0000000000910641

AUTHOR

A. Jokinen

showing 85 related works from this author

High-precision electron-capture Q value measurement of 111In for electron-neutrino mass determination

2022

A precise determination of the ground state $^{111}$In ($9/2^+$) electron capture to ground state of $^{111}$Cd ($1/2^+$) $Q$ value has been performed utilizing the double Penning trap mass spectrometer, JYFLTRAP. A value of 857.63(17) keV was obtained, which is nearly a factor of 20 more precise than the value extracted from the Atomic Mass Evaluation 2020 (AME2020). The high-precision electron-capture $Q$ value measurement along with the nuclear energy level data of 866.60(6) keV, 864.8(3) keV, 855.6(10) keV, and 853.94(7) keV for $^{111}$Cd was used to determine whether the four states are energetically allowed for a potential ultra-low $Q$-value $\beta^{}$ decay or electron-capture deca…

Nuclear and High Energy PhysicsmassaspektrometriaNeutrino massUltra-low Q valueAstrophysics::High Energy Astrophysical PhenomenaPenning trapneutriinotFOS: Physical sciencesNuclear Experiment (nucl-ex)ydinfysiikkaNuclear ExperimentMass measurementsElectron capturePhysics Letters B
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STUDIES OF 12C USING β-DECAYS

2008

The nuclear structure of states in 12 C have been a subject of interest for both theory and experiment since the early days of nuclear physics. Many open questions remain, especially concerning the existence and properties of 0+ and 2+ states in the triple alpha continuum. A series of experiments have been performed using β-decay of 12 N and 12 B to probe these states. The latest experiment was performed at KVI using an implantation method, measuring the sum energy of the three α-particles directly. Preliminary results from this experiment will be presented.

PhysicsNuclear physicsNuclear and High Energy PhysicsSeries (mathematics)Continuum (design consultancy)Nuclear structureGeneral Physics and AstronomyBeta (velocity)International Journal of Modern Physics E
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Spectroscopy at the drip line: the case of 31Ar

2003

The beta decay of exotic nuclei is directly connected to many different and highly relevant issues. While along the years a hundred of nuclei have been identified as beta delayed proton (β-p) emitters only eight have been found to be β-2p emitters and the β-3p decay mode although energetically allowed has so far not been observed [1].

PhysicsProtonNuclear TheoryPhysics::Accelerator PhysicsAtomic physicsBeta (finance)SpectroscopyBeta decayLine (formation)
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New ion-guide for the production of beams of neutron-rich nuclei between Z=20–28

2005

It has been shown for the first time that quasi- and deep-inelastic reactions can be successfully incorporated into the conventional Ion-Guide Isotope Separator On-Line (IGISOL) technique. This is of particular interest for characterizing the decay properties of refractory elements and is applied to neutron rich nuclei between Z = 20-28. As a first step of this project, the kinematics of quasi- and deep-inelastic reactions, such as {sup 197}Au({sup 65}Cu,X)Y, were studied. Based on these studies, a specialized IGISOL target chamber was designed and built. This chamber was tested in on- and off-line conditions at the Jyvaskyla IGISOL facility. Yields of radioactive, projectile-like species s…

PhysicsNuclear physicsNuclear and High Energy PhysicsIsotopeRefractory metalsNeutronInstrumentationIonSeparator (electricity)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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In-beam test results of the Super-FRS GEM-TPC detector prototype with relativistic uranium ion beam

2023

As an essential part of the Super-FRS particle identification, the GEM-TPC detector in a twin field-cage configuration will provide position information at up to 1 MHz counting rate with a spatial resolution 95 %. This detector is designed to provide particle-beam tracking information of projectiles ranging from protons to uranium. The performance of the GEM-TPC detector in a single field-cage configuration and newly integrated AWAGS readout electronics with a differential output was studied at the FRS for the response to the uranium beam at 850 MeV/u with intensity up to 1000 ions/spill. The result shows that a clusterization algorithm developed for this analysis works properly. The spatia…

clusterizationNuclear and High Energy Physicsilmaisimetsuper-FRStutkimuslaitteettrackingydinfysiikka114 Physical sciencesGEM-TPCInstrumentationFAIRNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Observation of an ultralow- Q -value electron-capture channel decaying to As75 via a high-precision mass measurement

2022

Physical Review C
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Gas-silicon detector telescope for charged particle spectroscopy

1997

Abstract A gas-silicon detector telescope for charged particle spectroscopy has been constructed and tested. The lower detection limits were determined to be 155 keV for protons, 180 keV for deuterons and 350 keV for alpha particles. Typical energy resolution of the telescope measured for beta-delayed protons is 20 keV. Time resolution for the signals of the telescope was measured to be less than 10 ns. Examples of using the detector telescope in detection of beta-delayed proton activities are presented.

PhysicsNuclear and High Energy PhysicsProtonPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaDetectorResolution (electron density)Astrophysics::Instrumentation and Methods for AstrophysicsAlpha particle01 natural sciencesCharged particlelaw.inventionNuclear physicsTelescopeDeuteriumlaw0103 physical sciencesNuclear Experiment010306 general physicsSpectroscopyInstrumentationAstrophysics::Galaxy Astrophysics
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β - and γ -spectroscopy study of Pd119 and Ag119

2022

Physical Review C
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An ion cooler-buncher for high-sensitivity collinear laser spectroscopy at ISOLDE

2008

International audience; A gas-filled segmented linear Paul trap has been installed at the focal plane of the high-resolution separator (HRS) at CERN-ISOLDE. As well as providing beams with a reduced transverse emittance, this device is also able to accumulate the ions and release the sample in bunches with a well-defined time structure. This has recently permitted collinear laser spectroscopy with stable and radioactive bunched beams to be demonstrated at ISOLDE. Surface-ionized 39, 44, 46K and 85Rb beams were accelerated to 30keV, mass separated and injected into the trap for subsequent extraction and delivery to the laser setup. The ions were neutralized in a charge exchange cell and exci…

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhotonIon beam010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Laser01 natural sciences7. Clean energyIonlaw.inventionBuncheslaw0103 physical sciencesPhysics::Accelerator PhysicsThermal emittancePhysics::Atomic PhysicsIon trapAtomic physics010306 general physics
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Two-proton emission in the decay of Ar-31

1998

18 pages, 7 figures, 2 tables.-- PACS nrs.: 23.40.Hc; 27.30.+t.

PhysicsNuclear and High Energy PhysicsRadioactivity Ar-31(beta(+)p) [from Ca(p3pxn) reaction]Be-6Delayed 2-proton emissionNuclear TheoryOn-line mass separationAl-22Measured beta-delayed E-p pp-coinCaO target3-particle decaysNucleiNuclear physicsSystematicsIsobaric processSurface barrier Si detectorsAtomic physicsProton emissionNuclear ExperimentGround stateSpin (physics)Ar-31 deduced beta 2p-decay channels
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Precise half-life measurement of the Si-26 ground state

2008

The beta-decay half-life of 26Si was measured with a relative precision of 1.4*10e3. The measurement yields a value of 2.2283(27) s which is in good agreement with previous measurements but has a precision that is better by a factor of 4. In the same experiment, we have also measured the non-analogue branching ratios and could determine the super-allowed one with a precision similar to the previously reported measurements. The experiment was done at the Accelerator Laboratory of the University of Jyvaskyla where we used the IGISOL technique with the JYFLTRAP facility to separate pure samples of 26Si.

