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Two-photon laser isotope separation of atomic uranium: Spectroscopic studies, excited-state lifetimes, and photoionization cross sections
57
Citations
5
References
1976
Year
EngineeringNuclear PhysicsAtomic Emission SpectroscopyNuclear DataIon Beam InstrumentationChemistryElectronic Excited StateExcited-state LifetimesNuclear MaterialsAtomic BeamRadiologyPhotoionization Cross SectionsAccelerator Mass SpectrometryPhotochemistryPhysicsNuclear SecurityAtomic PhysicsPercent EnrichmentExcited State PropertyExperimental Nuclear PhysicsLaser PhotochemistryNatural SciencesSpectroscopyApplied PhysicsMass SpectrometryRadioanalytical ChemistryAtomic UraniumNuclear ExperimentsUranium Vapor
Experimental studies are described wherein an atomic beam of uranium vapor produced by electron-beam evaporation is selectively excited and ionized by light from two short-pulse narrow-bandwidth, tuned dye lasers, and detected and analyzed by a mass spectrometer. The total number of ions per pulse produced is small; however, the time of production is known precisely. By counting single ions, using digital logic, and multiplexing the mass spectrometer between U <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">238</sup> and U <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">235</sup> , it is possible to measure isotope ratios as a function of exciter wavelength and to correct for background effects and spurious ions. These results demonstrated 50 percent enrichment of U <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">235</sup> /U <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">238</sup> . Excited-state lifetimes were measured by observing yields as a function of the delay between the two laser pulses. In addition, for an excitation wavelength of 4266.325 Å, the variation of two-step photoionization efficiency was measured as a function of the wavelength of the ionizing laser. The maximum yield at an ionizing wavelength of 3609 Å corresponds to a cross section of <tex xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2 \times 10^{-17}</tex> cm <sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup> for matched linewidths. Also the ionization potential of uranium was determined to be 6.187 ± 0.002 eV.
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