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The main objective of these benchmarks is to contribute to research and development of neutronics on fast neutron spectrum cores in ADS through the experimental data with the use of differing external neutron (14 MeV neutrons generated by D-T reactions; spallation neutrons generated by 100 MeV protons and Pb-Bi target), carried out at the Kyoto University Critical Assembly (KUCA) A-core. Special thanks are due the KUCA and the fixed-filed alternative gradient (FFAG) accelerator staff for support and patience throughout a series of ADS experiments carried out at KUCA.

These experimental benchmarks were contributed to the Coordinated Research Project (CRP) T33002 in the International Atomic Energy Agency (IAEA), as entitled "Accelerator Driven Systems (ADS) and Use of Low-Enriched Uranium in ADS, " from 2016 to 2019. The main objective of these benchmarks is to contribute to research and development of neutronics on Uranium-Lead (U-Pb) cores in ADS through the experimental data with the use of differing external neutron (14 MeV neutrons generated by D-T reactions; spallation neutrons generated by 100 MeV protons and Pb-Bi target), carried out at the Kyoto University Critical Assembly (KUCA) A-core. Special thanks are due the KUCA and the fixed-filed alternative gradient (FFAG) accelerator staff for support and patience throughout a series of ADS experiments carried out at KUCA.

The European Spallation Source Neutrino Super Beam (ESSνSB) is a proposed neutrino oscillation experiment to be held in Lund and which takes advantage of the ESS linac firstly designed to study spallation neutrons. Here we study the capability of this facility to discover the yet unknown parameters in the neutrino sector, such as the existence of CP violation. We optimize the physics performance as a function of the baseline and running time of the experiment in each polarity and make an in depth study of the impact of particular systematic errors., QC 20200617

Experiments with the natural uranium target assembly “QUINTA” exposed to 4 and 8 GeV deuteron beams of the Nuclotron accelerator at the Joint Institute for Nuclear Research (Dubna) are analyzed. The reaction rates of 27Al(n,y1)24Na, 27Al(n,y2)22Na and 27Al(n,y3)7Be reactions with effective threshold energies of 5, 27, and 119 MeV were measured at both 4 GeV and 8 GeV deuteron beam energies. The average neutron fluxes between the effective threshold energies and the effective ends of the neutron spectra (which are 800 or 1000 MeV for 4 or 8 GeV deuterons) were determined. The evidence for the intensity shift of the neutron spectra to higher neutron energies with the increase of the deuteron energy from 4 GeV to 8 GeV was found from the ratios of the average neutron fluxes. The reaction rates and the average neutron fluxes were calculated with the MCNPX 2.7 code.

Experimental studies on the uranium- and thorium-loaded acceleratordriven system (ADS) are being conducted for basic research of nuclear transmutation analyses with the combined use of the core at the Kyoto University Critical Assembly (KUCA) and the fixed-field alternating gradient (FFAG; 100 MeV protons) accelerator in the Kyoto University Research Reactor Institute. The ADS experiments with 100 MeV protons were carried out to investigate the neutronic characteristics of ADS, and the static and kinetic parameters were accurately analyzed through both the measurements and the Monte Carlo simulations of reactor physics parameters. An upcoming ADS at KUCA could be composed of highly enriched uranium fuel and Pb-Bi material, and the reaction rate ratio analyses (237Np and 241Am) of nuclear transmutation could be conducted in the ADS (hard spectrum core) at KUCA. The neutronic characteristics of Pb-Bi are expected to be examined through reactor physics experiments at KUCA with the use of solid Pb-Bi materials at the target and in the core.

Experiments with the natural uranium target assembly “QUINTA” exposed to 4 and 8 GeV deuteron beams of the Nuclotron accelerator at the Joint Institute for Nuclear Research (Dubna) are analyzed. The reaction rates of 27Al(n,y1)24Na, 27Al(n,y2)22Na and 27Al(n,y3)7Be reactions with effective threshold energies of 5, 27, and 119 MeV were measured at both 4 GeV and 8 GeV deuteron beam energies. The average neutron fluxes between the effective threshold energies and the effective ends of the neutron spectra (which are 800 or 1000 MeV for 4 or 8 GeV deuterons) were determined. The evidence for the intensity shift of the neutron spectra to higher neutron energies with the increase of the deuteron energy from 4 GeV to 8 GeV was found from the ratios of the average neutron fluxes. The reaction rates and the average neutron fluxes were calculated with the MCNPX 2.7 code.

