0000000000951102

AUTHOR

C. Nociforo

showing 47 related works from this author

Dipole excitations of neutron-proton asymmetric nuclei

2004

Dipole excitations of unstable short-lived nuclei has been investigated experimentally by utilizing the electromagnetic-excitation process with high-energy secondary beams. From an exclusive measurement of the neutron-decay channels, differential cross sections with respect to excitation energy, which are directly related to the photo-absorption cross section and accordingly to the dipole-strength function, have been derived. Light neutron-rich nuclei in the mass range fromA = 11 toA = 23 with mass-over-charge ratios up toA/Z≈ 2.8 have been investigated systematically. Much in contrast to stable nuclei, low-lying dipole excitations well below the giant dipole resonance region have been obse…

PhysicsNuclear and High Energy PhysicsDipoleBond dipole momentNuclear TheoryTransition dipole momentNeutronSum rule in quantum mechanicsElectric dipole transitionAtomic physicsNuclear ExperimentNucleonExcitationNuclear Physics A
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Exclusive measurements of nuclear breakup reactions of 17Ne

2014

F. Wamers et al.; 4 pags.; 2 figs. Open Access funded by Creative Commons Atribution Licence 2.0

Nuclear reactionPhysicsIsotopePhysicsQC1-999HadronNuclear Theorychemistry.chemical_elementBreakup530Nuclear physicsBaryonchemistryIsotopes of neonPhysics::Accelerator Physicsddc:530Statistical physicsNucleonNuclear ExperimentCarbon
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Coulomb dissociation of 27P

2011

International audience; In this work the astrophysical 26Si(p,γ)27P reaction is studied using the Coulomb dissociation technique. We performed a 27P Coulomb Dissociation experiment at GSI, Darmstadt (28 May-5 June 2007) using the ALADIN-LAND setup which allows complete-kinematic studies. A secondary 27P beam at 498 AMeV impinging a 515mg/cm2 Pb target was used. The relative energy of the outgoing system (26Si+p) is measured obtaining the resonant states of the 27P. Preliminary results show four resonant states measured at 0.36±0.07, 0.88±0.09, 1.5±0.2, 2.3±0.3 MeV and evidence of a higher state at around 3.1 MeV. The preliminary total cross section obtained for relative energies between 0 a…

History010308 nuclear & particles physicsChemistry[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesDissociation (chemistry)Computer Science ApplicationsEducationNuclear physics0103 physical sciencesCoulombAtomic physics010306 general physicsRelative energy
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Comparison of electromagnetic and nuclear dissociation of Ne-17

2018

8 pags., 10 figs., 3 tabs.

PhysicsCOLLISIONSInternal energy010308 nuclear & particles physics01 natural sciences7. Clean energySTATEDissociation (chemistry)CoincidenceCAPTUREReaction ratemedicine.anatomical_structureFragmentation (mass spectrometry)0103 physical sciencesmedicineHaloAtomic physics010306 general physicsGround stateDECAYNucleus
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A GEM-TPC in twin configuration for the Super-FRS tracking of heavy ions at FAIR

2018

The GEM-TPC [1] described herein will be part of the standard beam-diagnostics equipment of the Super-FRS [2] . This chamber will provide tracking information for particle identification at rates up to 1 MHz on an event-by-event basis. The key requirements of operation for these chambers are: close to 100% tracking efficiency under conditions of high counting rate, spatial resolution below 1 mm and a superb large dynamic range covering projectiles from Z=1 up to Z=92. The current prototype consists of two GEM-TPCs inside a single vessel, which are operating independently and have electrical drift fields in opposite directions. The twin configuration is done by flipping one of the GEM-TPCs o…

radioactive ion beamNuclear and High Energy PhysicsProtonfragment separatorPhysics::Instrumentation and Detectorssuper-FRSchemistry.chemical_elementTracking (particle physics)01 natural sciences7. Clean energyParticle identificationGSIXenonOptics0103 physical sciencesseurantaNuclear Experiment010306 general physicsInstrumentationImage resolutionPhysicsTime projection chamberta114010308 nuclear & particles physicsProjectilebusiness.industrytrackingfairtime projection chamberbeam adjustmentchemistrygas electron multiplierGas electron multiplierbusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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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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Measurement of the Dipole Polarizability of the Unstable Neutron-Rich NucleusNi68

2013

The E1 strength distribution in Ni68 has been investigated using Coulomb excitation in inverse kinematics at the RB3-LAND setup and by measuring the invariant mass in the one- and two-neutron decay channels. The giant dipole resonance and a low-lying peak (pygmy dipole resonance) have been observed at 17.1(2) and 9.55(17) MeV, respectively. The measured dipole polarizability is compared to relativistic random phase approximation calculations yielding a neutron-skin thickness of 0.17(2) fm. A method and analysis applicable to neutron-rich nuclei has been developed, allowing for a precise determination of neutron skins in nuclei as a function of neutron excess.

