NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = G.P.Couchell Found 21 matches. 1998TI09 Phys.Rev. C58, 905 (1998) S.V.Tipnis, J.M.Campbell, G.P.Couchell, S.Li, H.V.Nguyen, D.J.Pullen, W.A.Schier, E.H.Seabury, T.R.England Yields of Short-Lived Fission Products Produced following 235U(nth, f) NUCLEAR REACTIONS 235U(n, F), E=thermal; measured Eγ, Iγ, βγ-coin; deduced independent, cumulative short-lived fission fragment yields. Helium jet, tape transport.
doi: 10.1103/PhysRevC.58.905
1996BE92 Nucl.Instrum.Methods Phys.Res. A369, 263 (1996) P.R.Bennett, W.A.Schier, G.P.Couchell, E.S.Jacobs, D.J.Pullen, M.F.Villani Relative Efficiency Measurements of Fission Fragment Transfer with a Helium Jet NUCLEAR REACTIONS 235,238U, 239Pu(n, F), E=reactor; measured fission fragment decay associated X-ray spectra; deduced helium jet fission fragment transfer relative efficiency.
doi: 10.1016/0168-9002(95)00551-X
1992VI05 Nucl.Sci.Eng. 111, 422 (1992) M.F.Villani, G.P.Couchell, M.H.Haghighi, D.J.Pullen, W.A.Schier, Q.Sharfuddin Six-Group Decomposition of Composite Delayed Neutron Spectra from 235U Fission NUCLEAR REACTIONS 235U(n, F), E=thermal; measured composite delayed neutron spectra following fission. Constrained least-squares method, six-group decomposition.
doi: 10.13182/NSE92-A15489
1988SH13 Nucl.Sci.Eng. 98, 341 (1988) Q.Sharfuddin, W.A.Schier, R.S.Tanczyn, D.J.Pullen, M.H.Haghighi, L.Fisteag, G.P.Couchell Search for an Energy Dependence in 235U Delayed Neutron Spectra NUCLEAR REACTIONS 235U(n, F), E=fast; measured delayed neutron yield vs E following fission.
doi: 10.13182/NSE88-A23534
1986SH05 Nucl.Sci.Eng. 92, 350 (1986) J.Q.Shao, G.P.Couchell, J.J.Egan, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, E.D.Arthur Fast Neutron Inelastic Scattering Cross Sections of 238U for States between 680 and 1530 keV NUCLEAR REACTIONS 238U(n, n'), E=0.9-2.2 MeV; measured σ(θ), σ(En); deduced optical model parameters, σ(E). 238U level deduced B(λ). 239U deduced fission barrier parameters.
doi: 10.13182/NSE86-A17525
1986SH08 J.Phys.(London) G12, 237 (1986) E.Sheldon, L.E.Beghian, C.A.Ciarcia, G.P.Couchell, J.H.Dave, J.J.Egan, G.Goswami, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, J.Q.Shao Fast-Neutron Inelastic Scattering Cross Sections for the Principal Even-Even Actinide Nuclei. I: 232Th(n, n') NUCLEAR REACTIONS 232Th(n, n'γ), (n, n'), E=0.2-3.4 MeV; analyzed σ(θ), σ(E); deduced reaction mechanism. 232Th deduced consistent σ for rotational, vibrational level excitation.
doi: 10.1088/0305-4616/12/3/011
1986SH28 J.Phys.(London) G12, 443 (1986) E.Sheldon, L.E.Beghian, D.W.S.Chan, A.Chang, G.P.Couchell, J.J.Egan, G.Goswami, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, J.P.Shao, A.Wang Fast Neutron Inelastic-Scattering Cross Sections for the Principal Even-Even Actinide Nuclei. II: 238U(n, n') NUCLEAR REACTIONS 238U(n, n'), E=0.2-3.1 MeV; analyzed experimental, theoretical σ(E), σ(θ); deduced fluctuation σ factor F.
doi: 10.1088/0305-4616/12/5/009
1986TA18 Nucl.Sci.Eng. 94, 353 (1986) R.S.Tanczyn, Q.Sharfuddin, W.A.Schier, D.J.Pullen, M.H.Haghighi, L.Fisteag, G.P.Couchell Composite Delayed Neutron Energy Spectra for Thermal Fission of 235U NUCLEAR REACTIONS 235U(n, F), E=thermal; measured delayed neutron yields following fission. Plastic, liquid, 6Li glass scintillators.
doi: 10.13182/NSE86-A18346
1985CI05 Nucl.Sci.Eng. 91, 428 (1985) C.A.Ciarcia, G.P.Couchell, J.J.Egan, G.H.R.Kegel, S.Q.Li, A.Mittler, D.J.Pullen, W.A.Schier, J.Q.Shao Neutron Inelastic Scattering Cross Sections for States above 700 keV in 232Th NUCLEAR REACTIONS 232Th(n, n'), E=0.95-2.1 MeV; measured σ(θ). 232Th levels deduced possible J, π, K.
doi: 10.13182/NSE85-A18359
1985DA21 Nucl.Sci.Eng. 91, 187 (1985) J.H.Dave, J.J.Egan, G.P.Couchell, G.H.R.Kegel, A.Mittler, D.J.Pullen, W.A.Schier, E.Sheldon Cross Sections, Transition Schemes, and Branching Ratios for 232Th from the 232Th(n, n'γ) Reaction NUCLEAR REACTIONS 232Th(n, n'γ), E=0.77-2.1 MeV; measured Eγ, Iγ; deduced σ(θγ). 232Th deduced levels, γ-branching ratios, possible J, π. Statistical compound nucleus model.
