0000000000705745

AUTHOR

A. Welker

showing 23 related works from this author

High-Statistics Sub-Barrier Coulomb Excitation of $^{106,108,110}$Sn

2020

International audience; A Coulomb excitation campaign on $^{106,108,110}$Sn at 4.4–4.5 MeV/u was launched at the HIE-ISOLDE facility at CERN. Larger excitation cross sections and γ-ray statistics were achieved compared to previous experiments at ∼2.8 MeV/u. More precise $(B(E2;0_{1}^{ + } \to 2_{1}^{ + }))$ values, lifetimes of states via the Doppler shift attenuation method, and new $(B(E2;0_{1}^{ + } \to 2_{x}^{ + })), (B(E2;2_{1}^{ + } \to 4_{1}^{ + }))$ and $(Q(2_{1}^{ + }))$ values from the new Miniball data will be obtained and applied to test modern nuclear structure theories.

Physics010308 nuclear & particles physicsCoulomb excitation0103 physical sciencesshell modelNuclear Physics - ExperimentCoulomb excitationAtomic physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010306 general physics01 natural sciencesnuclear collectivity
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Accumulation of positrons from a LINAC based source

2020

International audience; The GBAR experiment aims to measure the gravitational acceleration of antihydrogen H̅. It will use H̅+ ions formed by the interaction of antiprotons with a dense positronium cloud, which will require about 1010 positrons to produce one H̅+. We present the first results on the positron accumulation, reaching 3.8±0.4×108 e+ collected in 560 s.

010302 applied physicsPhysicsMeasure (physics)General Physics and Astronomy02 engineering and technology021001 nanoscience & nanotechnologyGravitational acceleration01 natural sciencesLinear particle acceleratorPositroniumNuclear physicsPositronPositron plasma; Positron accumulation; Antimatter; Penning-Malmberg trap; Greaves-Surko trap; GBAR[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]AntiprotonAntimatter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Physics::Accelerator PhysicsPhysics::Atomic Physics0210 nano-technologyAntihydrogenComputingMilieux_MISCELLANEOUSActa Physica Polonica A
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Laser Spectroscopy of Neutron-Rich Hg207,208 Isotopes: Illuminating the Kink and Odd-Even Staggering in Charge Radii across the N=126 Shell Closure

2021

The mean-square charge radii of $^{207,208}$Hg ($Z=80, N=127,128$) have been studied for the first time and those of $^{202,203,206}$Hg ($N=122,123,126$) remeasured by the application of in-source resonance-ionization laser spectroscopy at ISOLDE (CERN). The characteristic \textit{kink} in the charge radii at the $N=126$ neutron shell closure has been revealed, providing the first information on its behavior below the $Z=82$ proton shell closure. A theoretical analysis has been performed within relativistic Hartree-Bogoliubov and non-relativistic Hartree-Fock-Bogoliubov approaches, considering both the new mercury results and existing lead data. Contrary to previous interpretations, it is d…

PhysicsProtonNuclear TheoryShell (structure)General Physics and AstronomyCharge (physics)Coupling (probability)01 natural sciencesAtomic orbitalPairing0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsSpectroscopyPhysical Review Letters
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A pulsed high-voltage decelerator system to deliver low-energy antiprotons

2021

International audience; The GBAR (Gravitational Behavior of Antihydrogen at Rest) experiment at CERN requires efficient deceleration of 100 keV antiprotons provided by the new ELENA synchrotron ring to synthesize antihydrogen. This is accomplished using electrostatic deceleration optics and a drift tube that is designed to switch from -99 kV to ground when the antiproton bunch is inside – essentially a charged particle “elevator” – producing a 1 keV pulse. We describe the simulation, design, construction and successful testing of the decelerator device at -92 kV on-line with antiprotons from ELENA.

Nuclear and High Energy PhysicsDrift tubeGeneral RelativityIon-optic simulationsCERN Labdrift tubeAstrophysics::High Energy Astrophysical Phenomena[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Charged-particle opticsfabrication7. Clean energy01 natural sciencesanti-p: decelerationlaw.inventionNuclear physicslaw0103 physical sciencessynchrotronPhysics::Atomic Physics010306 general physicsAntihydrogennumerical calculationsInstrumentationaccelerator: designPhysicsantihydrogenLarge Hadron Collider010308 nuclear & particles physicsHigh voltageCharged particleSynchrotron[PHYS.PHYS.PHYS-GEN-PH]Physics [physics]/Physics [physics]/General Physics [physics.gen-ph]Pulse (physics)beam opticsAntiprotonPhysics::Accelerator Physics
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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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Coulomb Excitation of Proton-rich N=80 Isotones at HIE-ISOLDE