PhysicsDipolePolarizabilityNuclear TheoryTransition dipole momentGeneral Physics and AstronomyResonanceNeutronCoulomb excitationAtomic physicsElectric dipole transitionNuclear ExperimentRandom phase approximationPhysical Review Letters
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Exclusive measurement of breakup reactions with the one-neutron halo nucleus11Be

2003

Electromagnetic and nuclear inelastic scattering of the halo nucleus ${}^{11}\mathrm{Be}$ have been investigated by a measurement of the one-neutron removal channel, utilizing a secondary ${}^{11}\mathrm{Be}$ beam with an energy of 520 MeV/nucleon impinging on lead and carbon targets. All decay products, i.e., ${}^{10}\mathrm{Be}$ fragments, neutrons, and $\ensuremath{\gamma}$ rays have been detected in coincidence. Partial cross sections for the population of ground and excited states in ${}^{10}\mathrm{Be}$ were determined for nuclear diffractive breakup as well as for electromagnetically induced breakup. The partial cross sections for ground-state transitions have been differentiated fur…

PhysicsNuclear and High Energy Physicseducation.field_of_studyNuclear TheoryPopulationHalo nucleusInelastic scatteringExcited stateNeutronContinuum (set theory)Atomic physicsNuclear ExperimenteducationNucleonEnergy (signal processing)Physical Review C
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Rate capability of a cryogenic stopping cell for uranium projectile fragments produced at 1000 MeV/u

2016

At the Low-Energy Branch (LEB) of the Super-FRS at FAIR, projectile and fission fragments will be produced at relativistic energies, separated in-flight, energy-bunched, slowed down and thermalized in a cryogenic stopping cell (CSC) filled with ultra-pure He gas. The fragments are extracted from the stopping cell using a combination of DC and RF electric fields and gas flow. A prototype CSC for the LEB has been developed and successfully commissioned at the FRS Ion Catcher at GSI. Ionization of He buffer gas atoms during the stopping of energetic ions creates a region of high space charge in the stopping cell. The space charge decreases the extraction efficiency of stopping cells since the …

Nuclear and High Energy PhysicsEXTRACTIONFissionBuffer gasION-CATCHER01 natural sciencesSpace chargeIonHEAVY-IONSNuclear physicsMOBILITIESElectric fieldIonization0103 physical sciencesRate capabilityddc:530SPECTROMETER010306 general physicsNuclear ExperimentInstrumentationSUPER-FRSHIGH-PRECISION EXPERIMENTSta114010308 nuclear & particles physicsChemistryProjectileBEAMSPERFORMANCEGAS CELLSpace chargeExtraction efficiencyExtraction timeCryogenic gas-filled stopping cellAtomic physicsBeam (structure)Nuclear Instruments & Methods in Physics Research Section B-Beam Interactions with Materials and Atoms
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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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Summary of the HypHI Phase 0 experiment and future plans with FRS at GSI (FAIR Phase 0)

2016

WOS: 000381331200014

PhysicsNuclear and High Energy PhysicsCOLLISIONSLifetime measurement010308 nuclear & particles physicsInvariant massLIFETIMEHeavy ion induced reactionHYPERNUCLEAR SPECTROSCOPY01 natural sciencesNuclear physicsShort lifetimeStatistical analysesFRS and Super-FRS0103 physical sciencesRI-beamHeavy ionInvariant massLIGHT HYPERFRAGMENTS010306 general physicsSpectroscopyRELATIVISTIC HYPERNUCLEINuclear Physics A
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Nuclear structure “southeast” ofPb208: Isomeric states inHg208andTl209

2009

The nuclear structure of neutron-rich N>126 nuclei has been investigated following their production via relativistic projectile fragmentation of a E/A=1 GeV U-238 beam. Metastable states in the N=128 isotones Hg-208 and Tl-209 have been identified. Delayed gamma-ray transitions are interpreted as arising from the decay of I-pi=(8(+)) and (17/2(+)) isomers, respectively. The data allow for the so far most comprehensive verification of the shell-model approach in the region determined by magic numbers Z 126.

PhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryHadronNuclear structureBaryonNuclear physicsUranium-238Excited stateMetastabilityNeutronAtomic physicsNuclear ExperimentNucleonPhysical Review C
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Evidence for Pygmy and Giant Dipole Resonances inSn130andSn132

2005

The dipole strength distribution above the one-neutron separation energy was measured in the unstable $^{130}\mathrm{Sn}$ and the double-magic $^{132}\mathrm{Sn}$ isotopes. The results were deduced from Coulomb dissociation of secondary Sn beams with energies around $500\text{ }\text{ }\mathrm{MeV}/\mathrm{\text{nucleon}}$, produced by in-flight fission of a primary $^{238}\mathrm{U}$ beam. In addition to the giant dipole resonance, a resonancelike structure (``pygmy resonance'') is observed at a lower excitation energy around 10 MeV exhausting a few percent of the isovector $E1$ energy-weighted sum rule. The results are discussed in the context of a predicted new dipole mode of excess neut…

PhysicsDipoleIsovectorGiant resonanceNuclear TheoryGeneral Physics and AstronomyResonanceNeutronSum rule in quantum mechanicsAtomic physicsNuclear ExperimentNucleonExcitationPhysical Review Letters
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Dipole response of neutron-rich Sn isotopes

2007

The neutron-rich isotopes 129–133Sn were studied in a Coulomb excitation experiment at about 500 AMeV using the FRS-LAND setup at GSI. From the exclusive measurement of all projectile-like particles following the excitation and decay of the projectile in a high-Z target, the energy differential cross section can be extracted. At these beam energies dipole transitions are dominating, and within the semi-classical approach the Coulomb excitation cross sections can be transformed into photoabsorption cross sections. In contrast to stable Sn nuclei, a substantial fraction of dipole strength is observed at energies below the giant dipole resonance (GDR). For 130Sn and 132Sn this strength is loca…

PhysicsNuclear and High Energy PhysicsDipoleNuclear TheoryTransition dipole momentNeutronCoulomb excitationElectric dipole transitionAtomic physicsNuclear ExperimentNucleonResonance (particle physics)ExcitationNuclear Physics A
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Coulomb excitation of exotic nuclei at the R3B-LAND setup

2012

Exotic Ni isotopes have been measured at the R3B-LAND setup at GSI in Darmstadt, using Coulomb excitation in inverse kinematics at beam energies around 500 MeV/u. As the experimental setup allows kinematically complete measurements, the excitation energy was reconstructed using the invariant mass method. The GDR and additional low-lying strength have been observed in 68Ni, the latter exhausting 4.1(1.9)% of the E1 energy-weighted sum rule. Also, the branching ratio for the non-statistical decay of the excited 68Ni nuclei was measured and amounts to 24(4)%.

PhysicsHistoryInverse kinematicsBranching fractionFOS: Physical sciencesExotic isotopes R3B LAND GSI Coulomb excitation inverse kinematics GDR PDRCoulomb excitationComputer Science ApplicationsEducationNuclear physicsExcited stateInvariant massSum rule in quantum mechanicsNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear ExperimentBeam (structure)Excitation
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Measurement of the92,93,94,100Mo(γ,n) reactions by Coulomb Dissociation

2016

6th Nuclear Physics in Astrophysics Conference (NPA), Lisbon, Portugal, 19 May 2013 - 24 May 2013; Journal of physics / Conference Series 665, 012034 (2016). doi:10.1088/1742-6596/665/1/012034

PhysicsHistoryPhoton010504 meteorology & atmospheric sciencesIsotopeStable isotope ratiochemistry.chemical_element53001 natural sciencesDissociation (chemistry)Computer Science ApplicationsEducationNuclear physicschemistryNucleosynthesisMolybdenum0103 physical sciencesCoulombddc:530Atomic physics010303 astronomy & astrophysicsProduction chain0105 earth and related environmental sciencesJournal of Physics: Conference Series
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Coulomb breakup of psd-shell neutron-rich nuclei

2005

Inelastic scattering of loosely bound nuclei by Coulomb interaction at intermediate energies (400?600 MeV/nucleon) has been utilized as a spectroscopic tool for exotic nuclei. The observed electromagnetic dipole (E1) strength above the one neutron threshold of neutron-rich C, Be, B and O isotopes can be explained by a non-resonant transition of a neutron into the continuum. The shape of these strength distributions reflects properties of the wavefunction of the released neutron in the nucleus and hence ground-state properties of these isotopes. Neutron capture cross-sections such as for the 14C(n,?) 15C reaction which are of astrophysical relevance can be deduced indirectly.

