0000000001234109

AUTHOR

P. Spagnoletti

showing 27 related works from this author

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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α -decay spectroscopy of the N=130 isotones Ra218 and Th220 : Mitigation of α -particle energy summing with implanted nuclei

2019

© 2019 American Physical Society. An analysis technique has been developed in order to mitigate energy summing due to sequential short-lived α decays from nuclei implanted into a silicon detector. Using this technique, α-decay spectroscopy of the N=130 isotones Ra218 (Z=88) and Th220 (Z=90) has been performed. The energies of the α particles emitted in the Ra218→Rn214 and Th220→Ra216 ground-state-to-ground-state decays have been measured to be 8381(4) keV and 8818(13) keV, respectively. The half-lives of the ground states of Ra218 and Th220 have been measured to be 25.99(10) μs and 10.4(4) μs, respectively. The half-lives of the ground states of the α-decay daughters, Rn214 and Ra216, have …

Physics010308 nuclear & particles physicsBranching fraction0103 physical sciencesSilicon detectorAtomic physics010306 general physicsSpectroscopy01 natural sciencesα particlesEnergy (signal processing)Physical Review C
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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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A charge plunger device to measure the lifetimes of excited nuclear states where transitions are dominated by internal conversion

2020

Abstract A charge plunger device has been commissioned based on the DPUNS plunger (Taylor et al., 2013) using the in-flight mass separator MARA at the University of Jyvaskyla. The 152 Sm (32 S ,4 n )180 Pt reaction was used to populate excited states in 180 Pt . A lifetime measurement of the 2 1 + state was performed by applying the charge plunger technique, which relies on the detection of the charge state-distribution of recoils rather than the detection of the emitted γ rays. This state was a good candidate to test the charge plunger technique as it has a known lifetime and depopulates through a converted transition that competes strongly with γ -ray emission. The lifetime of the 2 1 + s…

PhysicsPlungerNuclear and High Energy PhysicsInternal conversionExcited stateCharge (physics)Atomic physicsInstrumentationMeasure (mathematics)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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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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Dealing with contaminants in Coulomb excitation of radioactive beams

2020

Abstract Data analysis of the Coulomb excitation experiment of the exotic 206Hg nucleus, recently performed at CERN’s HIE-ISOLDE facility, needs to account for the contribution to target excitation due to the strongly-present beam contaminant 130Xe. In this paper, the contamination subtraction procedure is presented.

PhysicsHistoryLarge Hadron Collider010308 nuclear & particles physicsCoulomb excitationSubtraction proceduretutkimuslaitteetCoulomb excitationContaminationhiukkaskiihdyttimet01 natural sciencesAccelerators and Storage Rings3100Computer Science ApplicationsEducationNuclear physics0103 physical sciencesPhysics::Accelerator PhysicsNuclear Physics - Experiment010306 general physicsNuclear ExperimentydinfysiikkaBeam (structure)ExcitationRadioactive beams
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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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Quadrupole deformation of Xe-130 measured in a Coulomb-excitation experiment

2020

Physical review / C 102(5), 054304 (2020). doi:10.1103/PhysRevC.102.054304

DiagonalSemiclassical physicsBEAMCoulomb excitationhiukkasfysiikka[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structure530114 Physical sciences01 natural sciencessähkömagneettiset ilmiötnukleonitsymbols.namesakeMatrix (mathematics)NUCLEAR-DATA SHEETS0103 physical sciencesPhenomenological modelNuclear Physics - Experimentddc:530010306 general physicsPhysicsScience & Technology010308 nuclear & particles physicsPhysicsnucleon distributionBohr modelPhysics Nuclearelectromagnetic transitionsSTATESSHAPESQuadrupolePhysical SciencessymbolsAtomic physicsydinfysiikkaHamiltonian (quantum mechanics)
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α -decay branching ratio of Pt180

2020

PhysicsNuclear physics010308 nuclear & particles physicsBranching fraction0103 physical sciencesAlpha decay010306 general physics01 natural sciencesPhysical Review C
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Lifetime measurements of excited states in $^{163}$W and the implications for the anomalous B(E2) ratios in transitional nuclei

2019

Grahn, Tuomas/0000-0002-6255-2279; Herzan, Andrej/0000-0002-6736-7638; Cullen, Dave/0000-0002-0041-1606; Barber, Liam/0000-0002-7409-9352; Keatings, James Michael/0000-0003-4271-8021; SAYGI, BAHADIR/0000-0001-5406-506X; Greenlees, Paul/0000-0002-5986-5274; Spagnoletti, Pietro/0000-0002-7674-989X; Parr, Edward/0000-0001-6204-4461; Bondili, S Nara Singh/0000-0002-4096-2429

Nuclear and High Energy PhysicsspektroskopiaNuclear TheoryMean lifetimes[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencessymbols.namesake0103 physical sciencesCollective modelmedicineNeutronGamma spectroscopy010306 general physicsNuclear ExperimentPhysicsmean lifetimes010308 nuclear & particles physicsRecoil-distance Doppler-shift methodlcsh:QC1-999Nuclear deformationGamma-ray SpectroscopyCore (optical fiber)Rotational modelmedicine.anatomical_structureB(E2) reduced transition probabilitiesgamma-ray spectroscopyExcited statesymbolsAtomic physicsydinfysiikkaNucleusDoppler effectlcsh:Physics
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Population of lead isotopes in binary reactions using a Rb 94 radioactive beam

2020

8 pags., 9 figs.