doi: 10.13182/NSE85-A27441
1984SC45 Nucl.Instrum.Methods 227, 549 (1984) W.A.Schier, G.P.Couchell, D.J.Pullen, N.M.Sampas, C.A.Ciarcia, M.H.Haghighi, Q.Sharfuddin, R.S.Tanczyn New Experimental System for Measuring Composite Delayed-Neutron Spectra following Fission NUCLEAR REACTIONS 235U(n, F), E=fast, thermal; measured delayed neutron fission yields vs En. Pilot U, 6Li-glass scintillators, β-neutron tof system.
doi: 10.1016/0168-9002(84)90214-6
1979BE19 Nucl.Sci.Eng. 69, 191 (1979) L.E.Beghian, G.H.R.Kegel, T.V.Marcella, B.K.Barnes, G.P.Couchell, J.J.Egan, A.Mittler, D.J.Pullen, W.A.Schier Neutron Scattering Cross Sections of Uranium-238 NUCLEAR REACTIONS 238U(n, n), (n, n'), E=0.9-3.1 MeV; measured σ(E, θ); deduced disagreement between observed, evaluated inelastic σ.
doi: 10.13182/NSE79-A20610
1978KA21 Nucl.Sci.Eng. 67, 34 (1978) P.T.Karatzas, G.P.Couchell, B.K.Barnes, L.E.Beghian, P.Harihar, A.Mittler, D.J.Pullen, E.Sheldon, N.B.Sullivan Neutron Inelastic Scattering Cross Sections for Natural Chromium Determined from the (n, n'γ) Reaction NUCLEAR REACTIONS Cr(n, n'γ), E=0.84-3.97 MeV; measured σ(E, Eγ), total inelastic σ(E). 52,53,54,50Cr levels deduced γ-branching.
doi: 10.13182/NSE78-A27235
1978LE14 Phys.Rev. C18, 1185 (1978) R.V.LeClaire, J.J.Egan, L.E.Beghian, G.P.Couchell, G.H.R.Kegel, S.C.Mathur, A.Mittler, W.A.Schier Cross Sections in the 59Co(n, n'γ)59Co Reaction from 1.1 to 3.3 MeV NUCLEAR REACTIONS 59Co(n, n'γ), E=1.1-3.3 MeV; measured σ(E, Eγ, θ); deduced σ(n, n'). 59Co deduced levels, J, π, γ-branching.
doi: 10.1103/PhysRevC.18.1185
1977CO15 Nucl.Phys. A286, 322 (1977) J.A.Correia, W.A.Schier, L.E.Beghian, G.P.Couchell, J.J.Egan, G.H.R.Kegel, R.V.Leclaire, A.Mittler 55Mn(n, n'γ) Cross-Section Studies for E = 1.0-3.6 MeV NUCLEAR REACTIONS 55Mn(n, n'γ), En=1.0-3.6 MeV; measured σ(E;Eγ, θ); deduced absolute σ(E, Eγ). 55Mn deduced levels, J, π, γ-decay branching ratios.
doi: 10.1016/0375-9474(77)90411-0
1976SC20 Nucl.Phys. A266, 16 (1976) W.A.Schier, G.P.Couchell, J.J.Egan, P.Harihar, S.C.Mathur, A.Mittler, E.Sheldon Spin and Parity Assignments for 23Na Levels from the 19F(α, p)22Ne Reaction NUCLEAR REACTIONS 19F(α, p), (α, α), E=2.5-5 MeV; measured absolute σ(E, Ep, θ); deduced optical potential. 23Na deduced levels, J, π, L.
doi: 10.1016/0375-9474(76)90279-7
1975SA05 Nucl.Phys. A245, 317 (1975) L.G.Sanin, W.A.Schier, B.K.Barnes, G.P.Couchell, J.J.Egan, P.Harihar, A.Mittler, E.Sheldon Spin and Parity Assignments for 33S Levels from the 29Si(α, n)32S Reaction NUCLEAR REACTIONS 29Si(α, n), (α, α), E=3.5-5.5 MeV; measured absolute σ(E, En, θ); deduced optical potential. 33S deduced levels, J, π, L. Enriched target.
doi: 10.1016/0375-9474(75)90180-3
1975SC40 Nucl.Phys. A254, 80 (1975) W.A.Schier, B.K.Barnes, G.P.Couchell, J.J.Egan, P.Harihar, S.C.Mathur, A.Mittler, E.Sheldon Spin and Parity Assignments for 35Cl Levels from the 31P(α, p)34S Reaction NUCLEAR REACTIONS 31P(α, p), (α, α), E=3.25-5.50 MeV; measured absolute σ(E, En, θ); deduced optical potential. 35Cl deduced resonances J, π, L.
doi: 10.1016/0375-9474(75)90583-7
1968BA23 Phys.Rev. 170, 995 (1968) D.P.Balamuth, G.P.Couchell, G.E.Mitchell Isobaric-Analog Resonances in Se Isotopes NUCLEAR STRUCTURE 77Br, 79Br, 81Br, 83Br; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.170.995
1967CO02 Bull.Am.Phys.Soc. 12, No.1, 129, HF6(1967) G.P.Couchell, D.P.Balamuth, R.N.Horoshko, G.E.Mitchell Study of Isobaric Analog States by the (p, n) Reaction
1967CO04 Phys.Rev. 161, 1147 (1967) G.P.Couchell, D.P.Balamuth, R.N.Horoshko, G.E.Mitchell Study of Analog States by the (p, n) Reaction NUCLEAR STRUCTURE 75As, 76Se, 71Ga, 81Br, 77As, 66Zn; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.1147
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