NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.F.Auchampaugh Found 32 matches. 1990FE02 Nucl.Instrum.Methods Phys.Res. A287, 595 (1990) W.C.Feldman, G.F.Auchampaugh, D.M.Drake A Technique to Measure the Neutron Lifetime from Low-Earth Orbit RADIOACTIVITY 1n(β-); analyzed, discussed mean T1/2 measurement techniques. Low-earth orbit.
doi: 10.1016/0168-9002(90)91584-X
1989RE01 Phys.Rev. C39, 766 (1989) D.A.Resler, H.D.Knox, P.E.Koehler, R.O.Lane, G.F.Auchampaugh Structure of 14C via Elastic and Inelastic Neutron Scattering from 13C: Measurement and R-matrix analysis NUCLEAR REACTIONS 13C(n, n), (n, n'), E=4.5-11 MeV; measured σ(θ); deduced 13C(n, α)10Be σ. 14C deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1103/PhysRevC.39.766
1988RA12 Nucl.Sci.Eng. 98, 348 (1988) P.Ramakrishnan, G.E.Mitchell, C.R.Gould, S.A.Wender, G.F.Auchampaugh Photon Production Cross Section for 181Ta NUCLEAR REACTIONS 181Ta(n, X), E=2-100 MeV; measured photon production σ(E, Eγ); deduced σ(E).
doi: 10.13182/NSE88-A23535
1988RA13 Nucl.Sci.Eng. 98, 357 (1988) P.Ramakrishnan, G.E.Mitchell, C.R.Gould, S.A.Wender, G.F.Auchampaugh, R.C.Little Neutron-Induced Photon Production Cross Sections NUCLEAR REACTIONS Ta(n, X), E < 20 MeV; measured Eγ, Iγ, photon production σ(E, Eγ); deduced σ(E).
doi: 10.13182/NSE88-A23536
1986AU01 Phys.Rev. C33, 125 (1986) G.F.Auchampaugh, G.de Saussure, D.K.Olsen, R.W.Ingle, R.B.Perez, R.L.Macklin Resolution of the Nature of the Coupling in Subthreshold Fission in 238U + n NUCLEAR REACTIONS 238U(n, γ), (n, n), E=700-740 eV; measured σ(E). 239U deduced resonance, Γn, Γγ, barrier, other parameters.
doi: 10.1103/PhysRevC.33.125
1986GO14 Radiat.Eff. 92, 139 (1986) C.R.Gould, J.Dave, G.E.Mitchell, P.Ramakrishnan, G.F.Auchampaugh, R.C.Little, S.A.Wender Photon Production Cross Section Measurements for Ta and Be NUCLEAR REACTIONS Ta, 9Be(n, γ), E=2-25 MeV; measured γ-ray production σ.
doi: 10.1080/00337578608208307
1986KO10 Nucl.Phys. A453, 429 (1986) P.E.Koehler, H.D.Knox, D.A.Resler, R.O.Lane, G.F.Auchampaugh Structure of 19O from Measurement and R-Matrix Analysis of σ(θ) for 18O(n, n)18O and 18O(n, n')18O*(1.98 MeV) NUCLEAR REACTIONS 18O(n, n), (n, n'), E=5-7.5 MeV; measured σ(θ). 19O deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1016/0375-9474(86)90446-X
1986LI14 Radiat.Eff. 95, 239 (1986) P.W.Lisowski, S.A.Wender, G.F.Auchampaugh The WNR/PSR Facility - Neutron Physics Capabilities from Sub-Thermal to 800 MeV NUCLEAR REACTIONS 12C(p, n), E at 1050 MeV/c; measured σ(θ) vs neutron momentum.
doi: 10.1080/00337578608208702
1984AU01 Phys.Rev. C29, 174 (1984) G.F.Auchampaugh, M.S.Moore, J.D.Moses, R.O.Nelson, R.C.Extermann, C.E.Olsen, N.W.Hill, J.A.Harvey Nature of the Coupling in Subthreshold Fission of 238Np NUCLEAR REACTIONS 237Np(n, F), (n, X), E-1-600 eV; measured fission, total σ(E). 238Np deduced fission strength function, sharp, broad levels, Γ, subthreshold fission characteristics. Multi-level R-matrix fits.
doi: 10.1103/PhysRevC.29.174
1984WE11 Nucl.Instrum.Methods 220, 371 (1984) S.A.Wender, G.F.Auchampaugh, J.F.Wilkerson, N.W.Hill, L.R.Nilsson, N.R.Roberson A High-Energy Gamma-Ray Detector System for Fast Neutron-Induced Reactions NUCLEAR REACTIONS 12C(n, n'), E=4.9-100 MeV; measured γ-spectra, σ(θγ) vs E. 40Ca(n, γ), E=2-20 MeV; measured absolute σ(θγ=90°) vs E. Pulsed neutron source, bismuth germanate crystal detector.