PhysicsNuclear and High Energy PhysicsNuclear TheoryInelastic scatteringNeutron scatteringInelastic neutron scatteringNuclear physicsNeutron capturer-processNeutronAtomic physicsNuclear ExperimentNucleons-processJournal of Physics G: Nuclear and Particle Physics
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Nuclear-matter density distribution in the neutron-rich nuclei 12,14Be from proton elastic scattering in inverse kinematics

2012

Abstract In the present work, the differential cross sections for small-angle proton elastic scattering on the 12,14 Be nuclei were measured in inverse kinematics, using secondary radioactive beams with energies near 700 MeV/u produced with the fragment separator FRS at GSI. The main part of the experimental setup was the active target IKAR, which was used simultaneously as a target and a detector for the recoil protons. Auxiliary detectors for projectile tracking and isotope identification completed the setup. The measured differential cross sections were analyzed using the Glauber multiple-scattering theory. For the evaluation of the data several phenomenological nuclear-matter density pa…

Nuclear reactionPhysicsElastic scatteringNuclear and High Energy PhysicsIsotopeProtonNuclear TheoryNuclear matterNuclear physicsRecoilNeutronAtomic physicsNuclear ExperimentGlauberNuclear Physics A
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The FRS Ion Catcher

2013

At the FRS Ion Catcher at GSI, projectile and fission fragments are produced at relativistic energies, separated in-flight, range-focused, slowed down and thermalized in a cryogenic stopping cell. A multiple-reflection time-of-flight mass spectrometer (MR-TOF-MS) is used to perform direct mass measurements and to provide an isobarically clean beam for further experiments, such as mass-selected decay spectroscopy. A versatile RF quadrupole transport and diagnostics unit guides the ions from the stopping cell to the MR-TOF-MS, provides differential pumping, ion identification and includes reference ion sources. The FRS Ion Catcher serves as a test facility for the Low-Energy Branch of the Sup…

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsFissionMass spectrometry01 natural sciencesIonHEAVY-IONSNuclear physicsENERGYGSI0103 physical sciencesddc:530NuclideNuclear Experiment010306 general physicsInstrumentationSUPER-FRSDirect mass measurementta114010308 nuclear & particles physicsChemistryProjectileMultiple-reflection time-of-flight mass spectrometerExtraction timeTIMECryogenic gas-filled stopping cellQuadrupoleISOBAR-SEPARATIONFacility for Antiproton and Ion ResearchAtomic physicsProjectile fragmentationBeam (structure)Exotic nucleiSYSTEMNuclear Instruments & Methods in Physics Research Section B-Beam Interactions with Materials and Atoms
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'beta'-decay studies of neutron-rich 'TL', 'PB', and 'BI' isotopes

2014

The fragmentation of relativistic uranium projectiles has been exploited at the Gesellschaft fur Schwerionenforschung laboratory to investigate the β decay of neutron-rich nuclei just beyond 208Pb. This paper reports on β-delayed γ decays of 211-213Tl, 215Pb, and 215-219Bi de-exciting states in the daughters 211-213Pb, 215Bi, and 215-219Po. The resulting partial level schemes, proposed with the help of systematics and shell-model calculations, are presented. The role of allowed Gamow-Teller and first-forbidden β transitions in this mass region is discussed. © 2014 American Physical Society.

PhysicsNuclear and High Energy PhysicsIsotopeSHELL modelchemistry.chemical_elementUraniumBeta decayrelativistic projectile fragmentationRISING spectrometerIonizing radiationNuclear physicschemistrySPINDouble beta decaySubatomic Physicsr-processNeutronbeta decayAtomic physics
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Coulomb breakup of 23O

2005

Abstract The ground-state structure of the near-drip-line nucleus 23O has been investigated in a one-neutron Coulomb breakup reaction. Differential cross sections d σ / d E * for electromagnetic excitation of 23O projectiles (422 MeV/nucleon) incident on a lead target have been obtained from the measurement of the momenta of all breakup products including γ rays. The analysis of the deduced dipole-transition probability into the continuum infers a 2 s 1 / 2 ⊗ O 22 ( 0 + ) ground state configuration with a spectroscopic factor of 0.77(10) and thus a ground-state spin I π ( O 23 ) = 1 / 2 + , resolving earlier conflicting experimental findings. Final-state interaction is of significant influe…

PhysicsNuclear and High Energy PhysicsNuclear TheoryCoulombScattering lengthNeutron scatteringAtomic physicsNuclear ExperimentNucleonGround stateBreakupExcitationSpin-½Physics Letters B
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Study of the $^{15}$O(2p, γ )$^{17}$Ne cross section by Coulomb dissociation of $^{17}$Ne for the rp process of nucleosynthesis

2014

Acta physica Polonica / B 45(2), 229 - 234 (2014). doi:10.5506/APhysPolB.45.229

PhysicsRadiative captureNuclear structureGeneral Physics and AstronomySigma25.40.Lw 25.70.De 26.30.Ca 27.20.+nrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Dissociation (chemistry)Nuclear physicsNucleosynthesisTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYCoulombddc:530Atomic physicsExcitationComputingMilieux_MISCELLANEOUS
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Target dependence in the study of collective modes in stable and exotic Ni nuclei

2010

The appearance of the pygmy-dipole-resonance is a recently observed phenomenon that can be related to neutron-matter properties. Its study can be a tool to determine the nuclear symmetry-energy parameters and thus can contribute constraining neutron star models. We present the ( γ,n ) cross sections for different Ni isotopes obtained from a measurement in inverse kinematics at about 500 MeV/u in the LAND reaction setup at GSI. The question of the disentanglement of the Coulomb and nuclear contributions is addressed.

