NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = C.Romano Found 8 matches. 2022KO12 Phys. Rev. Res. 4, 021001 (2022) K.Kolos, V.Sobes, R.Vogt, C.E.Romano, M.S.Smith, L.A.Bernstein, D.A.Brown, M.T.Burkey, Y.Danon, M.A.Elsawi, B.L.Goldblum, L.H.Heilbronn, S.L.Hogle, J.Hutchinson, B.Loer, E.A.McCutchan, M.R.Mumpower, E.M.O'Brien, C.Percher, P.N.Peplowski, J.J.Ressler, N.Schunck, N.W.Thompson, A.S.Voyles, W.Wieselquist, M.Zerkle Current nuclear data needs for applications
doi: 10.1103/PhysRevResearch.4.021001
2022RO17 Nucl.Technology 208, 1696 (2022) C.Romano, R.Venkataraman, D.Glasgow, B.Roach Measurement of the Effective Capture Cross Section of 238Np in the High Flux Isotope Reactor NUCLEAR REACTIONS 237Np(n, γ), E thermal; measured reaction products, Eγ, Iγ; deduced σ, resonance integral, Westcott factor. Comparison with ENDF/B-VIII.0 and JENDL-4.0 libraries. ORNL Neutron Activation Analysis (NAA) laboratory at High Flux Isotope Reactor (HFIR).
doi: 10.1080/00295450.2022.2070353
2021BR10 Nucl.Instrum.Methods Phys.Res. A1009, 165485 (2021) D.P.Broughton, S.Croft, C.Romano, A.Favalli Sensitivity of the simulation of passive neutron emission from UF6 cylinders to the uncertainties in both 19F(α, n) energy spectrum and thick target yield of 234U in UF6 NUCLEAR REACTIONS 19F(α, n), E<10 MeV; analyzed available data; deduced Passive Neutron Enrichment Meter (PNEM) detector parameters for the verification of bulk 235U content.
doi: 10.1016/j.nima.2021.165485
2019BE41 Ann.Rev.Nucl.Part.Sci. 69, 109 (2019) L.A.Bernstein, D.A.Brown, A.J.Koning, B.T.Rearden, C.E.Romano, A.A.Sonzogni, A.S.Voyles, W.Younes Our Future Nuclear Data Needs
doi: 10.1146/annurev-nucl-101918-023708
2011DA20 J.Korean Phys.Soc. 59, 1649s (2011) Y.Danon, R.Block, J.Thompson, C.Romano Fission Physics and Cross Section Measurements with a Lead Slowing down Spectrometer NUCLEAR REACTIONS 235U, 239Pu(n, F), E=thermal, 0.1 eV-2 keV; measured fission fragments E; deduced preneutron fission fragment yields vs TKE and mass, σ. 147,149Sm(n, α), E=0.01-1.E5 eV; measured reaction products; deduced σ. Compared to other data, ENDF/B-VII.0, JENDL-3.2. Measurements using LSDS (Lead Slowing Down Spectrometer).
doi: 10.3938/jkps.59.1649
2010RO04 Phys.Rev. C 81, 014607 (2010) C.Romano, Y.Danon, R.Block, J.Thompson, E.Blain, E.Bond Fission fragment mass and energy distributions as a function of incident neutron energy measured in a lead slowing-down spectrometer NUCLEAR REACTIONS 235U(n, F), E=0.1-1 keV; measured fission fragments, fission σ, yield, TKE trends and fission mode ratio trends in resonance region, pre- and post-neutron emission mass distributions in lead-slowing down spectrometer (LSDS). 252Cf(SF); used as a reference. Comparisons with ENDF/B-VII.0.
doi: 10.1103/PhysRevC.81.014607
2006RO22 Nucl.Instrum.Methods Phys.Res. A562, 771 (2006) C.Romano, Y.Danon, R.C.Haight, S.A.Wender, D.J.Vieira, E.M.Bond, R.S.Rundberg, J.B.Wilhelmy, J.M.O'Donnell, A.F.Michaudon, T.A.Bredeweg, D.Rochman, T.Granier, T.Ethvignot Measurements of (n, α) cross-section of small samples using a lead-slowing-down-spectrometer NUCLEAR REACTIONS 6Li(n, α), E ≈ 0.1-10000 eV; measured Eα, σ(E). Lead-slowing-down spectrometer.
doi: 10.1016/j.nima.2006.02.052
2006RO28 Nucl.Instrum.Methods Phys.Res. A564, 400 (2006) D.Rochman, R.C.Haight, J.M.O'Donnell, S.A.Wender, D.J.Vieira, E.M.Bond, T.A.Bredeweg, J.B.Wilhelmy, T.Granier, T.Ethvignot, M.Petit, Y.Danon, C.Romano Cross-section measurements for 239Pu(n, f) and 6Li(n, α) with a lead slowing-down spectrometer NUCLEAR REACTIONS 239Pu(n, F), E < 100 keV; measured fission σ. 6Li(n, α), E < 10 keV; measured σ. Lead slowing-down spectrometer.
doi: 10.1016/j.nima.2006.03.032
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