0000000000089547

AUTHOR

S. Czajkowski

showing 9 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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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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Primary-residue production cross sections and kinetic energies in 1AGeV 208Pb on deuteron reactions

2002

Abstract The production cross sections and the kinematical properties of primary residual nuclei have been studied in the reaction 208 Pb(1  A  GeV)+d. Isotopic distributions were measured for all elements from titanium ( Z =22) to lead ( Z =82). The measured kinematical properties of the residues were also used to disentangle the relevant reaction mechanisms, spallation–evaporation and spallation–fission. The fragment separator FRS at GSI, Darmstadt, was used to separate and identify the reaction products. The measured quantities are important for the design and planning of future radioactive-beam facilities and accelerator-driven systems. The measured data of the present work are comprehe…

Nuclear physicsNuclear reactionPhysicsNuclear and High Energy PhysicsReaction mechanismResidue (chemistry)DeuteriumRecoil velocityMass spectrumCharge densityKinetic energyNuclear Physics A
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The $\beta$-delayed one- and two-proton emission of $^{27}$S

2001

In an experiment performed at the GANIL LISE3 facility, radioactive 27S isotopes have been produced by projectile fragmentation of a 95 AMeV 36Ar primary beam. After selection by means of the LISE3 separator, the isotope of interest was implanted in a silicon-detector telescope where its half-life ( T 1/2 = 15.5(15) ms) and its main decay branches were measured.

PhysicsNuclear and High Energy PhysicsDecay schemeIsotopes of germanium010308 nuclear & particles physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesBeta-decay stable isobarsNuclear physics0103 physical sciencesBeta particleIsotopes of zirconiumIsotopes of siliconProton emission010306 general physicsRadioactive decay
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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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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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Spectroscopic studies of neutron-deficient light nuclei: decay properties of 21Mg, 25Si and 26P

2003

Neutron‐deficient nuclei with Tz equals to −3/2 and −2 have been produced at the GANIL/LISE3 facility in fragmentation reactions of a 95 MeV/u 36Ar primary beam in a 12C target. For the first time, β‐delayed proton and β‐γ emission has been simultaneously observed in the decay of 21Mg, 25Si and 26P. The decay scheme of the latter is proposed and the Gamow‐Teller strength distribution in its β decay is compared to shell‐model calculations based on the USD interaction. The B(GT) values derived from the absolute measurement of the β‐branching ratios are in agreement with the quenching factor of about 60% obtained for allowed Gamow‐Teller transitions in this mass region. A precise half‐life of …

23.50.+z 23.40.-s 23.20.Lv 27.30.+tPhysicsDecay schemeProtonIsotopes of germaniumBranching fractionNuclear Theory[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energyNuclear physicsDouble beta decayNeutronProton emissionAtomic physicsNuclear ExperimentRadioactive decayAIP Conference Proceedings
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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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