Search results for "ISOLTRAP"

showing 10 items of 64 documents

Mass spectrometry and decay spectroscopy of isomers across the Z=82 shell closure

2013

Recent results from a measurement campaign studying the isomerism in neutron-deficient Tl isotopes are presented. The measurements make use of a nuclear spectroscopy setup coupled to the high-resolution Penning-trap mass spectrometer ISOLTRAP at CERN's radioactive ion-beam facility ISOLDE. The mass values of 190,194Tl are improved and a mass-spin-state assignment is carried out. An additional mass measurement of the grandparent nuclide 198At allows the deduction of the spin-state ordering in 190Tl. As a result, the excitation energies of the isomers in both Tl isotopes are determined for the first time to Eex(194Tl)=260(15) keV and E ex(190Tl)=89(12) keV. Furthermore, this allows anchoring …

PhysicsNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsClosure (topology)Shell (structure)ISOLTRAPMass spectrometry01 natural sciencesIon trappingISOLTRAPPenning ion trapTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITY0103 physical sciencesisomersddc:530Atomic physicsNuclear Experiment010306 general physicsSpectroscopyZ=82mass spectrometry
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Mass measurements on neutron-deficient Sr and neutron-rich Sn isotopes with the ISOLTRAP mass spectrometer

2005

Abstract The atomic masses of 76,77,80,81,86,88 Sr and 124,129,130,131,132 Sn were measured by means of the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. 76 Sr is now the heaviest N = Z nucleus for which the mass is measured to a precision better than 35 keV. For the tin isotopes in the close vicinity of the doubly magic nucleus 132 Sn, mass uncertainties below 20 keV were achieved. An atomic mass evaluation was carried out taking other experimental mass values into account by performing a least-squares adjustment. Some discrepancies between older experimental values and the ones reported here emerged and were resolved. The results of the new adjustment and their impact will be pr…

PhysicsNuclear and High Energy Physicsatomic masses010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryISOLTRAP01 natural sciencesISOLTRAPAtomic massNuclear physicsMasstin0103 physical sciencesIsotopes of tinNeutronstrontiumAtomic physics010306 general physicsNuclear ExperimentQuadrupole mass analyzerhigh-precision mass spectrometryHybrid mass spectrometer07.75.+h 21.10.Dr 32.10.Bi
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High-accuracy mass spectrometry with stored ions

2006

Abstract Like few other parameters, the mass of an atom, and its inherent connection with the atomic and nuclear binding energy is a fundamental property, a unique fingerprint of the atomic nucleus. Each nuclide comes with its own mass value different from all others. For short-lived exotic atomic nuclei the importance of its mass ranges from the verification of nuclear models to a test of the Standard Model, in particular with regard to the weak interaction and the unitarity of the Cabibbo–Kobayashi–Maskawa quark mixing matrix. In addition, accurate mass values are important for a variety of applications that extend beyond nuclear physics. Mass measurements on stable atoms now reach a rela…

PhysicsNuclear physicsAtomic nucleusAtomGeneral Physics and AstronomyNuclear binding energyPhysics::Atomic PhysicsNuclideMass spectrometryPenning trapISOLTRAPAtomic massPhysics Reports
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Approaching theN=82shell closure with mass measurements of Ag and Cd isotopes

2010

Mass measurements of neutron-rich Cd and Ag isotopes were performed with the Penning trap mass spectrometer ISOLTRAP. The masses of ${}^{112,114\ensuremath{-}124}$Ag and ${}^{114,120,122\ensuremath{-}124,126,128}$Cd, determined with relative uncertainties between $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}8}$ and $2\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}7}$, resulted in significant corrections and improvements of the mass surface. In particular, the mass of $^{124}\mathrm{Ag}$ was previously unknown. In addition, other masses that had to be inferred from $Q$ values of nuclear decays and reactions have now been measured directly. The analysis includes various mass…

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physicsQ value21.10.Dr 21.30.Fe 27.60.+jHadron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesISOLTRAPIsotopes of cadmium0103 physical sciencesIsotopes of tinNuclear Physics - ExperimentAtomic physics010306 general physicsNucleonEnergy (signal processing)Physical Review C
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rp-process nucleosynthesis at extreme temperature and density conditions

1998

We present nuclear reaction network calculations to investigate the influence of nuclear structure on the rp-process between Ge and Sn in various scenarios. Due to the lack of experimental data for neutron-deficient nuclei in this region, we discuss currently available model predictions for nuclear masses and deformations as well as methods of calculating reaction rates (Hauser-Feshbach) and beta-decay rates (QRPA and shell model). In addition, we apply a valence nucleon (NpNn) correlation scheme for the prediction of masses and deformations. We also describe the calculations of 2p-capture reactions, which had not been considered before in this mass region. We find that in X-ray bursts 2p-c…

PhysicsNuclear reactionNuclear physicsNucleosynthesisNuclear TheoryNuclear structureGeneral Physics and Astronomyp-Nucleirp-processNuclear ExperimentNucleonISOLTRAPp-process
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Precision Mass Measurements of Cr58–63 : Nuclear Collectivity Towards the N=40 Island of Inversion