Experiments with the natural uranium target assembly “QUINTA” exposed to 4 and 8 GeV deuteron beams of the Nuclotron accelerator at the Joint Institute for Nuclear Research (Dubna) are analyzed. The reaction rates of 27Al(n,y1)24Na, 27Al(n,y2)22Na and 27Al(n,y3)7Be reactions with effective threshold energies of 5, 27, and 119 MeV were measured at both 4 GeV and 8 GeV deuteron beam energies. The average neutron fluxes between the effective threshold energies and the effective ends of the neutron spectra (which are 800 or 1000 MeV for 4 or 8 GeV deuterons) were determined. The evidence for the intensity shift of the neutron spectra to higher neutron energies with the increase of the deuteron energy from 4 GeV to 8 GeV was found from the ratios of the average neutron fluxes. The reaction rates and the average neutron fluxes were calculated with the MCNPX 2.7 code.

Experiments with the natural uranium target assembly “QUINTA” exposed to 4 and 8 GeV deuteron beams of the Nuclotron accelerator at the Joint Institute for Nuclear Research (Dubna) are analyzed. The reaction rates of 27Al(n,y1)24Na, 27Al(n,y2)22Na and 27Al(n,y3)7Be reactions with effective threshold energies of 5, 27, and 119 MeV were measured at both 4 GeV and 8 GeV deuteron beam energies. The average neutron fluxes between the effective threshold energies and the effective ends of the neutron spectra (which are 800 or 1000 MeV for 4 or 8 GeV deuterons) were determined. The evidence for the intensity shift of the neutron spectra to higher neutron energies with the increase of the deuteron energy from 4 GeV to 8 GeV was found from the ratios of the average neutron fluxes. The reaction rates and the average neutron fluxes were calculated with the MCNPX 2.7 code.

Experiments with the natural uranium target assembly “QUINTA” exposed to 4 and 8 GeV deuteron beams of the Nuclotron accelerator at the Joint Institute for Nuclear Research (Dubna) are analyzed. The reaction rates of 27Al(n,y1)24Na, 27Al(n,y2)22Na and 27Al(n,y3)7Be reactions with effective threshold energies of 5, 27, and 119 MeV were measured at both 4 GeV and 8 GeV deuteron beam energies. The average neutron fluxes between the effective threshold energies and the effective ends of the neutron spectra (which are 800 or 1000 MeV for 4 or 8 GeV deuterons) were determined. The evidence for the intensity shift of the neutron spectra to higher neutron energies with the increase of the deuteron energy from 4 GeV to 8 GeV was found from the ratios of the average neutron fluxes. The reaction rates and the average neutron fluxes were calculated with the MCNPX 2.7 code.

Scandium-47 (T1/=3.41d) forms stable complexes with aminopolycarboxylic acids, useful as tumor biomarkers or antigens. Its therapeutic beta emissions at 441.1 keV and 600.5 keV are coupled with an imageable 159.4 keV gamma to permit in vivo-tracking of compound biodistribution. Currently, its wider clinical application is hindered by lack of availability, even as interest grows in radioscandium-based pharmaceuticals. We have investigated the Ti-47(n,np)Sc-47, 50Ti(n,3p) Sc-47,V-nat(n,x)Sc-47, and Ti-nat(n,x)Sc-47 reactions as potential routes to therapeutically relevant quantities of Sc-47. Targets of V-nat, Ti-nat and enriched Ti-47 (95.7% isotopic abundnace) and Ti-50 (83.1%) oxide targets were exposed to the spallation neutrons resulting from the proton-irradiation of RbCl and Ga targets at the Los Alamos National Laboratory (LANL) Isotope Production Facility (IPF). Radioisotopic purities of 47Sc in excess of 90% are achieved by activation of Ti-47 targets with an instantaneous production rate of 0.29+/-0.03 micro-Ci/g per Ah, and small yields of Ca-47 produce Sc-47 with 100% purity from activation of Ti-50., The original document contains color images.