PhysicsNuclear physicsHistoryNeutron starIsotopeInverse kinematicsNuclear TheoryCoulombAtomic physicsNuclear ExperimentComputer Science::DatabasesComputer Science ApplicationsEducationJournal of Physics: Conference Series
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Experimental study of the 15O(2p, γ)17Ne cross section by Coulomb Dissociation for the rp process

2016

6th Nuclear Physics in Astrophysics Conference (NPA), Lisbon, Portugal, 19 May 2013 - 24 May 2013; Journal of physics / Conference Series 665, 012046 (2016). doi:10.1088/1742-6596/665/1/012046

HistoryChemistryNuclear structurechemistry.chemical_elementrp-process[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]530Dissociation (chemistry)Computer Science ApplicationsEducationIonSubatomär fysikFragmentation (mass spectrometry)Subatomic PhysicsCoulombNuclear Physics - ExperimentBerylliumAtomic physicsNuclear Experiment[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Excitation
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Coulomb dissociation of 27P: A reaction of astrophysical interest

2011

The ground-state decay of 26Al(0+) (T 1/2=1.05× 106) has a shorter life-time than the Universe. The presence of this element in the Galaxy was measured via g-ray spectroscopy, showing that the nucleosynthesis of this element is an ongoing process in stars. The proton-capture reaction 26Si(p,γ) 27P competes with the production of 26Al(0+) by β-decay. Coulomb dissociation of 27P has been suggested as an indirect method to measure radiative-proton capture when the direct reaction is not feasible. Such an experiment was performed at GSI with a secondary 27P beam produced by fragmenting a 36Ar primary beam at 500 A MeV. Two main observables are preliminarily presented in this work: the reaction …

PhysicsStarsNucleosynthesisCoulombCoulomb barrierObservableAtomic physicsSpectroscopyDissociation (chemistry)Galaxy
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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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First experimental results of a cryogenic stopping cell with short-lived, heavy uranium fragments produced at 1000 MeV/u

2013

A cryogenic stopping cell (CSC) has been commissioned with U-238 projectile fragments produced at 1000 MeV/u. The spatial isotopic separation in flight was performed with the FRS applying a monoenergetic degrader. For the first time, a stopping cell was operated with exotic nuclei at cryogenic temperatures (70 to 100K). A helium stopping gas density of up to 0.05mg/cm(3) was used, about two times higher than reached before for a stopping cell with RF ion repelling structures. An overall efficiency of up to 15%, a combined ion survival and extraction efficiency of about 50%, and extraction times of 24ms were achieved for heavy a-decaying uranium fragments. Mass spectrometry with a multiple-r…

Materials scienceGeneral Physics and Astronomychemistry.chemical_elementMass spectrometry7. Clean energy01 natural sciencesIonNuclear physicsENERGYGSIION-OPTICAL SYSTEMS0103 physical sciencesddc:530010306 general physicsSpectroscopySUPER-FRSHeliumSHIPTRAPCATCHER010308 nuclear & particles physicsProjectileExtraction (chemistry)UraniumBEAMSTIMEchemistryFLIGHT MASS-SPECTROMETRYMATTEROverall efficiencyEurophysics Letters
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Structure of N >= 126 nuclei produced in fragmentation of (238)U

2009

The nuclear structure of neutron‐rich N⩾126 nuclei have been investigated following their production via relativistic projectile fragmentation of a E/A = 1 GeV 238U beam on a Be target. The cocktail of secondary beam products were separated and identified using the GSI FRagment Separator (FRS). The nuclei of interest were implanted in a high‐granularity active stopper detector set‐up consisting of 6 double sided silicon strip detectors. The associated gamma‐ray transitions were detected with the RISING array, consisting of 15 Euroball cluster Ge‐detectors. Time‐correlated gamma decays from individually identified nuclear species have been recorded, allowing the clean identification of isome…

PhysicsNuclear reactionPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryGamma rayParticle detectorSemiconductor detectorNuclear physicsUranium-238High Energy Physics::ExperimentGamma spectroscopyAtomic physicsNuclear ExperimentBeam (structure)Radioactive decay
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Nuclear symmetry energy and neutron skins derived from pygmy dipole resonances