2018

The neutron-rich isotopes $^{58-63}$Cr were produced for the first time at the ISOLDE facility and their masses were measured with the ISOLTRAP spectrometer. The new values are up to 300 times more precise than those in the literature and indicate significantly different nuclear structure from the new mass-surface trend. A gradual onset of deformation is found in this proton and neutron mid-shell region, which is a gateway to the second island of inversion around \emph{N}=40. In addition to comparisons with density-functional theory and large-scale shell-model calculations, we present predictions from the valence-space formulation of the \emph{ab initio} in-medium similarity renormalization…

PhysicsProtonIsotope010308 nuclear & particles physicsIsland of inversionNuclear TheoryAb initioNuclear structureGeneral Physics and AstronomyRenormalization group01 natural sciences7. Clean energyISOLTRAPNuclear physics0103 physical sciencesPhysics::Atomic and Molecular ClustersNeutronNuclear Experiment010306 general physicsPhysical Review Letters
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First Glimpse of the N=82 Shell Closure below Z=50 from Masses of Neutron-Rich Cadmium Isotopes and Isomers

2020

We probe the $N=82$ nuclear shell closure by mass measurements of neutron-rich cadmium isotopes with the ISOLTRAP spectrometer at ISOLDE-CERN. The new mass of $^{132}\mathrm{Cd}$ offers the first value of the $N=82$, two-neutron shell gap below $Z=50$ and confirms the phenomenon of mutually enhanced magicity at $^{132}\mathrm{Sn}$. Using the recently implemented phase-imaging ion-cyclotron-resonance method, the ordering of the low-lying isomers in $^{129}\mathrm{Cd}$ and their energies are determined. The new experimental findings are used to test large-scale shell-model, mean-field, and beyond-mean-field calculations, as well as the ab initio valence-space in-medium similarity renormalizat…

PhysicsSpectrometerAb initioShell (structure)Closure (topology)General Physics and AstronomyRenormalization group7. Clean energy01 natural sciencesISOLTRAPIsotopes of cadmium0103 physical sciencesPhysics::Atomic and Molecular ClustersNeutronAtomic physicsNuclear Experiment010306 general physicsPhysical Review Letters
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Mass measurements of $^{56-57}$Cr and the question of shell reincarnation at N = 32

2005

Binding energies determined with high accuracy provide smooth derivatives of the mass surface for analysis of shell and pairing effects. Measurements with the Penning trap mass spectrometer ISOLTRAP at CERN-ISOLDE were made for $^{56-57}$Cr for which an accuracy of 4 $\times 10^{-8}$ was achieved. Analysis of the mass surface for the supposed new N = 32 shell closure rather indicates a sub-shell closure, but of a different nature than known cases such as $^{94}$Sr.

PhysicsSurface (mathematics)Nuclear and High Energy Physics010308 nuclear & particles physicsBinding energyShell (structure)Closure (topology)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trapMass spectrometry01 natural sciencesISOLTRAPPairing0103 physical sciencesAtomic physics010306 general physicsNuclear Experiment
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ISOLTRAP Mass Measurements for Weak-Interaction Studies

2005

International audience; The conserved-vector-current (CVC) hypothesis of the weak interaction and the unitarity of the Cabibbo-Kobayashi-Maskawa (CKM) matrix are two fundamental postulates of the Standard Model. While existing data on CVC supports vector current conservation, the unitarity test of the CKM matrix currently fails by more than two standard deviations. High-precision mass measurements performed with the ISOLTRAP experiment at ISOLDE/CERN provide crucial input for these fundamental studies by greatly improving our knowledge of the decay energy of super-allowed beta decays. Recent results of mass measurements on the beta emitters 18Ne, 22Mg, 34Ar, and 74Rb as pertaining to weak-i…

Physicselementary particle weak interactionsParticle physicsLarge Hadron ColliderUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::Phenomenology12.15.Hh 23.40.Bw 11.40.HaWeak interaction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesISOLTRAPStandard ModelNuclear physicsMatrix (mathematics)Decay energy0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsbeta-decay
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Critical-Point Boundary for the Nuclear Quantum Phase Transition NearA=100from Mass Measurements ofKr96,97

2010

Mass measurements of (96,97)Kr using the ISOLTRAP Penning-trap spectrometer at CERN-ISOLDE are reported, extending the mass surface beyond N=60 for Z=36. These new results show behavior in sharp contrast to the heavier neighbors where a sudden and intense deformation is present. We interpret this as the establishment of a nuclear quantum phase transition critical-point boundary. The new masses confirm findings from nuclear mean-square charge-radius measurements up to N=60 but are at variance with conclusions from recent gamma-ray spectroscopy.

Quantum phase transitionPhysicsIsotopeSpectrometer010308 nuclear & particles physicsGeneral Physics and AstronomyIsotopes of krypton01 natural sciencesISOLTRAPCritical point (thermodynamics)0103 physical sciencesGamma spectroscopyAtomic physicsNuclear Experiment010306 general physicsSpectroscopyPhysical Review Letters
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