PhysicsNuclear and High Energy PhysicsBranching fraction010308 nuclear & particles physicsFOS: Physical sciencesHalf-life01 natural sciencesNuclear physics0103 physical sciencesRelative precisionNuclear Experiment (nucl-ex)010306 general physicsGround stateNuclear ExperimentNuclear Physics
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Applications of the total absorption technique to improve reactor decay heat calculations: study of the beta decay of [sup 102,104,105]Tc

2009

The decay heat of the fission products plays an important role in predicting the heat‐up of nuclear fuel after reactor shutdown. This form of energy release is calculated as the sum of the energy‐weighted activities of all fission products P(t) = ΣEiλiNi(t), where Ei is the decay energy of nuclide i (gamma and beta component), λi is the decay constant of nuclide i and Ni(t) is the number of nuclide i at cooling time t. Even though the reproduction of the measured decay heat has improved in recent years, there is still a long standing discrepancy at t∼1000 s cooling time for some fuels. A possible explanation for this disagreement can been found in the work of Yoshida et al. [1], who demonst…

Nuclear physicsFission productsIsotopeDecay energyChemistryDouble beta decayNuclideDecay heatExponential decayNuclear ExperimentBeta decayAIP Conference Proceedings
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Studying exotic nuclides close to the N = Z line at the HIGISOL facility

2003

The ion guide [1, 2] for heavy-ion fusion-evaporation reactions (HIGISOL) which was developed by Beraud et al. [3] has been implemented at the IGISOL facility in Jyvaskyla [4]. This system was modified over the past 5 years. Figure 1 shows the present set-up. The HIGISOL takes advantage of the different angular distributions of primary beam and reaction products: the primary beam is stopped in front of the stopping chamber and the reaction products enter the stopping chamber through a thin foil passing the beam stop. This so called “shadow” method removes the plasma effect since the primary beam is not ionising the stopping gas. In order to improve ion optical properties, mainly to reduce t…

PhysicsNuclear physicsDc voltageIon beamPlasma effectSkimmer (machine)NuclideBeam (structure)Line (formation)Ion
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Direct measurement of the mass difference of 72As-72Ge rules out 72As as a promising β-decay candidate to determine the neutrino mass

2021

Preprint of paper published on Physical Review C We report the first direct determination of the ground-state to ground-state electron-capture Q-value for the 72As to 72Ge decay by measuring their atomic mass difference utilizing the double Penning trap mass spectrometer, JYFLTRAP. The Q-value was measured to be 4343.596(75) keV, which is more than a 50-fold improvement in precision compared to the value in the most recent Atomic Mass Evaluation 2020. Furthermore, the new Qvalue was found to be 12.4(40) keV (3.1 σ) lower. With the significant reduction of the uncertainty of the ground-state to ground-state Q-value value combined with the level scheme of 72Ge from γ-ray spectro…

neutriinothiukkasfysiikkamassa (fysiikka)ydinfysiikka
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Results of DTAS Campaign at IGISOL : Overview

2023

The β decays of more than twenty fission fragments were measured in the first experiments with radioactive-ion beams employing the Decay Total Absorption γ-ray Spectrometer. In this work, we summarize the main results obtained so far from this experimental campaign carried out at the Ion Guide Isotope Separator On-Line facility. The advances introduced for these studies represent the state-of-the-art of our analysis methodology for segmented spectrometers. peerReviewed

spektrometriatutkimuslaitteetspektrometritGeneral Physics and Astronomyydinfysiikka
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Single-Neutron States inS133n

1996

The location of several single-neutron states in ${}^{133}\mathrm{Sn}$ has been identified. The ${p}_{3/2}$, ${h}_{9/2}$, and ${f}_{5/2}$ states were found at 853.7, 1560.9, and 2004.6 keV, respectively, by measuring $\ensuremath{\gamma}$ rays in coincidence with delayed neutrons following the decay of ${}^{134}\mathrm{In}$. Crucial for obtaining the new data were the improved yields at the mass-separator facility ISOLDE-PSB at CERN. A semiempirically adjusted Woods-Saxon calculation, based on parameters from the Pb region and normalized on the mass data at ${}^{132}\mathrm{Sn}$, reproduces the new single particle energies with good precision.

PhysicsNuclear physicsParticle physicsLarge Hadron ColliderGeneral Physics and AstronomyParticleNeutronDelayed neutronCoincidencePhysical Review Letters
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Production of radioactive Ag ion beams with a chemically selective laser ion source

1997

Abstract We have developed a chemically selective laser ion source at the CERN-ISOLDE facility in order to study neutron-rich Ag nuclides. A pulsed laser system with high repetition rate has been used based on high-power coppe-vapour pump lasers and dye lasers. With this source significant reductions of the isobaric background has been achieved.

Nuclear and High Energy PhysicsDye laserIon beamChemistryNuclear TheoryRadiochemistryPhysics::OpticsLaserIon sourceIonlaw.inventionIon beam depositionlawPhysics::Accelerator PhysicsIsobaric processPhysics::Atomic PhysicsNuclideNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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β-decay half-life of70Kr: A bridge nuclide for therpprocess beyondA=70

2000

The -decay half-life of 70 Kr has been measured for the first time at the ISOLDE PSB Facility at CERN. Mass separated 70 Kr ions were produced by 1 GeV proton induced spallation reactions in a Nb foil. The measured half-life is 57(21) ms. This value is consistent with the half-life calculated assuming a pure Fermi decay, but is clearly lower than the value used in a recent rp-process reaction flow calculation. The result shows that the reaction flow via two-proton-capture of 68 Se is 2.5 times faster than previously calculated assuming an astrophysical temperature of 1.5 GK and a density of 10 6 g/cm 3 .

PhysicsNuclear and High Energy PhysicsDecay schemeProton010308 nuclear & particles physicsHalf-liferp-process01 natural sciences7. Clean energyBeta decayNuclear physicsDouble beta decay0103 physical sciencesSpallationNuclideAtomic physics010306 general physicsPhysical Review C
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High-statistics measurement of the β-delayed α spectrum of 20Na

2013

A measurement of the 20Na β-delayed alpha spectrum with a high-granularity setup has allowed the decay scheme to be revised on several points. Three new transitions of low intensity are found at low α -particle energy. An R-matrix fit of the complete spectrum gives an improved description of the decay and indicates feeding to the broad 2+ α-cluster state close to 9MeV. c Societa Italiana di Fisica / Springer-Verlag 2013

PhysicsNuclear and High Energy PhysicsParticle and Nuclear PhysicsDecay schemeNuclear Fusion010308 nuclear & particles physicsSpectrum (functional analysis)FOS: Physical sciencesAlpha (ethology)01 natural sciencesIntensity (physics)Computational physics20Na0103 physical sciencesNuclear Physics Heavy Ions HadronsBeta (velocity)Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentEnergy (signal processing)
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Fine structure in the beta-delayed proton decay of 33Ar

1996

9 pages, 2 figures, 2 tables.-- PACS nrs.: 21.60.Cs; 23.40.−s; 27.30.+t; 29.30.Ep.