2007

By exploiting Coulomb dissociation of high-energy radioactive beams of the neutron-rich nuclei $^{129\ensuremath{-}132}\mathrm{Sn}$ and $^{133,134}\mathrm{Sb}$, their dipole-strength distributions have been measured. A sizable fraction of ``pygmy'' dipole strength, energetically located below the giant dipole resonance, is observed in all of these nuclei. A comparison with available pygmy resonance data in stable nuclei ($^{208}\mathrm{Pb}$ and $N=82$ isotones) indicates a trend of strength increasing with the proton-to-neutron asymmetry. On theoretical grounds, employing the RQRPA approach, a one-to-one correlation is found between the pygmy strength and parameters describing the density d…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryHadronNuclear structureElementary particlereactions induced by unstable nucleiCoulomb excitation01 natural sciencesNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Dipole0103 physical sciencesIsotopes of tinNeutronAtomic physicsCoulomb excitation by heavy ionsNuclear Experiment010306 general physicsNucleonnuclear giant resonancesPhysical Review C
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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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Isomeric decay spectroscopy of theBi217isotope

2014

The structure of the neutron-rich bismuth isotope 217Bi has been studied for the first time. The fragmentation of a primary 238U beam at the FRS-RISING setup at GSI was exploited to perform γ-decay spectroscopy, since μs isomeric states were expected in this nucleus. Gamma rays following the decay of a t1/2=3 μs isomer were observed, allowing one to establish the low-lying structure of 217Bi. The level energies and the reduced electric quadrupole transition probability B(E2) from the isomeric state are compared to large-scale shell-model calculations.

PhysicsNuclear and High Energy PhysicsIsotopeGamma rayIsomeric shiftmedicine.anatomical_structureFragmentation (mass spectrometry)QuadrupolemedicineGamma spectroscopyAtomic physicsNuclear ExperimentSpectroscopyNucleusPhysical Review C
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Relativistic Coulomb excitation of Kr 88

2016

International audience; To investigate the systematics of mixed-symmetry states in N=52 isotones, a relativistic Coulomb excitation experiment was performed during the PreSPEC campaign at the GSI Helmholtzzentrum für Schwerionenforschung to determine E2 transition strengths to 2+ states of the radioactive nucleus $^{88}$Kr. Absolute transition rates could be measured towards the first and third 2+ states. For the latter a mixed-symmetry character is suggested on the basis of the indication for a strong M1 transition to the fully symmetric 21+ state, extending the knowledge of the N=52 isotones below Z=40. A comparison with the proton-neutron interacting boson model and shell-model predictio…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryNuclear structureState (functional analysis)Coulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physicsgamma-ray spectroscopySubatomic Physicsrelativistic Coulomb excitationnuclear structure0103 physical sciencesGamma spectroscopyAtomic physicsInteracting boson modelNuclear Experiment010306 general physics
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β-delayed neutron emission measurements around the third r-process abundance peak

2013

This contribution summarizes an experiment performed at GSI (Germany) in the neutron-rich region beyond N=126. The aim of this measurement is to provide the nuclear physics input of relevance for r-process model calculations, aiming at a better understanding of the third r-process abundance peak. Many exotic nuclei were measured around 211Hg and 215Tl. Final ion identification diagrams are given in this contribution. For most of them, we expect to derive halflives and and β-delayed neutron emission probabilities. The detectors used in this experiment were the Silicon IMplantation and Beta Absorber (SIMBA) detector, based on an array of highly segmented silicon detectors, and the BEta deLayE…

PhysicsNuclear physicsPhysics::Instrumentation and DetectorsNucleosynthesisNeutron emissionDouble beta decayDetectorr-processNuclear ExperimentDelayed neutronAbundance of the chemical elementsIon
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Coulomb dissociation of P 27 at 500 MeV/u

2016

J. Marganiec et al. ; 15 págs.; 14 figs.; 6 tabs.

Physics010308 nuclear & particles physicsS-factorMonte Carlo methodNuclear structureResonance[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesDissociation (chemistry)Intruder stateNuclear physics0103 physical sciencesCoulombAtomic physics010306 general physicsNuclear ExperimentExcitation
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New μs Isomers in the Neutron-rich 210Hg Nucleus

2013

Neutron-rich nuclei in the lead region, beyond N = 126, have been studied at the FRS-RISING setup at GSI, exploiting the fragmentation of a primary uranium beam. Two isomeric states have been identified in Hg-210: the 8(+) isomer expected from the seniority scheme in the vg(9/2) shell and a second one at low spin and low excitation energy. The decay strength of the 8(+) isomer confirms the need of effective three-body forces in the case of neutron-rich lead isotopes. The other unexpected low-lying isomer has been tentatively assigned as a 3(-) state, although this is in contrast with theoretical expectations. (C) 2013 Elsevier B.V. All rights reserved.

