0000000000089558

AUTHOR

Thomas Aumann

showing 57 related works from this author

Low-energy fission investigated in reactions of 750 AMeV 238U-ions with Pb and Be targets

1996

Charge distributions of fragments from low energy nuclear fission are investigated in reactions of highly fissile238U projectiles at relativistic energies (750 A·MeV) with a heavy (Pb) and a light (Be) target. The fully stripped fission fragments are separated by the Fragment Separator (FRS). Their high kinetic energies in the laboratory system allow the identification of all atomic numbers by using Multiple-Sampling Ionization Chambers (MUSIC). The elemental distributions of fragments observed at larger magnetic rigidities than the238U projectiles show asymmetric break-up and odd-even effects. They indicate a low energy fission process, induced mainly by dissociation in the electro-magneti…

PhysicsCold fissionNuclear and High Energy PhysicsCluster decay010308 nuclear & particles physicsFissionNuclear TheoryKinetic energy01 natural sciences7. Clean energyDissociation (chemistry)Effective nuclear chargeIonNuclear physicsLow energyNuclear fissionIonization0103 physical sciencesNuclear fusionAtomic physicsNuclear Experiment010306 general physicsZeitschrift für Physik A Hadrons and nuclei
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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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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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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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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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Thermonuclear reactionS30(p,γ)Cl31studied via Coulomb breakup ofCl31

2014

Coulomb breakup at high energy in inverse kinematics of proton-rich Cl-31 was used to constrain the thermonuclear S-30(p,gamma)Cl-31 capture reaction rate under typical Type I x-ray burst conditions. This reaction is a bottleneck during rapid proton-capture nucleosynthesis (rp process), where its rate depends predominantly on the nuclear structure of Cl-31. Two low-lying states just above the proton-separation threshold of S-p = 296( 50) keV in Cl-31 have been identified experimentally using the (RB)-B-3-LAND setup at the GSI Helmholtzzentrum fur Schwerionenforschung GmbH. Both states are considered to play a key role in the thermonuclear S-30( p,gamma)Cl-31 capture reaction. Excitation ene…

PhysicsNuclear physicsReaction rateNuclear and High Energy PhysicsThermonuclear fusionProtonNucleosynthesisNuclear structureCoulomb excitationAtomic physicsrp-processExcitationPhysical Review C
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ASY-EOS experiment at GSI

2012

The elliptic-flow ratio of neutrons with respect to protons in reactions of neutron rich Heavy-Ion at intermediate energies has been recently proposed as an observable sensitive to the strength of the symmetry term in the nuclear equation of state (EOS) at supra-saturation densities. The recent results obtained from the existing FOPI/LAND data for 197Au+197Au collisions at 400 MeV/nucleon in comparison with the UrQMD model allowed a first estimate of the symmetry term of the EOS but suffer from a considerable statistical uncertainty. In order to obtain an improved data set for Au+Au collisions and to extend the study to other systems, a new experiment was carried out at the GSI laboratory b…

PhysicssezelePhysicsQC1-999Nuclear Theorysymmetry energyObservableNuclear equation of state[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nuclear equation of stateSymmetry (physics)Term (time)Nuclear physicsPhysics and Astronomy (all)nucleus-nucleus collisionsNeutronNucleonNuclear ExperimentEPJ Web of Conferences
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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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Manifestation of the halo structure in momentum distributions from 6He fragmentation

1998

Abstract Experimental data on the momentum distribution in the fragmentation of a 240 MeV/u 6 He beam on a carbon target are compared with several models of the 6 He nucleus based on different physical assumptions. It is shown that the lack of a strict theoretical description of the fragmentation mechanism and, in particular, of the final state interaction prevents any contra or versa arguments for these models. The requirement of fragment ( 5 He) survival or spatial localization of a fragment in the 6 He wave function is an essential point in the reaction mechanism. The analysis of the 5 He momentum (sum of the neutron and the α-particle momenta) distribution is free from the effect of fin…

PhysicsNuclear and High Energy PhysicsNuclear physicsmedicine.anatomical_structureFragmentation (mass spectrometry)medicineNeutronSpatial localizationHaloAtomic physicsNuclear ExperimentWave functionNucleusNuclear PhysicsNuclear Physics A
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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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Development of quadrupole collectivity in the neutron-rich Ni, Zn, Ge, and Se isotopes

2003

An experiment was performed to study the collective properties of neutron-rich Ni, Zn, Ge, and Se isotopes. Of particular interest is the vicinity of the N = 50 and Z = 28 shell closures. For most neutron-rich nuclei in this region of the chart of nuclei the B(E2) values of the transitions from the ground to the first excited 2+ states are unknown. This information would give valuable insight into the changes in nuclear structure when going to more neutron-rich nuclei.