PhysicsMeasured beta-delayed protons Ep IpNuclear and High Energy PhysicsDeduced relative spectroscopic amplitudesAr-33 (from 1 GeV p on Nb-foil target selective mass separation)Proton decaySHELL modelShell nucleiShell-model calculationGas-Si telescope spectrometerShell modelEmissionBeta-delayed proton decayAmplitudeAtomic orbitalExcited stateBeta (plasma physics)Nuclear Physics - ExperimentAtomic physicsNuclear Physics A
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Off-line commissioning of the ISOLDE cooler

2007

International audience; Among the multiple progresses in radioactive ion beam (RIB) manipulation for physics experiments, the beam cooling and bunching in gas-filled RF traps has become a widely used technique. It is particularly well adapted to precision experiments, such as Penning trap mass spectrometry or collinear laser spectroscopy. At ISOLDE, an rf quadrupole cooler and ion buncher (RFQCB) has been designed and developed to deliver radioactive beams of improved quality among most of the on-line experiments. The results of the first off-line tests have shown that high transmission efficiencies could be achieved with different RIBs of alkali metals, as it was expected. During the later…

Nuclear and High Energy PhysicsRFQCBIon beam010308 nuclear & particles physicsChemistryNuclear engineering[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryPenning trap01 natural sciencesIon trappingISOLDEIonNuclear physicsEmittance0103 physical sciencesQuadrupoleTransmissionThermal emittance37.10.Rs; 37.10.Ty; 29.27.Eg010306 general physicsInstrumentationBeam (structure)
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Influences on the triple alpha process beyond the Hoyle state

2010

7 pags., 3 figs. -- International Symposium on Nuclear Astrophysics - Nuclei in the Cosmos - IX, 25-30 June 2006, CERN

Nuclear physicsPhysicsParticle physicsAstrophysics and AstronomyLarge Hadron ColliderNuclear astrophysicsState (functional analysis)Triple-alpha process
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Independent and cumulative yields of very neutron-rich nuclei in 20 MeVp- and 18–41 MeVd-induced fission ofU238

1991

Independent and cumulative yields in nearly symmetric fission have been measured for the first time by bombarding $^{238}\mathrm{U}$ with 20-MeV protons and with 18-, 25-, and 41-MeV deuterons. Isobaric charge dispersion has been determined in the A=110, A=112, and A=114 mass chains and, from asymmetric fission, in the A=80 mass chain. The average isobaric charges in the p+U reaction were 44.01\ifmmode\pm\else\textpm\fi{}0.20 (A=110), 45.15\ifmmode\pm\else\textpm\fi{}0.15 (A=112), and 45.74\ifmmode\pm\else\textpm\fi{}0.15 (A=114). The widths (standard deviations) of the charge dispersion curves were 0.82\ifmmode\pm\else\textpm\fi{}0.08 (A=112) and 0.54\ifmmode\pm\else\textpm\fi{}0.08 (A=114…

Nuclear reactionPhysicsNuclear and High Energy PhysicsIsotopes of germanium010308 nuclear & particles physicsQ valueFissionOrder (ring theory)Charge (physics)7. Clean energy01 natural sciencesNuclear physicsIsotopes of palladium0103 physical sciencesNeutronAtomic physics010306 general physicsPhysical Review C
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Odd-odd neutron-rich rhodium isotopes studied with the double Penning trap JYFLTRAP

2022

Precision mass measurements of neutron-rich rhodium isotopes have been performed at the JYFLTRAP Penning trap mass spectrometer at the Ion Guide Isotope Separator On-Line (IGISOL) facility. We report results on ground- and isomeric-state masses in $^{110,112,114,116,118}$Rh and the very first mass measurement of $^{120}$Rh. The isomeric states were separated and measured for the first time using the phase-imaging ion-cyclotron-resonance (PI-ICR) technique. For $^{112}$Rh, we also report new half-lives for both the ground state and the isomer. The results are compared to theoretical predictions using the BSkG1 mass model and discussed in terms of triaxial deformation.

Nuclear Theory (nucl-th)isotoopitmassaspektrometriaNuclear TheoryFOS: Physical sciencesNuclear Experiment (nucl-ex)ydinfysiikkaNuclear Experiment
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Selective laser ionization of radioactive Ni-isotopes

1997

Abstract A chemically selective laser ion source based on resonance ionization of atoms in a hot cavity has been applied in the study of Ni-isotopes at the CERN-ISOLDE on-line isotope separator. Laser ionization enhanced the yields of long-lived Ni-isotopes almost four orders of magnitude when compared to the yields obtained with the surface ionization mode of the source. As a result, high yields of long-lived Ni-isotopes were obtained. Separation efficiencies of 0.3 and 0.8% were obtained for Ni produced in uranium-carbide, produced from uranium-di-pthalocyanine, and Ta-foil targets, respectively. Ni was found to be released very slowly from the present target and ion source combination.

Nuclear and High Energy PhysicsChemical ionizationMatrix-assisted laser desorption electrospray ionizationChemistryRadiochemistryAnalytical chemistryThermal ionizationIon sourceAtmospheric-pressure laser ionizationIonizationPhysics::Atomic PhysicsNuclear ExperimentInstrumentationElectron ionizationAmbient ionizationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Discovery of a long-lived low-lying isomeric state in Ga-80

2010

Collinear laser spectroscopy was performed on the $^{80}\mathrm{Ga}$ isotope at ISOLDE, CERN. A low-lying isomeric state with a half-life much greater than $200$ ms was discovered. The nuclear spins and moments of the ground and isomeric states and the isomer shift are discussed. Probable spins and parities are assigned to both long-lived states (${3}^{\ensuremath{-}}$ and ${6}^{\ensuremath{-}}$) deduced from a comparison of the measured moments to shell-model calculations.

PhysicsNuclear and High Energy PhysicsParticle propertiesSpinsIsotope010308 nuclear & particles physicsParity (physics)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesQUADRUPOLE-MOMENTSIsomeric shift0103 physical sciencesPhysics::Atomic and Molecular ClustersNuclear Physics - ExperimentAtomic physics010306 general physicsSpectroscopyNuclear Experiment
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Branching ratios in theβdecays ofN12andB12

2009

Absolute branching ratios to unbound states in C-12 populated in the beta decays of N-12 and B-12 are reported. Clean sources of N-12 and B-12 were obtained using the isotope separation on-line (ISOL) method. The relative branching ratios to the different populated states were extracted using single-alpha as well as complete kinematics triple-alpha spectra. These two largely independent methods give consistent results. Absolute normalization is achieved via the precisely known absolute branching ratio to the bound 4.44 MeV state in C-12. The extracted branching ratios to the unbound states are a factor of three more precise than previous measurements. Branching ratios in the decay of Na-20 …

Nuclear physicsPhysicsNormalization (statistics)Nuclear and High Energy PhysicsBranching fractionlawDouble beta decayCarbon-12Alpha particleBeta decaySpectral lineIsotope separationlaw.inventionPhysical Review C
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Decay Spectroscopy for Nuclear Astrophysics: β-delayed Proton Decay

2011

In several radiative proton capture reactions important in novae and XRBs, the resonant parts play the capital role. We use decay spectroscopy techniques to find these resonances and study their properties. We have developed techniques to measure beta- and beta-delayed proton decay of sd-shell, proton-rich nuclei produced and separated with the MARS recoil spectrometer of Texas A&M University. The short-lived radioactive species are produced in-flight, separated, then slowed down (from about 40 MeV/u) and implanted in the middle of very thin Si detectors. This allows us to measure protons with energies as low as 200 keV from nuclei with lifetimes of 100 ms or less. At the same time we measu…

Nuclear physicsPhysicsProtonProton decayAstrophysics::High Energy Astrophysical PhenomenaIsotopes of chlorineNuclear astrophysicsAtomic physicsNuclear ExperimentNucleonBeta decayParticle detectorRadioactive decayAIP Conference Proceedings
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Breakup channels forC12triple-αcontinuum states

2009

The triple-alpha-particle breakup of states in the triple-alpha continuum of C-12 has been investigated by way of coincident detection of all three alpha particles of the breakup. The states have been fed in the beta decay of N-12 and B-12, and the alpha particles measured using a setup that covers all of the triple-alpha phase space. Contributions from the breakup through the Be-8(0(+)) ground state as well as other channels-interpreted as breakup through excited energies in Be-8-have been identified. Spins and parities of C-12 triple-alpha continuum states are deduced from the measured phase-space distributions for breakup through Be-8 above the ground state by comparison to a fully symme…

PhysicsNuclear and High Energy PhysicsAngular momentumExcited stateNuclear TheoryContinuum (design consultancy)Carbon-12Alpha particleAtomic physicsNuclear ExperimentSpin (physics)Ground stateBreakupPhysical Review C
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Penning trap for isobaric mass separation at IGISOL

2003

Abstract A cylindrical Penning trap has been built at the ion guide isotope separator facility IGISOL of the University of Jyvaskyla. The main goal of the Penning trap application is to purify low-energy radioactive ion beams. The aim is to make isobarically pure beams. The technical description is presented.

