0000000000968612

AUTHOR

M. Nyman

showing 69 related works from this author

In-beam and decay spectroscopy of very neutron deficient iridium nuclei

2005

Iridium nuclei at and beyond the proton drip line have been studied via fusion evaporation reactions. A reaction of 92Mo(78Kr, p2n) at a beam energy of 360 MeV and target thickness 500 µg cm−2 was employed to study 167,167mIr. A reaction of 112Sn(58Ni, p2n) at a beam energy of 266 MeV and target thickness 500 µg cm−2 was used to study 169,169mIr. The experiments were performed at the University of Jyvaskyla utilizing the RITU separator in conjunction with the focal plane GREAT spectrometer and the JUROGAM Ge array at the target position. Excited states feeding both the ground state and isomeric state in 169Ir, excited states feeding the ground state of 167Ir and the ground state alpha decay…

PhysicsNuclear and High Energy PhysicsProtonExcited stateNeutronAlpha decayAtomic physicsSpectroscopyGround stateBeam (structure)Neutron spectroscopyJournal of Physics G: Nuclear and Particle Physics
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Evolution of collectivity inHg180andHg182

2009

Lifetimes of yrast states in $^{180}\mathrm{Hg}$ up to the ${8}^{+}$ state and of the ${9}^{\ensuremath{-}}$ state have been extracted from recoil-decay tagged $\ensuremath{\gamma}$-ray spectra by using the recoil distance Doppler-shift method. In addition, lifetimes of yrast states up to the ${10}^{+}$ state in $^{182}\mathrm{Hg}$ have been extracted from recoil-gated $\ensuremath{\gamma}\ensuremath{\gamma}$-coincidence spectra. The present study addresses the evolution of collectivity of two competing shapes in neutron-deficient Hg nuclei as a function of $A$ and the configuration mixing at low spin.

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaYrastState (functional analysis)01 natural sciencesSpectral lineNuclear physicsRecoil0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsSpin (physics)Radioactive decayPhysical Review C
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New developments on the recoil distance doppler-shift method

2010

Absolute transition probabilities are fundamental observables for nuclear structure. The recoil-distance-Doppler-shift (RDDS) technique, also called plunger technique, is a well established tool for the determination of these important experimental quantities via the measurement of lifetimes of excited nuclear states. Nowadays nuclear structure investigations are concentrated on exotic nuclei which are often produced with extremely small cross sections or with very low beam intensities. In order to use the RDDS technique also for the investigation of very exotic nuclei this method has to be adapted to the specific needs of these special reactions. This article gives an overview on recent RD…

PhysicsHistoryProjectileNuclear TheoryNuclear structureObservableCoulomb excitationComputer Science ApplicationsEducationNuclear physicsRecoilExcited stateCoulombPhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentBeam (structure)Journal of Physics: Conference Series
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Evidence for prolate structure in light Pb isotopes from in-beamγ-ray spectroscopy ofPb185

2009

For the first time, excited states in {sup 185}Pb have been observed in in-beam {gamma}-ray spectroscopic measurements using the recoil-decay tagging method. The resulting level scheme reveals a strongly coupled yrast band structure that originates from coupling of the i{sub 13/2} quasineutron to a prolate deformed core. The band is also observed to de-excite via the spherical {alpha}-decaying 13/2{sup +}isomeric state.

PhysicsNuclear and High Energy PhysicsExcited stateYrastGamma spectroscopyAlpha decayAtomic physicsElectronic band structureCoupling (probability)SpectroscopyRadioactive decayPhysical Review C
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Anomalous transition strength in the proton-unbound nucleus I5653109

2011

A lifetime measurement has been made for the first excited 11/2(+) state in the proton-unbound nucleus (109)(53)I56 using the recoil-distance Doppler-shift method in conjunction with recoil-proton ...

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsConjunction (astronomy)Nuclear Theory01 natural sciences7. Clean energyNuclear physicsmedicine.anatomical_structureTransition strengthExcited state0103 physical sciencesmedicinePhysics::Atomic PhysicsAtomic physicsNuclear Experiment010306 general physicsNucleusPhysics Letters B
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A Recoil-Beta Tagging Study of N = Z nucleus [sup 66]As

2011

A Recoil‐Beta Tagging (RBT) experiment was recently performed at the accelerator laboratory at the University of Jyvaskyla in order to identify T = 1 excited states in the medium‐heavy N = Z = 33 nucleus 66As. The fusion‐evaporation reaction 28Si(40Ca,pn)66As was employed at a beam energy of 75 MeV. The experiment was carried out utilising the JUROGAM II γ‐ray spectrometer in conjunction with the gas‐filled recoil separator RITU and the GREAT focal plane spectrometer system. The half‐lives and ordering of the two known isomeric states in 66As have been determined. In addition, several new prompt γ‐ray transitions from excited states both bypassing and decaying to the isomeric states in 66As…

Nuclear reactionPhysicsNuclear physicsRecoilSpectrometerExcited stateNeutronGamma spectroscopyIsotopes of siliconAtomic physicsNuclear ExperimentRadioactive decayAIP Conference Proceedings
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Decays of new nuclides and isomers beyond the proton drip line - The influence of neutron configurations

2008

Bozok University;Erciyes University;et al.;Istanbul University;Nigde University;The Turkish Atomic Energy Authority (TAEK)

PhysicsProtonGamma rayAlpha particleSegmented Si and Ge detectors. Measured E ? E proton E ? T 1/2Nuclear physicsNuclear Reactions 58 Ni+ 106 Cd at 290300310 MeV beam energyBeta particleNeutronEnriched targetsNuclideAlpha decayGas-filled recoil separatorAtomic physicsNuclear ExperimentGround state
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Shape coexistence at the proton drip-line: First identification of excited states inPb180

2010

Excited states in the extremely neutron-deficient nucleus {sup 180}Pb have been identified for the first time using the JUROGAM II array in conjunction with the RITU recoil separator at the Accelerator Laboratory of the University of Jyvaeskylae. This study lies at the limit of what is presently achievable with in-beam spectroscopy, with an estimated cross section of only 10 nb for the {sup 92}Mo({sup 90}Zr,2n){sup 180}Pb reaction. A continuation of the trend observed in {sup 182}Pb and {sup 184}Pb is seen, where the prolate minimum continues to rise beyond the N=104 midshell with respect to the spherical ground state. Beyond-mean-field calculations are in reasonable correspondence with the…

PhysicsNuclear reactionNuclear and High Energy PhysicsProton010308 nuclear & particles physicsNeutron emissionHadron01 natural sciencesExcited state0103 physical sciencesAtomic physics010306 general physicsGround stateSpectroscopyNucleonPhysical Review C
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Recoil-beta tagging: A novel technique for studying proton-drip-line nuclei

