Publication | Open Access
AMS Applications in Nuclear Astrophysics: New Results for <sup>13</sup>C(n,<i>γ</i>) <sup>14</sup>C and <sup>14</sup>N(n,p) <sup>14</sup>C
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2012
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EngineeringNuclear PhysicsNuclear DataNeutron PoisonsNew ResultsNuclear MaterialsHigh-energy Nuclear ReactionAccelerator Mass SpectrometryPhysicsNuclear TheoryNeutron SourceNuclear ReactionsAms ApplicationsHigh-energy AstrophysicsNucleosynthesisNuclear AstrophysicsAstrophysicsEnvironmental RadiochemistryExperimental Nuclear PhysicsNatural SciencesRadioanalytical ChemistryNuclear Experiments
Abstract The technique of accelerator mass spectrometry (AMS) offers a complementary tool for studying long-lived radionuclides in nuclear astrophysics: (1) as a tool for investigating nucleosynthesis in the laboratory; and (2) via a direct search of live long-lived radionuclides in terrestrial archives as signatures of recent nearby supernova-events. A key ingredient to our understanding of nucleosynthesis is accurate cross-section data. AMS was applied for measurements of the neutron-induced cross sections 13 C(n, γ ) and 14 N(n,p), both leading to the long-lived radionuclide 14 C. Solid samples were irradiated at Karlsruhe Institute of Technology with neutrons closely resembling a Maxwell–Boltzmann distribution for kT = 25 keV, and with neutrons of energies between 123 and 178 keV. After neutron activation the amount of 14 C nuclides in the samples was measured by AMS at the VERA (Vienna Environmental Research Accelerator) facility. Both reactions, 13 C(n, γ ) 14 C and 14 N(n,p) 14 C, act as neutron poisons in s-process nucleosynthesis. However, previous experimental data are discordant. The new data for both reactions tend to be slightly lower than previous measurements for the 25 keV Maxwell–Boltzmann energy distribution. For the higher neutron energies no previous data did exist for 13 C(n, γ ), but model calculations indicated a strong resonance structure between 100 and 300 keV which is confirmed by our results. Very limited information is available for 14 N(n,p) at these energies. Our new data at 123 and 178 keV suggest lower cross sections than expected from previous experiments and data evaluations.
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