0000000000520723

AUTHOR

C. Scheidenberger

showing 70 related works from this author

Erratum to: “Mass measurements on neutron-deficient Sr and neutron-rich Sn isotopes with the ISOLTRAP mass spectrometer” [Nucl. Phys. A 763 (2005) 45]

2006

Nuclear physicsPhysicsNuclear and High Energy PhysicsIsotope0103 physical sciencesNeutron010306 general physicsMass spectrometry010303 astronomy & astrophysics01 natural sciencesISOLTRAPNuclear Physics A
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On-line commissioning of SHIPTRAP

2006

Abstract The on-line commissioning of the Penning-trap mass spectrometer SHIPTRAP was successfully completed with a mass measurement of holmium and erbium radionuclides produced at SHIP. A large fraction of contaminant ions created in the stopping cell was identified to originate from the buffer-gas supply system. Using a liquid nitrogen cold trap they were reduced to a tolerable amount and mass measurements of Er 147 , Er 148 , and Ho 147 with relative uncertainties of about 1 × 1 0 − 6 were performed.

010308 nuclear & particles physicsAnalytical chemistrychemistry.chemical_elementLiquid nitrogen[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Condensed Matter PhysicsMass spectrometryPenning trap01 natural sciencesAtomic massIonMasschemistry07.75.+h; 21.10.Dr0103 physical sciencesPhysical and Theoretical Chemistry010306 general physicsHolmiumInstrumentationSpectroscopyCold trap
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Three-body correlations in electromagnetic dissociation of Borromean nuclei: The 6He case

2005

20 pages, 2 tables, 9 figures, 1 appendix.-- PACS nrs.: 25.60.-t; 27.20.+n; 25.70.De; 25.75.Gz.-- Printed version published Sep 5, 2005.

PhysicsNuclear and High Energy PhysicsParticle correlationsCoulomb excitationCoulomb excitationDissociation (chemistry)Coincidence[PACS] Reactions induced by unstable nucleiAmplitude6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)[PACS] Particle correlations and fluctuationsNeutronHe-6[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsSeries expansionGround stateUnstable nucleiNuclear Physics A
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Precision experiments with time-resolved Schottky mass spectrometry

2004

Abstract A large area on the mass surface of neutron-deficient nuclides (36≤Z≤85) was measured with time-resolved Schottky mass spectrometry at the FRS-ESR facilities. The masses of 114 nuclides were obtained for the first time from which 43 were determined via known decay energies. The improved mass accuracy of 30 keV allowed to study the isospin dependence of nuclear pairing, to precisely locate the one-proton dripline for odd-Z isotopes from Tb to Pa and to make crucial tests of the predictive powers of modern mass models.

PhysicsNuclear and High Energy PhysicsIsotopeResolution (mass spectrometry)Nuclear TheoryThermal ionization mass spectrometryMass spectrometryNuclear physicsNuclideTime-of-flight mass spectrometryAtomic physicsNuclear ExperimentRadioactive decayAccelerator mass spectrometryNuclear Physics A
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Invariant mass spectrum and α-n correlation function studied in the fragmentation of 6He on a carbon target

1998

13 pags, 5 figures.-- PACS nrs.: 24.60.−t; 25.70.Ef; 27.20.+n.

PhysicsNuclear and High Energy PhysicsReaction mechanismMomentum distributionsBreakupSpectral lineIon[PACS] Reactions induced by unstable nucleiBreakup reactions6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)Halo nucleiFragmentation mechanism[PACS] ResonancesSecondary radioactive beamsInvariant massNeutronHe-5He-6Invariant mass spectra[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Atomic physicsGround stateExotic nucleiNuclear Physics A
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Decay studies in the A∼225 Po-Fr region from the DESPEC campaign at GSI in 2021

2022

The HISPEC-DESPEC collaboration aims at investigating the struc-ture of exotic nuclei formed in fragmentation reactions with decay spectroscopymeasurements, as part of the FAIR Phase-0 campaign at GSI. This paper reportson first results of an experiment performed in spring 2021, with a focus on beta-decaystudies in the Po-Fr nuclei in the 220 < A <230 island of octupole deformationexploiting the DESPEC setup. Ion-beta correlations and fast-timing techniques arebeing employed, giving an insight into this difficult-to-reach region. peerReviewed

ydinfysiikka
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Measurements of the dipole response with radioactive beams

2001

PhysicsNuclear and High Energy PhysicsDipoleAtomic physics
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Systematic investigation of the drip-line nuclei 11Li and 14Be and their unbound subsystems 10Li and 13Be

2007

Fragmentation reactions in a carbon target with beams of 11Li and 14Be at relativistic energies have been studied in a kinematically complete experiment at the ALADIN-LAND setup at GSI. Excited states in 11Li and 14Be were obtained from the data in the inelastic channel. The measured cross sections with the core nucleus in the final state show that in the 14Be case core polarization plays an important role. In the one-neutron knockout channels the measured angular correlations between fragment and neutron are asymmetric, which demonstrates the presence of states with different parities in the 11Li and 14Be ground states. For 10Li a low-lying virtual s-state, a p-state and evidence for a d-s…

PhysicsNuclear physicsNuclear and High Energy PhysicsFragmentation (mass spectrometry)Excited stateHalo nucleusNeutronAtomic physicsNuclear ExperimentPolarization (waves)Ground stateNuclear Physics A
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First Measurement of Severalβ-Delayed Neutron Emitting Isotopes BeyondN=126

2016

The β-delayed neutron emission probabilities of neutron rich Hg and Tl nuclei have been measured together with β-decay half-lives for 20 isotopes of Au, Hg, Tl, Pb, and Bi in the mass region N≳126. These are the heaviest species where neutron emission has been observed so far. These measurements provide key information to evaluate the performance of nuclear microscopic and phenomenological models in reproducing the high-energy part of the β-decay strength distribution. This provides important constraints on global theoretical models currently used in r-process nucleosynthesis.

PhysicsIsotope010308 nuclear & particles physicsNeutron emissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGeneral Physics and Astronomy01 natural sciencesMass formulaNuclear physics13. Climate actionNucleosynthesis0103 physical sciencesr-processNeutronNuclear Experiment010306 general physicss-processDelayed neutronPhysical Review Letters
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Few-neutron removal from238U at relativistic energies

1995

As part of a comprehensive study of uranium fragmentation at relativistic energies at the GSI projectile fragment separator, FRS, inclusive neutron-removal cross sections have been measured for severalxn channels at projectile energies of 600 and 950A MeV using targets of Al, Cu and Pb. The variation of the experimental cross sections with target nuclear charge is used to disentangle nuclear and electromagnetic contributions. The electromagnetic cross sections agree surprisingly well with a simple harmonic oscillator calculation of giant dipole resonances based on measured photonuclear cross sections and do not require an extra enhancement of the two-phonon giant dipole excitation as conclu…

PhysicsNuclear and High Energy PhysicsProjectileNuclear Theorychemistry.chemical_elementSimple harmonic motionUraniumEffective nuclear chargeNuclear physicsDipoleFragmentation (mass spectrometry)chemistryNuclear fusionNeutronAtomic physicsNuclear ExperimentNuclear PhysicsZeitschrift für Physik A Hadrons and Nuclei
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Mass measurements on neutron-deficient Sr and neutron-rich Sn isotopes with the ISOLTRAP mass spectrometer