2006

Abstract Tagging with charged particles and γ -rays at the focal plane of recoil separators has proven, over the last two decades, to be a very powerful tool for the identification of excited states in exotic nuclei produced with very low cross-sections. One of the key areas so far unexplored in terms of the tagging methodology has been performing correlations with β -particles at the focal plane of a recoil separator. A new technique entitled Recoil-Beta Tagging (RBT) has been developed, this technique exploits the unusual properties of Fermi super-allowed β emitters, which have both a short half-life ( ∼ 100 ms ) and high β + -endpoint energy. Correlating with such β -particles using a do…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsDetector[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesCharged particleSemiconductor detectorNuclear physicsRecoilPositronExcited state27.50.þe; 29.30.Kv; 29.40.Wk0103 physical sciencesAtomic physics010306 general physicsNuclear ExperimentInstrumentationFermi Gamma-ray Space Telescope
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Investigation of nuclear collectivity in the neutron mid-shell nucleusPb186

2007

For the first time, non-yrast structures of the neutron mid-shell nucleus $^{186}\mathrm{Pb}$ have been identified in an in-beam \ensuremath{\gamma}-ray spectroscopy measurement using the recoil-decay tagging technique. The yrast band has been tentatively extended up to ${I}^{\ensuremath{\pi}}=20{}^{+},$ revealing a similar backbend to that observed in the Pt and Hg isotones. Three new bands and several other transitions have been observed. Calculations carried out in the framework of the interacting boson model together with mean-field studies using the generator coordinate method provide arguments for the association of one of the new bands with an oblate shape. The present data also show…

PhysicsMass numberNuclear and High Energy PhysicsGenerator (category theory)YrastNuclear TheoryNuclear physicsMean field theoryNeutronGamma spectroscopyInteracting boson modelAtomic physicsNuclear ExperimentSpectroscopyPhysical Review C
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First observation of excited states inHg17595

2009

Excited states of the neutron-deficient nucleus Hg-175, populated using fusion-evaporation reactions, are reported for the first time. The spin and parity of the ground state has been determined to ...

PhysicsNuclear and High Energy Physicsmedicine.anatomical_structureExcited stateNuclear TheorymedicineParity (physics)Alpha decayAtomic physicsNuclear ExperimentGround stateNucleusPhysical Review C
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Evidence for oblate structure inPb186

2005

In-beam $\ensuremath{\gamma}\ensuremath{\gamma}$ coincidence data have been collected for $^{186}\mathrm{Pb}$ by combining the JUROGAM Ge-detector array and the GREAT spectrometer with the RITU gas-filled recoil separator for recoil-decay tagging measurements. In addition to the known prolate yrast band in $^{186}\mathrm{Pb}$, these data have enabled a new low-lying side band to be identified. Based on the analysis of its decay pattern and comparison with Interacting Boson Model (IBM) calculations, the new band is associated with an oblate shape.

PhysicsNuclear physicsNuclear and High Energy PhysicsSpectrometerYrastStructure (category theory)Nuclear structureGamma spectroscopyInteracting boson modelRadioactive decayCoincidencePhysical Review C
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Structure of rotational bands in 253No

2009

In-beam gamma-ray and conversion electron spectroscopic studies have been performed on the 253 No nucleus. A strongly coupled rotational band has been identified and the improved statistics allows an assignment of the band structure as built on the $\ensuremath 9/2^-[734]_{\nu}$ ground state. The results agree with previously known transition energies but disagree with the tentative structural assignments made in earlier work.

PhysicsStrongly coupledNuclear and High Energy Physics[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physicsHadronStructure (category theory)Electron01 natural sciences0103 physical sciencesStrong couplingNuclear fusion21.10.-k Properties of nuclei; nuclear energy levels - 23.20.Lv γ transitions and level energies - 29.30.Dn Electron spectroscopy - 27.90.+b A ≤ 220Atomic physics010306 general physicsGround stateElectronic band structure
Eur. Phys. J. A 42, 333 (2009)

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Shape coexistence in odd-mass Au isotopes: Determination of the excitation energy of the lowest intruder state in ^{179}Au

2011

Abstract Phenomenon of the shape coexistence has been investigated in 17979Au100. This very neutron-deficient isotope, 18 neutrons away from the stable gold isotope 19779Au118, was studied by a combination of α-decay and isomer-decay spectroscopy employing the ritu gas-filled separator and the great focal-plane spectrometer at the University of Jyvaskyla. A new isomer with t 1 / 2 = 328 ( 2 ) ns was observed and states associated with π d 3 / 2 − 1 , π s 1 / 2 − 1 , π f 7 / 2 + 1 and π h 9 / 2 + 1 structures were revealed. The implications of these results on the systematics of π h 9 / 2 + 1 and π f 7 / 2 + 1 intruder structures in the odd-mass gold isotopes are discussed. The minimum of th…

Mass numberPhysicsNuclear and High Energy PhysicsIsotopeta114010308 nuclear & particles physicsIsomer in 179Au7. Clean energy01 natural sciencesIntruder stateπh9/2+1 and πf7/2+1 intruder structures around N=1040103 physical sciencesNeutronAlpha decayIsotopes of goldAtomic physics010306 general physicsSpectroscopyExcitationPhysics Letters B
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Isomeric and ground-state properties of78171Pt,76167Os, and74163W

2010

Decay paths, half-lives, and excitation energies of the i(13/2) bandheads of the neutron-deficient nuclei Pt-171, Os-167, and W-163 have been established for the first time. Gamma-ray transitions, ...

PhysicsNuclear and High Energy PhysicsBranching fractionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryElectronInternal conversionNuclear magnetic resonanceAlpha decayAtomic physicsNuclear ExperimentGround stateSpin (physics)ExcitationRadioactive decayPhysical Review C
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γ-Ray Spectroscopy at the Limits: First Observation of Rotational Bands inLr255

2009

The rotational band structure of Lr-255 has been investigated using advanced in-beam gamma-ray spectroscopic techniques. To date, Lr-255 is the heaviest nucleus to be studied in this manner. One ro ...

Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGeneral Physics and AstronomyMoment of inertia01 natural sciencesNuclear physicsmedicine.anatomical_structureMean field theory0103 physical sciencesmedicineGamma spectroscopyAlpha decayAtomic physicsNuclear Experiment010306 general physicsElectronic band structureNucleusPhysical Review Letters
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Collectivity and Configuration Mixing inPb186,188andPo194

2006

Lifetimes of prolate intruder states in {sup 186}Pb and oblate intruder states in {sup 194}Po have been determined by employing, for the first time, the recoil-decay tagging technique in recoil distance Doppler-shift lifetime measurements. In addition, lifetime measurements of prolate states in {sup 188}Pb up to the 8{sup +} state were carried out using the recoil-gating method. The B(E2) values have been deduced from which deformation parameters vertical bar {beta}{sub 2} vertical bar =0.29(5) and vertical bar {beta}{sub 2} vertical bar =0.17(3) for the prolate and the oblate bands, respectively, have been extracted. The results also shed new light on the mixing between different shapes.