Radioactive ion beamsNuclear and High Energy PhysicsIsotopeChemistrySeparator (oil production)Penning trapMass separationIonNuclear physicsPhysics::Accelerator PhysicsIsobaric processPhysics::Atomic PhysicsIon trapAtomic physicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Direct determination of the atomic mass difference of the pairs As76−Se76 and Tb155−Gd155 rules out As76 and Tb155 as possible candidates for electro…

2022

Physical Review C
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TAS measurements for reactor physics and nuclear structure

2011

In this contribution we will present recent total absorption measurements of the beta decay of neutron‐rich nuclei performed at the IGISOL facility of the Univ. of Jyvaskyla. In the measurements the JYFL Penning Trap was used as a high resolution isobaric separator. The total absorption technique will be described and the impact of recent results in the fields of reactor physics (decay heat calculations) and nuclear structure will be discussed.

PhysicsNuclear physicsNuclear reactionNuclear TheoryNuclear structureNeutronDecay heatNuclear ExperimentNucleonAbsorption (electromagnetic radiation)Penning trapRadioactive decayAIP Conference Proceedings
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Optimization of krypton yields for rp-process studies at ISOLDE(CERN)

2004

The production of neutron-deficient krypton isotopes having astrophysical importance has been studied at the ISOLDE PBS facility at CERN. To investigate several effects on the yield a Monte Carlo code has been extensively applied.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsKryptonIsotopes of kryptonchemistry.chemical_elementrp-process7. Clean energy01 natural sciencesNuclear physicschemistryMonte carlo codeYield (chemistry)0103 physical sciencesPhysics::Accelerator PhysicsPhysics::Atomic PhysicsNuclear Experiment010306 general physicsNuclear Physics A
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Evolution of deformation in the neutron-rich Zr region from excited intruder state to the ground state.

1994

Strong evidence for the existence of previously postulated deformed excited states in $^{98}\mathrm{Zr}_{58}$ has been obtained by an accurate measurement of the ${\mathrm{\ensuremath{\rho}}}^{2}$(${0}_{3}^{+}$\ensuremath{\rightarrow}${0}_{2}^{+}$) value for the decay of the second excited ${0}^{+}$ state at 1436 keV. In the neighboring isotope $^{99}\mathrm{Zr}_{59}$, at the edge of the region of strong ground-state deformation, evidence is found for a rotational band built on the state at 614 keV. Systematics of the excitation energies of the deformed states in Zr nuclei and their Sr neighbors show that the apparent sudden onset of deformation is explained by the steady lowering of a stro…

PhysicsNuclear and High Energy PhysicsExcited stateStrong interactionQuasiparticleNeutronGamma spectroscopyAtomic physicsGround stateXXExcitationIntruder statePhysical review. C, Nuclear physics
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Mass measurements towards doubly magic Ni-78 : Hydrodynamics versus nuclear mass contribution in core-collapse supernovae

2022

International audience; We report the first high-precision mass measurements of the neutron-rich nuclei 74,75Ni and the clearly identified ground state of 76Cu, along with a more precise mass-excess value of 78Cu, performed with the double Penning trap JYFLTRAP at the Ion Guide Isotope Separator On-Line (IGISOL) facility. These new results lead to a quantitative estimation of the quenching for the N=50 neutron shell gap. The impact of this shell quenching on core-collapse supernova dynamics is specifically tested using a dedicated statistical equilibrium approach that allows a variation of the mass model independent of the other microphysical inputs. We conclude that the impact of nuclear m…

NUCLEOSYNTHESISIONSCore-collapse supernovaNuclear and High Energy PhysicsScience & TechnologyIMPACTPhysicsPenning trapR-PROCESSneutronitAstronomy & Astrophysics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]114 Physical sciencesSTATEPhysics Particles & FieldsPhysics NuclearSPECTROMETRYPhysical SciencesISOTOPESNuclear massNuclear Physics - ExperimentydinfysiikkaShell gap
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Non-analog β decay of 74Rb

2001

The magnitude of the Coulomb mixing parameter δ 1 has been experimentally deduced, for the first time, for the β decay of 74 Rb. The estimated magnitude is derived from the feeding of the non-analog first excited 0 + state in 74 Kr. The inferred upper limit of 0.07% is small compared to theoretical predictions. The half-life was measured to be 64.90(9) ms.  2001 Published by Elsevier Science B.V.

PhysicsNuclear and High Energy PhysicsExcited stateMagnitude (astronomy)CoulombAtomic physicsBeta decayMixing (physics)Physics Letters B
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Dy159 Electron-Capture: A New Candidate for Neutrino Mass Determination

2021

010308 nuclear & particles physics0103 physical sciencesGeneral Physics and Astronomy010306 general physics01 natural sciencesPhysical Review Letters
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β-decay of [sup 23]Al and nova nucleosynthesis

2010

We have studied the β‐decay of 23Al with a novel detector setup at the focal plane of the MARS separator at the Texas A&M University to resolve existing controversies about the proton intensities of the IAS in 23Mg and to determine the absolute proton branching ratios by combining our results to the latest γ‐decay data. Experimental technique, results and the relevance for nova nucleosynthesis are discussed.

PhysicsNuclear physicsProtonNucleosynthesisBranching fractionDouble beta decayHadronGamma rayHigh Energy Physics::ExperimentAstrophysicsNucleonRadioactive decayAIP Conference Proceedings
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Wien filter for cooled low-energy radioactive ion beams

2002

A Wien filter for cooled radioactive ion beams has been designed at Ion Guide Isotope Separator On Line technique (IGISOL). The purpose of such device is to eliminate doubly charged ions from the mass separated singly charged ions, based on q=+2→q=+1 charge exchange process in an ion cooler. The performance of the Wien filter has been tested off-line with a discharge ion source as well as on-line with a radioactive beam. The electron capture process of cooled q=+2 ions has been investigated in a radiofrequency quadrupole ion cooler with varying partial pressures of nitrogen. Also, the superasymmetric fission production yields of 68<A<78 nuclei have been deduced.

PhysicsNuclear and High Energy PhysicsWien filterIsotopeFissionElectron captureIon sourceIonIon beam depositionPhysics::Plasma PhysicsQuadrupoleAtomic physicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Direct determination of the atomic mass difference of the pairs As 76 − Se 76 and Tb 155 − Gd 155 rules out As 76 and Tb 155 as possible candidates f…

Physical Review C
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Measurement of the $2^+\rightarrow 0^+$ ground-state transition in the $\beta$ decay of $^{20}$F

2018

We report the first detection of the second-forbidden, non-unique, $2^+\rightarrow 0^+$, ground-state transition in the $\beta$ decay of $^{20}$F. A low-energy, mass-separated $^{20}\rm{F}^+$ beam produced at the IGISOL facility in Jyv\"askyl\"a, Finland, was implanted in a thin carbon foil and the $\beta$ spectrum measured using a magnetic transporter and a plastic-scintillator detector. The $\beta$-decay branching ratio inferred from the measurement is $b_{\beta} = [ 0.41\pm 0.08\textrm{(stat)}\pm 0.07\textrm{(sys)}] \times 10^{-5}$ corresponding to $\log ft = 10.89(11)$, making this one of the strongest second-forbidden, non-unique $\beta$ transitions ever measured. The experimental resu…