2005

Abstract The atomic masses of 76,77,80,81,86,88 Sr and 124,129,130,131,132 Sn were measured by means of the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. 76 Sr is now the heaviest N = Z nucleus for which the mass is measured to a precision better than 35 keV. For the tin isotopes in the close vicinity of the doubly magic nucleus 132 Sn, mass uncertainties below 20 keV were achieved. An atomic mass evaluation was carried out taking other experimental mass values into account by performing a least-squares adjustment. Some discrepancies between older experimental values and the ones reported here emerged and were resolved. The results of the new adjustment and their impact will be pr…

PhysicsNuclear and High Energy Physicsatomic masses010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometryISOLTRAP01 natural sciencesISOLTRAPAtomic massNuclear physicsMasstin0103 physical sciencesIsotopes of tinNeutronstrontiumAtomic physics010306 general physicsNuclear ExperimentQuadrupole mass analyzerhigh-precision mass spectrometryHybrid mass spectrometer07.75.+h 21.10.Dr 32.10.Bi
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A linear radiofrequency quadrupole ion trap for the cooling and bunching of radioactive ion beams

2000

A linear radiofrequency quadrupole ion guide and beam buncher has been installed at the ISOLTRAP mass spectrometry experiment at the ISOLDE facility at CERN. The apparatus is being used as a beam cooling, accumulation, and bunching system. It operates with a buffer gas that cools the injected ions and converts the quasicontinuous 60- keV beam from the ISOLDE facility to 2.5-keV beam pulses with improved normalized transverse emittance. Recent measurements suggest a capture efficiency of the ion guide of up to 40% and a cooling and bunching efficiency of at least 12% which is expected to still be increased. The improved ISOLTRAP setup has so far been used very successfully in three on-line e…

PhysicsNuclear and High Energy PhysicsIon beam010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Ion gunAccelerators and Storage Rings01 natural sciences7. Clean energyISOLTRAPNuclear physicsIon beam deposition0103 physical sciencesPhysics::Accelerator PhysicsIon trapAtomic physicsQuadrupole ion trapBeam emittanceNuclear Experiment010306 general physicsBeam (structure)Nuclear Physics A
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Recent developments for high-precision mass measurements of the heaviest elements at SHIPTRAP

2013

Abstract Atomic nuclei far from stability continue to challenge our understanding. For example, theoretical models have predicted an “island of stability” in the region of the superheavy elements due to the closure of spherical proton and neutron shells. Depending on the model, these are expected at Z = 114, 120 or even 126 and N = 172 or 184. Valuable information on the road to the island of stability is derived from high-precision mass measurements, which give direct access to binding energies of short-lived trans-uranium nuclei. Recently, direct mass measurements at SHIPTRAP have been extended to nobelium and lawrencium isotopes around the deformed shell gap N = 152. In order to further …

Nuclear and High Energy PhysicsProtonIsotopeChemistryNuclear TheoryBinding energychemistry.chemical_elementIsland of stabilityNuclear physicsAtomic nucleusNeutronNobeliumInstrumentationLawrenciumNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Mass measurement of cooled neutron-deficient bismuth projectile fragments with time-resolved Schottky mass spectrometry at the FRS-ESR facility

2005

Masses of 582 neutron-deficient nuclides ($30\leq{Z}\leq{85}$) were measured with time-resolved Schottky mass spectrometry at the FRS-ESR facility at GSI, 117 were used for calibration. The masses of 71 nuclides were obtained for the first time. A typical mass accuracy of 30 $\mu$u was achieved. These data have entered the latest atomic mass evaluation. The mass determination of about 140 additional nuclides was possible via known energies ($Q$-values) of $\alpha-$, $\beta-$, or proton decays. The obtained results are compared with the results of other measurements.

Nuclear and High Energy PhysicsA=79–207ProtonAtomic massesNuclear Theorychemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometry01 natural sciences7. Clean energyBismuthmassesNuclear physicsZ=30–850103 physical sciencesNeutronNuclide010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physicsTime-resolved Schottky mass spectrometrySchottky diodeAtomic massMasschemistrymeasured
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Direct mass measurements of neutron-deficient xenon isotopes with the ISOLTRAP mass spectrometer

2000

Abstract The masses of Xe isotopes with 124⩾ A ⩾114 have been measured using the ISOLTRAP spectrometer at the on-line mass separator ISOLDE/CERN. A mass resolving power of 500 000 was chosen resulting in an accuracy of δm ≈12 keV for all isotopes investigated. Conflicts with existing mass data of several standard deviations were found.

PhysicsNuclear and High Energy PhysicsSpectrometer[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Physics::Instrumentation and Detectors010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometry01 natural sciencesISOLTRAPAtomic massIsotopes of oxygenNuclear physics0103 physical sciencesIsotopes of xenonAtomic physicsParticle PhysicsNuclear Experiment010306 general physicsQuadrupole mass analyzerHybrid mass spectrometer
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Approaching the precursor nuclei of the third r-process peak with RIBs

2013

The rapid neutron nucleosynthesis process involves an enormous amount of very exotic neutron-rich nuclei, which represent a theoretical and experimental challenge. Two of the main decay properties that affect the final abundance distribution the most are half-lives and neutron branching ratios. Using fragmentation of a primary $^{238}$U beam at GSI we were able to measure such properties for several neutron-rich nuclei from $^{208}$Hg to $^{218}$Pb. This contribution provides a short update on the status of the data analysis of this experiment, together with a compilation of the latest results published in this mass region, both experimental and theoretical. The impact of the uncertainties …

HistoryNeutron emissionNuclear TheoryFOS: Physical sciencesNeutronPhysics and Astronomy(all)nucl-ex01 natural sciences530EducationNuclear physicsNucleosynthesis/dk/atira/pure/subjectarea/asjc/31000103 physical sciencesNuclear Physics - Experimentddc:530NeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsNeutrons:Energies::Energia nuclear [Àrees temàtiques de la UPC]010308 nuclear & particles physicsBranching fractionNuclear energyComputer Science ApplicationsUranium-238r-processEnergia nuclears-processNucleosynthesisRadioactive decay
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Two- and three-body correlations: breakup of halo nuclei

2004

4 pages, 2 figures.

Nuclear physicsPhysicsNuclear and High Energy PhysicsSpinsCoincidentNuclear TheoryNeutronHaloNuclear ExperimentGround stateBreakup
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A linear radiofrequency ion trap for accumulation, bunching, and emittance improvement of radioactive ion beams

2000

An ion beam cooler and buncher has been developed for the manipulation of radioactive ion beams. The gas-filled linear radiofrequency ion trap system is installed at the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. Its purpose is toaccumulate the 60-keV continuous ISOLDE ion beam with high efficiency and to convert it into low-energy low-emittance ion pulses. The efficiency was found to exceed 10\,\% in agreement with simulations. A more than 10-fold reduction of the ISOLDE beam emittance can be achieved. The system has been used successfully for first on-line experiments. Its principle, setup and performance will be discussed. An ion beam cooler and buncher has been developed fo…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsIon beamIon trapFOS: Physical sciencesMass spectrometryIon cooling01 natural sciencesISOLTRAPIonNuclear physics0103 physical sciencesThermal emittance[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentRadioactive ion beamsIon guide21.10.Dr; 2.10.Bi; 07.75.+hPhysicsOn-line mass spectrometry010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Penning trapAccelerators and Storage RingsIon buncherPhysics::Accelerator PhysicsIon trapBeam emittance
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Observation of a dramatic hindrance of the nuclear decay of isomeric states for fully ionized atoms