PhysicsNuclear physicsRecoilDeformation (mechanics)General Physics and AstronomyHigh Energy Physics::ExperimentBeta (velocity)State (functional analysis)Prolate spheroidElectronic band structureMolecular physicsMixing (physics)Radioactive decayPhysical Review Letters
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Spectroscopic factor and proton formation probability for the d3/2 proton emitter 151Lu

2017

The quenching of the experimental spectroscopic factor for proton emission from the short-lived $d_{3/2}$ isomeric state in $^{151m}$Lu was a long-standing problem. In the present work, proton emission from this isomer has been reinvestigated in an experiment at the Accelerator Laboratory of the University of Jyv\"{a}skyl\"{a}. The proton-decay energy and half-life of this isomer were measured to be 1295(5) keV and 15.4(8) $\mu$s, respectively, in agreement with another recent study. These new experimental data can resolve the discrepancy in the spectroscopic factor calculated using the spherical WKB approximation. Using the R-matrix approach it is found that the proton formation probabilit…

Nuclear and High Energy PhysicsWork (thermodynamics)Nuclear TheoryProton3106Proton decayFOS: Physical sciencesProton energy01 natural sciencesproton emitterWKB approximationNuclear Theory (nucl-th)Nuclear physicsA=1510103 physical sciencesrecoil-decay taggingddc:530WKB approximationNuclear Experiment (nucl-ex)spectroscopic factorProton emissionNuclear Experiment010306 general physicsNuclear ExperimentCommon emitterPhysicsQuenching (fluorescence)ta114010308 nuclear & particles physicsSpectroscopic factorProton emitterproton formation probabilitylcsh:QC1-999Proton formation probability3. Good healthRecoil-decay taggingAtomic physicslcsh:PhysicsPhysics Letters B
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Decay of aπh11/2⊗νh11/2microsecond isomer in61136Pm75

2008

An experiment has been performed to populate several extremely neutron-deficient nuclei around the mass-140 region of the nuclear chart, using a beam of {sup 54}Fe on a {sup 92}Mo target at an energy of 315 MeV. Analysis of these data using recoil-isomer tagging has established that the yrast {pi}h{sub 11/2} x {nu}h{sub 11/2},J{sup {pi}}=(8{sup +}), bandhead state in {sup 136}Pm is isomeric with a half-life of 1.5(1) {mu}s. This isomeric state decays via a 43-keV, probable-E1 transition to a J{sup {pi}}=(7{sup -}) state. Consideration of the theoretical Nilsson orbitals near the Fermi surface suggests that the J{sup {pi}}=(8{sup +}) state has a {nu}h{sub 11/2}[505](11/2){sup -} x {pi}h{sub …

PhysicsNuclear and High Energy PhysicsDecay schemeFermi levelOrder (ring theory)Fermi surfaceMicrosecondCrystallographysymbols.namesakeInternal conversionAtomic orbitalsymbolsAtomic physicsEnergy (signal processing)Physical Review C
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Collectivity ofPo196at low spin

2009

Absolute electromagnetic transition probabilities in $^{196}\mathrm{Po}$ have been measured using the recoil distance Doppler-shift technique. The lifetimes of the three lowest yrast states in $^{196}\mathrm{Po}$ were extracted from singles \ensuremath{\gamma}-ray spectra by using the recoil-decay tagging method. In addition, configuration mixing calculations of angular momentum projected mean-field states have been carried out for $^{196}\mathrm{Po}$. The present study sheds light on the onset of collectivity and mixing of competing structures in neutron-deficient Po nuclei.

PhysicsNuclear and High Energy PhysicsAngular momentum010308 nuclear & particles physicsYrast01 natural sciencesSpectral lineNuclear physicsRecoilMean field theory0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsSpin (physics)Radioactive decayPhysical Review C
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Quasiparticle alignments andα-decay fine structure of175Pt

2014

Excited states and decay properties of ${}^{175}$Pt have been investigated using the ${}^{92}$Mo${(}^{86}\mathrm{Sr},2pn)$ fusion-evaporation reaction. The JUROGAM I $\ensuremath{\gamma}$-ray spectrometer and the GREAT spectrometer were used in conjunction with the gas-filled recoil separator RITU for the measurement of the radiation at the target and focal plane positions, respectively. Two new band structures, assigned to be based on the ${I}^{\ensuremath{\pi}}=({{}^{7}{/}_{2}}^{\ensuremath{-}})$ ground state in ${}^{175}$Pt, have been established and the known yrast band has been extended up to ${I}^{\ensuremath{\pi}}=({{}^{49}{/}_{2}}^{+})$. Rotational properties of the excited states i…

PhysicsNuclear and High Energy PhysicsFormalism (philosophy of mathematics)ta114Excited stateYrastQuasiparticleAlpha decayAtomic physicsGround stateRecoil separatorPhysical Review C
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High-Kstructure inFm250and the deformed shell gaps atN=152andZ=100

2008

The structure of high-spin and nonyrast states of the transfermium nucleus $^{250}\mathrm{Fm}$ has been studied in detail. The isomeric nature of a two-quasiparticle excitation has been exploited in order to obtain spectroscopic data of exceptional quality. The data allow the configuration of an isomer first discovered over 30 years ago to be deduced, and provide an unambiguous determination of the location of neutron single-particle states in a very heavy nucleus. A comparison to the known two-quasiparticle structure of $^{254,252}\mathrm{No}$ confirms the existence of the deformed shell gaps at $N=152$ and $Z=100$.

PhysicsNuclear and High Energy PhysicsShell (structure)Structure (category theory)Order (ring theory)medicine.anatomical_structureQuality (physics)medicineNeutronAtomic physicsNuclear ExperimentNucleusExcitationSpin-½Physical Review C
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Isomer-tagged differential-plunger measurements in proton-unbound 144Ho

2010

The lifetime of an excited state above a weakly populated isomer in the proton-unbound odd-odd nucleus 144Ho has been measured using the recoil distance Doppler shift method. This measurement represents the first differential-plunger lifetime measurement to utilize recoil-isomer tagging. The first excited I[pi]=(10+) state above the two-quasiparticle [pi]h11/2[circle times operator][nu]h11/2(8+) isomer was determined to have a lifetime of [tau]=6(1)�ps. Potential energy surface calculations, based on the configuration-constrained blocking method, predict the isomeric state to have [gamma]-soft triaxial-nuclear shape with [gamma][approximate]24�. The lifetime of the (10+) state can be unders…

PhysicsNuclear and High Energy PhysicsProton010308 nuclear & particles physicsOperator (physics)Quantum number01 natural sciencesRecoilExcited state0103 physical sciencesPotential energy surfaceQuasiparticleAtomic physics010306 general physicsSpin (physics)Physics Letters B
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Competing Decay Modes of a High-spin Isomer in the Proton-unbound Nucleus $^{158}$Ta

2015

An isomeric state at high spin and excitation energy was recently observed in the proton-unbound nucleus 158Ta. This state was observed to decay by both α and γ decay modes. The large spin change r ...