3106PopulationNuclear TheoryBinary number[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyParticle detectorNuclear physicsnuclear reaction ; transfer reaction ; radioactive beam0103 physical sciencesNuclear ReactionsNeutronNuclear Physics - Experiment010306 general physicseducationNuclear Experimentnuclear reactionsPhysicseducation.field_of_studyisotoopitScience & TechnologyIsotope010308 nuclear & particles physicsPhysicsPhysics NuclearPhysical Sciencestransfer reactionsPhysics::Accelerator Physicslow and intermediate energy heavy-ion reactionslyijymodels nad methods for nuclear reactionsNucleonydinfysiikkaBeam (structure)Radioactive beamPhysical Review C
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Evolution of Octupole Deformation in Radium Nuclei from Coulomb Excitation of Radioactive Ra222 and Ra228 Beams

2020

There is sparse direct experimental evidence that atomic nuclei can exhibit stable "pear" shapes arising from strong octupole correlations. In order to investigate the nature of octupole collectivity in radium isotopes, electric octupole (E3) matrix elements have been determined for transitions in ^{222,228}Ra nuclei using the method of sub-barrier, multistep Coulomb excitation. Beams of the radioactive radium isotopes were provided by the HIE-ISOLDE facility at CERN. The observed pattern of E3 matrix elements for different nuclear transitions is explained by describing ^{222}Ra as pear shaped with stable octupole deformation, while ^{228}Ra behaves like an octupole vibrator.

PhysicsIsotopeNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementCoulomb excitation01 natural sciencesRadiumMatrix (mathematics)chemistryExcited state0103 physical sciencesAtomic nucleusCoulombPhysics::Accelerator PhysicsPhysics::Atomic PhysicsAtomic physicsDeformation (engineering)Nuclear Experiment010306 general physicsPhysical Review Letters
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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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The observation of vibrating pear-shapes in radon nuclei

2019

6 pags., 4 fig.s, 1 tab. -- Open Access funded by Creative Commons Atribution Licence 4.0

Physics beyond the Standard ModelScienceNuclear TheoryGeneral Physics and Astronomychemistry.chemical_elementRadon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesArticleGeneral Biochemistry Genetics and Molecular BiologyRadiumQuantum state0103 physical sciencesCP: violationground stateNuclear Physics - ExperimentPhysics::Atomic PhysicsExperimental nuclear physicslcsh:Science010306 general physicsnumerical calculationsNuclear ExperimentPhysicsMultidisciplinaryIsotope010308 nuclear & particles physicsnew physicsnucleusQradonGeneral ChemistryPublisher Correctionradiumexotic nucleielectric momentchemistryradioactivityMoment (physics)Atomic nucleusCP violationlcsh:QExotic atoms and moleculesAtomic physicsydinfysiikka
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Coulomb excitation of pear-shaped nuclei

2019

There is a large body of evidence that atomic nuclei can undergo octupole distortion and assume the shape of a pear. This phenomenon is important for measurements of electric-dipole moments of atoms, which would indicate CP violation and hence probe physics beyond the Standard Model of particle physics. Isotopes of both radon and radium have been identified as candidates for such measurements. Here, we have observed the low-lying quantum states in 224Rn and 226Rn by accelerating beams of these radioactive nuclei. We show that radon isotopes undergo octupole vibrations but do not possess static pear-shapes in their ground states. We conclude that radon atoms provide less favourable condition…

PhysicsIsotope010308 nuclear & particles physicsPhysicsQC1-999Physics beyond the Standard Modelchemistry.chemical_elementRadonCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural scienceschemistryQuantum state0103 physical sciencesMoment (physics)Atomic nucleusCP violationNuclear Physics - ExperimentPhysics::Atomic PhysicsAtomic physics010306 general physicsydinfysiikka
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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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Lifetime measurements of excited states in ¹⁶³W and the implications for the anomalous B(E2) ratios in transitional nuclei

2019

This letter reports lifetime measurements of excited states in the odd-N nucleus $^{163}$W using the recoil-distance Doppler shift method to probe the core polarising effect of the i13/2 neutron orbital on the underlying soft triaxial even-even core. The ratio B(E2:21/2+→17/2+)/B(E2:17/2+→13/2+) is consistent with the predictions of the collective rotational model. The deduced B(E2) values provide insights into the validity of collective model predictions for heavy transitional nuclei and a geometric origin for the anomalous B(E2) ratios observed in nearby even-even nuclei is proposed.