High Energy Physics::ExperimentNuclear Experiment
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Direct measurement of the mass difference of $^{72}$As-$^{72}$Ge rules out $^{72}$As as a promising $\beta$-decay candidate to determine the neutrino…

2021

We report the first direct determination of the ground-state to ground-state electron-capture $Q$-value for the $^{72}$As to $^{72}$Ge decay by measuring their atomic mass difference utilizing the double Penning trap mass spectrometer, JYFLTRAP. The $Q$-value was measured to be 4343.596(75)~keV, which is more than a 50-fold improvement in precision compared to the value in the most recent Atomic Mass Evaluation 2020. Furthermore, the new $Q$-value was found to be 12.4(40)~keV (3.1 $\sigma$) lower. With the significant reduction of the uncertainty of the ground-state to ground-state $Q$-value value combined with the level scheme of $^{72}$Ge from $\gamma$-ray spectroscopy, we confirm that th…

nucleus: semileptonic decayexperimental methodsPenning trapenergy: ground stateelectron: captureElectroweak Interaction[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]energy: transitionmass: spectrometernuclide: mass differenceneutrino: massNuclear Experimentexperimental resultsSymmetries
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High-Precision Q -Value Measurement Confirms the Potential of Cs 135 for Absolute Antineutrino Mass Scale Determination

Physical Review Letters
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High-precision measurement of a low Q value for allowed β−-decay of 131I related to neutrino mass determination

2022

The ground-state-to-ground-state β−-decay 131I (7/2+) → 131Xe (3/2+) Q value was determined with high precision utilizing the double Penning trap mass spectrometer JYFLTRAP at the IGISOL facility. The Q value of this β−-decay was found to be Q = 972.25(19) keV through a cyclotron frequency ratio measurement with a relative precision of 1.6 × 10−9. This was realized using the phase-imaging ion-cyclotron-resonance technique. The new Q value is more than 3 times more precise and 2.3σ higher (1.45 keV) than the value extracted from the Atomic Mass Evaluation 2020. Our measurement confirms that the β−-decay to the 9/2+ excited state at 971.22(13) keV in 131Xe is energetically allowed with a Q va…

β− decayNuclear and High Energy PhysicsScience & TechnologyPhysicsPenning trapLow Q valuebeta(-) decayneutriinotAstronomy & AstrophysicsERRORSPhysics Particles & FieldsPhysics NuclearNeutrino massNUCLEAR-DATA SHEETSPhysical SciencesJYFLTRAPBETA-DECAYydinfysiikkaPhysics Letters B
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Fission studies at IGISOL/JYFLTRAP: Simulations of the ion guide for neutron-induced fission and comparison with experimental data

2020

For the production of exotic nuclei at the IGISOL facility, an ion guide for neutron-induced fission has been developed and tested in experiments. Fission fragments are produced inside the ion guide and collected using a helium buffer gas. Meanwhile, a GEANT4 model has been developed to simulate the transportation and stopping of the charged fission products. In a recent measurement of neutron-induced fission yields, implantation foils were located at different positions in the ion guide. The gamma spectra from these foils and the fission targets are compared to the results from the GEANT4 simulation. In order to allow fission yield measurements in the low yield regions, towards the tails a…

Nuclear TheorytutkimuslaitteethiukkaskiihdyttimetNuclear Experimentydinfysiikka
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Experimental study of $^{100}$Tc $\beta$ decay with total absorption $\gamma$-ray spectroscopy

2017

International audience; The β decay of Tc100 has been studied by using the total absorption γ-ray spectroscopy technique at the Ion Guide Isotope Separator On-Line facility in Jyväskylä. In this work the new Decay Total Absorption γ-ray Spectrometer in coincidence with a cylindrical plastic β detector has been employed. The β intensity to the ground state obtained from the analysis is in good agreement with previous high-resolution measurements. However, differences in the feeding to the first-excited state as well as weak feeding to a new level at high excitation energy have been deduced from this experiment. Theoretical calculations performed in the quasiparticle random-phase approximatio…

densitymolybdenum: double-beta decayexcited state: energytotal-absorption counterrandom phase approximation: quasiparticletechnetium: semileptonic decay[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]benchmarkefficiencygamma rayground statespectrometerbranching ratio[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]numerical calculationsphononrutheniumMonte Carloexperimental results
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Measurement of the 2+--0+ ground-state transition in the ß decay of 20F

2020

12 pags., 16 figs., 4 tabs.

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Total Absorption Spectroscopy Study of $^{92}$Rb Decay: A Major Contributor to Reactor Antineutrino Spectrum Shape

2015

The antineutrino spectra measured in recent experiments at reactors are inconsistent with calculations based on the conversion of integral beta spectra recorded at the ILL reactor. $^{92}$Rb makes the dominant contribution to the reactor spectrum in the 5-8 MeV range but its decay properties are in question. We have studied $^{92}$Rb decay with total absorption spectroscopy. Previously unobserved beta feeding was seen in the 4.5-5.5 region and the GS to GS feeding was found to be 87.5(25)%. The impact on the reactor antineutrino spectra calculated with the summation method is shown and discussed.

High Energy Physics - Experiment (hep-ex)FOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear ExperimentHigh Energy Physics - Experiment
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Measurement of the 2+→0+ ground-state transition in the β decay of 20F

2019

We report the first detection of the second-forbidden, nonunique, 2+→0+, ground-state transition in the β decay of 20F. A low-energy, mass-separated 20F+ beam produced at the IGISOL facility in Jyväskylä, Finland, was implanted in a thin carbon foil and the β spectrum measured using a magnetic transporter and a plastic-scintillator detector. The β-decay branching ratio inferred from the measurement is bβ=[0.41±0.08(stat)±0.07(sys)]×10−5 corresponding to logft=10.89(11), making this one of the strongest second-forbidden, nonunique β transitions ever measured. The experimental result is supported by shell-model calculations and has significant implications for the final evolution of stars tha…

High Energy Physics::Experimentydinfysiikka
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Observation of an ultralow-Q-value electron-capture channel decaying to 75As via a high-precision mass measurement

2022

A precise determination of the atomic mass of 75As has been performed utilizing the double Penning trap mass spectrometer, JYFLTRAP. The mass excess is measured to be −73035.519(42)keV/c2, which is a factor of 21 more precise and 1.3(9)keV/c2 lower than the adopted value in the newest Atomic Mass Evaluation (AME2020). This value has been used to determine the ground-state–to–ground-state electron-capture decay Q value of 75Se and β− decay Q value of 75Ge, which are derived to be 866.041(81) keV and 1178.561(65) keV, respectively. Using the nuclear energy-level data of 860.00(40) keV, 865.40(50) keV (final states of electron capture), and 1172.00(60) keV (final state of β− decay) for the exc…

massaspektrometrianeutriinothiukkasfysiikkaydinfysiikkaarseeni
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Total absorption γ-ray spectroscopy of the β decays of 96gs,mY

2022

The β decays of the ground state (gs) and isomeric state (m) of 96Y have been studied with the total absorption γ-ray spectroscopy technique at the Ion Guide Isotope Separator On-Line facility. The separation of the 8+ isomeric state from the 0− ground state was achieved thanks to the purification capabilities of the JYFLTRAP double Penning trap system. The β-intensity distributions of both decays have been independently determined. In the analyses the deexcitation of the 1581.6 keV level in 96Zr, in which conversion electron emission competes with pair production, has been carefully considered and found to have significant impact on the β-detector efficiency, influencing the β-intensity di…

beta decayydinfysiikkanuclear structure and decays
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Determination of β-decay ground state feeding of nuclei of importance for reactor applications

