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Aqueous harvesting of 88Zr at a radioactive-ion-beam facility for cross-section measurements
Isotope harvesting is a method of collecting the long-lived radioisotopes that build up during the operation of ion-beam facilities in a way that is useful for subsequent research. As a demonstration of this method for the collection of a group IV metal at a fragmentation facility, the high-energy Z...
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Published in: | Physical review. C 2021-02, Vol.103 (2) |
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Main Authors: | , , , , , , , , , , , , , , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | Isotope harvesting is a method of collecting the long-lived radioisotopes that build up during the operation of ion-beam facilities in a way that is useful for subsequent research. As a demonstration of this method for the collection of a group IV metal at a fragmentation facility, the high-energy Zr88 secondary beam produced from a 140-MeV/u Mo92 primary beam at the National Superconducting Cyclotron Laboratory (NSCL) was stopped in a water target. The setup aimed to mimic the aqueous beam dump that will be implemented at the Facility for Rare Isotope Beams (FRIB). The collected Zr88 and accompanying Y 88 decay daughter were radiochemically extracted from the solution and made into target samples suitable for neutron-capture cross-section measurements. These samples were then irradiated at two reactor facilities, and the Zr88 average thermal-neutron-capture cross section ( σT ) and resonance integral ( I ) were determined to be σT=(8.04±0.63)×105 b and I=(2.53±0.28)×106 b. The σT value agrees well with previous results and I , determined for the first time here, was found to be the largest measured resonance integral by two orders of magnitude. The Y 88 thermal-neutron-capture cross section was determined to be less than 1.8×104 b. This work demonstrates the steps needed to make cross-section measurements with samples produced via aqueous isotope harvesting. |
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ISSN: | 2469-9985 2469-9993 |