doi: 10.1016/0167-5087(84)90298-9
1983PE15 Phys.Rev. C28, 1635 (1983) R.B.Perez, G.de Saussure, J.H.Todd, T.J.Yang, G.F.Auchampaugh Measurement of the 232Th(n, f) Subthreshold and Near-Subthreshold Cross Section NUCLEAR REACTIONS 232Th(n, F), E=0.00001-1.6 MeV; measured fission σ(E).
doi: 10.1103/PhysRevC.28.1635
1982LI23 Phys.Rev.Lett. 49, 255 (1982) P.W.Lisowski, R.E.Shamu, G.F.Auchampaugh, N.S.P.King, M.S.Moore, G.L.Morgan, T.S.Singleton Search For Resonance Structure In The np Total Cross Section Below 800 Mev NUCLEAR REACTIONS 1H(n, x), E=39-793 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry 12761.
doi: 10.1103/PhysRevLett.49.255
1981AU03 Phys.Rev. C24, 503 (1981) G.F.Auchampaugh, S.Plattard, N.W.Hill, G.de Saussure, R.B.Perez, J.A.Harvey K Components for the ≈ 1.4-, ≈ 1.6-, and ≈ 1.7-MeV Structures in the Fission of 232Th + n NUCLEAR REACTIONS, Fission 232Th(n, F), E=1.3-1.8 MeV; measured σ(fission, E). 233Th deduced rotational band K, relative fission strengths.
doi: 10.1103/PhysRevC.24.503
1981LA05 Phys.Rev. C23, 1883 (1981) R.O.Lane, H.D.Knox, P.Hoffmann-Pinther, R.M.White, G.F.Auchampaugh States in 14C from σ(total) and σ(elastic)(θ) for 13C + n: Measurement, R-matrix analysis, and model calculations NUCLEAR STRUCTURE 14C; calculated levels. Weak coupling model, effective interactions. NUCLEAR REACTIONS 13C(n, n), E=1.25-6.5 MeV; measured σ(θ). 14C deduced levels, J, π, reduced widths. R-matrix analysis.
doi: 10.1103/PhysRevC.23.1883
1981PL01 Phys.Rev.Lett. 46, 633 (1981) S.Plattard, G.F.Auchampaugh, N.W.Hill, G.de Saussure, J.A.Harvey, R.B.Perez Some Spectroscopic Properties of Fine Structures Observed near the 231Pa(n, f)Fission Threshold NUCLEAR REACTIONS, Fission 231Pa(n, F), E=140-400 keV; measured σ(E). 232Pa deduced resonances, J, π, vibrational character, < Γf >, asymmetrically deformed fission barrier third minimum.
doi: 10.1103/PhysRevLett.46.633
1979AU07 Nucl.Sci.Eng. 69, 30 (1979) G.F.Auchampaugh, S.Plattard, N.W.Hill Neutron Total Cross-Section Measurements of 9Be, 10,11B, and 12,13C from 1.0 to 14 MeV Using the 9Be(d, n)10B Reaction as a 'White' Neutron Source NUCLEAR REACTIONS 9Be, 10,11B, 12,13C(n, X), E=1.0-14 MeV [from 9Be(d, n)]; measured σ. 11,12B deduced fine structure around 9-MeV excitation.
doi: 10.13182/NSE79-A21282
1978HO15 Phys.Lett. 79B, 39 (1978) D.J.Horen, G.F.Auchampaugh, J.A.Harvey On the Question of a Giant M1 Resonance Near 8 MeV in 208Pb NUCLEAR REACTIONS 207Pb(n, X), E=600-627 keV; measured σ(θ). 208Pb deduced levels, L, J, π, Γ, E1 character of levels near 8 MeV. R matrix analysis. Enriched targets.
doi: 10.1016/0370-2693(78)90430-6
1977DR09 Nucl.Sci.Eng. 63, 401 (1977) D.M.Drake, G.F.Auchampaugh, E.D.Arthur, C.E.Ragan, P.G.Young Double-Differential Beryllium Neutron Cross Sections at Incident Neutron Energies of 5.9, 10.1, and 14.2 MeV NUCLEAR REACTIONS Be(n, 2n), E=5.9, 10.1, 14.2 MeV; measured σ(θ).
doi: 10.13182/NSE77-A27057
1975AU06 Phys.Rev. C12, 1126 (1975) G.F.Auchampaugh, J.Halperin, R.L.Macklin, W.M.Howard Kilovolt 33S(n, α0) and 33S(n, γ) Cross Sections: Importance in the Nucleosynthesis of the Rare Nucleus 36S NUCLEAR REACTIONS 33S(n, α), E=10-700 keV; measured σ(E, Eα). 33S(n, γ), E=10-700 keV; measured σ(E, Eγ). 34S deduced resonances, Γ.