2020

In β-decay studies the determination of the decay probability to the ground state (g.s.) of the daughter nucleus often suffers from large systematic errors. The difficulty of the measurement is related to the absence of associated delayed γ-ray emission. In this work we revisit the 4πγ−β method proposed by Greenwood and collaborators in the 1990s, which has the potential to overcome some of the experimental difficulties. Our interest is driven by the need to determine accurately the β-intensity distributions of fission products that contribute significantly to the reactor decay heat and to the antineutrinos emitted by reactors. A number of such decays have large g.s. branches. The method is…

nuclear reactorsHigh Energy Physics::Experimentbeta decayydinfysiikkanuclear structure and decaysspectrometers and spectroscopic techniques
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Precision mass measurements of $^{67}$Fe and $^{69,70}$Co : Nuclear structure toward N=40 and impact on r -process reaction rates

2020

International audience; Accurate mass measurements of neutron-rich iron and cobalt isotopes Fe67 and Co69,70 have been realized with the JYFLTRAP double Penning-trap mass spectrometer. With novel ion-manipulation techniques, the masses of the Co69,70 ground states and the 1/2− isomer in Co69 have been extracted for the first time. The measurements remove ambiguities in the previous mass values and yield a smoother trend on the mass surface, extending it beyond N=40. The moderate N=40 subshell gap has been found to weaken below Ni68, a region known for shape coexistence and increased collectivity. The excitation energy for the 1/2− intruder state in Co69 has been determined for the first tim…

[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Structure
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New insights into triaxiality and shape coexistence from odd-mass $^{109}$Rh

2018

International audience; Rapid shape evolutions near A=100 are now the focus of much attention in nuclear science. Much of the recent work has been centered on isotopes with Z≤40, where the shapes are observed to transition between near-spherical to highly deformed with only a single pair of neutrons added. At higher Z, the shape transitions become more gradual as triaxiality sets in, yet the coexistence of varying shapes continues to play an important role in the low-energy nuclear structure, particularly in the odd-Z isotopes. This work aims to characterize competing shapes in the triaxial region between Zr and Sn isotopes using ultrafast timing techniques to measure lifetimes of excited s…

Nuclear Theorycollective levels[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ydinfysiikkaNuclear ExperimentNuclear Structurenuclear structure and decays
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Low-spin excitations in 89Br populated in β−decay of 89Se

2022

Low-spin, excited states of the 89Br nucleus, populated in β− decay of 89Se have been studied for the first time. The 89Se nuclei were produced in proton-induced fission of natural thorium using the IGISOL facility and separated using a dipole magnet and the coupled JYFLTRAP Penning trap. Gamma radiation following the β− decay of 89Se was measured with an array of high-resolution germanium detectors. Levels scheme of 89Br was extended by 12 new levels and 31 new γ transitions. Spin-parity (3/2+) has been proposed for the ground state of the 89Se mother nucleus, replacing the (5/2+) assignment reported in data bases. The observed Gamow-Teller β− transition to the 1754.5-keV level indicates a…

astrofysiikkaIGISOLydinfysiikka
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Dy159 Electron-Capture: A New Candidate for Neutrino Mass Determination

2021

International audience; The ground state to ground state electron-capture Q value of Dy159 (3/2-) has been measured directly using the double Penning trap mass spectrometer JYFLTRAP. A value of 364.73(19) keV was obtained from a measurement of the cyclotron frequency ratio of the decay parent Dy159 and the decay daughter Tb159 ions using the novel phase-imaging ion-cyclotron resonance technique. The Q values for allowed Gamow-Teller transition to 5/2- and the third-forbidden unique transition to 11/2+ state with excitation energies of 363.5449(14) keV and 362.050(40) keV in Tb159 were determined to be 1.18(19) keV and 2.68(19) keV, respectively. The high-precision Q value of transition 3/2-…

mass: scaleenergy: decayPenning trapdysprosiumelectron: capturesemileptonic decayneutrino: mass[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]sensitivityexperimental results
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Relative proton and γ widths of astrophysically important states in 30S studied in the β-delayed decay of 31Ar

2013

Resonances just above the proton threshold in 30S affect the 29P(p,gamma)30S reaction under astrophysical conditions. The (p,gamma)-reaction rate is currently determined indirectly and depends on the properties of the relevant resonances. We present here a method for finding the ratio between the proton and gamma partial widths of resonances in 30S. The widths are determined from the beta-2p and beta-p-gamma decay of 31Ar, which is produced at the ISOLDE facility at the European research organization CERN. Experimental limits on the ratio between the proton and gamma partial widths for astrophysical relevant levels in 30S have been found for the first time. A level at 4688(5) keV is identif…

26.30.−k 23.40.Hc 27.30.+tAstrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesddc:530Experimental nuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Study of the $��$-decay of $^{100}$Tc with Total Absorption $��$-Ray Spectroscopy

2017

The \b{eta}-decay of 100 Tc has been studied using the Total Absorption ��-Ray Spectroscopy technique at IGISOL. In this work the new DTAS spectrometer in coincidence with a cylindrical plastic \b{eta} detector has been employed. The \b{eta}-intensity to the ground state obtained from the analysis is in good agreement with previous high-resolution measurements. However, differences in the feeding to the first excited state as well as weak feeding to a new level at high excitation energy have been deduced from this experiment. Theoretical calculations performed in the quasiparticle random- phase approximation (QRPA) framework are also reported. Comparison of these calculations with our measu…

FOS: Physical sciencesHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)Nuclear Experiment
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Precision mass measurements of Fe 67 and Co 69 , 70 : Nuclear structure toward N = 40 and impact on r -process reaction rates

Physical Review C
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Study of the $\beta$-decay of $^{100}$Tc with Total Absorption $\gamma$-Ray Spectroscopy

2017

The \b{eta}-decay of 100 Tc has been studied using the Total Absorption {\gamma}-Ray Spectroscopy technique at IGISOL. In this work the new DTAS spectrometer in coincidence with a cylindrical plastic \b{eta} detector has been employed. The \b{eta}-intensity to the ground state obtained from the analysis is in good agreement with previous high-resolution measurements. However, differences in the feeding to the first excited state as well as weak feeding to a new level at high excitation energy have been deduced from this experiment. Theoretical calculations performed in the quasiparticle random- phase approximation (QRPA) framework are also reported. Comparison of these calculations with our…

High Energy Physics::ExperimentNuclear ExperimentNuclear Experiment
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β- and γ-spectroscopy study of 119Pd and 119Ag

2022

Neutron-rich 119Pd nuclei were produced in fission of natural uranium, induced by 25-MeV protons. Fission fragments swiftly extracted with the Ion Guide Isotope Separation On-Line method were mass separated using a dipole magnet and a Penning trap, providing mono-isotopic samples of 119Pd. Their β− decay was measured with γγ- and βγ-spectroscopy methods using low-energy germanium detectors and a thin plastic scintillator. Two distinct nuclear-level structures were observed in 119Ag, based on the 1/2− and 7/2+ isomers reported previously. The β−-decay work was complemented by a prompt-γ study of levels in 119Ag populated in spontaneous fission of 252Cf, performed using the Gammasphere array …

electromagnetic transitionsrare and new isotopesbeta decayisomer decaysydinfysiikkapalladiumnuclear structure and decays
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Multiparticle emission in the decay of Ar 31

2014

A multihit capacity setup was used to study the decay of the dripline nucleus 31Ar, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the β-delayed three-proton decay of 31Ar is presented for the first time together with a quantitative analysis of the β-delayed 2pγ decay. A new method for determination of the spin of low-lying levels in the βp daughter 30S using proton-proton angular correlations is presented and used to determine that the spin of the 5.2-MeV level is most likely 3+ with 4+ also possible. The half-life of 31Ar is found to be 15.1(3) ms. An improved analysis of the Fermi β strength including the β3p-decay mode gives a total measured branching ratio of 3.60…

