NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = J.J.Egan Found 28 matches. 2000KO61 Nucl.Phys. A679, 147 (2000) Y.J.Ko, J.J.Egan, G.H.R.Kegel, D.J.DeSimone, P.-N.Seo, P.G.Young Thulium-169 Neutron Inelastic Scattering Cross Section Measurements via the 169Tm(n, n'γ) Reaction NUCLEAR REACTIONS 169Tm(n, n'γ), E < 1.1 MeV; measured Eγ, Iγ(θ), σ(E), level excitation functions. 169Tm deduced levels, transition intensities, γ-branching.
doi: 10.1016/S0375-9474(00)00340-7
1997DE54 Nucl.Instrum.Methods Phys.Res. A388, 443 (1997) D.J.DeSimone, G.H.R.Kegel, J.J.Egan, P.Bertone, P.Staples Studies of a Poenitz-Type Black Neutron Detector as a Neutron Flux Monitor NUCLEAR REACTIONS 7Li(p, n), E=2.7-4 MeV; measured zero-degree σ(Ep, θ); deduced detector characteristics.
doi: 10.1016/S0168-9002(97)00008-9
1997ST21 Nucl.Sci.Eng. 126, 168 (1997) P.Staples, J.J.Egan, G.H.R.Kegel, A.Mittler The 14N(n, n'γ) Cross Section of the 2.313-MeV First Excited State NUCLEAR REACTIONS 14N(n, n'γ), E=2.65-3.55 MeV; measured γ production σ, σ(θ).
doi: 10.13182/NSE97-A24470
1996YU05 Nucl.Sci.Eng. 122, 366 (1996) G.Yue, M.O'Connor, J.J.Egan, G.H.R.Kegel Neutron Scattering Angular Distributions in 239Pu at 570 and 700 keV NUCLEAR REACTIONS 239Pu(n, n), (n, n'), E=0.5, 0.7 MeV; measured σ(θ), σ(En); deduced angle integrated σ.
doi: 10.13182/NSE96-A24171
1995ST22 Nucl.Phys. A591, 41 (1995) P.Staples, J.J.Egan, G.H.R.Kegel, A.Mittler, M.L.Woodring Prompt Fission Neutron Energy Spectra Induced by Fast Neutrons NUCLEAR REACTIONS 235U, 239Pu(n, F), E=0.5-3.5 MeV; measured prompt fission neutron spectra; deduced mass dependence. Model comparison.
doi: 10.1016/0375-9474(95)00119-L
1994OC03 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.260 (1994) M.O'Connor, G.Yue, J.Chen, C.Narayan, G.H.R.Kegel, J.J.Egan Elastic and inelastic neutron scattering in 197Au at 1.5 MeV NUCLEAR REACTIONS 197Au(n, n), 197Au(n, n'), E=1.5 MeV; measured products, 197Au; deduced σ(θ). Data were imported from EXFOR entry 14002.
1994YU05 Proc.Intern.Conf.Nuclear Data for Science and Technology, Gatlinburg, Tennesse, 9-13 May, 1994, J.K.Dickens, Ed., American Nuclear Society, Vol.1, p.248 (1994) G.Yue, M.O'Connor, J.J.Egan, G.H.R.Kegel Neutron scattering cross sections for 239Pu at 700 keV NUCLEAR REACTIONS 239Pu(n, n'), 239Pu(n, n), E=700 keV; measured products, 239Pu; deduced σ(θ). Data were imported from EXFOR entry 14000. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14000. 1988GO18 Nucl.Sci.Eng. 100, 48 (1988) G.C.Goswami, J.J.Egan, G.H.R.Kegel, A.Mittler, E.Sheldon Neutron Scattering Cross Sections up to 2.4 MeV for the Ground and First Two Excited States of 232Th NUCLEAR REACTIONS 232Th(n, n'), (n, n), E ≤ 2.4 MeV; measured σ(θ) vs E; deduced σ.
doi: 10.13182/NSE88-A29014
1986EG03 Radiat.Eff. 95, 203 (1986) J.J.Egan, E.D.Arthur, G.Kegel, A.Mittler, J.Q.Shao A Comparison of Measured and Calculated Neutron Inelastic Scattering Cross Sections for Vibrational States from 680 to 1060 keV in 238U NUCLEAR REACTIONS 238U(n, n'), E=0.9-2.2 MeV; measured σ(E); deduced model parameters. Tof. Coupled channel, DWBA calculations.