2020

Abstract A projectile Coulomb-excitation experiment was performed at the radioactive ion beam facility HIE-ISOLDE at CERN. The radioactive 140Nd and 142Sm ions were post accelerated to the energy of 4.62 MeV/A and impinged on a 1.45 mg/cm2-thin 208Pb target. The γ rays depopulating the Coulomb-excited states were recorded by the HPGe-array MINIBALL. The scattered charged particles were detected by a double-sided silicon strip detector in forward direction. Experimental γ-ray intensities were used for the determination of electromagnetic transition matrix elements. Preliminary results for the reduced transition strength of the B ( M 1 ; 2 3 + → 2 1 + ) = 0.35 ( 19 ) μ N 2 of 140Nd and a firs…

HistoryIon beamProtonSiliconPhysics::Instrumentation and Detectorschemistry.chemical_elementCoulomb excitationhiukkasfysiikka01 natural sciences3100EducationIonNuclear physics0103 physical sciencesNuclear Physics - Experiment010306 general physicsNuclear ExperimentPhysicsLarge Hadron Collider010308 nuclear & particles physicsProjectileCharged particleComputer Science ApplicationschemistryPhysics::Accelerator Physicsydinfysiikka
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Examining the N=28 shell closure through high-precision mass measurements of Ar46–48

2020

The strength of the $N=28$ magic number in neutron-rich argon isotopes is examined through high-precision mass measurements of $^{46\text{--}48}\mathrm{Ar}$, performed with the ISOLTRAP mass spectrometer at ISOLDE/CERN. The new mass values are up to 90 times more precise than previous measurements. While they suggest the persistence of the $N=28$ shell closure for argon, we show that this conclusion has to be nuanced in light of the wealth of spectroscopic data and theoretical investigations performed with the SDPF-U phenomenological shell model interaction. Our results are also compared with ab initio calculations using the valence space in-medium similarity renormalization group and the s…

PhysicsArgonValence (chemistry)010308 nuclear & particles physicsSHELL modelchemistry.chemical_elementIsotopes of argonRenormalization groupMass spectrometry01 natural sciencesISOLTRAPchemistryAb initio quantum chemistry methods0103 physical sciencesPhysics::Atomic and Molecular ClustersAtomic physics010306 general physicsPhysical Review C
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Charge radii, moments, and masses of mercury isotopes across the N=126 shell closure

2021

Combining laser spectroscopy in a Versatile Arc Discharge and Laser Ion Source, with Penning-trap mass spectrometry at the CERN-ISOLDE facility, this work reports on mean-square charge radii of neutron-rich mercury isotopes across the $N = 126$ shell closure, the electromagnetic moments of $^{207}$Hg and more precise mass values of $^{206-208}$Hg. The odd-even staggering (OES) of the mean square charge radii and the kink at $N = 126$ are analyzed within the framework of covariant density functional theory (CDFT), with comparisons between different functionals to investigate the dependence of the results on the underlying single-particle structure. The observed features are defined predomina…

Nuclear Theorynucl-thShell (structure)FOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometrynucl-ex7. Clean energy01 natural sciencesNuclear Theory (nucl-th)Atomic orbital0103 physical sciencesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)010306 general physicsSpectroscopyNuclear ExperimentPhysics010308 nuclear & particles physicsCharge (physics)Ion sourceddc:3. Good healthPairingNuclear Physics - TheoryDensity functional theoryAtomic physicsPräzisionsexperimente - Abteilung Blaum
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Positron production using a 9 MeV electron linac for the GBAR experiment

2020

For the GBAR (Gravitational Behaviour of Antihydrogen at Rest) experiment at CERN's Antiproton Decelerator (AD) facility we have constructed a source of slow positrons, which uses a low-energy electron linear accelerator (linac). The driver linac produces electrons of 9 MeV kinetic energy that create positrons from bremsstrahlung-induced pair production. Staying below 10 MeV ensures no persistent radioactive activation in the target zone and that the radiation level outside the biological shield is safe for public access. An annealed tungsten-mesh assembly placed directly behind the target acts as a positron moderator. The system produces $5\times10^7$ slow positrons per second, a performan…

safetyAntimatterNuclear and High Energy PhysicsCERN LabPhysics - Instrumentation and DetectorstungstenPositronAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesElectron01 natural sciences7. Clean energyLinear particle acceleratorpositron: particle source010305 fluids & plasmaselectron: pair productionNuclear physicselectron: linear acceleratorPositronPositron; Linear accelerator; Antimatter; Antihydrogen; Gravitation0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental TechniquesNuclear Experiment010306 general physicsAntihydrogenphysics.ins-detInstrumentationenergy: lowantihydrogenPhysicsLarge Hadron Collidergravitation 2Instrumentation and Detectors (physics.ins-det)linear acceleratorAntiproton DeceleratorPair productionradioactivityAntimattergravitation: accelerationPhysics::Accelerator PhysicsHigh Energy Physics::Experimentperformancepositron: yieldGravitationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Shape staggering of midshell mercury isotopes from in-source laser spectroscopy compared with density-functional-theory and Monte Carlo shell-model c…