NUCLEAR EXPERIMENTmultiparticle emissionCIENCIAANÁLISIS ESPECTROSCÓPICOBETA DESINTEGRATIONPROTONFÍSICA NUCLEARFÍSICA
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Penning-trap-assisted study of excitations in $^{88}$Br populated in β decay of $^{88}$Se

2017

Excited levels of 88Br populated in the β decay of 88Se have been studied by means of βγ and γ γ spectroscopy methods. Neutron-rich parent 88Se nuclei were produced with proton-induced fission of 238U using the Ion Guide Isotope Separator On-Line (IGISOL) method and separated from contaminants using a dipole magnet and the coupled JYFLTRAP Penning trap at the Accelerator Laboratory of the University of Jyvaskyl ¨ a. The level scheme ¨ of 88Br has been constructed and log f t values of levels were determined. The ground-state spin of 88Br is now firmly determined to be 1−. Low-energy levels in 88Br were interpreted as members of the πp3/2(νd5/2) 3, πp−1 3/2(νd5/2) 3, πf −1 5/2 (νd5/2) 3, and…

beta decay[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]excitations
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Discovery of an Exceptionally Strong β -Decay Transition of $^{20}$F and Implications for the Fate of Intermediate-Mass Stars

2019

A significant fraction of stars between 7-11 solar masses are thought to become supernovae, but the explosion mechanism is unclear. The answer depends critically on the rate of electron capture on $^{20}$Ne in the degenerate oxygen-neon stellar core. However, due to the unknown strength of the transition between the ground states of $^{20}$Ne and $^{20}$F, it has not previously been possible to fully constrain the rate. By measuring the transition, we have established that its strength is exceptionally large and enhances the capture rate by several orders of magnitude. This has a decisive impact on the evolution of the core, increasing the likelihood that the star is (partially) disrupted b…

tähdetAstrophysics - Solar and Stellar AstrophysicsNuclear TheoryastrofysiikkaAstrophysics::Solar and Stellar Astrophysicsddc:530ydinfysiikkaAstrophysics - High Energy Astrophysical PhenomenaNuclear Experiment
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Total absorption γ-ray spectroscopy of the β-delayed neutron emitters 137I and 95Rb

2019

The decays of the β-delayed neutron emitters 137I and 95Rb have been studied with the total absorption γ-ray spectroscopy technique. The purity of the beams provided by the JYFLTRAP Penning trap at the ion guide isotope separator on-line facility in Jyväskylä allowed us to carry out a campaign of isotopically pure measurements with the decay total absorption γ-ray spectrometer, a segmented detector composed of 18 NaI(Tl) modules. The contamination coming from the interaction of neutrons with the spectrometer has been carefully studied, and we have tested the use of time differences between prompt γ rays and delayed neutron interactions to eliminate this source of contamination. Due to the s…

Astrophysics::High Energy Astrophysical Phenomenaastrofysiikkanuclear astrophysicsbeta decayNuclear Experimentydinfysiikkanuclear structure&decays
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Direct determination of the atomic mass difference of the pairs 76As−76Se and 155Tb−155Gd rules out 76As and 155 Tb as possible candidates for electr…

2022

The first direct determination of the ground-state–to–ground-state Q values of the β− decay 76As→76Se and the electron-capture decay 155Tb→155Gd was performed utilizing the double Penning trap mass spectrometer JYFLTRAP. By measuring the atomic mass difference of the decay pairs via the phase-imaging ion-cyclotron-resonance technique, the Q values of 76As→76Se and 155Tb→155Gd were determined to be 2959.265(74) keV and 814.94(18) keV, respectively. The precision was increased relative to earlier measurements by factors of 12 and 57, respectively. The new Q values are 1.33 keV and 5 keV lower compared to the values adopted in the most recent Atomic Mass Evaluation 2020. With the newly determi…

neutriinothiukkasfysiikkaydinfysiikka
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High-precision $Q$-value measurement confirms the potential of $^{135}$Cs for antineutrino-mass detection

2020

The ground-state-to-ground-state $\beta$-decay $Q$-value of $^{135}\textrm{Cs}(7/2^+)\to\,^{135}\textrm{Ba}(3/2^+)$ was directly measured for the first time utilizing the Phase-Imaging Ion-Cyclotron Resonance (PI-ICR) technique at the JYFLTRAP Penning-trap setup. It is the first direct determination of this $Q$-value and its value of 268.66(30)\,keV is a factor of three more precise than the currently adopted $Q$-value in the Atomic Mass Evaluation 2016. Moreover, the $Q$-value deduced from the $\beta$-decay endpoint energy has been found to deviate from our result by approximately 6 standard deviations. The measurement confirms that the first-forbidden unique $\beta^-$-decay transition $^{…

FOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment
researchProduct

Design of a High Intensity Neutron Source for Neutron-Induced Fission Yield Studies

2013

The upgraded IGISOL facility with JYFLTRAP, at the accelerator laboratory of the University of Jyv\"askyl\"a, has been supplied with a new cyclotron which will provide protons of the order of 100 {\mu}A with up to 30 MeV energy, or deuterons with half the energy and intensity. This makes it an ideal place for measurements of neutron-induced fission products from various actinides, in view of proposed future nuclear fuel cycles. The groups at Uppsala University and University of Jyv\"askyl\"a are working on the design of a neutron converter that will be used as neutron source in fission yield studies. The design is based on simulations with Monte Carlo codes and a benchmark measurement that …

Nuclear TheoryFOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Multi-particle emission in the decay of $^{31}$Ar

2014

A multi-hit capacity setup was used to study the decay of the dripline nucleus 31Ar, produced at the ISOLDE facility at CERN. A spectroscopic analysis of the beta-delayed three-proton decay of 31Ar is presented for the first time together with a quantitative analysis of the beta-delayed two-proton-gamma-decay. A new method for determination of the spin of low-lying levels in the beta-proton-daughter 30S using proton-proton angular correlations is presented and used for the level at 5.2 MeV, which is found to be either a 3+ or 4+ level, with the data pointing towards the 3+. The half-life of 31Ar is found to be 15.1(3) ms. An improved analysis of the Fermi beta-strength gives a total measure…

Physics::Accelerator PhysicsFOS: Physical sciencesNuclear Physics - Experiment[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment23.40.Hc 27.30.+t
researchProduct

Enhanced Gamma-Ray Emission from Neutron Unbound States Populated in Beta Decay

2015

International audience; Total absorption spectroscopy was used to investigate the beta-decay intensity to states above the neutron separation energy followed by gamma-ray emission in 87,88Br and 94Rb. Accurate results were obtained thanks to a careful control of systematic errors. An unexpectedly large gamma intensity was observed in all three cases extending well beyond the excitation energy region where neutron penetration is hindered by low neutron energy. The gamma branching as a function of excitation energy was compared to Hauser-Feshbach model calculations. For 87Br and 88Br the gamma branching reaches 57% and 20% respectively, and could be explained as a nuclear structure effect. So…

Astrophysics::High Energy Astrophysical PhenomenaFOS: Physical sciencesNuclear Experiment (nucl-ex)[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear ExperimentNuclear Experiment
researchProduct

Observation of an ultralow- Q -value electron-capture channel decaying to As 75 via a high-precision mass measurement

Physical Review C
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High-Precision Q-Value Measurement Confirms the Potential of 135Cs for Absolute Antineutrino Mass Scale Determination

2020

The ground-state-to-ground-state β-decay Q value of Cs135(7/2+)→Ba135(3/2+) has been directly measured for the first time. The measurement was done utilizing both the phase-imaging ion-cyclotron resonance technique and the time-of-flight ion-cyclotron resonance technique at the JYFLTRAP Penning-trap setup and yielded a mass difference of 268.66(30) keV between Cs135(7/2+) and Ba135(3/2+). With this very small uncertainty, this measurement is a factor of 3 more precise than the currently adopted Q value in the Atomic Mass Evaluation 2016. The measurement confirms that the first-forbidden unique β--decay transition Cs135(7/2+)→Ba135(11/2-) is a candidate for antineutrino mass measurements wit…

particles and fieldsnuclear physicsneutriinotNuclear Physics - Experimenthiukkasfysiikkaydinfysiikka
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Mass measurements and implications for the energy of the high-spin isomer in 94Ag.