Nuclear Experiment
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Coulomb excitation of Rn-222

2022

The nature of quadrupole and octupole collectivity in 222Rn was investigated by determining the electric-quadrupole (E2) and octupole (E3) matrix elements using subbarrier, multistep Coulomb excitation. The radioactive 222Rn beam, accelerated to 4.23 MeV/u, was provided by the HIE-ISOLDE facility at CERN. Data were collected in the Miniball γ-ray spectrometer following the bombardment of two targets, 120Sn and 60Ni. Transition E2 matrix elements within the ground-state and octupole bands were measured up to 10ℏ and the results were consistent with a constant intrinsic electric-quadrupole moment, 518(11)efm2. The values of the intrinsic electric-octupole moment for the 0+→3− and 2+→5− transi…

Science & TechnologyPhysics NuclearSTATESPhysicsSHAPESPhysical SciencesISOTOPESRADON
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Lifetime measurements of yrast states in ¹⁷⁸ Pt using the charge plunger method with a recoil separator

2021

Abstract Lifetime measurements in \(^{178}\)Pt with excited states de-exciting through \(\gamma\)-ray transitions and internal electron conversions have been performed. Ionic charges were selected by the in-flight mass separator MARA and measured at the focal plane in coincidence with the \(4^{+}_{1}→2^{+}_{1}\) 257 keV γ-ray transition detected using the JUROGAM 3 spectrometer. The resulting charge-state distributions were analysed using the differential decay curve method (DDCM) framework to obtain a lifetime value of 430(20) ps for the \(2^{+}_{1}\) state. This work builds on a method that combines the charge plunger technique with the DDCM analysis. As an alternative analysis, ions were…

platinaydinfysiikka
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Coulomb excitation of 222Rn

2022

Physical Review C
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Quadrupole and octupole collectivity in the semi-magic nucleus 80,206Hg126

2023

The first low-energy Coulomb-excitation measurement of the radioactive, semi-magic, two proton-hole nucleus 206Hg, was performed at CERN’s recently-commissioned HIE-ISOLDE facility. Two γ rays depopulating low-lying states in 206Hg were observed. From the data, a reduced transition strength B(E2; 2+ 1 → 0+ 1 ) = 4.4(6) W.u was determined, the first such value for an N = 126 nucleus south of 208Pb, which is found to be slightly lower than that predicted by shell-model calculations. In addition, a collective octupole state was identified at an excitation energy of 2705 keV, for which a reduced B(E3) transition probability of 30+10−13 W.u was extracted. These results are crucial for understand…

isotoopitelohopeaydinfysiikka
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Coulomb excitation of 222Rn

2022

International audience; The nature of quadrupole and octupole collectivity in $^{222}$Rn was investigated by determining the electric-quadrupole (E2) and octupole (E3) matrix elements using subbarrier, multistep Coulomb excitation. The radioactive $^{222}$Rn beam, accelerated to 4.23 MeV/u, was provided by the HIE-ISOLDE facility at CERN. Data were collected in the Miniball $\gamma$ -ray spectrometer following the bombardment of two targets, $^{120}$Sn and $^{60}$Ni. Transition E2 matrix elements within the ground-state and octupole bands were measured up to 10 ¯h and the results were consistent with a constant intrinsic electric-quadrupole moment, 518(11) $e$ fm$^2$ . The values of the int…

A ≥ 220electromagnetic transitionsnuclear structure & decaysNuclear Physics - Experimentradon[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikka114 Physical sciences
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α-decay spectroscopy of the N = 130 isotones 218Ra and 220Th: Mitigation of α-particle energy summing with implanted nuclei

2019

An analysis technique has been developed in order to mitigate energy summing due to sequential short-lived α decays from nuclei implanted into a silicon detector. Using this technique, α-decay spectroscopy of the N=130 isotones 218Ra (Z=88) and 220Th (Z=90) has been performed. The energies of the α particles emitted in the 218Ra→214Rn and 220Th→216Ra ground-state-to-ground-state decays have been measured to be 8381(4) keV and 8818(13) keV, respectively. The half-lives of the ground states of 218Ra and 220Th have been measured to be 25.99(10) μs and 10.4(4) μs, respectively. The half-lives of the ground states of the α-decay daughters, 214Rn and 216Ra, have been measured to be 259(3) ns and …

nuclear data analysis and compilationalpha decayydinfysiikkaspectrometers and spectroscopic techniques
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Single-particle states and parity doublets in odd-Z 221Ac and 225Pa from α-decay spectroscopy

2022

Low-lying states in the odd-Z isotopes 22189Ac132 and 22591Pa134 have been studied using α-particle and αγ-coincidence spectroscopy in the 225Pa→221Ac→217Fr decay chain. Ground-state spin and parity assignments of Iπ = 5/2− are proposed for both 221Ac and 225Pa, with the odd proton occupying the Ω = 5/2 orbital of the quadrupole-octupole deformed shell model in both nuclei. In 221Ac, excited states in the bands based on the Ω = 5/2 and Ω = 3/2 orbitals have been identified, including proposed parity-doublet states. The results suggest that reflection-asymmetric deformation of the ground state persists in the odd-A members of the isotope chains down to N = 132 for Ac and N = 134 for Pa, befo…

ydinfysiikka
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