measurements of nobelium and lawrencium isotope…

PhysicsNuclear and High Energy PhysicsRadionuclideChemistryFermiumNuclear TheoryNuclear structurechemistry.chemical_elementActinideSuperheavy ElementsCondensed Matter PhysicsPenning trapMass spectrometryAtomic massNuclear physicsNobeliumNuclidePhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentNucleonInstrumentationSpectroscopySpontaneous fissionLawrenciumInternational Journal of Mass Spectrometry
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ISOLTRAP mass measurements of exotic nuclides at

2005

The ISOLTRAP experiment at the ISOLDE facility at CERN is a Penning trap mass spectrometer for on-line mass measurements on short-lived radionuclides. It allows the determination of atomic masses of exotic nuclides with a relative uncertainty of only 10−8. The results provide important information for, e.g., weak interaction studies and nuclear models. Recent ISOLTRAP investigations and applications of high-precision mass measurements are discussed.

PhysicsNuclear and High Energy PhysicsRadionuclideLarge Hadron Collider010308 nuclear & particles physicsWeak interactionPenning trapMass spectrometry01 natural sciencesISOLTRAPAtomic massNuclear physics0103 physical sciencesNuclideNuclear Experiment010306 general physicsNuclear Physics A
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α-decay properties ofPb181

1996

The isotope {sup 181}Pb was produced in {sup 92}Mo bombardments of {sup 90}Zr and, together with other reaction products, was passed through a recoil mass separator and implanted in a double-sided silicon strip detector for {alpha}-particle assay. The half-life and energy of the main {sup 181}Pb {alpha} transition were determined to be 45 (20) ms and 7065 (20) keV, respectively. This {sup 181}Pb {ital E}{sub {alpha}} agrees with one previously measured value [7044 (15) keV], but not with the one [7211 (10) keV] used as input to the 1993 Atomic Mass Evaluation. The 6180-keV {alpha} transition assigned to {sup 181}Tl by Bolshakov {ital et} {ital al}. was observed, but the 6566-keV {alpha} par…

PhysicsNuclear and High Energy PhysicsRecoilSiliconchemistryIsotopeAnalytical chemistrychemistry.chemical_elementAlpha particleAlpha decayAtomic massPhysical Review C
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Direct mass measurement of N $\sim$ Z nuclei with A = 64–80 using the CSS2 cyclotron

2005

International audience; The masses of ten neutron-deficient nuclides near the N = Z line with A = 64–80 have been measured with the direct time-of-flight technique using the CSS2 cyclotron as a high-resolution spectrometer. All measured masses agree with the 2003 atomic mass evaluation and are compared to the predictions of the finite range droplet model. The atomic mass excesses obtained for $^{68}$Se and $^{80}$Y are -53.958(246) MeV and -60.971(180) MeV, respectively. The new results for $^{68}$Se and $^(80}$Y are compared to other recent experimental values.

PhysicsNuclear and High Energy PhysicsSpectrometer010308 nuclear & particles physicsCyclotron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Finite range7. Clean energy01 natural sciencesMass measurementAtomic masslaw.inventionNuclear physicslaw0103 physical sciencesNuclide010306 general physicsNuclear ExperimentLine (formation)
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Extension of Penning-trap mass measurements to very short-lived nuclides

2000

Abstract Mass measurements on 33,34,42,43 Ar have been performed at the ISOLTRAP spectrometer. An accuracy of δm ≈4 keV has been achieved for all measured isotopes. With 33 Ar it is the first time that a nuclide with a half-life shorter than one second has been investigated using a Penning trap. This became possible due to the recently installed linear radio-frequency ion-trap system and an improved, faster measurement cycle.

PhysicsNuclear and High Energy PhysicsSpectrometerIsotope010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trap7. Clean energy01 natural sciencesISOLTRAPAtomic massNuclear physics13. Climate action0103 physical sciencesNuclear Physics - ExperimentIon trapNuclideAtomic physics010306 general physicsHybrid mass spectrometerNuclear Physics A
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Direct mass measurements ofSe68andY80

2008

The masses of neutron-deficient nuclides near the $N=Z$ line with $A=64\text{\ensuremath{-}}80$ have been determined using a direct time-of-flight technique which employed a cyclotron as a high-resolution spectrometer. The measured atomic masses for $^{68}\mathrm{Se}$ and $^{80}\mathrm{Y}$ were 67.9421(3) u and 79.9344(2) u, respectively. The new values agree with the 2003 Atomic Mass Evaluation. The result for $^{68}\mathrm{Se}$ confirms that this nucleus is a waiting point of the rp-process, and that for $^{80}\mathrm{Y}$ resolves the conflict between earlier measurements. Using the present results and the 2003 Atomic Mass Evaluation compilation, the empirical interaction between the last…

PhysicsNuclear and High Energy PhysicsSpectrometerProton010308 nuclear & particles physicsCyclotron01 natural sciencesAtomic masslaw.inventionNuclear magnetic resonancelaw0103 physical sciencesNeutronNuclideAtomic physicsNuclear Experiment010306 general physicsLine (formation)Physical Review C
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Direct mass measurements of neutron-deficient xenon isotopes with the ISOLTRAP mass spectrometer

2000

Abstract The masses of Xe isotopes with 124⩾ A ⩾114 have been measured using the ISOLTRAP spectrometer at the on-line mass separator ISOLDE/CERN. A mass resolving power of 500 000 was chosen resulting in an accuracy of δm ≈12 keV for all isotopes investigated. Conflicts with existing mass data of several standard deviations were found.

PhysicsNuclear and High Energy PhysicsSpectrometer[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Physics::Instrumentation and Detectors010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometry01 natural sciencesISOLTRAPAtomic massIsotopes of oxygenNuclear physics0103 physical sciencesIsotopes of xenonAtomic physicsParticle PhysicsNuclear Experiment010306 general physicsQuadrupole mass analyzerHybrid mass spectrometer
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