PhysicsDecay schemeta114ProtontantalumBranching fractionisomeric statesGeneral Physics and Astronomymedicine.anatomical_structureDouble beta decaymedicineAtomic physicsNuclear ExperimentNucleusExcitationSpin-½Acta Physica Polonica B
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Decay of the high-spin isomer in 160Re: Changing single-particle structure beyond the proton drip line

2011

WOS: 000286708700015

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonta114Gas-filled recoil separator Si and Ge strip detectorsNUCLEAR REACTIONS Ni-58+Cd-106 at 290300 MeV beam energy enriched targetsMeasured E gamma t1/2ParticleNeutronNuclear reactionsAtomic physicsProton emissionGround stateMeasuredLine (formation)Spin-½Physics Letters B
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Lifetime measurements and shape coexistence inDy144

2010

The known level scheme of {sup 144}Dy has been extended and lifetime measurements have been made with the recoil-distance Doppler-shift method. Reduced transition probabilities and deformations have been determined for four low-lying transitions. These states form part of the first observed band crossing, giving information on the change in nuclear deformation resulting from the rearrangement of h{sub 11/2} protons in the nucleus. Two bands built upon excited 10{sup +} states have been assigned pi(h{sub 11/2}){sup 2} prolate and nu(h{sub 11/2}){sup -2} oblate configurations with tau=12(2)ps and 0.01<tau < or approx. 16ns, respectively. These long lifetimes are reasoned to be a result of sha…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsBranching fractionHadron01 natural sciencesDipoleExcited state0103 physical sciencesAtomic physics010306 general physicsSpin (physics)NucleonMagnetic dipoleDimensionless quantityPhysical Review C
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Transition probability studies in175Au

2013

Transition probabilities have been measured between the low-lying yrast states in 175Au by employing the recoil distance Doppler-shift method combined with the selective recoil-decay tagging technique. Reduced transition probabilities and magnitudes of transition quadrupole moments have been extracted from measured lifetimes allowing dramatic changes in nuclear structure within a low excitation-energy range to probed. The transition quadrupole moment data are discussed in terms of available systematics as a function of atomic number and aligned angular momentum.

HistoryAngular momentumChemistryYrastNuclear structureFunction (mathematics)Computer Science ApplicationsEducationRecoilQuadrupoleRange (statistics)Physics::Atomic PhysicsAtomic numberAtomic physicsJournal of Physics: Conference Series
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Blurring the Boundaries: Decays of Multiparticle Isomers at the Proton Drip Line

2014

A multiparticle spin-trap isomer has been discovered in the proton-unbound nucleus Ta85 73158. The isomer mainly decays by γ-ray emission with a half-life of 6.1(1) μs. Analysis of the γ-ray data shows that the isomer lies 2668 keV above the known 9+ state and has a spin 10 higher and negative parity. This 19- isomer also has an 8644(11) keV, 1.4(2)% α-decay branch that populates the 9+ state in Lu154. No proton-decay branch from the isomer was identified, despite the isomer being unbound to proton emission by 3261(14) keV. This remarkable stability against proton emission is compared with theoretical predictions, and the implications for the extent of observable nuclides are considered. © …

PhysicsGeneral Physicsta114Astrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyObservableParity (physics)total data readoutmedicine.anatomical_structurePhysics::Atomic and Molecular Clustersmedicinegreat spectrometerAlpha decayNuclidePhysics::Chemical PhysicsAtomic physicsProton emissionNuclear ExperimentNucleusPhysical Review Letters
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Competing quasiparticle configurations in W-163

2010

WOS: 000274002700019

PhysicsNuclear and High Energy PhysicsIsotopeNeutron emissionStable isotope ratioExcited stateQuasiparticleParity (physics)NuclideAtomic physics[0-Belirlenecek]Radioactive decay
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Single-particle and collective excitations in the transitional nucleus 166Os

2021

The mean lifetimes of the lowest energy 2(+), 8(+) and 9(-) states in Os-166 have been measured using the recoil distance Doppler-shift method in conjunction with a selective recoil-decay tagging t ...

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsConjunction (astronomy)01 natural sciencesmedicine.anatomical_structureRecoil0103 physical sciencesQuasiparticlemedicineParticlePhysics::Atomic PhysicsAtomic physicsNuclear Experiment010306 general physicsNucleusEnergy (signal processing)Journal of Physics G: Nuclear and Particle Physics
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Lifetime measurements probing triple shape coexistence in ^{175}Au

2011

Lifetimes of the low-lying excited states in the very neutron-deficient nucleus ${}^{175}$Au have been measured by the recoil-distance Doppler-shift method using $\ensuremath{\gamma}$-ray spectra obtained with the recoil-decay tagging technique. Transition quadrupole moments and reduced transition probabilities extracted for this odd-$Z$ nucleus indicate the existence of three different shapes and the competition between collective and noncollective structures.

PhysicsNuclear and High Energy Physicsmedicine.anatomical_structureta114Excited stateNuclear TheoryQuadrupolemedicinePhysics::Atomic PhysicsAtomic physicsNuclear ExperimentNucleusSpectral linePhysical Review C
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Low-lying excited states in the neutron-deficient isotopes163Os and165Os

2013

Excited states in the neutron-deficient isotopes Os-163 and Os-165 were identified using the JUROGAM and GREAT spectrometers in conjunction with the RITU gas-filled separator. The Os-163 and Os-165 nuclei were populated via the Cd-106(Ni-60,3n) and Mo-92(Kr-78,2p3n) reactions at bombarding energies of 270 MeV and 357 MeV, respectively. Gamma-ray emissions from these nuclei have been established unambiguously using the recoil-decay tagging technique and a coincidence analysis has allowed level schemes to be established. These results suggest that the yrast states are based upon negative-parity configurations originating from the f(7/2) and h(9/2) orbitals.

Nuclear physicsPhysicsNuclear and High Energy PhysicsSpectrometerIsotopeAtomic orbitalExcited stateYrastNuclear TheoryNeutronAtomic physicsNuclear ExperimentCoincidencePhysical Review C
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α-Decay branching ratios measured by γ-ray tagging

2008

Abstract The nuclides 168–170Pt were produced by bombarding isotopically enriched 92,94Mo targets with 336, 348 MeV 78Kr ions. Prompt γ rays were detected at the target position and provided a selection criterion for the 168–170Pt nuclei. This technique enables the problem of the background from higher-energy α decays in the spectrum to be circumvented. The Pt nuclei were separated in flight using the gas-filled separator RITU and implanted into the GREAT spectrometer, which was used to study subsequent α decays. The α -decay branching ratios of 164–166Os were deduced from the fraction of selected 168–170Pt nuclei correlated with α decays of 164–166Os. The resulting branching ratios agree w…

PhysicsNuclear reactionNuclear and High Energy PhysicsIsotopeBranching fractionNuclideAlpha decayAtomic physicsInstrumentationRadioactive decayCharged particleSpectral lineNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Discovery of the proton emitting nucleus $^{159}$Re

2007

Fund. para Cienc. Tecnol., FCT, Minist. Cienc. Tecnol.;Fundacao Calouste Gulbenkian;Fundacao Luso-Americana

Si detectorsnuclear spinMeasured E pProtonHadron02 engineering and technologyrhenium[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNuclear physicsIsotopes of cadmium0202 electrical engineering electronic engineering information engineeringnuclei with mass number 150 to 189Enriched targetsradioactive decay periodsNuclideIsotopeChemistryNuclear structure020206 networking & telecommunicationsT1/213. Climate action020201 artificial intelligence & image processing23.50.+z; 27.70.+q; 21.10.Tg; 21.10.HwGas-filled recoil separatorNucleonRadioactive decayNuclear reactions 58Ni + 106Cd at 300 MeV beam energyproton emission decay
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Excited states in the proton-unbound nuclide Ta-158