2008

Nuclides in the vicinity of 94Ag have been studied with the Penning trap mass spectrometer JYFLTRAP at the Ion-Guide Separator On-Line. The masses of the two-proton-decay daughter 92Rh and the beta-decay daughter 94Pd of the high-spin isomer in 94Ag have been measured, and the masses of 93Pd and 94Ag have been deduced. When combined with the data from the one-proton or two-proton-decay experiments, the results lead to contradictory mass excess values for the high-spin isomer in 94Ag, -46370(170) or -44970(100) keV, corresponding to excitation energies of 6960(400) or 8360(370) keV, respectively.

FOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentPhysical review letters
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Excited states in 87Br populated in β decay of 87Se

2019

Excited levels in 87Br, populated in β decay of 87Se, have been studied by means of γ-ray spectroscopy using an array of broad energy Ge detectors. 87Se nuclei were produced by irradiating a natural Th target with 25-MeV protons. Fission products were extracted from the target chamber using the IGISOL technique, then separated on a dipole magnet and Penning trap (JYFLTRAP) setup. The scheme of excited levels of 87Br has been significantly extended. 114 new transitions and 51 new levels were established. β feedings and log(ft) values of levels were determined. The upper limit for β feeding to the ground state of 87Br was determined to be 23(5)%. Ground state spin and parity 5/2− was confirme…

electromagnetic transitionsnuclear spin and parityshell modelbeta decayydinfysiikkanuclear structure and decays
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Measurement of the 2+→0+ ground-state transition in the β decay of F 20

2019

| openaire: EC/H2020/654002/EU//ENSAR2 We report the first detection of the second-forbidden, nonunique, 2(+) -> 0(+), ground-state transition in the beta decay of F-20. A low-energy, mass-separated F-20(+) beam produced at the IGISOL facility in Jyvaskyla, Finland, was implanted in a thin carbon foil and the beta spectrum measured using a magnetic transporter and a plastic-scintillator detector. The beta-decay branching ratio inferred from the measurement is b(beta) = [0.41 +/- 0.08(stat) +/- 0.07(sys)] x 10(-5) corresponding to log ft = 10.89(11), making this one of the strongest second-forbidden, nonunique beta transitions ever measured. The experimental result is supported by shell-mode…

3106ELEMENTSHigh Energy Physics::Experiment
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Measurement of the 2 + → 0 + ground-state transition in the β decay of F 20

Physical Review C
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Novel Penning-trap techniques reveal isomeric states in $^{128}$In and $^{130}$In for the first time

2020

Isomeric states in $^{128}$In and $^{130}$In have been studied with the JYFLTRAP Penning trap at the IGISOL facility. By employing novel ion manipulation techniques, different states were separated and masses of six beta-decaying states were measured. JYFLTRAP was also used to select the ions of interest for identification at a post-trap decay spectroscopy station. A new beta-decaying high-spin isomer feeding the $15^-$ isomer in $^{128}$Sn has been discovered in $^{128}$In at $1797.6(20)$ keV. Shell-model calculations employing a CD-Bonn potential re-normalized with the perturbative G-matrix approach suggest this new isomer to be a $16^+$ spin-trap isomer. In $^{130}$In, the lowest-lying $…

Physics::Atomic and Molecular ClustersFOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment
researchProduct

Dy 159 Electron-Capture: A New Candidate for Neutrino Mass Determination

Physical Review Letters
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Discovery of an Exceptionally Strong β -Decay Transition of F 20 and Implications for the Fate of Intermediate-Mass Stars

Physical Review Letters
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First β-decay scheme of 107Nb : New insight into the low-energy levels of 107Mo

2019

Monoisotopic samples of 107Nb nuclei, produced in the proton-induced fission of 238U and separated using the IGISOL mass separator coupled to a Penning trap, were used to perform β- and γ-coincidence spectroscopy of 107Mo. Gamma transitions and excited levels in 107Mo were observed in β decay for the first time. Spin and parity 1/2+ for the ground state of 107Mo is proposed, to replace the previous 5/2+ assignment. The experimental β-decay half-life of 107Nb was estimated to be 0.27±0.02 s. peerReviewed

electromagnetic transitionsbeta decayydinfysiikkanuclear structure and decays
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Mass of astrophysically relevant 31Cl and the breakdown of the isobaric multiplet mass equation

2015

The mass of $^{31}$Cl has been measured with the JYFLTRAP double Penning trap mass spectrometer at the Ion-Guide Isotope Separator On-Line (IGISOL) facility. The determined mass-excess value, -7034.7(34) keV, is 15 times more precise than in the Atomic Mass Evaluation 2012. The quadratic form of the isobaric multiplet mass equation for the T=3/2 quartet at A=31 fails ($\chi^2_n$=11.6) and a non-zero cubic term, d=-3.5(11) keV, is obtained when the new mass value is adopted. $^{31}$Cl has been found to be less proton-bound with a proton separation energy of $S_p$=265(4) keV. Energies for the excited states in $^{31}$Cl and the photodisintegration rate on $^{31}$Cl have been determined with s…

massaspektrometriaprotonitisotoopitklooriphotodisintegrationastrofysiikkaFOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear Experimentisobaric multiplet mass equationydinfysiikkaNuclear Experiment
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Three beta-decaying states in In and In resolved for the first time using Penning-trap techniques

2020

Isomeric states in $^{128}$In and $^{130}$In have been studied with the JYFLTRAP Penning trap at the IGISOL facility. By employing state-of-the-art ion manipulation techniques, three different beta-decaying states in $^{128}$In and $^{130}$In have been separated and their masses measured. JYFLTRAP was also used to select the ions of interest for identification at a post-trap decay spectroscopy station. A new beta-decaying high-spin isomer feeding the 15− isomer in $^{128}$Sn has been discovered in $^{128}$In at 1797.6(20) keV. Shell-model calculations employing a CD-Bonn potential re-normalized with the perturbative G-matrix approach suggest this new isomer to be a 16+ spin-trap isomer. In …

Physics Letters
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Direct measurement of the mass difference of As 72 − Ge 72 rules out As 72 as a promising β -decay candidate to determine the neutrino mass

Physical Review C
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β - and γ -spectroscopy study of Pd 119 and Ag 119

Physical Review C
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Precision mass measurements of 67Fe and 69,70Co: Nuclear structure toward N = 40 and impact on r-process reaction rates

2020

Accurate mass measurements of neutron-rich iron and cobalt isotopes 67Fe and 69,70Co have been realized with the JYFLTRAP double Penning-trap mass spectrometer. With novel ion-manipulation techniques, the masses of the 69,70Co ground states and the 1/2− isomer in 69Co have been extracted for the first time. The measurements remove ambiguities in the previous mass values and yield a smoother trend on the mass surface, extending it beyond N=40. The moderate N=40 subshell gap has been found to weaken below 68Ni, a region known for shape coexistence and increased collectivity. The excitation energy for the 1/2− intruder state in 69Co has been determined for the first time and is compared to lar…

energy levels and level densitiesnuclear astrophysicsr processhiukkasfysiikkaydinfysiikkanuclear structure and decaysbinding energy and masses
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