doi: 10.1080/00337578608208696
1986KE09 Radiat.Eff. 93, 237 (1986) G.H.R.Kegel, J.J.Egan, A.Mittler, G.D.Brady, J.Q.Shao Gamma Radiation from Neutron Irradiated U-235 NUCLEAR REACTIONS 235U(n, n'γ), E=100-500 keV; measured Eγ, Iγ, γ production σ(E); deduced fission fragment isomer decay related γ-spectra.
doi: 10.1080/00337578608207461
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
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
1982CH21 Phys.Rev. C26, 841 (1982) D.W.S.Chan, J.J.Egan, A.Mittler, E.Sheldon Analyses of Fast Neutron Inelastic Scattering Cross Sections to Higher (Vibrational) States of 232Th and 238U. I. Standard Formalism NUCLEAR REACTIONS 232Th, 238U(n, n'γ), E=0.8-2.5 MeV; measured γ-yields; deduced σ(inelastic) vs E. 232Th, 238U deduced levels, J, π, K, rotational, vibrational bands, band parameters. Compound nucleus, direct interaction model analysis.
doi: 10.1103/PhysRevC.26.841
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
1979SU11 Nucl.Sci.Eng. 70, 294 (1979) N.B.Sullivan, J.J.Egan, G.H.R.Kegel, P.Harihar Neutron Inelastic Scattering in Silicon-28 to 4.15 MeV NUCLEAR REACTIONS 28Si(n, n'γ), E=1.96-4.15 MeV; measured σ(θγ), integral σ. Statistical model calculation.
doi: 10.13182/NSE79-A20150
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
1972EG01 Phys.Rev. C5, 1562 (1972) J.J.Egan, K.K.Sekharan, G.C.Dutt, J.E.Wiest, F.Gabbard 2.335-MeV Isobaric Analog Resonance in 51V + p and the Excited States Of 51Cr Studied via the (p, n) and (p, nγ) Reactions NUCLEAR REACTIONS 51V(p, n), E=1.5-5 MeV; measured σ(E;Eγ, En, θ(γ), θ(n)); 51V(p, p), E=2.1-2.45 MeV; measured σ(E). 51Cr deduced levels, J, π. 52Cr deduced isobaric analog resonances, J, π, L(p).
doi: 10.1103/PhysRevC.5.1562
1970EG02 Phys.Rev. C1, 1767 (1970) J.J.Egan, G.C.Dutt, M.McPherson, F.Gabbard Isobaric Analog Resonances in the 68Zn(p, n)68Ga Reaction from 4 to 5 MeV NUCLEAR REACTIONS 68Zn(p, n), E=4-4.15, 4.7-5.0 MeV; measured σ(E;En, θ). 68Ga deduced levels. 69Ga deduced isobaric analog resonances, level-width, J, π.
doi: 10.1103/PhysRevC.1.1767
1969DU03 Phys.Rev. 180, 1222 (1969) G.C.Dutt, F.Gabbard, R.Schrils, J.J.Egan Measurements and Analyses of the s1/2 Analog Resonance in the 88Sr(p, n)88Y Reaction NUCLEAR REACTIONS 88Sr(p, n), E=4.8-6.2 MeV; measured σ(E). 89Y deduced isobaric analog resonance.
doi: 10.1103/PhysRev.180.1222
1968DU10 Phys.Rev. 176, 1289(1968) G.C.Dutt, F.Gabbard, J.J.Egan, J.E.Wiest 2- Isobaric Analog Resonance in the 89Y(p, n2)89Zr Reaction and the Excited States of 89Zr NUCLEAR REACTIONS 89Y(p, n), E=4.807 MeV; measured σ(Ep), σ(En, θ). 89Zr deduced levels, J, π.
doi: 10.1103/PhysRev.176.1289
1966YO02 Bull.Am.Phys.Soc. 11, No.4, 510, A13 (1966) T.Young, F.Gabbard, J.D.Brandenberger, J.D.Reber, J.J.Egan Ar40(p, n)K40 Reaction, 2.3 - 5.0 MeV NUCLEAR STRUCTURE 40K; measured not abstracted; deduced nuclear properties.
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