2019

Neutron-deficient Hg177-185 isotopes were studied using in-source laser resonance-ionization spectroscopy at the CERN-ISOLDE radioactive ion-beam facility in an experiment combining different detection methods tailored to the studied isotopes. These include either α-decay tagging or multireflection time-of-flight gating for isotope identification. The endpoint of the odd-even nuclear shape staggering in mercury was observed directly by measuring for the first time the isotope shifts and hyperfine structures of Hg177-180. Changes in the mean-square charge radii for all mentioned isotopes, magnetic dipole, and electric quadrupole moments of the odd-A isotopes and arguments in favor of I=7/2 s…

nucl-thNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]3106ResearchInstitutes_Networks_Beacons/photon_science_instituteharmonic-oscillator basisMonte Carlo methodFOS: Physical sciencesPhoton Science Institute[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear Structure01 natural sciences7. Clean energyodd-massNuclear Theory (nucl-th)Atomic orbitalCharge radius0103 physical sciencesNuclear Physics - ExperimentDalton Nuclear InstituteNeutronneutron-deficient hgNuclear Experiment (nucl-ex)nuclear charge-distribution010306 general physicsNuclear ExperimentNuclear ExperimentHyperfine structurePhysics010308 nuclear & particles physicsGénéralitésexcited structuresstatesResearchInstitutes_Networks_Beacons/dalton_nuclear_institutehyperfine-structure13. Climate actionNuclear Physics - Theoryoblate-prolate transitionaxially deformed solutionQuadrupolemomentsDensity functional theoryAtomic physicsPräzisionsexperimente - Abteilung BlaumMagnetic dipole
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Restoring the valence-shell stabilization in Nd 140

2020

A projectile Coulomb-excitation experiment was performed at the radioactive-ion beam facility HIE-ISOLDE at CERN to obtain E2 and M1 transition matrix elements of Nd-140 using the multistep Coulomb-excitation code GOSIA. The absolute M1 strengths, B(M1; 2(2)(-) -> 2(1)(+)) = 0.033(8)mu(2)(N), B(M1 ; 2(3)(+) -> 2(1)(+)) = 0.26(-0.10)(+0.11)mu(2)(N), and B(M1; 2(4)+ -> 2(1)(+)) <0.04 mu(2)(N) identify the 2(3)(+) state as the main fragment of the one-quadrupole-phonon proton-neutron mixed-symmetry state of Nd-140. The degree of F-spin mixing in Nd-140 was quantified with the determination of the mixing matrix element VF-mix <7(-7)(-13) keV. Peer reviewed

PhysicsScience & TechnologyProton010308 nuclear & particles physicsProjectilePhysicsMIXED-SYMMETRYStochastic matrixAnalytical chemistryCoulomb excitationPROTON114 Physical sciences01 natural sciencesPhysics NuclearSTATESPhysical Sciences0103 physical sciencesMatrix element010306 general physicsValence electronBeam (structure)Mixing (physics)Physical Review C
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Search for Isovector Valence-Shell Excitations in 140 Nd and 142 Sm via Coulomb excitation reactions of radioactive ion beams

2018

Projectile Coulomb excitation experiments were performed at HIE-ISOLDE at CERN with the radioactive ion beams of 140Nd and 142Sm. Ions with an energy of 4:62 MeV/A were impinging on a 1.45 mg/cm2 thick 208Pb target. The γ-rays depopulating the Coulomb-excited states were recorded by the HPGe-array MINIBALL and scattered particles were detected by a double-sided silicon strip detector. Experimental intensities were used for the determination of electromagnetic transition matrix elements. A preliminary result of the B(M1; 2+3 → 2+1) of 140Nd and an upper limit for the case of 142Sm are revealing the main fragments of the proton-neutron mixed-symmetry 2+1;ms states.