2003

Abstract The half-lives of isomeric states of fully ionized 144Tb, 149Dy and 151Er have been measured. These nuclides were produced via fragmentation of about 900 MeV/u 209Bi projectiles, separated in flight with the fragment separator (FRS) and stored in the cooler ring (ESR). The decay times of the cooled fragments have been measured with time-resolved Schottky spectrometry. We observed for the first time drastic increases of the half-lives of bare isomers by factors of up to 30 compared to their neutral counterparts. This is due to the exclusion of the strong internal conversion and electron-capture channels in the radioactive decay of these bare nuclei. The experimental results are in g…

PhysicsNuclear and High Energy PhysicsSchottky diodeHighly-charged ionsRing (chemistry)Mass spectrometryHalf-livesStorage ringsInternal conversionFragmentation (mass spectrometry)IonizationNuclideAtomic physicsNuclear ExperimentExotic nucleiRadioactive decayPhysics Letters B
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Nature of seniority symmetry breaking in the semimagic nucleus $^{94}Ru$

2022

Physical review / C 105(3), L031304 (2022). doi:10.1103/PhysRevC.105.L031304

Nuclear Theoryddc:530Nuclear Experimentydinfysiikka530
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Energy and range focusing of in-flight separated exotic nuclei – A study for the energy-buncher stage of the low-energy branch of the Super-FRS

2003

Abstract The relative momentum spread of in-flight separated exotic nuclear beams produced in fragmentation and/or fission reactions is of the order of a few percent. A new technique is presented, which reduces the momentum spread significantly, and first experimental results obtained with relativistic projectile fragments are shown. This technique is the key to experiments with slowed-down and stopped beams, in particular for the efficient stopping of relativistic exotic nuclei in gas-filled stopping cells. It will be employed at the energy-buncher stage of the low-energy branch of the Super-FRS facility. The ion-optical design of the energy buncher is presented and a brief outlook to the …

Nuclear physicsPhysicsNuclear and High Energy PhysicsLow energyFissionProjectileNuclear TheoryPhysics::Accelerator PhysicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Direct mass measurements on neutron-deficient xenon isotopes with the ISOLTRAP mass spectrometer

2002

The masses of Xe isotopes with 124 A 114 have been measured using the ISOLTRAP spectrometer at the on-line mass separator ISOLDE/CERN. A mass resolving power of 500000 was chosen resulting in an accuracy of m 12 keV for all isotopes investigated. Con icts with existing mass data of several standard deviations were found. peerReviewed

massaspektrometriaatomic massesXenon isotopesPhysics::Instrumentation and Detectorspenning trapNuclear Experimentradioactive ions
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Continuum excitations in6He

1999

T. Aumann et al. ; 11 pags.; 6 figs.; 2 tabs. ; PACS number(s): 27.20.1n, 25.60.Gc, 25.70.De, 29.30.Hs

PhysicsNuclear and High Energy PhysicsAngular distributionContinuum (topology)Giant resonanceExcited stateQuantum mechanicsCoulomb excitationInelastic scatteringAtomic physicsIsotopes of heliumResonance (particle physics)Physical Review C
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First spatial isotopic separation of relativistic uranium projectile fragments

1994

Abstract Spatial isotopic separation of relativistic uranium projectile fragments has been achieved for the first time. The fragments were produced in peripheral nuclear collisions and spatially separated in-flight with the fragment separator FRS at GSI. A two-fold magnetic-rigidity analysis was applied exploiting the atomic energy loss in specially shaped matter placed in the dispersive central focal plane. Systematic investigations with relativistic projectiles ranging from oxygen up to uranium demonstrate that the FRS is a universal and powerful facility for the production and in-flight separation of monoisotopic, exotic secondary beams of all elements up to Z = 92. This achievement has …

Nuclear and High Energy PhysicsTheoryofComputation_COMPUTATIONBYABSTRACTDEVICES010308 nuclear & particles physicsChemistryProjectileNuclear TheoryTheoryofComputation_GENERALSeparator (oil production)chemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]UraniumAccelerators and Storage RingsComputingMethodologies_ARTIFICIALINTELLIGENCE01 natural sciencesNuclear physicsComputingMethodologies_PATTERNRECOGNITIONCardinal point0103 physical sciencesMonoisotopic massAtomic physicsNuclear Experiment010306 general physicsInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Lifetime measurement of neutron-rich even-even molybdenum isotopes

2017

D. Ralet et al. -- 11 pags., 10 figs., 3 tabs.

chemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesNuclear physicsSubatomic Physics0103 physical sciencesNeutronddc:530010306 general physicsMass numberPhysicsIsotope010308 nuclear & particles physicsrelativistic projectile fragmentation3. Good healthsecondary fragmentationgamma-ray spectroscopychemistryMolybdenumExcited stateQuadrupoleFísica nuclearAGATAAtomic physicsEnergy (signal processing)
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Giant resonances in unstable oxygen isotopes

1999

Abstract Electromagnetic and nuclear breakup of the neutron-rich Oxygen isotopes ranging from A = 17 to A = 22 is studied experimentally in reactions at energies around 600 MeV/u. The beams were produced in fragmentation reactions and separated by the GSI Fragment Separator FRS. By measuring the four-momenta of all decay products after inelastic scattering and neutron decay of the projectile, the excitation energy is determined. From the differential cross sections dσ dE ∗ for electromagnetic excitation, the E1-strength distributions can be deduced. For 18,20,22O, low-lying dipole strength is observed, exhausting about 5% of the Thomas Reiche Kuhn sumrule for energies up to 5 MeV above the …

PhysicsNuclear reactionNuclear and High Energy PhysicsScatteringNuclear TheoryInelastic scatteringIsotopes of oxygenNuclear physicsDipoleGiant resonanceNeutronAtomic physicsNuclear ExperimentExcitationNuclear Physics A
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First isochronous mass spectrometry at the experimental storage ring ESR

2000

Short-lived exotic nuclei can be produced and separated with the high-energy secondary nuclear beam facility FRS at GSI. These nuclides can be injected and stored in the storage ring ESR. The lower lifetime limit of the presently existing methods for mass measurements on these nuclides at the ESR is about a few seconds. We have developed and investigated an isochronous operational mode of the ESR, that makes mass measurements of nuclides with lifetimes down to a few ls feasible. It has been commissioned in experiments using long-lived nuclides with known masses. A mass resolving power of about 150 000 has been achieved in a "rst pilot experiment. A suitable detector system has been implemen…

PhysicsNuclear and High Energy PhysicsResolution (mass spectrometry)SpectrometerIsotopeMass spectrometryIsotope separationlaw.inventionNuclear physicslawMeasuring instrumentNuclideInstrumentationStorage ringNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Dawning of the N=32 shell closure seen through precision mass measurements of neutron-rich titanium isotopes

2018

A precision mass investigation of the neutron-rich titanium isotopes 51 − 55 Ti was performed at TRIUMF’s Ion Trap for Atomic and Nuclear science (TITAN). The range of the measurements covers the N = 32 shell closure, and the overall uncertainties of the 52 − 55 Ti mass values were significantly reduced. Our results conclusively establish the existence of the weak shell effect at N = 32 , narrowing down the abrupt onset of this shell closure. Our data were compared with state-of-the-art ab initio shell model calculations which, despite very successfully describing where the N = 32 shell gap is strong, overpredict its strength and extent in titanium and heavier isotones. These measurements a…

Materials scienceNuclear Theorynucl-thNuclear TheoryAb initioGeneral Physics and Astronomychemistry.chemical_elementFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Mass spectrometrynucl-ex01 natural sciencesNuclear Theory (nucl-th)symbols.namesake0103 physical sciencesPhysics::Atomic and Molecular ClustersNeutron[ PHYS.NEXP ] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentIsotope010308 nuclear & particles physicsStarke Wechselwirkung und exotische Kerne – Abteilung BlaumPenning trapchemistry13. Climate actionsymbolsIon trapAtomic physicsTitan (rocket family)Titanium
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Searching for the 5H resonance in the t+n+n system

2003

19 pages, 7 figures, 2 tables, 2 appendices.-- PACS nrs.: 27.10.+h; 25.60.Gc.-- Printed version published Jul 28, 2003.