2016

Excited states in the neutron-deficient odd-odd proton-unbound nuclide $^{158}\mathrm{Ta}$ have been investigated in two separate experiments. In the first experiment, $^{166}\mathrm{Ir}$ nuclei were produced in the reactions of 380 MeV $^{78}\mathrm{Kr}$ ions with an isotopically enriched $^{92}\mathrm{Mo}$ target. The $\ensuremath{\alpha}$-decay chain of the ${9}^{+}$ state in $^{166}\mathrm{Ir}$ was analyzed. Fine structure in the $\ensuremath{\alpha}$ decay of the ${9}^{+}$ state in $^{162}\mathrm{Re}$ established a 66 keV difference in excitation energy between the lowest-lying ${9}^{+}$ and ${10}^{+}$ states in $^{158}\mathrm{Ta}$. Higher-lying states in $^{158}\mathrm{Ta}$ were popul…

Physicsta114Protontantalum010308 nuclear & particles physics01 natural sciencesIonExcited state0103 physical sciencesGamma spectroscopyNuclideProton emissionAtomic physicsNuclear Experiment010306 general physicsexcited statesEnergy (signal processing)Excitation
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Mass-140 isomers near the proton dripline

2005

An experiment has been performed in Jyvaskyla, Finland, using Jurogam in conjunction with RITU and GREAT. This experiment populated several extremely neutron-deficient nuclei around the mass-140 region of the nuclei chart, using the 92Mo(54Fe, α2n) reaction at 245 MeV. Analysis of these data has revealed several previously unobserved isomeric states, in several nuclei. One of these has been assigned to 143Dy with a half-life of 1.2 ± 0.3 µs. The energies of the prompt γ rays in the band built upon the isomer are in agreement with those previously observed.

PhysicsNuclear physicsNuclear and High Energy PhysicsProtonNeutronmacromolecular substancesJournal of Physics G: Nuclear and Particle Physics
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Spectroscopy of193Bi

2014

An experiment aiming to study the shape coexistence in 193Bi has been performed at the Accelerator laboratory of the University of Jyväskylä, Finland (JYFL). Many new states have been found, hugely extending the previously known level scheme of 193Bi. The Iπ=292+${I^\pi } = {{{29} \over 2}^ + }$ member of the πi13/2 band de-excites also to the previously, only tentatively placed long-lived isomeric state. This link determines the energy of the isomeric state to be 2260(1) keV and suggests a spin and parity of (272+)$\left( {{{{{27} \over 2}}^ + }} \right)$. The half-life of the isomeric state was measured to be 84.4(6) µs. A level structure on top of this isomeric state was constructed. How…

Physicsta114IsotopePhysicsQC1-999Level structureParity (physics)Statistical physicsAtomic physicsSpectroscopyEPJ Web of Conferences
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Identification of Excited States in theTz=1NucleusXe110: Evidence for Enhanced Collectivity near theN=Z=50Double Shell Closure

2007

Gamma-ray transitions have been identified for the first time in the extremely neutron-deficient (N=Z+2) nucleus {sup 110}Xe, and the energies of the three lowest excited states in the ground-state band have been deduced. The results establish a breaking of the normal trend of increasing first excited 2{sup +} and 4{sup +} level energies as a function of the decreasing neutron number as the N=50 major shell gap is approached for the neutron-deficient Xe isotopes. This unusual feature is suggested to be an effect of enhanced collectivity, possibly arising from isoscalar n-p interactions becoming increasingly important close to the N=Z line.

PhysicsIsotopeIsoscalarNuclear TheoryShell (structure)General Physics and Astronomymedicine.anatomical_structureNeutron numberExcited statemedicineNeutronAtomic physicsNucleusLine (formation)Physical Review Letters
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Lifetimes of odd-spin yrast states inHg182

2010

Lifetimes of excited states in $^{182}\mathrm{Hg}$ were extracted from recoil-gated $\ensuremath{\gamma}$-ray spectra and recoil-gated $\ensuremath{\gamma}\ensuremath{\gamma}$-coincidence matrices using the recoil distance Doppler-shift method. States were populated using the $^{96}\mathrm{Mo}$($^{88}\mathrm{Sr}$,$2n$)$^{182}\mathrm{Hg}$ fusion-evaporation reaction. Measured lifetimes allowed transition probabilities, transition quadrupole moments, quadrupole deformation parameters, and transition dipole moments to be deduced for the band formed by the odd-spin yrast states. The experimental results confirm the low degree of octupole collectivity in this mass region.

PhysicsNuclear reactionNuclear and High Energy PhysicsDegree (graph theory)010308 nuclear & particles physicsYrast01 natural sciencesSpectral lineDipoleExcited state0103 physical sciencesQuadrupolePhysics::Atomic PhysicsAtomic physics010306 general physicsSpin (physics)Physical Review C
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Nuclear levels in proton-unboundI109: Relative single-particle energies beyond the proton drip line

2007

A level scheme has been constructed for the proton-unbound, T-z=3/2 nuclide I-109(53)56 following a recoil-decay-tagging experiment using the Ni-58(Fe-54, p2n gamma) reaction at a beam energy of 19 ...

PhysicsNuclear physicsNuclear and High Energy PhysicsIsotopeProtonNuclear structureGamma spectroscopyNuclideNuclear ExperimentSpectroscopyRadioactive decayLine (formation)Physical Review C
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Coulomb shifts and shape changes in the mass 70 region

2007

The technique of recoil beta tagging has been developed which allows prompt gamma decays in nuclei from excited states to be correlated with electrons from their subsequent short-lived beta decay. This technique is ideal for studying nuclei very far from stability and improves in sensitivity for very short-lived decays and for high decay Q-values. The method has allowed excited states in 78Y to be observed for the first time, as well as an extension in the knowledge of T=1 states in 74Rb. From this new information it has been possible to compare Coulomb energy differences (CED) between T=1 states in 70Br/70Se, 74Rb/74Kr, and 78Y/78Sr. The A=70 CED exhibit an anomalous behavior which is inco…

PhysicsNuclear and High Energy PhysicsGamma rayNuclear structureFOS: Physical sciencesElectronRecoilExcited stateDouble beta decayCoulombSensitivity (control systems)Atomic physicsNuclear Experiment (nucl-ex)Nuclear Experiment
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Comparison of gamma-ray coincidence and low-background gamma-ray singles spectrometry

2011

Aerosol samples have been studied under different background conditions using gamma-ray coincidence and low-background gamma-ray singles spectrometric techniques with High-Purity Germanium detectors. Conventional low-background gamma-ray singles counting is a competitive technique when compared to the gamma-gamma coincidence approach in elevated background conditions. However, measurement of gamma-gamma coincidences can clearly make the identification of different nuclides more reliable and efficient than using singles spectrometry alone. The optimum solution would be a low-background counting station capable of both singles and gamma-gamma coincidence spectrometry.