doi: 10.1103/PhysRevC.12.1126
1975AU07 Phys.Rev. C12, 1850 (1975) Parameters of the Subthreshold Fission Structure in 240Pu NUCLEAR REACTIONS 240Pu(n, F), E=0.5-10 keV; measured σ; deduced fission widths.
doi: 10.1103/PhysRevC.12.1850
1973AU03 Phys.Rev. C7, 2085 (1973); Erratum Phys.Rev. C8, 1968 (1973) Parameters of the Subthreshold Fission Structure in 242Pu NUCLEAR REACTIONS 242Pu(n, X), E=0.6-81 keV; measured σ(E). 243Pu deduced resonances, level-width.
doi: 10.1103/PhysRevC.7.2085
1971AU06 Nucl.Phys. A171, 31 (1971) G.F.Auchampaugh, J.A.Farrell, D.W.Bergen Neutron-Induced Fission Cross Sections of 242Pu and 244Pu NUCLEAR REACTIONS, Fission 242,244Pu(n, F), E=20 eV-10 MeV; measured σ(E). 243,244Pu deduced level spacings, resonance parameters, second barrier widths.
doi: 10.1016/0375-9474(71)90360-5
1968AU07 Nucl.Phys. A112, 329 (1968) G.F.Auchampaugh, C.D.Bowman, J.E.Evans Neutron-Induced Fission Cross Sections Of 232U NUCLEAR REACTIONS 232U(n, n), (n, f), E=-0.6 eV-1.9 keV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12383.
doi: 10.1016/0375-9474(68)90205-4
1968BO57 Phys.Rev. 166, 1219 (1968) C.D.Bowman, G.F.Auchampaugh, S.C.Fultz, R.W.Hoff Neutron-Induced Fission Cross Section of Am242 NUCLEAR REACTIONS, Fission 242mAm(n, F), E=0.02 eV - 6 MeV; measured σ(E). 243Am deduced resonance parameters.
doi: 10.1103/PhysRev.166.1219
1967ST38 Phys.Rev. 154, 1111 (1967) W.F.Stubbins, C.D.Bowman, G.F.Auchampaugh, M.S.Coops Neutron-Induced Resonance Fission Cross Section of Pu238 NUCLEAR REACTIONS 238Pu(n, n), 238Pu(n, f), 238Pu(n, x), E=2.0-299.2 eV; measured products; deduced resonance parameters, σ, σ(). Data were imported from EXFOR entry 12489.
doi: 10.1103/PhysRev.154.1111
1966AU07 Phys.Rev. 146, 840 (1966) G.F.Auchampaugh, C.D.Bowman, M.S.Coops, S.C.Fultz Neutron total cross sections of 242Pu NUCLEAR REACTIONS 242Pu(n, n), 242Pu(n, x), E=0.0253-388.2 eV; measured products; deduced resonance parameters, σ, σ(E). Data were imported from EXFOR entry 12546.
doi: 10.1103/PhysRev.146.840
1965AU02 WASH-1064, p.46 (1965); and Priv.Comm. (1966) G.F.Auchampaugh, C.D.Bowman, M.S.Coops, S.C.Fultz Total Cross Section of Pu242
1965BO06 Phys.Rev. 137, B326 (1965) C.D.Bowman, M.S.Coops, G.F.Auchampaugh, S.C.Fultz Subthreshold Neutron-Induced Fission Cross Section of Am241 NUCLEAR STRUCTURE 241Am; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.137.B326
1964BO03 Bull. Am. Phys. Soc. 9, No. 1, 19, BC4 (1964) C.D.Bowman, M.S.Coops, G.F.Auchampaugh, S.C.Fultz Subthreshold-Fission Cross Section of Am241 NUCLEAR STRUCTURE, Fission 242Am; measured not abstracted; deduced nuclear properties.
1964BO39 Phys.Rev. 133, B676 (1964) C.D.Bowman, G.F.Auchampaugh, S.C.Fultz Photodisintegration of U235 NUCLEAR REACTIONS 235U(γ, F), (γ, n), (γ, 2n), E=6-23 MeV; measured σ(E); deduced giant resonance structure. 235U deduced quadrupole moment.
doi: 10.1103/PhysRev.133.B676
1963BR09 Phys.Rev. 129, 2723 (1963) R.L.Bramblett, J.T.Caldwell, G.F.Auchampaugh, S.C.Fultz Photoneutron Cross Sections of Ta181 and Ho165 NUCLEAR STRUCTURE 165Ho, 181Ta; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.129.2723
1962BO01 Bull.Am.Phys.Soc. 7, No.1, 22, F2 (1962) C.D.Bowman, G.F.Auchampaugh, C.P.Jupiter, S.C.Fultz High-Resolution Neutron Time-of-Flight Measurements in the eV Region NUCLEAR STRUCTURE 236U; measured not abstracted; deduced nuclear properties.
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