PhysicsNuclear and High Energy PhysicsIsotopechemistry.chemical_elementUraniummedicine.anatomical_structurechemistryFragmentation (mass spectrometry)Subatomic PhysicsmedicineNeutronAtomic physicsNucleusExcitation
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First Observation of the Unbound NucleusNe15

2014

We report on the first observation of the unbound proton-rich nucleus Ne-15. Its ground state and first excited state were populated in two-neutron knockout reactions from a beam of 500 MeV/u Ne-17. The Ne-15 ground state is found to be unbound by 2.522(66) MeV. The decay proceeds directly to O-13 with simultaneous two-proton emission. No evidence for sequential decay via the energetically allowed 2(-) and 1(-) states in F-14 is observed. The Ne-15 ground state is shown to have a strong configuration with two protons in the (sd) shell around O-13 with a 63(5)% (1s(1/2))(2) component.

Physicsmedicine.anatomical_structureExcited stateNuclear TheorymedicineShell (structure)Physics::Accelerator PhysicsGeneral Physics and AstronomyAtomic physicsNuclear ExperimentGround stateNucleusBeam (structure)Physical Review Letters
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Experimental program of the Super-FRS Collaboration at FAIR and developments of related instrumentation

2016

The physics program at the super-conducting fragment separator (Super-FRS) at FAIR, being operated in a multiple-stage, high-resolution spectrometer mode, is discussed. The Super-FRS will produce, separate and transport radioactive beams at high energies up to 1.5 AGeV, and it can be also used as a stand-alone experimental device together with ancillary detectors. Various combinations of the magnetic sections of the Super-FRS can be operated in dispersive, achromatic or dispersion-matched spectrometer ion-optical modes, which allow measurements of momentum distributions of secondary-reaction products with high resolution and precision. A number of unique experiments in atomic, nuclear and h…

Nuclear and High Energy PhysicsMesonNeutron emissionCOHERENT EXCITATIONProjectile fragments01 natural sciences114 Physical scienceslaw.inventionNuclear physicsENERGYlaw0103 physical sciencesSCATTERINGSPECTROMETERFACILITY010306 general physicsSpectroscopyNuclear ExperimentInstrumentationPhysicsta114IsotopeSpectrometerNUCLEI010308 nuclear & particles physicsScatteringDetectorMagnetic spectrometerPERFORMANCEINVERSE KINEMATICSPRODUCTSSTATESAchromatic lensExperiments
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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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Low-lying electric dipole gamma-continuum for the unstable Fe-62,64 nuclei : Strength evolution with neutron number

2020

6 pags., 4 figs.

62Nuclear and High Energy Physics64PhononAstrophysics::High Energy Astrophysical PhenomenaBinding energyNuclear TheoryCoulomb excitation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciences64Fe530Dipole excitation around neutron threshold62FeSubatomär fysik0103 physical sciencesSubatomic Physicsddc:530NeutronNuclear Physics - ExperimentNuclear structure010306 general physicsNuclear ExperimentPhysics010308 nuclear & particles physics62 Fe62; Fe; 64; Fe; Dipole excitation around neutron threshold; Nuclear structureNuclear structure64 FeFelcsh:QC1-999DipoleFe-64Neutron numberFe-62AGATAAtomic physicslcsh:Physics
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Coulomb and nuclear excitations of narrow resonances in 17Ne

2016

Physics letters / B 759, 200 - 205 (2016). doi:10.1016/j.physletb.2016.05.073

PhysicsNuclear and High Energy PhysicsTeoría de los quantaInternal energySpins010308 nuclear & particles physicsProjectile310601 natural sciences530lcsh:QC1-999Mass formulaNuclear physics0103 physical sciencesPhysical SciencesCoulombIsobaric processFysikddc:530Atomic physics010306 general physicsMultipletExcitationlcsh:PhysicsPhysics Letters B
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Investigation of the Dipole Response in Exotic Nuclei – Experiments at the LAND-R$^3$B Setup

2012

We present experimental results on the electromagnetic excitation of neutron-rich nickel isotopes, making use of the (RB)-B-3-LAND setup at GSI. Exotic beams were produced at approximately 500 MeV/u and their reactions were studied in inverse kinematics. Integral cross sections for Ni-58 are discussed and compared to previous data, providing a validation of our experimental method. The El excitation-energy distribution of the unstable Ni-68 is presented as well, showing an excess in cross section in the 1n decay channel when compared only with a typical Giant Dipole Resonance.

