Search results for " uranium"

showing 10 items of 24 documents

Ion beam analysis and alpha spectrometry of sources electrodeposited on several backings

1998

Abstract Alpha sources of several activities were prepared by electrodeposition of natural uranium onto four different backings: stainless steel, Ni, Mo and Ti. The influence of the activity, the type of backing, and the process of heating the source on the energy resolution of the spectra were investigated using alpha spectrometry and Rutherford Backscattering Spectrometry (RBS) techniques. Diffusion profiles of the radioactive deposits in the backings were obtained from RBS and related to the results using alpha spectrometry

Nuclear and High Energy PhysicsIon beam analysisMaterials scienceAlpha spectrometryResolution (mass spectrometry)Radiochemistrytechnology industry and agricultureAnalytical chemistryNatural uraniumRutherford backscattering spectrometryInstrumentation
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Delayed-neutrons from arsenic isotopes 84As, 85As and 86As

1973

Abstract Short-lived arsenic isotopes were produced by thermal-neutron fission of 235U and isolated within 2·5 sec by volatilization of arsenic hydride. The existence of a strong delayed-neutron precursor of 2·05±0·05 sec half-life among the arsenic isotopes is confirmed and its assignment to 85As ascertained by milking of the daughter product 33 sec 85Se and 3·1 min 84Se, which is the final nucleus in the neutron decay branch of 85As. A delayed-neutron yield of 7·8 ± 1·2 neutrons/104 fissions was obtained for 85As. A new isotope, 0·9 ± 0·2 sec 86As, was detected by delayed-neutron counting and by following the decay of its most prominent γ-ray. The mass assignment was verified by milking o…

Nuclear fission productCluster decayPolymers and PlasticsIsotopeIsotopes of uraniumChemistryNeutron emissionIsotopes of samariumRadiochemistryMaterials ChemistryFission product yieldDelayed neutronJournal of Inorganic and Nuclear Chemistry
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Mass mapping of a new area of neutron-deficient suburanium nuclides

2002

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

Nuclear physicsPhysicsNuclear and High Energy PhysicsIsotopes of uraniumIsotopeNuclear TheoryMass spectrumNeutronNuclideNuclear ExperimentMass spectrometryRadioactive decayIsotopes of thoriumNuclear Physics A
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New levels in 118Pd observed in the beta-decay of very neutron-rich 118Rh isotope

2006

We investigate the β decay of very neutron-rich 118Rh isotope using on-line mass-separated sources which are produced by applying 25 MeV proton induced symmetric fission of natural uranium at the IGISOL facility. The β–γ and γ–γ coincidence spectroscopy is employed to establish the level scheme of daughter nucleus 118Pd. Five low-lying new levels are identified for the first time with tentative spin and parity assignments based on the even-mass Pd systematics.

PhysicsIsotopeFissionNuclear TheoryGeneral Physics and AstronomyNatural uraniumBeta decayCoincidenceNuclear physicsmedicine.anatomical_structuremedicineNeutronNuclear ExperimentSpectroscopyNucleus
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New Short-Lived IsotopeU221and the Mass Surface NearN=126

2015

Two short-lived isotopes ^{221}U and ^{222}U were produced as evaporation residues in the fusion reaction ^{50}Ti+^{176}Yb at the gas-filled recoil separator TASCA. An α decay with an energy of E_{α}=9.31(5)  MeV and half-life T_{1/2}=4.7(7)  μs was attributed to ^{222}U. The new isotope ^{221}U was identified in α-decay chains starting with E_{α}=9.71(5)  MeV and T_{1/2}=0.66(14)  μs leading to known daughters. Synthesis and detection of these unstable heavy nuclei and their descendants were achieved thanks to a fast data readout system. The evolution of the N=126 shell closure and its influence on the stability of uranium isotopes are discussed within the framework of α-decay reduced widt…

PhysicsIsotopeIsotopes of uraniumAnalytical chemistryGeneral Physics and AstronomyNuclear fusionAlpha decayAtomic physicsRecoil separatorPhysical Review Letters
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Beta Decay of68–74Niand Level Structure of Neutron-Rich Cu Isotopes

