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Hash Hashemian: Visionary leadership
As Dr. Hashem M. “Hash” Hashemian prepares to step into his term as President of the American Nuclear Society, he is clear that he wants to make the most of this unique moment.
A groundswell in public approval of nuclear is finding a home in growing governmental support that is backed by a tailwind of technological innovation. “Now is a good time to be in nuclear,” Hashemian said, as he explained the criticality of this moment and what he hoped to accomplish as president.
R. Dóczi, V. Semkova, A. Fenyvesi, N. Yamamuro, Cs. M. Buczkó, J. Csikai
Nuclear Science and Engineering | Volume 129 | Number 2 | June 1998 | Pages 164-174
Technical Paper | doi.org/10.13182/NSE98-A1970
Articles are hosted by Taylor and Francis Online.
Precise cross sections were measured for the 90Zr(n,)87mSr, 94Zr(n,)91Sr, 92Mo(n,)89m+gZr, 45Sc(n,)42K, 51V(n,)48Sc, 59Co(n,)56Mn, 93Nb(n,)90mY, 92Mo(n,p)92mNb, 96Mo(n,p)96Nb, 97Mo(n,p)97m+gNb, 90Zr(n,p)90mY, 91Zr(n,p)91mY, 92Zr(n,p)92Y, and 60Ni(n,p)60m+gCo reactions in the 7- to 14.7-MeV neutron energy range. Excitation functions were completed with a number of new differential data.Spectrum-averaged (n,) and (n,p) cross sections were measured for the 54Fe(n,)51Cr, 68Zn(n,)65Ni, 27Al(n,)24Na, 58Ni(n,p)58m+gCo, 64Zn(n,p)64Cu, 59Co(n,p)59Fe, 94Zr(n,p)94Y, 56Fe(n,p)56Mn, 46Ti(n,p)46m+gSc, 47Ti(n,p)47Sc, 48Ti(n,p)48Sc, and 62Ni(n,)59Fe reactions in addition to those aforementioned using a thick target Be(d,n) neutron field at Ed = 9.72 MeV. Results were compared with the ENDF/B-VI, IRDF90, JENDL-3, BROND, JEF-2, CENDL-2, and ADL-3 data files and the SINCROS-II system for testing the validation of differential data and the nuclear model calculations.