SiliconPhysics::Instrumentation and DetectorsQC1-999chemistry.chemical_elementCoulomb excitation01 natural sciencesIon0103 physical sciencesNuclear Physics - ExperimentNuclear Experiment010306 general physicsCoulomb excitation experimentsPhysicsLarge Hadron ColliderIsovectorta114010308 nuclear & particles physicsProjectilePhysicsDetectorchemistryPhysics::Accelerator PhysicsAtomic physicsValence electronydinfysiikkaEPJ Web of Conferences
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Change in structure between the $I = 1/2$ states in $^{181}$Tl and $^{177,179}$Au

2018

Abstract The first accurate measurements of the α-decay branching ratio and half-life of the I π = 1 / 2 + ground state in 181Tl have been made, along with the first determination of the magnetic moments and I = 1 / 2 spin assignments of the ground states in 177,179Au. The results are discussed within the complementary systematics of the reduced α-decay widths and nuclear g factors of low-lying, I π = 1 / 2 + states in the neutron-deficient lead region. The findings shed light on the unexpected hindrance of the 1 / 2 + → 1 / 2 + , 181Tl → g 177 Aug α decay, which is explained by a mixing of π 3 s 1 / 2 and π 2 d 3 / 2 configurations in 177Aug, whilst 181Tlg remains a near-pure π 3 s 1 / 2 .…

Nuclear and High Energy PhysicsHadronNuclear physicsThallium nuclei[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences0103 physical sciencesddc:530Nuclear Physics - ExperimentLaser spectroscopy010306 general physicsSpin (physics)PhysicsMagnetic moment010308 nuclear & particles physicsBranching fractionLandé g-factorGold nucleiDecay spectroscopylcsh:QC1-9993. Good healthNuclear deformationPräzisionsexperimente - Abteilung BlaumAtomic physicsGround stateNucleonlcsh:PhysicsDimensionless quantity
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Spectroscopy of the long-lived excited state in the neutron-deficient nuclides Po195,197,199 by precision mass measurements

2017

Direct mass measurements of the low-spin 3/2(-) and high-spin 13/2(+) states in the neutron-deficient isotopes Po-195 and Po-197 were performed with the Penning-trap mass spectrometer ISOLTRAP at ISOLDE-CERN. These measurements allow the determination of the excitation energy of the isomeric state arising from the nu i(13/2) orbital in Po-195,Po-197. Additionally, the excitation energy of isomeric states of lead, radon, and radium isotopes in this region were obtained from alpha-decay chains. These excitation energies complete the knowledge of the energy systematics in the region and confirm that the 13/2(+) states remain isomeric, independent of the number of valence neutrons.

PhysicsIsotopeSpectrometer010308 nuclear & particles physics01 natural sciences7. Clean energyISOLTRAPNuclear physicsExcited state0103 physical sciencesNeutronNuclideAtomic physicsNuclear Experiment010306 general physicsSpectroscopyExcitationPhysical Review C
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Shape coexistence in Au 187 studied by laser spectroscopy

2020

Hyperfine-structure parameters and isotope shift of the 9/2$^−$ isomeric state in $^{187}$Au relative to $^{197}$Au for the 267.6-nm atomic transition have been measured for the first time using the in-source resonance-ionization spectroscopy technique. The magnetic dipole moment and change in the mean-square charge radius for this 9/2$^−$ isomer have been deduced. The observed large isomer shift relative to the 1/2$^+$ ground state in $^{187}$Au confirms the occurrence of the shape coexistence in $^{187}$Au proposed earlier from the analysis of the nuclear spectroscopic data and particle plus triaxial rotor calculations. The analysis of the magnetic moment supports the previously proposed …

PhysicsMagnetic momentIsotope010308 nuclear & particles physicsNuclear structure01 natural sciences7. Clean energyCharge radius0103 physical sciencesPhysics::Atomic and Molecular ClustersParticleDeformation (engineering)Atomic physics010306 general physicsGround stateSpectroscopyPhysical Review C
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Development of a PbWO 4 detector for single-shot positron annihilation lifetime spectroscopy at the GBAR experiment

2020

International audience; We have developed a PbWO 4 (PWO) detector with a large dynamic range to measure the intensity of a positron beam and the absolute density of the ortho-positronium (o-Ps) cloud it creates. A simulation study shows that a setup based on such detectors may be used to determine the angular distribution of the emission and reflection of o-Ps to reduce part of the uncertainties of the measurement. These will allow to improve the precision in the measurement of the cross section for the (anti) hydrogen formation by (anti) proton-positronium charge exchange and to optimize the yield of antihydrogen ion which is an essential parameter in the GBAR experiment.