1998

The isotopes ${}^{68--74}\mathrm{Ni}$, of interest both for nuclear physics and astrophysics, have been produced in proton-induced fission of ${}^{238}\mathrm{U}$ and ionized in a laser ion guide coupled to an on-line mass separator. Their $\ensuremath{\beta}$ decay was studied by means of $\ensuremath{\beta}$- $\ensuremath{\gamma}$ and $\ensuremath{\gamma}$- $\ensuremath{\gamma}$ spectroscopy. Half-lives have been determined and production cross sections extracted. A partial level scheme is presented for ${}^{73}\mathrm{Cu}$ and additional levels for ${}^{71}\mathrm{Cu}$, providing evidence for a sharply lowered position of the $\ensuremath{\pi}{1f}_{5/2}$ orbital as occupancy of the $\ens…

PhysicsIsotopes of germaniumIsotopes of uraniumIsotopes of palladiumIsotopes of samariumIsotopes of xenonGeneral Physics and AstronomyIsotopes of zirconiumProduction (computer science)NeutronAtomic physicsPhysical Review Letters
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Production of neutron-rich isotopes in fission of uranium induced by neutrons of 20 MeV average energy

2000

In the context of a parameter study conducted by several laboratories for future European radioactive beam facilities based on fast-neutron induced fission, in particular for the SPIRAL-II project at GANIL, we have measured the yields of neutron-rich isotopes in the mass range of 88 to 144. These nuclei were obtained as fission products of natural uranium bombarded by neutrons of 20 MeV average energy emitted by a thick carbon target irradiated by 50 MeV deuterons. Yields have been measured using on-line mass separation with the ion-guide method. Compared with proton-induced fission at 25 MeV the magnitude of cross-sections, except for the symmetric region, is similar. Z-distributions of is…

PhysicsNuclear and High Energy PhysicsCold fissionIsotopes of uranium010308 nuclear & particles physicsNeutron emissionIsotopes of samariumNuclear TheoryFission product yield[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciences7. Clean energyFast fissionNuclear physicsUranium-2380103 physical sciencesPhysics::Accelerator PhysicsNuclear Experiment010306 general physicsLong-lived fission product
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Fine structure in the alpha decays of 226U and 230Pu

1999

The nuclei 226U and 230Pu have been populated via reactions involving 208Pb targets bombarded by 22Ne and 26Mg projectiles. Fusion-evaporation residues were separated in-flight using a gas-filled recoil separator. A position-sensitive Si-strip detector was employed at the focal plane in order to identify correlated α-decay chains. Two fine structure α-decay lines have been observed. The first, with an energy of 7385(5) keV, is assigned as the α decay from 226U to the first excited 2+ state of 222Th. The second line, observed for the first time in this work, has an energy of 6961(30) keV and is assigned as the α decay from 230Pu to the first excited 2+ state of 226U. The excitation energy of…

PhysicsNuclear and High Energy PhysicsIsotopeIsotopes of uranium[PHYS.NEXP] Physics [physics]/Nuclear Experiment [nucl-ex]Excited stateHadronNuclear fusionAlpha decayAtomic physics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]ExcitationRadioactive decay
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Determination of the content in uranium oxide particles by fission track analysis

2004

Abstract One of the most important tasks of nuclear safeguards is to control the activities in nuclear facilities worldwide. These activities include the enrichment of 235 U . To identify enrichments above the maximum authorised level in commercial enrichment plants (usually 5% 235 U ) swipe tests are performed and the 235 U enrichment is determined in the sampled uranium oxide particles. A method is described that allows to measure the 235 U content in small particles (around 1 μm in diameter) by the use of fission tracks. It is based on the fact that in uranium fuel, only 235 U atoms are fissile with thermal neutrons and contribute to the amount of fission tracks counted for individual pa…

PhysicsNuclear and High Energy PhysicsIsotopes of uraniumFissionRadiochemistrychemistry.chemical_elementUraniumEnriched uraniumNuclear physicschemistry.chemical_compoundchemistryUranium-235Uranium oxideParticleNeutronInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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(e,e′f)-Coincidence Experiments on Uranium Isotopes

1986

(e,e′f)-coincidence experiments represent the most powerful tool to investigate the decay properties of giant multipole resonances, especially of the isoscalar giant quadrupole resonance (GQR), in heavy nuclei. Besides the advantages of the inelastic electron scattering, the coincidence between the fission fragments and the scattered electron causes a complete suppression of the huge radiation tail. The study of the fission decay of giant resonances in heavy nuclei provides interesting information about the coupling of the collective phenomena of fission and giant resonances. In particular the fission decay of the GQR has been subject of controversial experimental studies, using hadrons [1]…

PhysicsNuclear physicsIsotopes of uraniumFissionIsoscalarGiant resonanceNuclear TheoryQuadrupoleHadronResonanceElectronNuclear Experiment
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