PhysicsNuclear reactionNuclear and High Energy PhysicsComparisons with previous resultsMeasured triton and neutron relative energy spectra energy and angular correlationsHyperspherical harmonic expansion analysisResonance[PACS] Properties of specific nuclei listed by mass ranges: A ≤ 5Nuclear Reactions C(6Hent) (6He2nt) E=240 MeV/nucleonNuclear physicsNuclear magnetic resonanceA ≤ 5 [[PACS] Properties of specific nuclei listed by mass ranges]45H deduced resonance features[PACS] Breakup and momentum distributionsNuclear Physics A
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Direct mass measurements above uranium bridge the gap to the island of stability

2010

The mass of an atom incorporates all its constituents and their interactions. The difference between the mass of an atom and the sum of its building blocks (the binding energy) is a manifestation of Einstein's famous relation E = mc(2). The binding energy determines the energy available for nuclear reactions and decays (and thus the creation of elements by stellar nucleosynthesis), and holds the key to the fundamental question of how heavy the elements can be. Superheavy elements have been observed in challenging production experiments, but our present knowledge of the binding energy of these nuclides is based only on the detection of their decay products. The reconstruction from extended d…

Nuclear physicsMass numberMultidisciplinaryMass excessAtomic mass constantIsotopeChemistryNuclideAtomic physicsNuclear ExperimentAtomic massBeta-decay stable isobarsSpontaneous fission
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High-resolution, accurate MR-TOF-MS for short-lived, exotic nuclei of few events in their ground and low-lying isomeric states

2019

Mass measurements of fission and projectile fragments, produced via $^{238}$U and $^{124}$Xe primary beams, have been performed with the multiple-reflection time-of-flight mass spectrometer (MR-TOF-MS) of the FRS Ion Catcher with a mass resolving powers (FWHM) up to 410,000 and an uncertainty of $6\cdot 10^{-8}$. The nuclides were produced and separated in-flight with the fragment separator FRS at 300 to 1000 MeV/u and thermalized in a cryogenic stopping cell. The data-analysis procedure was developed to determine with highest accuracy the mass values and the corresponding uncertainties for the most challenging conditions: down to a few events in a spectrum and overlapping distributions, ch…

Physics - Instrumentation and DetectorsFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)Nuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Breakdown of the Isobaric Multiplet Mass Equation atA=33,T=3/2

2001

Mass measurements on ${}^{33,34,42,43}\mathrm{Ar}$ were performed using the Penning trap mass spectrometer ISOLTRAP and a newly constructed linear Paul trap. This arrangement allowed us, for the first time, to extend Penning trap mass measurements to nuclides with half-lives below one second ( ${}^{33}\mathrm{Ar}$: ${T}_{1/2}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}174\mathrm{ms}$). A mass accuracy of about ${10}^{\ensuremath{-}7}$ $(\ensuremath{\delta}m\ensuremath{\approx}4\mathrm{keV})$ was achieved for all investigated nuclides. The isobaric multiplet mass equation was checked for the $A\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}33$, $T\phantom{\rule{0ex}{0ex}}=\phantom…

Mass formulaPhysicsMass numberGeneral Physics and AstronomyIsobaric processIon trapAtomic physicsQuadratic form (statistics)Penning trapISOLTRAPMultipletPhysical Review Letters
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Production and trapping of carbon clusters for absolute mass measurements at ISOLTRAP

2001

Singly-charged carbon clusters C/sub n//sup +/ (n >or= 1) have been produced by laser-induced desorption and fragmentation of C/sub 60/ fullerenes and have been injected into and stored in the Penning trap system of the ISOLTRAP mass spectrometer at ISOLDE/CERN. The present study is the first step to extend the until now direct mass measurements at ISOLTRAP to absolute mass measurements by using clusters of /sup 12/C. (10 refs).

PhysicsNuclear and High Energy PhysicsFullereneTrappingPenning trapMass spectrometryISOLTRAPMassFragmentation (mass spectrometry)DesorptionPhysics::Atomic and Molecular ClustersNuclear Physics - ExperimentAtomic physicsNuclear Experiment
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Accurate masses of neutron-deficient nuclides close to

2001

Abstract Mass measurements with the Penning-trap mass spectrometer ISOLTRAP at ISOLDE/CERN are extended to nonsurface ionizable species using newly developed ion-beam bunching devices. Masses of 179–197Hg, 196,198Pb, 197Bi, 198Po and 203At were determined with an accuracy of 1×10 −7 corresponding to δm≈20  keV. Applying a resolving power of up to 3.7×10 6 ground and isomeric states of 185,187,191,193,197Hg were separated. First experimental values for the isomeric excitation energy of 187,191Hg are obtained. A least-squares adjustment has been performed and theoretical approaches are discussed to model the observed fine structure in the binding energy.

PhysicsNuclear and High Energy PhysicsBinding energyNeutronNuclideAtomic physicsMass spectrometryPenning trapISOLTRAPAtomic massExcitationNuclear Physics A
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Photoneutron cross sections for unstable neutron-rich oxygen isotopes.

2000

The dipole response of stable and unstable neutron-rich oxygen nuclei of masses A = 17 to A = 22 has been investigated experimentally utilizing electromagnetic excitation in heavy-ion collisions at beam energies about 600 MeV/nucleon. A kinematically complete measurement of the neutron decay channel in inelastic scattering of the secondary beam projectiles from a Pb target was performed. Differential electromagnetic excitation cross sections d sigma/dE were derived up to 30 MeV excitation energy. In contrast to stable nuclei, the deduced dipole strength distribution appears to be strongly fragmented and systematically exhibits a considerable fraction of low-lying strength.

