0000000001314932

AUTHOR

A. Piechaczek

showing 7 related works from this author

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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New subshell closure atN=58emerging in neutron-rich nuclei beyondNi78

2010

The structure of neutron-rich nuclei beyond $^{78}\mathrm{Ni}$ was studied using postaccelerated radioactive beams of $^{83,84,85}\mathrm{Ga}$ utilizing $\ensuremath{\beta} \ensuremath{\gamma}$ and $\ensuremath{\beta}\ensuremath{-}n \ensuremath{\gamma}$ spectroscopy. Our data, when combined with energy level systematics, suggests a possible new spherical subshell closure at $N=58$ is created by the nearly degenerated $\ensuremath{\nu}3{s}_{1/2}$ and $\ensuremath{\nu}2{d}_{5/2}$ orbitals being well separated from other orbitals above $N=50$. The near degeneracy of these states could be evidenced by isomerism in this region. The energies of the ${2}_{1}^{+}$ and proposed ${4}_{1}^{+}$ states …

PhysicsRadioactive ion beamsNuclear and High Energy PhysicsIsotopes of germaniumAtomic orbitalDouble beta decayNuclear structureGamma spectroscopyNeutronAtomic physicsSpectroscopyPhysical 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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Shell structure beyond the proton drip line studied via proton emission from deformed 141Ho

2008

Abstract Fine structure in proton emission from the 7 / 2 − [ 523 ] ground state and from the 1 / 2 + [ 411 ] isomer in deformed nucleus 141Ho was studied by means of fusion-evaporation reactions and digital signal processing. Proton transitions to the first excited 2+ state in 140Dy, with the branching ratio of I p g s ( 2 + ) = 0.9 ± 0.2 % and I p m ( 2 + ) = 1.7 ± 0.5 % , were observed. The data are analyzed within the non-adiabatic weak coupling model assuming a large quadrupole deformation of the daughter nucleus 140Dy as predicted by the self-consistent theory. Implications of this result on coexistence effects around N = 74 are discussed. Significant modifications of the proton shell…

PhysicsNuclear and High Energy PhysicsProtonProton radioactivity; Proton shell structure; Two-body tensor interactionsNuclear TheoryHadronElementary particleExcited stateQuadrupoleProton emissionAtomic physicsNuclear ExperimentNucleonGround statePhysics Letters B
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Beta decay of the new isotope101Sn

1995

The very neutron-deficient isotope 101Sn was produced in a 50Cr(58Ni, 2p5n) reaction and its decay properties were determined for the first time. By using chemically selective ion sources of an on-line mass separator, the energy spectrum and the half-life (3 ± 1 s) of beta-delayed protons of 101Sn were measured. These results are compared to theoretical predictions.

PhysicsDecay schemeIsotopeSeparator (oil production)Condensed Matter PhysicsBeta decayAtomic and Molecular Physics and OpticsBeta-decay stable isobarsIonNuclear physicsEnergy spectrumAtomic physicsNuclear ExperimentMathematical PhysicsPhysica Scripta
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"Table 2" of "Few neutron removal from U-238 at relativistic energies"

1997

Uranium fragmentation.

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

1997

Uranium fragmentation.

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