PhysicsIsotopes of seleniumIsotopes of germaniumExcited stateNuclear TheoryQuadrupoleIsotopes of zincNuclear structureNeutronCoulomb excitationAtomic physicsNuclear Experiment
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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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Lithium isotopes beyond the drip line

2008

The unbound isotopes 10Li, 12Li and 13Li have been observed after nucleon-knockout reactions at relativistic energies with 11Li and 14Be beams impinging on a liquid hydrogen target. The channels , and were analysed in the ALADIN-LAND setup at GSI. The 10Li data confirm earlier findings, while the 12Li and 13Li nuclei were observed for the first time. The relative-energy spectrum shows that the ground state of 12Li can be described as a virtual s-state with a scattering length of -13.7(1.6) fm. A broad energy spectrum was found for the channel. Based on the assumption that the relative-energy spectrum is dominated by a correlated background presumably stemming from initial correlations in th…

PhysicsNuclear and High Energy PhysicsIsotopeIsotopes of lithiumNuclear TheoryScattering lengthResonance (particle physics)Nuclear physicsEnergy spectrumAtomic physicsNuclear ExperimentGround stateLiquid hydrogenLine (formation)Physics Letters B
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Shell evolution of $N=40$ isotones towards $^{60}$Ca: First spectroscopy of $^{62}$Ti

2020

7 pags., 4 figs., 1 tab.

Nuclear and High Energy PhysicsNuclear TheoryNuclear TheoryAb initioFOS: Physical sciencesShell evolution[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesShell evolution ; Radioactive beams ; Gamma-ray spectroscopyNuclear Theory (nucl-th)Gamma-ray spectroscopy; Radioactive beams; Shell evolution0103 physical sciencesddc:530Gamma-ray spectroscopyNuclear Experiment (nucl-ex)010306 general physicsSpectroscopyNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsIsland of inversionIsotonePhysicsStarke Wechselwirkung und exotische Kerne – Abteilung BlaumFísicalcsh:QC1-999Excited stateQuadrupoleAtomic physicsNucleonGround statelcsh:PhysicsRadioactive beams
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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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A large-area scintillating fibre detector for relativistic heavy ions

1998

Abstract A scintillating fibre detector for relativistic heavy ions with an active area of 50 × 50 cm 2 has been developed and was tested with various ion beams (1 ≤ Z ≤ 92). At count rates of up to 10 5 particles/s, the position resolution was found to be determined by the fibre width of 1 mm; depending on the nuclear charge of the beam, efficiencies between 89% and 100% and time resolutions between 800 and 200 ps (FWHM) were obtained.

Position sensitive photomultiplierPhysicsNuclear and High Energy PhysicsFull width at half maximumPosition resolutionDetectorScintillating fibreAtomic physicsInstrumentationEffective nuclear chargeBeam (structure)IonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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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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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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The HypHI Phase 0 experiment

2010

10th International Conference on Hypernuclear and Strange Particle Physics -- SEP 14-18, 2009 -- Tokai, JAPAN

PhysicsNuclear and High Energy PhysicsCarbon graphiteProjectilehypernuclear spectroscopyPhase (waves)LambdaNuclear physicsheavy ion induced reactioninvariant massHeavy ionENERGY NUCLEAR COLLISIONSAtomic physicsSpectroscopyNuclear Physics A
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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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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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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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The electronion scattering experiment ELISe at the International Facility for Antiproton and Ion Research (FAIR) - A conceptual design study

2011

The electronion scattering experiment ELISe is part of the installations envisaged at the new experimental storage ring at the International Facility for Antiproton and Ion Research (FAIR) in Darmstadt, Germany. It offers an unique opportunity to use electrons as probe in investigations of the structure of exotic nuclei. The conceptual design and the scientific challenges of ELISe are presented. © 2011 Elsevier B.V. All rights reserved.