PhysicsPhysics::Instrumentation and Detectors[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]DetectorMeasure (physics)General Physics and Astronomy7. Clean energyIonNuclear physicsCross section (physics)[PHYS.QPHY]Physics [physics]/Quantum Physics [quant-ph]PACS: 78.70.Bj 41.75.Fr 36.10.DrYield (chemistry)Reflection (physics)[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]AntihydrogenSpectroscopyComputingMilieux_MISCELLANEOUS
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Characterization of the shape-staggering effect in mercury nuclei

2018

In rare cases, the removal of a single proton (Z) or neutron (N) from an atomic nucleus leads to a dramatic shape change. These instances are crucial for understanding the components of the nuclear interactions that drive deformation. The mercury isotopes (Z = 80) are a striking example1,2: their close neighbours, the lead isotopes (Z = 82), are spherical and steadily shrink with decreasing N. The even-mass (A = N + Z) mercury isotopes follow this trend. The odd-mass mercury isotopes 181,183,185Hg, however, exhibit noticeably larger charge radii. Due to the experimental difficulties of probing extremely neutron-deficient systems, and the computational complexity of modelling such heavy nucl…

Quantum phase transitionPhysicsIsotope010308 nuclear & particles physicsNuclear TheoryGeneral Physics and Astronomy[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences3100Atomic orbital13. Climate action0103 physical sciencesAtomic nucleusQuadrupoleNuclear Physics - ExperimentNeutronNuclidePräzisionsexperimente - Abteilung BlaumAtomic physics010306 general physicsSpectroscopyNuclear Experiment
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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 $^{132}$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 $^{132}$Sn. Using the recently implemented phase-imaging ion-cyclotron-resonance method, the ordering of the low-lying isomers in $^{129}$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 renormalization group.

Nuclear Theorynucl-thIsòtops[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryFOS: Physical sciencesEspectroscòpia nuclear[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear spectroscopyNuclear Theory (nucl-th)IsotopesNuclear Physics - TheoryPhysics::Atomic and Molecular Clustersddc:530Nuclear Physics - ExperimentPräzisionsexperimente - Abteilung BlaumNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentNuclear Physics
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Laser Spectroscopy of Neutron-Rich $^{207,208}$Hg Isotopes: Illuminating the Kink and Odd-Even Staggering in Charge Radii across the $N=126$ Shell Cl…

2021

The mean-square charge radii of $^{207,208}$Hg ($Z=80, N=127,128$) have been studied for the first time and those of $^{202,203,206}$Hg ($N=122,123,126$) remeasured by the application of in-source resonance-ionization laser spectroscopy at ISOLDE (CERN). The characteristic \textit{kink} in the charge radii at the $N=126$ neutron shell closure has been revealed, providing the first information on its behavior below the $Z=82$ proton shell closure. A theoretical analysis has been performed within relativistic Hartree-Bogoliubov and non-relativistic Hartree-Fock-Bogoliubov approaches, considering both the new mercury results and existing lead data. Contrary to previous interpretations, it is d…

Nuclear Theorynucl-th[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]Nuclear TheoryFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear Theory (nucl-th)Nuclear Physics - TheoryNuclear Physics - ExperimentNuclear Experiment (nucl-ex)Präzisionsexperimente - Abteilung BlaumNuclear ExperimentNuclear ExperimentNuclear Physics
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Spectroscopy of the long-lived excited state in the neutron-deficient nuclides $^{195,197,199}$Po by precision mass measurements

2017

Direct mass measurements of the low-spin 3/2− and high-spin 13/2+ states in the neutron-deficient isotopes Po195 and Po197 were performed with the Penning-trap mass spectrometer ISOLTRAP at ISOLDE-CERN. These measurements allow the determination of the excitation energy of the isomeric state arising from the νi13/2 orbital in Po195,197. Additionally, the excitation energy of isomeric states of lead, radon, and radium isotopes in this region were obtained from α-decay chains. These excitation energies complete the knowledge of the energy systematics in the region and confirm that the 13/2+ states remain isomeric, independent of the number of valence neutrons. Direct mass measurements of the …

FOS: Physical sciencesNuclear Physics - ExperimentPräzisionsexperimente - Abteilung BlaumNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear ExperimentNuclear Experiment
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Hyperfine anomaly in gold and magnetic moments of $I^{\pi}$ $= 11/2^{−}$ gold isomers

2020

Physical review / C 101(3), 034308 (2020). doi:10.1103/PhysRevC.101.034308

Nuclear Physics - Experimentddc:530Physics::Atomic Physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structure530
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Precision Mass Measurement of $^{58-63}$Cr: 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…

Nuclear Theory (nucl-th)Nuclear Theorynucl-thNuclear Physics - TheoryNuclear TheoryPhysics::Atomic and Molecular ClustersFOS: Physical sciencesNuclear Physics - ExperimentNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-exNuclear ExperimentNuclear Experiment
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