NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = H.Farrar Found 9 matches. 1989OL03 Appl.Radiat.Isot. 40, 199 (1989) B.M.Oliver, M.M.Bretscher, H.Farrar Mass spectrometric determinations of the absolute tritium activities of NBS tritiated water standards RADIOACTIVITY 3H(β-); measured decay products; deduced T1/2. Comparison with available data. U.S. National Bureau of Standards tritiated water Standard Reference Materials.
doi: 10.1016/0883-2889(89)90148-2
1987OL04 Int.J.Appl.Radiat.Isotop. 38, 959 (1987) B.M.Oliver, H.Farrar IV, M.M.Bretscher Tritium Half-life Measured by Helium-3 Growth RADIOACTIVITY 3H(β-) [from 6Li(n, t), 7Li(n, n't), E=reactor spectrum]; measured T1/2. Helium-3 growth method.
doi: 10.1016/0883-2889(87)90268-1
1986KN01 Nucl.Sci.Eng. 92, 491 (1986) D.W.Kneff, B.M.Oliver, H.Farrar IV, L.R.Greenwood Helium Production in Pure Elements, Isotopes, and Alloy Steels by 14.8 MeV Neutrons NUCLEAR REACTIONS Be, B, C, O, F, Al, Si, Ti, V, Cr, Mn, Fe, Co, Ni, Cu, Y, Zr, Nb, Mo, Ag, Sn, Ta, Pt, Au, Pb(n, α), E=14.8 MeV; measured α-production σ.
doi: 10.13182/NSE86-A18608
1975FA09 Nucl.Technology 25, 305 (1975) H.Farrar, IV, W.N.McElroy, E.P.Lippincott Helium Production Cross Section of Boron for Faster-Reactor Neutron Spectra NUCLEAR REACTIONS 10B(n, α), E=0.69-0.85 MeV; measured helium concentration; deduced σ and uncertainties. Comparison with available data.
doi: 10.13182/NT75-A24371
1964FA12 Can.J.Phys. 42, 2063 (1964) H.Farrar, W.B.Clarke, H.G.Thode, R.H.Tomlinson Cumulative yields of the heavy fragments in the thermal-neutron fission of 241Pu NUCLEAR REACTIONS 241Pu(n, F)131Xe/132Xe/133Xe/134Xe/135Xe/136Xe/138Xe/133Cs/135Cs/137Cs/136Ba/138Ba/140Ba/140Ce/141Ce/142Ce/144Ce/142Nd/143Nd/144Nd/145Nd/146Nd/148Nd/150Nd/147Sm/148Sm/149Sm/150Sm/151Sm/152Sm/154Sm/137Cs, E thermal; measured fission products with mass spectrometer; deduced fission yields. Comparison with available data.
doi: 10.1139/p64-191
1962FA07 Nucl.Phys. 34, 367 (1962) Cumulative Yields Of The Heavy Fragments In U235 Thermal Neutron Fission NUCLEAR REACTIONS 235U(n, f), E=0.0253 eV; measured products, 138Ba, 137Ba, 136Ba, 140Ba, 144Ce, 141Ce, 140Ce, 142Ce, 150Nd, 148Nd, 147Nd, 146Nd, 145Nd, 144Nd, 143Nd, 154Sm, 152Sm, 151Sm, 150Sm, 147Sm, 149Sm, 153Eu, 151Eu, 139Ba; deduced yields. Data were imported from EXFOR entry 13064.
doi: 10.1016/0029-5582(62)90227-4
1962FA08 Can.J.Phys. 40, 1017 (1962) H.Farrar, H.R.Fickel, R.H.Tomlinson Cumulative yields of light fragments in U235 thermal neutron fission NUCLEAR REACTIONS 235U(n, F)86Sr/88Sr/89Sr/90Sr/91Sr/90Zr/91Zr/92Zr/93Zr/94Zr/95Zr/96Zr/83Kr/84Kr/85Kr/86Kr/85Rb/87Rb/89Y/91Y/95Mo/97Mo/98Mo/100Mo/72Zn/73Ga/74Ga/77As/78As/79As/81Se/101Ru/102Ru/103Ru/104Ru/105Ru/106Ru/107Ru/109Pd/111Ag, E thermal; measured fission products with mass spectrometer; deduced fission yields. Comparison with available data.
doi: 10.1139/p62-107
1962FA10 Can.J.Phys. 40, 943 (1962) Structure in the mass-yield distribution for U235 Fission NUCLEAR REACTIONS 235U(n, F), E thermal; analyzed available data; deduced corrections to cumulative yields for delayed neutron emission in A=86-90, 136-139 regions.
doi: 10.1139/p62-100
1961FA03 Can.J.Chem. 39, 681 (1961) H.Farrar, A.K.Dasgupta, R.H.Tomlinson Half-Life of Cs137 NUCLEAR STRUCTURE 137Cs; measured not abstracted; deduced nuclear properties.
doi: 10.1139/v61-081
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