Nuclear reactionPhysicsDipoleScatteringNuclear TheoryHadronGeneral Physics and AstronomyNeutronInelastic scatteringAtomic physicsNuclear ExperimentNucleonExcitationPhysical review letters
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Invariant-mass spectroscopy of $^{10}$Li and $^{11}$Li

1997

Break-up of secondary Li-11 ion beams (280 MeV/nucleon) on C and Pb targets into Li-9 and neutrons is studied experimentally. Cross sections and neutron multiplicity distributions are obtained, characterizing different reaction mechanisms. Invariant-mass spectroscopy for Li-11 and Li-10 is performed. The E1 strength distribution, deduced from electromagnetic excitation of Li-11 up to an excitation energy of 4 MeV comprises similar to 8% of the Thomas-Reiche-Kuhn energy-weighted sumrule strength. Two low-lying resonance-like structures are observed for Li-10 at decay energies of 0.21(5) and 0.62(10) MeV, the former one carrying 26(10)% of the strength and likely to be associated with an s-wa…

PhysicsNuclear reactionNuclear and High Energy Physics010308 nuclear & particles physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Nuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesIon0103 physical sciencesInvariant massNeutronAtomic physicsMultiplicity (chemistry)Nuclear Experiment010306 general physicsNucleonSpectroscopyExcitationNuclear Physics
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Towards Shorter-Lived Nuclides in ISOLTRAP Mass Measurements

2001

Recently, the applicability of Penning trap mass spectrometry has been extended to nuclides with a half-life of less than one second. The mass of 33Ar(T 1/2 = 174 ms) was measured using the ISOLTRAP spectrometer with an accuracy of 4.2 keV. This measurement provided a stringent test of the Isobaric Multiplet Mass Equation (IMME) at mass number A = 33 and isospin T = 3/2. The fast measurement cycle that shows the way to other measurements of very-short-lived nuclides is presented. Furthermore, the results of the IMME test are displayed.

Nuclear physicsMass numberChemistryNuclideIon trapAtomic physicsMass spectrometryPenning trapISOLTRAPAtomic massHybrid mass spectrometer
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Extension of Penning-trap mass measurements to very short-lived nuclides

2000

Abstract Mass measurements on 33,34,42,43 Ar have been performed at the ISOLTRAP spectrometer. An accuracy of δm ≈4 keV has been achieved for all measured isotopes. With 33 Ar it is the first time that a nuclide with a half-life shorter than one second has been investigated using a Penning trap. This became possible due to the recently installed linear radio-frequency ion-trap system and an improved, faster measurement cycle.

PhysicsNuclear and High Energy PhysicsSpectrometerIsotope010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trap7. Clean energy01 natural sciencesISOLTRAPAtomic massNuclear physics13. Climate action0103 physical sciencesNuclear Physics - ExperimentIon trapNuclideAtomic physics010306 general physicsHybrid mass spectrometerNuclear Physics A
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Neutron momentum distributions from "core break-up" reactions of halo nuclei

1995

Neutron angular distributions from violent break-up reactions of Li-11 and Be-11 have been measured at 28 MeV/u and 280 MeV/u and at 41 MeV/u and 460 MeV/u, respectively. The derived neutron momentum distributions show a narrow component in transverse momentum that is within uncertainties independent of beam energy and target charge. This component is suggested to be simply related to the momentum distribution of the loosely bound halo neutron(s) in the projectiles.

PhysicsBreak-UpProjectileAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGeneral Physics and AstronomyNuclear physicsTransverse momentumPhysics::Accelerator PhysicsNeutronHaloAtomic physicsNuclear ExperimentBeam energyNuclear Physics
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Simultaneous Measurement ofβ−Decay to Bound and Continuum Electron States

2005

We report the first measurement of a ratio {lambda}{sub {beta}{sub b}}/{lambda}{sub {beta}{sub c}} of bound-state ({lambda}{sub {beta}{sub b}}) and continuum-state ({lambda}{sub {beta}{sub c}}) {beta}{sup -}-decay rates for the case of bare {sup 207}Tl{sup 81+} ions. These ions were produced at the GSI fragment separator FRS by projectile fragmentation of a {sup 208}Pb beam. After in-flight separation with the B{rho}-{delta}E-B{rho} method, they were injected into the experimental storage-ring ESR at an energy of 400.5A MeV, stored, and electron cooled. The number of both the {sup 207}Tl{sup 81+} ions and their bound-state {beta}{sup -}-decay daughters, hydrogenlike {sup 207}Pb{sup 81+} ion…

PhysicsCrystallographyBound stateGeneral Physics and AstronomyContinuum (set theory)ElectronAtomic physicsLambdaBeta decayEnergy (signal processing)Spectral lineIonPhysical Review Letters
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Measurement of the dipole response of neutron-rich nuclei in the A∼20 region

2002

Abstract Coulomb break up of the neutron-rich 15,17 C and 17–22 O isotopes has been studied experimentally using secondary beams at energies of 500–600 MeV/u. A comparison between differential cross sections, d σ/ d E ∗ , with that obtained from a binary model shows that the main ground-state configuration of 15 C is 14 C(0 + )⊗ ν S 1/2 as expected. For 17 C, our preliminary data analysis reveals that the predominant (∼64%) configuration of the ground state is 16 C(2 + )⊗ ν s , d . For 17–22 O, the low-lying E1 strength amounts up to about 12% of the energy weighted sum rule strength depending on neutron number. The energy weighted E1 strength (integrated up to 15 MeV excitation energy) inc…

PhysicsNuclear and High Energy PhysicsDipoleIsotopeNeutron numberCoulombNeutronSum rule in quantum mechanicsAtomic physicsGround stateExcitationNuclear Physics A
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Dissociation of 8He into 6He + n + X at 240 MeV/u

1995

4 pages, 3 figures, 2 tables.

PhysicsNuclear and High Energy PhysicsPhysical chemistryDissociation (chemistry)
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Fragmentation of exotic oxygen isotopes

2003

Abrasion-ablation models and the empirical EPAX parametrization of projectile fragmentation are described. Their cross section predictions are compared to recent data of the fragmentation of secondary beams of neutron-rich, unstable 19,20,21O isotopes at beam energies near 600 MeV/nucleon as well as data for stable 17,18O beams.

PhysicsNuclear physicsIsotopeFragmentation (mass spectrometry)Nuclear TheoryGeneral Physics and AstronomyPhysics::Accelerator PhysicsAtomic physicsNucleonNuclear ExperimentProjectile fragmentationIsotopes of oxygenBeam (structure)
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New results with stored exotic nuclei at relativistic energies

2004

Recently, much progress has been made with stored exotic nuclei at relativistic velocities ( v c = 0.7 ) . Fragments of 208Pb and 209Bi projectiles and fission products from 238U ions were produced, separated in flight with the fragment separator FRS, and injected into the storage-cooler ring ESR for precision measurements. 114 new masses of neutron-deficient isotopes in the lead region have been measured with time-resolved Schottky Mass Spectrometry (SMS). A new isospin dependence of the pairing energy was observed due to the improved mass accuracy of typically 1.5×10-7 (30 keV). New masses of short-lived neutron-rich fission fragments have been obtained with Isochronous Mass Spectrometry …

PhysicsNuclear and High Energy PhysicsFission productsIsotopeFissionNuclear TheoryMass spectrometrylaw.inventionIonNuclear physicslawIsospinAtomic physicsNuclear ExperimentSpectroscopyElectron coolingNuclear Physics A
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β -decay half-lives and β -delayed neutron emission probabilities for several isotopes of Au, Hg, Tl, Pb, and Bi, beyond N=126

2017

Background: Previous measurements of Beta-delayed neutron emitters comprise around 230 nuclei, spanning from the 8He up to 150La. Apart from 210Tl, with a minuscule branching ratio of 0.07%, no other neutron emitter is measured yet beyond A = 150. Therefore new data are needed, particularly in the heavy mass region around N=126, in order to guide theoretical models and to understand the formation of the third r-process peak at A 195. Purpose: To measure both, Beta-decay half-lives and neutron branching ratios of several neutron-rich Au, Hg, Tl, Pb and Bi isotopes beyond N = 126. Method: Ions of interest are produced by fragmentation of a 238U beam, selected and identifed via the GSI-FRS fra…

PhysicsIsotope010308 nuclear & particles physicsBranching fraction01 natural sciences7. Clean energyIon0103 physical sciencesNeutron detectionr-processNeutronAtomic physics010306 general physicss-processDelayed neutronPhysical Review C
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Study of Basic Nuclear Properties of Highly-Charged, Unstable Nuclei at the SIS-FRS-ESR Complex

2004

Recent progress in experiments with exotic nuclear beams at the SIS-FRS-ESR facility is summarized. New results on gross properties of exotic nuclei like binding energy, half-lives, and decay modes are presented. A brief outlook to future experiments is given.