Nuclear physicsPhysicsCross section (physics)DipolePhysics and Astronomy (miscellaneous)IsotopeInverse kinematicsDetectorAtomic physicsNuclear ExperimentResonance (particle physics)ExcitationProgress of Theoretical Physics Supplement
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Mass measurements of As, Se, and Br nuclei, and their implication on the proton-neutron interaction strength toward the N=Z line

2021

Mass measurements of the $^{69}$As, $^{70,71}$Se and $^{71}$Br isotopes, produced via fragmentation of a $^{124}$Xe primary beam at the FRS at GSI, have been performed with the multiple-reflection time-of-flight mass spectrometer (MR-TOF-MS) of the FRS Ion Catcher with an unprecedented mass resolving power of almost 1,000,000. For the $^{69}$As isotope, this is the first direct mass measurement. A mass uncertainty of 22 keV was achieved with only 10 events. For the $^{70}$Se isotope, a mass uncertainty of 2.6 keV was obtained, corresponding to a relative accuracy of $\delta$m/m = 4.0$\times 10^{-8}$, with less than 500 events. The masses of the $^{71}$Se and $^{71}$Br isotopes were measured…

nucl-thNuclear TheoryFOS: Physical sciencesInteraction strengthnucl-exMass spectrometry01 natural sciences7. Clean energyarseeniIonNuclear Theory (nucl-th)Nuclear physicsFragmentation (mass spectrometry)0103 physical sciencesddc:530NeutronbromiNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsIsotope010308 nuclear & particles physicsMass measurementAtomic massseleeniydinfysiikkaPhysical Review C
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βdecay of102Y produced in projectile fission of238U

2012

The population of 102Zr following the β decay of 102Y produced in the projectile fission of 238U at the GSI facility in Darmstadt, Germany has been studied. 102Y is known to ß decay into 102Zr via two states, one of high spin and the other low spin. These states preferentially populate different levels in the 102Zr daughter. In this paper the intensities of transitions in 102Zr observed are compared with those from the decay of the low-spin level studied at the TRISTAN facility at Brookhaven National Laboratory and of the high-spin level studied at the JOSEF separator at the Kernforschungsanlage Jülich.

PhysicsHistoryeducation.field_of_studyCluster decayFissionProjectilePopulationBeta decayddc:Computer Science ApplicationsEducationNuclear physicsSubatomic PhysicsHigh Energy Physics::ExperimentAtomic physicsNuclear ExperimentSpin (physics)National laboratoryeducationJournal of Physics: Conference Series
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Angular momentum population in fragmentation reactions

2009

Neutron-deficient nuclei with N = 126 have been populated following projectile fragmentation of a 238U beam with energy 1 GeV/A. The decay of several previously reported isomers has been measured. This will allow us to calculate high-spin isomeric ratios and compare them with model calculations to allow a better understanding of the reaction mechanism. Algora, Alejandro, Alejandro.Algora@ific.uv.es ; Molina Palacios, Francisco Manuel, Francisco.Molina@ific.uv.es ; Rubio Barroso, Berta, Berta.Rubio@ific.uv.es

UNESCO::FÍSICA::Física molecular:FÍSICA [UNESCO]:FÍSICA::Física molecular [UNESCO]UNESCO::FÍSICANeutron-deficient nucleiProjectile fragmentationHigh-spin isometric ratiosNeutron-deficient nuclei ; Projectile fragmentation ; High-spin isometric ratios ; Reaction mechanismReaction mechanism
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Proton-proton correlations observed in two-proton decay of $^{19}$Mg and $^{16}$Ne

2008

Proton-proton correlations were observed for the two-proton decays of the ground states of $^{19}$Mg and $^{16}$Ne. The trajectories of the respective decay products, $^{17}$Ne+p+p and $^{14}$O+p+p, were measured by using a tracking technique with microstrip detectors. These data were used to reconstruct the angular correlations of fragments projected on planes transverse to the precursor momenta. The measured three-particle correlations reflect a genuine three-body decay mechanism and allowed us to obtain spectroscopic information on the precursors with valence protons in the $sd$ shell.

Nuclear TheoryFOS: Physical sciencesNuclear Experiment (nucl-ex)Nuclear ExperimentNuclear Experiment
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Unveiling the two-proton halo character of 17Ne: Exclusive measurement of quasi-free proton-knockout reactions

2022

7 pags., 5 figs.

Subatomär fysikNuclear and High Energy PhysicsFísica-Modelos matemáticosSubatomic PhysicsNuclear TheoryPartículasFOS: Physical sciencesddc:530Nuclear Experiment (nucl-ex)Nuclear experimentNuclear ExperimentNuclear Experiment530
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