0000000000681964

AUTHOR

J. M. Keatings

showing 15 related works from this author

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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Nuclear structure of Te isotopes beyond neutron magic number N=82

2021

15 pags., 10 figs., 4 tabs.

PhysicsIsotope[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsNuclear TheoryNuclear structureNuclear Structure7. Clean energy01 natural sciencesNuclear physicsFragmentation (mass spectrometry)Excited state0103 physical sciencesNeutron010306 general physicsNucleonNuclear ExperimentBeam (structure)Magic number (physics)
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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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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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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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Evolution of proton single-particle states in neutron-rich Sb isotopes beyond N=82

2020

11 pags., 8 figs., 2 tabs.

PhysicsProtonIsotope010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaNuclear structure[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structure7. Clean energy01 natural sciencesBeta decayNuclear physicsNeutron numberExcited state0103 physical sciencesNeutronNuclear Experiment010306 general physicsExcitationPhysical Review C
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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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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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Identification of excited states in 107,52Te55

2021

Excited states in the extremely neutron-deficient nucleus 107Te have been identified from two separate experiments using the recoil-decay tagging technique. Two connected structures were observed on the basis of γγ-coincidence relations and tentatively assigned as built on the mixed-parentage νg7/2d5/2 and νh11/2 intruder configurations. The observed structures were compared with large-scale shell-model calculations and total Routhian surface calculations. Collective behavior was discovered to persist in the νh11/2 band of 107Te which highlights the shape-polarizing effect of a single valence neutron occupying the h11/2 intruder orbit as the N=50 shell closure is approached. peerReviewed

isotoopittelluurinuclear physicsnuclear structureydinfysiikka
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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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