PhysicsElastic scatteringNuclear and High Energy PhysicsScatteringNuclear TheoryHadronBinding energyGeneral Physics and AstronomyHalf-lifeBeta decayAtomic massNuclear physicsAtomic physicsNuclear ExperimentRadioactive decayActa Physica Hungarica A) Heavy Ion Physics
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Experimental Setup for hypernuclear study at the Super-FRS

2014

GSI Scientific Report 2013 - GSI Report 2014-1

Physics
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Recent Upgrades of the SHIPTRAP Setup: On the Finish Line Towards Direct Mass Spectroscopy of Superheavy Elements

2016

With the Penning-trap mass spectrometer SHIPTRAP at GSI, Darmstadt, it is possible to investigate exotic nuclei in the region of the heaviest elements. Few years ago, challenging experiments led to the direct measurements of the masses of neutron-deficient isotopes with Z = 102,103 around N = 152. Thanks to recent advances in cooling and ion-manipulation techniques, a major technical upgrade of the setup has been recently accomplished to boost its efficiency. At present, the gap to reach more rare and shorter-lived species at the limits of the nuclear landscape has been narrowed. ispartof: pages:423-429 ispartof: Acta Physica Polonica B vol:48 issue:3 pages:423-429 ispartof: location:Zakopa…

PhysicsIsotopePenning trapGeneral Physics and AstronomyFinish lineSuperheavy Elements[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Accelerator Physics and InstrumentationPenning trapMass spectrometry01 natural sciences7. Clean energy010305 fluids & plasmasNuclear physicsUpgrade0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physics
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Mass mapping of a new area of neutron-deficient suburanium nuclides

2002

Abstract The masses of 64 short-lived neutron-deficient nuclides covering the element range from tungsten to uranium have been obtained for the first time. They have been evaluated by combining directly measured masses from Schottky mass spectrometry with linked experimental Q-values in α-decay chains. Based on these new mass data we have determined the one-proton and two-proton drip-lines as well as the size of the “littoral shallow” of the sea of instability. No evidence of a Thomas–Ehrman shift has been found in the region of the investigated heavy nuclides. A peculiar behavior of two-proton separation energies has been observed in the lead region. The predictive power of various mass mo…

Nuclear physicsPhysicsNuclear and High Energy PhysicsIsotopes of uraniumIsotopeNuclear TheoryMass spectrumNeutronNuclideNuclear ExperimentMass spectrometryRadioactive decayIsotopes of thoriumNuclear Physics A
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Study of the Unstable NucleusL10iin Stripping Reactions of the Radioactive ProjectilesB11eandL11i

1995

Reactions of the halo systems Be-11 and Li-11 (at 460 and 280 MeV/nucleon) with a carbon target demonstrate that (n + Li-9) has an (unbound) l = 0 ground state very close to the threshold. The neutron halo of Li-11 has appreciable (1s(1/2))(2) and (0p(1/2))(2) components.

PhysicsStripping (chemistry)ProjectileAnalytical chemistryGeneral Physics and Astronomychemistry.chemical_elementmedicine.anatomical_structurechemistrymedicineNeutronHaloAtomic physicsNucleonGround stateNucleusCarbonPhysical Review Letters
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Fast-timing Measurement in \(^{96}\)Pd: Improved Accuracy for the Lifetime of the \(4_1^{+}\) State

2023

Direct lifetime measurements via γ–γ coincidences using the FATIMA fast-timing LaBr3(Ce) array were performed for the excited states below previously reported isomers. In the N = 50 semi-magic 96Pd nucleus, lifetimes below the I π = 8+ seniority isomer were addressed as a benchmark for further analysis. The results for the I π = 2+ and 4 + states confirm the published values. Increased accuracy for the lifetime value was achieved for the 4 + state. peerReviewed

General Physics and AstronomyydinfysiikkaActa Physica Polonica B Proceedings Supplement
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Halo excitations in fragmentation of He at 240 MeV/u on carbon and lead targets

2000

Dissociation of a 240 MeV/u beam of He-6, incident on carbon and lead targets, has been studied in kinematically complete experiments to investigate low-lying excitation modes in the halo nucleus He-6. It is shown that alignment effects characterize the inelastic scattering and allow an unambiguous assignment of the spin of a narrow resonance observed in the excitation energy spectrum. The differential cross sections for the He-6 inelastic scattering on carbon and lead targets were deduced from the measured moments of the two neutrons and the a-particle. An analysis of these distributions shows that quadrupole and, possibly, monopole excitations characterize the hadronic interaction, while …

PhysicsNuclear and High Energy PhysicsFragmentation (mass spectrometry)QuadrupoleCoulombHalo nucleusNeutronAtomic physicsInelastic scatteringResonance (particle physics)ExcitationNuclear Physics A
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Extending Penning trap mass measurements with SHIPTRAP to the heaviest elements

2013

Penning-trap mass spectrometry of radionuclides provides accurate mass values and absolute binding energies. Such mass measurements are sensitive indicators of the nuclear structure evolution far away from stability. Recently, direct mass measurements have been extended to the heavy elements nobelium (Z=102) and lawrencium (Z=103) with the Penning-trap mass spectrometer SHIPTRAP. The results probe nuclear shell effects at N=152. New developments will pave the way to access even heavier nuclides.

Nuclear physicschemistryBinding energychemistry.chemical_elementNuclear binding energyTransactinide elementNuclideNobeliumAtomic physicsMass spectrometryPenning trapLawrenciumAIP Conference Proceedings
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Development and test of iron-free quadrupole lenses with high magnetic flux densities

2003

Abstract Iron-free magnetic quadrupole lenses have been developed for the focusing of energetic bunched heavy-ion beams. These devices are operated in a pulsed mode and provide very strong magnetic fields. A magnetic flux density of more than 14 T has been reached in a 100 mm long quadrupole with a 20 mm wide aperture, which corresponds to a magnetic flux density of ∼1400 T/m. The pulse duration of the applied electric current is approximately 300 μs with a flat top of several μs. The calculated and measured field properties of the quadrupoles are presented. In a first test experiment with a fast-extracted 650 MeV/u 197 Au 79+ beam (bunch length ∼500 ns) at GSI the focusing properties could…

PhysicsNuclear and High Energy PhysicsMagnetQuadrupolePhysics::Accelerator PhysicsPulse durationElectric currentAtomic physicsQuadrupole magnetInstrumentationMagnetic fluxStorage ringMagnetic fieldNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Superallowed Gamow-Teller decay of the doubly magic nucleus $^{100}$Sn