Astrophysics::High Energy Astrophysical Phenomena[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]010403 inorganic & nuclear chemistryMass spectrometry01 natural sciencesComprehensive Nuclear-Test-Ban TreatyCoincidence030218 nuclear medicine & medical imagingNuclear physics03 medical and health sciences0302 clinical medicineBackground RadiationAir Pollution RadioactiveNuclideGamma ray spectrometryBackground radiationNuclear PhysicsPhysicsAerosolsRadiation surveillanceRadiationta114GermaniumGamma rayGamma-ray spectrometry0104 chemical sciencesSpectrometry GammaGamma Rays22Na
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Evidence for enhanced collectivity in Te-I-Xe nuclei near the N = Z = 50 double shell closure

2007

Gamma‐ray transitions have been identified for the first time in the extremely neutron‐deficient Tz = 1 nuclide 110Xe and the energies of the three lowest excited states in the ground‐state band have been deduced. A level scheme has also been constructed for the proton‐unbound, Tz = 3/2 nuclide 109I, exhibiting band structures built on g7/2 and h11/2 states in a weakly deformed, triaxial nucleus. In addition, a third band is proposed to be built on a g7/2 orbital coupled to an octupole‐vibrational phonon of the 108Te core. The results were obtained in a recoil‐decay tagging experiment using the 58Ni(54Fe,2n/p2n) reaction at a beam energy of 195 MeV. The experiment was performed using the hi…

PhysicsSpectrometerPhononNeutron numberExcited stateNeutronGamma spectroscopyNuclideAtomic physicsNuclear ExperimentRadioactive decayAIP Conference Proceedings
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Isomer spectroscopy in254No

2006

Isomeric states in No-254 were investigated using a calorimetric method. Two different isomers were found with half-lives of T-1/2 = 266 +/- 2 ms and T-1/2 = 184 +/- 3 mu s, respectively. The domin ...

CrystallographyChemistryCondensed Matter PhysicsSpectroscopyMathematical PhysicsAtomic and Molecular Physics and OpticsPhysica Scripta
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Spectroscopy of the neutron-deficient isobars 163 Re and 163 W using tagging techniques

2008

Bozok University;Erciyes University;et al.;Istanbul University;Nigde University;The Turkish Atomic Energy Authority (TAEK)

PhysicsNuclear Reactions 60 Ni+ 106 Cd at 270 MeV beam energy enriched targetsSpectrometerProtonYrastNuclear TheorySegmented Si and Ge detectorsNeutron spectroscopyNuclear physicsMeasured E ?IsobarNeutronGasfilled recoil separatorNuclear ExperimentGround stateRadioactive decay
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Discovery of 157W and 161Os

2010

The nuclides W-157 and Os-161 have been discovered ill reactions of Ni-58 ion beams with a Cd-106 target. The Os-161 alpha-decay energy and half-life were 6890 +/- 12 keV and 640 +/- 60 mu s. The d ...

Nuclear physicsPhysicsNuclear reactionNuclear and High Energy PhysicsIsotopeBranching fractionNeutronNuclideAlpha decayAtomic physicsRadioactive decayIonPhysics Letters B
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Spectroscopy of the neutron-deficient nucleusOs16791

2009

Excited states of the nucleus Os-167 have been populated by the reaction Mo-92(Kr-78,2pn). The JUROGAM gamma-ray detector array has been used in conjunction with the RITU gas-filled separator and the GREAT spectrometer to observe prompt gamma rays in coincidence with recoiling fusion-evaporation residues and their subsequent decay by alpha particle emission. By correlating prompt gamma radiation with the characteristic alpha radioactivity of Os-167, it has been possible to extend the level scheme for this nucleus significantly. In particular, an extension of the yrast band and four previously unobserved bands are reported. In addition, the recoil distance Doppler-shift method was used to de…

Nuclear reactionPhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaYrastGamma rayAlpha particleNuclear physicsmedicine.anatomical_structureExcited statemedicineGamma spectroscopyNeutronAtomic physicsNuclear ExperimentNucleusPhysical Review C
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ANDES Measurements for Advanced Reactor Systems

2013

Abstract A significant number of new measurements was undertaken by the ANDES “Measurements for advanced reactor systems” initiative. These new measurements include neutron inelastic scattering from 23 Na, Mo, Zr, and 238 U, neutron capture cross sections of 238 U, 241 Am, neutron induced fission cross sections of 240 Pu, 242 Pu, 241 Am, 243 Am and 245 Cm, and measurements that explore the limits of the surrogate technique. The latter study the feasibility of inferring neutron capture cross sections for Cm isotopes, the neutron-induced fission cross section of 238 Pu and fission yields and fission probabilities through full Z and A identification in inverse kinematics for isotopes of Pu, Am…

Nuclear reactionPhysicsNuclear and High Energy Physicsta114FissionNuclear dataFission product yieldInelastic scattering[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNuclear physicsNeutron captureNeutronNuclear ExperimentDelayed neutron
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Probing the limit of nuclear existence: Proton emission from 159Re

2006

WOS: 000240847400007

Nuclear reactionNuclear and High Energy PhysicsSi detectorsProtonNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]measured E (p) (t)1 / 201 natural sciences7. Clean energyNuclear physicsEp0103 physical sciencesEnriched targetsNeutronNuclideProton emissionNuclear Experiment010306 general physics106Cd at 300 MeV beam energyPhysicsIsotope010308 nuclear & particles physics21.10.Hw; 21.10.Tg; 23.50.+z; 27.70.+q58Nit1/2NUCLEAR REACTIONS Ni-58+Cd-106 at 300 MeV beam energy13. Climate actionNuclear reactionsGas-filled recoil separatorAtomic physicsNucleonMeasuredRadioactive decayPhysics Letters B
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Precision measurements of proton emission from the ground states ofTa156andRe160

2011

The decays of the $\ensuremath{\pi}{d}_{3/2}$ ground states of $^{156}\mathrm{Ta}$ and $^{160}\mathrm{Re}$ have been studied in detail using the GREAT spectrometer. More than 7000 $^{160}\mathrm{Re}$ nuclei were produced in reactions of 290- and 300-MeV $^{58}\mathrm{Ni}$ ions with an isotopically enriched $^{106}\mathrm{Cd}$ target and separated in flight using the RITU separator. The proton and $\ensuremath{\alpha}$ decays of the $\ensuremath{\pi}{d}_{3/2}$ level were confirmed and the half-life and branching ratios of this state were determined with improved precision to be ${t}_{1/2}=611\ifmmode\pm\else\textpm\fi{}7$ $\ensuremath{\mu}$s and ${b}_{\mathrm{p}}=89\ifmmode\pm\else\textpm\fi…

PhysicsNuclear and High Energy PhysicsProtonBranching fractionHadronElementary particleAlpha decayAtomic physicsNucleonGround stateDimensionless quantityPhysical Review C
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Lifetimes of intruder states in 186Pb, 188Pb and 194Po

