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Nuclear Energy Conference & Expo (NECX)
September 8–11, 2025
Atlanta, GA|Atlanta Marriott Marquis
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Powering the future: How the DOE is fueling nuclear fuel cycle research and development
As global interest in nuclear energy surges, the United States must remain at the forefront of research and development to ensure national energy security, advance nuclear technologies, and promote international cooperation on safety and nonproliferation. A crucial step in achieving this is analyzing how funding and resources are allocated to better understand how to direct future research and development. The Department of Energy has spearheaded this effort by funding hundreds of research projects across the country through the Nuclear Energy University Program (NEUP). This initiative has empowered dozens of universities to collaborate toward a nuclear-friendly future.
Zhao Xuan, Zeng Fan-An
Nuclear Science and Engineering | Volume 89 | Number 4 | April 1985 | Pages 351-361
Technical Note | doi.org/10.13182/NSE85-A18626
Articles are hosted by Taylor and Francis Online.
Using the single-channel resonating group method, in which a central nucleon-nucleon potential containing a soft repulsive core (SRC) is adopted, the (d + d) scattering phase shifts, differential scattering cross sections, and total reaction cross sections at a series of energies <20 MeV with and without imaginary potentials are calculated. The agreement between the theoretical and experimental results is quite good. The main conclusions are: The (d + d) nonlocal kernel function KS (R, R') deduced is correct; hence, the discrepancy between the kernels in other similar work is clarified. The SRC causes a decrease in the total strength of the (d − d) direct potential VNs(R) and, in particular, the strength of VNs for short range and small channel spin s decreases much more. The SRC causes a decrease in the phase shifts δls(E) (toward the negative direction); the decrease is especially large when E is at or near a resonating energy. The SRC reduces the total reaction cross sections σR appreciably and causes a distinct increase in the differential scattering cross sections dσ/dΩ(θ) at the forward and backward angles; however, it does not greatly influence the differential cross sections at other angles.