2012

Expérience au GSI; The shell structure of atomic nuclei is associated with 'magic numbers' and originates in the nearly independent motion of neutrons and protons in a mean potential generated by all nucleons. During b1-decay, a proton transforms into a neutron in a previously not fully occupied orbital, emitting a positron-neutrino pair with either parallel or antiparallel spins, in a Gamow-Teller or Fermi transition, respectively. The transition probability, or strength, of a Gamow-Teller transition depends sensitively on the underlying shell structure and is usually distributed among many states in the neighbouring nucleus. Here we report measurements of the half-life and decay energy fo…

PhysicsMultidisciplinaryProton010308 nuclear & particles physicsProton decayNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta decayNuclear physicsDecay energy0103 physical sciencesAtomic nucleusPhysical SciencesFysikNeutronAtomic physics010306 general physicsNucleonNuclear ExperimentRadioactive decay
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Mass Measurements of Very Neutron-Deficient Mo and Tc Isotopes and Their Impact on rp Process Nucleosynthesis

2011

The masses of ten proton-rich nuclides, including the N=Z+1 nuclides 85-Mo and 87-Tc, were measured with the Penning trap mass spectrometer SHIPTRAP. Compared to the Atomic Mass Evaluation 2003 a systematic shift of the mass surface by up to 1.6 MeV is observed causing significant abundance changes of the ashes of astrophysical X-ray bursts. Surprisingly low alpha-separation energies for neutron-deficient Mo and Tc are found, making the formation of a ZrNb cycle in the rp process possible. Such a cycle would impose an upper temperature limit for the synthesis of elements beyond Nb in the rp process.

PhysicsIsotope010308 nuclear & particles physicsGeneral Physics and AstronomyFOS: Physical sciencesrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trapMass spectrometry7. Clean energy01 natural sciencesAtomic massNuclear physics13. Climate actionNucleosynthesis0103 physical sciencesNeutronNuclideNuclear Experiment (nucl-ex)010306 general physicsNuclear Experiment
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The Super-FRS Project at GSI

2002

The GSI projectile fragment separator FRS has demonstrated with many pioneering experiments the research potential of in-flight separators at relativistic energies. Although the present facility has contributed much to the progress in the field of nuclear structure physics, major improvements are desirable in the future. The characteristics of the proposed next-generation facility at GSI, the Super-FRS, will be presented and compared to other projects. The Super-FRS is a large-acceptance superconducting fragment separator followed by different experimental branches including a combination with a new storage-cooler ring system. This system consists of a collector ring (CR) and a new experime…

PhysicsNuclear and High Energy Physics[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]ProjectileScatteringNuclear structureSuperconducting magnetic energy storageElectron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]XXCharged particleNuclear physicsNuclear ExperimentInstrumentationElectron scatteringStorage ring
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Direct Mapping of Nuclear Shell Effects in the Heaviest Elements

2014

Quantum-mechanical shell effects are expected to strongly enhance nuclear binding on an "island of stability" of superheavy elements. The predicted center at proton number $Z=114,120$, or $126$ and neutron number $N=184$ has been substantiated by the recent synthesis of new elements up to $Z=118$. However the location of the center and the extension of the island of stability remain vague. High-precision mass spectrometry allows the direct measurement of nuclear binding energies and thus the determination of the strength of shell effects. Here, we present such measurements for nobelium and lawrencium isotopes, which also pin down the deformed shell gap at $N=152$.

PhysicsMultidisciplinaryIsotopeNuclear TheoryBinding energyShell (structure)FOS: Physical scienceschemistry.chemical_elementIsland of stabilityNuclear physicschemistryNeutron numberNobeliumAtomic numberNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentLawrenciumScience
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8He-6He: a comparative study of nuclear fragmentation reactions

2001

19 pages, 3 tables, 6 figures.-- PACS nrs.: 27.20.+n; 24.70.+s; 25.06.-t.-- Available online Dec 4, 2000.

PhysicsNuclear and High Energy Physics[PACS] Polarization phenomena in reactionsResonanceHalo nucleusInelastic scatteringDissociation (chemistry)6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Fragmentation (mass spectrometry)NeutronAtomic physics[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Ground stateExcitation
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He-8 - He-6: a comparative study of electromagnetic fragmentation reactions

2002

14 pages, 1 table, 2 figures.-- PACS nrs.:27.20.+n; 24.70.+.-- Available online Oct 8, 2001.

PhysicsNuclear and High Energy PhysicsNuclear Reactions: Pb(He-8xn He-6) E=227 MeV/nucleonNuclear TheoryHalo nucleusElectromagnetic fragmentationB(E1)Dissociation (chemistry)Nuclear physics6 ≤ A ≤ 19 [[PACS] Properties of specific nuclei listed by mass ranges]Measured σ σ(Θ) σ(E)He-8 deduced resonance energyPb(He-6xnα) E=240 MeV/nucleonNeutronAtomic physics[PACS] Properties of specific nuclei listed by mass ranges: 6 ≤ A ≤ 19Nuclear ExperimentPb(He-8xn He-6) E=227 MeV/nucleon [Nuclear Reactions]
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The FIRST experiment at GSI

2012

The FIRST (Fragmentation of Ions Relevant for Space and Therapy) experiment at the SIS accelerator of GSI laboratory in Darmstadt has been designed for the measurement of ion fragmentation cross-sections at different angles and energies between 100 and 1000 MeV/nucleon. Nuclear fragmentation processes are relevant in several fields of basic research and applied physics and are of particular interest for tumor therapy and for space radiation protection applications. The start of the scientific program of the FIRST experiment was on summer 2011 and was focused on the measurement of 400 MeV/nucleon 12C beam fragmentation on thin (8 mm) graphite target. The detector is partly based on an alread…

Nuclear and High Energy PhysicsIon beamPhysics::Instrumentation and Detectorsmedicine.medical_treatmentNuclear physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ScintillatorElementary-particleFIRST7. Clean energy01 natural sciencesParticle detectorWire chamberNuclear physicsDipole magnetFragmentationPARTICLE THERAPYhadrontherapy; fragmentation; nuclear physics; elementary-particle; instrumentation; experimental methodsHadrontherapy0103 physical sciencesmedicineNeutron detectionddc:530Gaseous detectorION-BEAM010306 general physicsNuclear ExperimentDETECTORInstrumentationGEANT4PARTICLE THERAPY; FLUKA CODE; ION-BEAM; FRAGMENTATION; BENCHMARKING; RADIOTHERAPY; TRANSPORT; DETECTOR; GEANT4; FIRSTPhysicsParticle therapyTime projection chamber010308 nuclear & particles physicsExperimental methodsDetectorScintillatorTRANSPORTSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Hadrontherapy; Fragmentation; Nuclear physics; Elementary-particle; Experimental methods; InstrumentationFLUKA CODEBENCHMARKINGElementary-particle; Experimental methods; Fragmentation; Hadrontherapy; Instrumentation; Nuclear physics; Instrumentation; Nuclear and High Energy PhysicsRADIOTHERAPY
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The dipole response of nuclei with large neutron excess

2003

The dipole response of neutron-rich nuclei in the mass range from A = 10 to A = 22 and with mass to charge ratios of 2.5 to 2.8 has been invesitigated experimentally utilizing electromagnetic excitation in heavy-ion collisions at beam energies around 600 MeV/u.