2008

Abstract Lifetimes of prolate intruder states in 186Pb and 188Pb and oblate intruder states in 194Po have been determined through recoil distance Doppler-shift lifetime measurements. Deformation parameters of | β 2 | = 0.29 ( 5 ) and | β 2 | = 0.17(3) have been extracted from experimental B ( E 2 ) values for the prolate and the oblate bands, respectively. The present study addresses the phenomenon of shape coexistence typical for the nuclei near Z = 82 and N = 104 , providing information on configuration mixing of intrinsic structures of the nuclei of interest. The results are compared with the available lifetime data and theoretical results for neutron-deficient Po, Pb, Hg and Pt nuclei. …

Nuclear reactionPhysicsNuclear and High Energy Physics21.10.Tg; 23.20.Lv; 27.70.+q; 27.80.+wquadrupole moment[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]010308 nuclear & particles physics114Cd(83Kr 3n)Prolate spheroid7. Clean energy01 natural sciencesdeformation parametersE=340–375 MeVRecoil108Pd106Pd0103 physical sciencesQuadrupoleOblate spheroidDeformation (engineering)Atomic physics010306 general physicsnuclear reactionsMixing (physics)
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γ-ray spectroscopy approaching the limits of existence of atomic nuclei: A study of the excited states ofPt168andPt169

2009

Excited states in the $N=90$ and $N=91$ Pt nuclei have been investigated using the JUROGAM and GREAT spectrometers in conjunction with the RITU gas-filled separator. These nuclei were populated via the reactions $^{92}\mathrm{Mo}(^{78}\mathrm{Kr},2n)$ and $^{94}\mathrm{Mo}(^{78}\mathrm{Kr},3n)$ at 335 and 348 MeV, respectively. The recoil-decay tagging technique has been used to correlate prompt $\ensuremath{\gamma}$ radiation with the characteristic $\ensuremath{\alpha}$ decays of $^{168}\mathrm{Pt}$ and $^{169}\mathrm{Pt}$. A $\ensuremath{\gamma}\text{\ensuremath{-}}\ensuremath{\gamma}$ analysis has allowed a level scheme for $^{168}\mathrm{Pt}$ to be reported for the first time and the l…

PhysicsNuclear reactionNuclear and High Energy PhysicsNeutron emissionYrastExcited stateAtomic nucleusGamma spectroscopyAlpha decayAtomic physicsInteracting boson modelPhysical Review C
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Nuclear isomers in superheavy elements as stepping stones towards the island of stability

2006

The stability of an atomic nucleus is determined by the outcome of a tug-of-war between the attractive strong nuclear force and the repulsive electrostatic force between the protons in the nucleus. If 100 protons and about 150 neutrons or more are assembled into a nucleus, the repulsion usually becomes dominant and causes the nucleus to fission. For certain 'magic numbers' of protons and neutrons this repulsion can be overcome and the nucleus stabilized. In particular an 'island of stability' is predicted beyond the actinides, where long-lived or even stable superheavy elements can exist, but its precise limits are unknown. Experiments can help determine where this island lies, however. Spe…

Multidisciplinary010308 nuclear & particles physicsChemistryFermiumNuclear TheoryStrong interactionchemistry.chemical_element01 natural sciences7. Clean energyIsland of stabilityNuclear physics0103 physical sciencesAtomic nucleusNuclear fusionNeutronNobeliumAtomic numberAtomic physicsNuclear Experiment010306 general physicsNature
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High-Kfour-quasiparticle states inGd138

2011

States above the known ${K}^{\ensuremath{\pi}}={8}^{\ensuremath{-}}$ 6 $\ensuremath{\mu}$s isomer in $^{138}\mathrm{Gd}$ have been populated with the $^{106}\mathrm{Cd}$($^{36}\mathrm{Ar}$,$2p2n$) reaction at a beam energy of 180 MeV at the University of Jyv\"askyl\"a, Finland. The recoil-isomer tagging technique was utilized to correlate delayed $\ensuremath{\gamma}$-ray decays, detected in the GREAT focal plane spectrometer, with prompt decays measured in the JUROGAM II spectrometer at the target position. The lifetime of the ${K}^{\ensuremath{\pi}}={8}^{\ensuremath{-}}$ isomeric state has been remeasured as 6.2(2) $\ensuremath{\mu}$s. Two high-lying strongly coupled bands have been estab…

PhysicsNuclear reactionNuclear and High Energy PhysicsNeutron emissionLandé g-factorQuasiparticleState (functional analysis)Atomic physicsRadioactive decayHigh-κ dielectricDimensionless quantityPhysical Review C
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Spectroscopy ofHo144using recoil-isomer tagging

2010

Excited states in the proton-unbound odd-odd nucleus $^{144}\mathrm{Ho}$ have been populated using the $^{92}\mathrm{Mo}(^{54}\mathrm{Fe},\mathit{pn})^{144}\mathrm{Ho}$ reaction and studied using the recoil-isomer-tagging technique. The alignment properties and signature splitting of the rotational band above the ${I}^{\ensuremath{\pi}}=({8}^{+})^{144m}\mathrm{Ho}$ isomer have been analyzed and the isomer confirmed to have a $\ensuremath{\pi}{h}_{11/2}\ensuremath{\bigotimes}\ensuremath{\nu}{h}_{11/2}$ two-quasiparticle configuration. The configuration-constrained blocking method has been used to calculate the shapes of the ground and isomeric states, which are both predicted to have triaxia…

PhysicsRare earth nucleiNuclear and High Energy PhysicsRecoilExcited stateHadronElementary particleFermionAtomic physicsNucleonSpectroscopyPhysical Review C
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The new vacuum-mode recoil separator MARA at JYFL

2008

Abstract A new vacuum-mode recoil separator MARA (Mass Analysing Recoil Apparatus) is under design and construction at the Department of Physics in the University of Jyvaskyla. The separator is intended to separate reaction products from the primary beam in mass region below A = 150 . The ion-optical configuration of the separator will be QQQDEDM, where a magnetic quadrupole (Q) triplet is followed by an electrostatic deflector (DE) and a magnetic dipole (DM). The total length of MARA will be less than 7.0 m and the first order resolving power more than 250 for a beam spot size of 2 mm. In this contribution the main properties of MARA are given and results from simulations are shown.

Nuclear physicsNuclear and High Energy PhysicsRecoilChemistrySeparator (oil production)Quadrupole magnetFirst orderInstrumentationMagnetic dipoleRecoil separatorNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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The influence of quasineutron configurations on 161Ta and nearby odd-A Nuclei

2011

Several strongly coupled bands in the neutron‐deficient nucleus 161Ta have been identified and quasiparticle configuration assignments have been made on the basis of rotational alignments and cranked shell model calculations. The level scheme elucidated for 161Ta highlights the competition between the ν(h9/2) and ν(i13/2) orbitals to form the yrast spectrum. The band structures in 161Ta also provide new insights into the structural features of other heavy odd‐A nuclei populated with much lower reaction cross sections in this region at the proton drip line.