Nuclear and High Energy PhysicselectronscatteringFORM-FACTORS[PHYS.PHYS.PHYS-ACC-PH]Physics [physics]/Physics [physics]/Accelerator Physics [physics.acc-ph]Electron[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]DATA-ACQUISITION SYSTEMNUCLEAR-STRUCTURE01 natural sciencesBINDING-ENERGIESCHARGE-DENSITY DISTRIBUTIONSIonCROSS-SECTIONSNuclear physicsNuclei far off stabilityConceptual designeA collider0103 physical sciencesCENTRAL DEPRESSIONElectron scattering010306 general physicsInstrumentationPhysics010308 nuclear & particles physicsScattering29.27.-a 25.30.Bf25.30.Dh21.10.Ft29.20.Dh29.30.-hRELATIVISTIC HEAVY-IONSEXOTIC NUCLEIFacility for Antiproton and Ion ResearchGIANT-RESONANCESStorage ring
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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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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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Hypernuclear production cross section in the reaction of 6Li + 12C at 2 A GeV

2015

WOS: 000358624800021

Particle physicsNuclear and High Energy PhysicsPopulationH-4(LAMBDA)BEAMLIFETIMEStrangenessHEAVY-ION COLLISIONSLambdaParticle identificationNuclear physicsHypernucleiInvariant massRapidityeducationNuclear ExperimentPhysicseducation.field_of_studyHeavy ion collisionHyperonRelativistic energyHypernucleuslcsh:QC1-999STATEProduction cross sectionQUANTUM MOLECULAR-DYNAMICSLIGHT HYPERNUCLEIYield ratioDECAYlcsh:PhysicsRELATIVISTIC HYPERNUCLEIPhysics Letters B
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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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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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Excitation and decay of two-phonon giant dipole resonances

1999

Abstract In heavy ion collisions at near relativistic energies, electromagnetic excitation of the double giant dipole resonance occurs with large cross sections. We summarize the presently available experimental data and discuss related theoretical efforts. Emphasis is paid to the question of anharmonicities and to the damping of the two-phonon states.

Nuclear physicsPhysicsNuclear reactionNuclear and High Energy PhysicsDipolePhononGiant resonanceCollective modelResonanceHeavy ionAtomic physicsExcitationNuclear Physics A
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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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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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Production of hypernuclei in peripheral HI collisions: The HypHI project at GSI

2012

ECT Workshop on Strange Hadronic Matter -- SEP 26-30, 2011 -- Trento, ITALY

PhysicsNuclear and High Energy PhysicsPhase (waves)chemistry.chemical_elementInvariant massLIFETIMEHeavy ion induced reactionHypernuclear spectroscopyNuclear physicschemistryMass spectrumLithiumHeavy ionInvariant massENERGY NUCLEAR COLLISIONSAtomic physicsSpectroscopyRELATIVISTIC HYPERNUCLEI
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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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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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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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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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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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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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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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Neutron removal in peripheral relativistic heavy-ion collisions

1995

We investigate the relativistic Coulomb fragmentation of $^{197}\mathrm{Au}$ by heavy ions, leading to one-, two-, and three-neutron removal. To resolve the ambiguity connected with the choice of a specific minimum impact parameter in a semiclassical calculation, a microscopic approach is developed based on nucleon-nucleon collisions (``soft-spheres'' model). This approach is compared with experimental data for $^{197}\mathrm{Au}$ at 1 GeV/nucleon and with a calculation using the ``sharp-cutoff'' approximation. We find that the harmonic-oscillator model predicting a Poisson distribution of the excitation probabilities of multiphonon states gives a good agreement with one-neutron removal cro…

PhysicsNuclear reactionNuclear and High Energy PhysicsNeutron emissionAstrophysics::High Energy Astrophysical PhenomenaNuclear TheorySemiclassical physicsPoisson's ratioNuclear physicssymbols.namesakeCoulombsymbolsNeutronAtomic physicsImpact parameterNuclear ExperimentNucleonPhysical Review C
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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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Electromagnetic and nuclear fission of238U in the reaction of 100, 500, and 1000 A�MeV208Pb with238U

1994

The folding- and azimuthal-angle and velocity distributions for the238U fission fragments have been measured in reactions with 100, 500, and 1000 A·MeV208Pb. These distributions were used to decompose the fission cross section into its electromagnetic and nuclear components. The fraction of electromagnetic fission was found to be 0.16±0.07, 0.48±0.08, and 0.60±0.04, respectively. The electromagnetic fission cross section as a function of the208Pb nucleus energy is compared with theoretical predictions. The measured fission cross section from nuclear reactions (≈1.5 b) is approximately constant between 100 and 1000 A·MeV.

Nuclear reactionPhysicsNuclear and High Energy PhysicsCold fissionCluster decayFissionNuclear TheoryAstrophysics::Cosmology and Extragalactic AstrophysicsNuclear physicsCross section (physics)Nuclear fissionNuclear fusionHigh Energy Physics::ExperimentNeutronAstrophysics::Earth and Planetary AstrophysicsNuclear ExperimentZeitschrift f�r Physik A Hadrons and Nuclei
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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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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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