PhysicsNuclear reactionDipoleNeutron emissionNuclear TheoryNeutronInelastic scatteringAtomic physicsNuclear ExperimentSpin (physics)ExcitationRadioactive decay
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Mass measurements on unstable Sn and Sr isotopes with the ISOLTRAP mass spectrometer

2001

Direct mass measurements have been performed on the isotopes 76,77,80,81Sr and 129,130,131,132Sn by means of the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. In the case of 76Sr the mass was measured for the first time and an accuracy of about 30 keV was reached (Fig. 1). The masses of the tin isotopes are known for a long time from Q β measurements.

PhysicsLarge Hadron ColliderIsotope[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex][PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Penning trapMass spectrometry01 natural sciencesISOLTRAP010305 fluids & plasmasNuclear physics0103 physical sciencesIsotopes of tin010306 general physics
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Experiments with stored exotic nuclei at relativistic energies

2006

Abstract A review and recent progress are presented from experiments on masses and lifetimes of bare and few-electron exotic nuclei at GSI. Relativistic rare isotopes produced via projectile fragmentation and fission were separated in flight by the fragment separator FRS and injected into the storage ring ESR. This worldwide unique experimental method gives access to all fragments with half-lives down to the microsecond range. The great research potential is demonstrated by the discovery of new isotopes along with simultaneous mass and lifetime measurements. Single particle decay measurements and the continuous recording of both stored mother and daughter nuclei open up a new era for nuclea…

PhysicsIsotopeFissionNuclear TheoryCondensed Matter PhysicsNuclear physicsMicrosecondParticle decayIonizationNuclear spectroscopyPhysical and Theoretical ChemistryAtomic physicsNuclear ExperimentInstrumentationProjectile fragmentationSpectroscopyStorage ringInternational Journal of Mass Spectrometry
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β-decay and β-delayed Neutron Emission Measurements at GSI-FRS Beyond N=126, for r-process Nucleosynthesis

2014

New measurements of very exotic nuclei in the neutron-rich region beyond N=126 have been performed at the GSI facility with the fragment separator (FRS). The aim of the experiment is to determine half-lives and β-delayed neutron emission branching ratios of isotopes of Hg, Tl and Pb in this region. This contribution summarizes final counting statistics for identification and for implantation, as well as the present status of the data analysis of the half-lives. In summary, isotopes of Pt, Au, Hg, Tl, Pb, Bi, Po, At, Rn and Fr were clearly identified and several of them (208-211Hg, 211-215Tl, 214-218Pb) were implanted with enough statistics to determine their half-lives. About half of them a…

PhysicsNuclear and High Energy PhysicsIsotope010308 nuclear & particles physicsNeutron emissionBranching fraction01 natural sciencesNuclear physicsNucleosynthesis0103 physical sciencesr-processNeutron010306 general physicss-processDelayed neutronNuclear Data Sheets
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Longitudinal and transverse momentum distributions of 9Li fragments from break-up of 11Li

1995

7 pages, 3 figures, 1 table.

PhysicsNuclear and High Energy PhysicsTransverse planeFull width at half maximumMomentum (technical analysis)Break-UpSignificant differenceTransverse momentumSigmaHaloAtomic physicsNuclear Physics
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Schottky mass measurements of stored and cooled neutron-deficient projectile fragments in the element range of 57≤Z≤84

2000

Abstract A novel method for direct, high precision mass measurements of relativistic exotic nuclei has been successfully applied in the storage ring ESR at GSI. The nuclei of interest were produced by projectile fragmentation of 930 MeV / u bismuth ions, separated in-flight by the fragment separator FRS, stored and cooled in the ESR. The mass values have been deduced from the revolution frequencies of the coasting cooled ions. We have measured 104 new mass values with a precision of about 100 keV and a resolving power of 3.5×10 5 for the neutron-deficient isotopes of the elements 57≤Z≤84 . This paper presents the experimental method, the mass evaluation and a table of the experimental mass …

PhysicsNuclear and High Energy PhysicsRange (particle radiation)IsotopeProjectileNuclear TheorySchottky diodechemistry.chemical_elementIonBismuthNuclear physicschemistryNeutronAtomic physicsNuclear ExperimentStorage ringNuclear Physics A
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FIRST experiment: Fragmentation of Ions Relevant for Space and Therapy

2013

International audience; Nuclear fragmentation processes are relevant in different fields of basic research and applied physics and are of particular interest for tumor therapy and for space radiation protection applications. The FIRST (Fragmentation of Ions Relevant for Space and Therapy) experiment at SIS accelerator of GSI laboratory in Darmstadt, has been designed for the measurement of different ions fragmentation cross sections at different energies between 100 and 1000 MeV/nucleon. The experiment is performed by an international collaboration made of institutions from Germany, France, Italy and Spain. The experimental apparatus is partly based on an already existing setup made of the …

HistorySilicon detectorApplied physicsPhysics::Instrumentation and DetectorsScintillator[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesSpace radiation030218 nuclear medicine & medical imagingEducationIonExperimental apparatuNuclear physics03 medical and health sciencesPhysics and Astronomy (all)0302 clinical medicineFragmentation (mass spectrometry)0103 physical sciencesNeutron detectionddc:530Silicon Vertex DetectorIon010306 general physicsNuclear ExperimentScintillation counterRadiation protectionPhysicsDetectorNuclear fragmentationComputer Science ApplicationsInternational collaborationProtection applicationMagnet[PHYS.PHYS.PHYS-MED-PH]Physics [physics]/Physics [physics]/Medical Physics [physics.med-ph]Scientific programInternational cooperationNucleonInteraction region
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"Table 2" of "Few neutron removal from U-238 at relativistic energies"

1997

Uranium fragmentation.

inorganic chemicalsU238 CU --&gt; U236 XU238 PB --&gt; U235 XU238 CU --&gt; U235 XU238 PB --&gt; U236 XU238 CU --&gt; U234 XU238 PB --&gt; U234 XIntegrated Cross Sectiontechnology industry and agricultureCross SectionU238 AL --&gt; U236 XSIGcomplex mixturesU238 AL --&gt; U237 XU238 PB --&gt; U237 XU238 CU --&gt; U237 XNUCLEUS NUCLEUS --&gt; U234 XInclusiveU238 AL --&gt; U234 XU238 AL --&gt; U235 XNUCLEUS NUCLEUS --&gt; U237 XNUCLEUS NUCLEUS --&gt; U236 XNUCLEUS NUCLEUS --&gt; U235 X
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"Table 1" of "Few neutron removal from U-238 at relativistic energies"

1997

Uranium fragmentation.

inorganic chemicalsU238 CU --&gt; U236 XU238 CU --&gt; U235 XU238 CU --&gt; U234 XCross Sectioncomplex mixturesU238 CU --&gt; U237 XNUCLEUS NUCLEUS --&gt; U234 XInclusiveNUCLEUS NUCLEUS --&gt; U233 XNUCLEUS NUCLEUS --&gt; U237 XNUCLEUS NUCLEUS --&gt; U236 XNUCLEUS NUCLEUS --&gt; U235 XU238 PB --&gt; U235 XU238 PB --&gt; U236 XU238 PB --&gt; U233 XU238 PB --&gt; U234 XIntegrated Cross Sectiontechnology industry and agricultureU238 AL --&gt; U236 XSIGU238 AL --&gt; U237 XU238 PB --&gt; U237 XU238 AL --&gt; U233 XU238 AL --&gt; U234 XU238 AL --&gt; U235 X
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