PhysicsProtonta114YrastNuclear TheoryNuclear structuremedicine.anatomical_structureAtomic orbitalQuasiparticlemedicineNeutronAtomic physicsNuclear ExperimentNucleusLine (formation)AIP Conference Proceedings
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Identification of new transitions feeding the high-spin isomers in $^{139}$Nd and $^{140}$Nd nuclei

2013

The population of the high-spin isomers in 139Nd and 140Nd was investigated using the 96Zr(48Ca,xn) reaction and the JUROGAM + RITU + GREAT setup employing the recoil decay tagging technique. Three transitions feeding the 23/2+ isomer in 139Nd and two transitions feeding the 20+ isomer in 140Nd were identified. The newly observed transitions allowed the excitation energy of the isomer to be established in 139Nd and to assign configurations to the states and bands deexcited by the observed transitions in both nuclei. peerReviewed

[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ComputingMilieux_MISCELLANEOUSExperimental Nuclear Physics
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Reinvestigation of the excited states in the proton emitter $^{151}$Lu: particle-hole excitations across the $N=Z=64$ subshell

2017

The excited states of the proton emitter $^{151}$Lu were reinvestigated in a recoil-decay tagging experiment at the Accelerator Laboratory of the University of Jyv\"askyl\"a (JYFL). The level scheme built on the ground state of $^{151}$Lu was updated with five new $\gamma$-ray transitions. Large-scale shell model calculations were carried out to interpret the experimental level scheme. It is found that the excitation energies of states above the $27/2^-$ and $23/2^+$ isomeric levels can be sensitive to excitations from $g_{7/2}$ and $d_{5/2}$ to single-particle orbitals above $N=Z=64$.

FOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment
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Decay of a 19(-) isomeric state in Lu-156

2018

A multiparticle spin-trap isomeric state having a half-life of 179(4) ns and lying 2601 keV above the yrast 10(+) state in Lu-156 has been discovered. The Lu-156 nuclei were produced by bombarding isotopically enriched Cd-106 targets with beams of Ni-58 ions, separated in flight using the gas-filled separator RITU and their decays were measured using the GREAT spectrometer. Analysis of the main decay path that populates yrast states observed previously suggests a spin-parity assignment of 19(-) for the isomeric state, which is consistent with isomeric states identified in the N = 85 isotones. Comparison with other decay paths in Lu-156 indicates that the [pi h(11/)(2)(-1) circle times nu h(…

Physical SciencesFysik
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Precision measurements of proton emission from the ground states of 156Ta and 160Re

2011

The decays of the πd3/2 ground states of 156Ta and 160Re have been studied in detail using the GREAT spectrometer. More than 7000 160Re nuclei were produced in reactions of 290- and 300-MeV 58Ni ions with an isotopically enriched 106Cd target and separated in flight using the RITU separator. The proton and α decays of the πd3/2 level were confirmed and the half-life and branching ratios of this state were determined with improved precision to be t1/2=611±7 μs and bp=89±1% and bα=11±1%, respectively. The α-decay branch populated the ground state of 156Ta, allowing improved values for the proton-decay energy and half-life to be obtained (Ep=1011±5 keV; t1/2=106±4 ms). The β decay of this leve…

nuclear physicsydinfysiikka
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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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Shape coexistence at the proton drip-line: First identification of excited states in 180Pb

2010

Excited states in the extremely neutron-deficient nucleus, 180Pb, have been identified for the first time using the JUROGAM II array in conjunction with the RITU recoil separator at the Accelerator Laboratory of the University of Jyvaskyla. This study lies at the limit of what is presently achievable with in-beam spectroscopy, with an estimated cross-section of only 10 nb for the 92Mo(90Zr,2n)180Pb reaction. A continuation of the trend observed in 182Pb and 184Pb is seen, where the prolate minimum continues to rise beyond the N=104 mid-shell with respect to the spherical ground state. Beyond mean-field calculations are in reasonable correspondence with the trends deduced from experiment.

[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]21.60.Ev 23.20.Lv 27.80.+wFOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment
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Reinvestigation of the excited states in the proton emitter 151Lu : Particle-hole excitations across the N=Z=64 subshell

2017

The excited states of the proton emitter 151Lu were reinvestigated in a recoil-decay tagging experiment at the Accelerator Laboratory of the University of Jyväskylä (JYFL). The level scheme built on the ground state of 151Lu was updated with five new γ -ray transitions. Large-scale shell model calculations were carried out in the model space consisting of the neutron and proton orbitals 0g7/2, 1d5/2, 1d3/2, 2s1/2, and 0h11/2 with the optimized monopole interaction in order to interpret the experimental level scheme of 151Lu. It is found that the excitation energies of states above the 27/2− and 23/2+ isomeric levels in 151Lu can be sensitive to excitations from g7/2 and d5/2 to single-parti…

electromagnetic transitionsydinfysiikka
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Spectroscopy of 193Bi

2014

spektroskopiashape coexistence
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Search for fingerprints of tetrahedral symmetry in 156gd

2009

Theoretical predictions suggest the presence of tetrahedral symmetry as an explanation for the vanishing intra-band E2 transitions at the bottom of the odd-spin negative-parity band in 156Gd. The present study reports on experiment performed to address this phenomenon. It allowed to remove certain ambiguouities related to the intra-band E2 transitions in the negative-parity bands, to determine the new inter-band transitions and reduced probability ratios B(E2)/B(E1) and, for the first time, to determine the experimental uncertainties related to the latter observable. peerReviewed

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Evidence for octupole collectivity in 172Pt

2020

Excited states in the extremely neutron-deficient nucleus 172Pt were populated via 96Ru(78Kr,2p) and 92Mo(83Kr,3n) reactions. The level scheme has been extended up to an excitation energy of  ~ 5 MeV and tentative spin-parity assignments up to Iπ = 18+. Linear polarization and angular distribution measurements were used to determine the electromagnetic E1 character of the dipole transitions connecting the positive-parity ground-state band with an excited side-band, firmly establishing it as a negative-parity band. The lowest member of this negative-parity structure was firmly assigned spin-parity 3-. In addition, we observed an E3 transition from this 3- state to the ground state, providing…

Subatomär fysikSubatomic Physicsydinfysiikka
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Search for Fingerprints of Tetrahedral Symmetry in $^{156}Gd$

2008

Theoretical predictions suggest the presence of tetrahedral symmetry as an explanation for the vanishing intra-band E2-transitions at the bottom of the odd-spin negative parity band in $^{156}Gd$. The present study reports on experiment performed to address this phenomenon. It allowed to determine the intra-band E2 transitions and branching ratios B(E2)/B(E1) of two of the negative-parity bands in $^{156}Gd$.

FOS: Physical sciences23.20.En 21.65.-f 21.10.Ma 21.60.-n[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear Experiment
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High-spin intruder band in $^{107}$In

2010

High-spin states in the neutron deficient nucleus $^{107}$In were studied via the $^{58}$Ni($^{52}$Cr, 3p) reaction. In-beam $\gamma$ rays were measured using the JUROGAM detector array. A rotational cascade consisting of ten $\gamma$-ray transitions which decays to the 19/2$^{+}$ level at 2.002 MeV was observed. The band exhibits the features typical for smooth terminating bands which also appear in rotational bands of heavier nuclei in the A$\sim$100 region. The results are compared with Total Routhian Surface and Cranked Nilsson-Strutinsky calculations.

Astrophysics::High Energy Astrophysical PhenomenaNuclear TheoryFOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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