NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = G.L.Morgan Found 43 matches. 2003DI03 Phys.Rev. C 67, 044606 (2003) F.S.Dietrich, J.D.Anderson, R.W.Bauer, S.M.Grimes, R.W.Finlay, W.P.Abfalterer, F.B.Bateman, R.C.Haight, G.L.Morgan, E.Bauge, J.-P.Delaroche, P.Romain Importance of isovector effects in reproducing neutron total cross section differences in the W isotopes NUCLEAR REACTIONS 182,184,186W(n, X), E=5-560 MeV; measured total σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.67.044606
2003MO26 Nucl.Instrum.Methods Phys.Res. B211, 297 (2003) G.L.Morgan, K.R.Alrick, A.Saunders, F.C.Cverna, N.S.P.King, F.E.Merrill, L.S.Waters, A.L.Hanson, G.A.Greene, R.P.Liljestrand, R.T.Thompson, E.A.Henry Total cross sections for the production of 22Na and 24Na in proton-induced reactions on 27Al from 0.40 to 22.4 GeV NUCLEAR REACTIONS 27Al(p, X)22Na/24Na, E=0.4-22.4 GeV; measured production σ. Activation technique, comparison with previous results.
doi: 10.1016/S0168-583X(03)01364-8
2001AB14 Phys.Rev. C63, 044608 (2001) W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, R.W.Finlay, R.C.Haight, G.L.Morgan Measurement of Neutron Total Cross Sections up to 560 MeV NUCLEAR REACTIONS H, Li, 6,7Li, B, 10,11B, C, 13C, F, Mg, S, P, K, Ca, Ti, V, Cr, Mn, Fe, Ni, Co, Y, Mo, In, W, 197Au, Hg, Pb, Th, 238U(n, X), E < 600 MeV; measured transmission neutron spectra; deduced total σ. Comparisons with model predictions, previous results.
doi: 10.1103/PhysRevC.63.044608
2000SN02 Nucl.Instrum.Methods Phys.Res. A440, 729 (2000) W.M.Snow, A.Bazhenov, C.S.Blessinger, J.D.Bowman, T.E.Chupp, K.P.Coulter, S.J.Freedman, B.K.Fujikawa, T.R.Gentile, G.L.Greene, G.Hansen, G.E.Hogan, S.Ishimoto, G.L.Jones, J.N.Knudson, E.Kolomenski, S.K.Lamoreaux, M.B.Leuschner, A.Masaike, Y.Masuda, Y.Matsuda, G.L.Morgan, K.Morimoto, C.L.Morris, H.Nann, S.I.Penttila, A.Pirozhkov, V.R.Pomeroy, D.R.Rich, A.Serebrov, E.I.Sharapov, D.A.Smith, T.B.Smith, R.C.Welsh, F.E.Wietfeldt, W.S.Wilburn, V.W.Yuan, J.Zerger Measurement of the Parity Violating Asymmetry Aγ in n(pol) + p → d + γ NUCLEAR REACTIONS 1H(polarized n, γ), E=low; calculated parity violation measurement systematic effects. Experiment proposal.
doi: 10.1016/S0168-9002(99)01071-2
1998AB21 Phys.Rev.Lett. 81, 57 (1998) W.P.Abfalterer, F.B.Bateman, F.S.Dietrich, Ch.Elster, R.W.Finlay, W.Glockle, J.Golak, R.C.Haight, D.Huber, G.L.Morgan, H.W.Witala Inadequacies of the Nonrelativistic 3N Hamiltonian in Describing the n + d Total Cross Section NUCLEAR REACTIONS 1,2H(n, X), E=7-600 MeV; measured σ; deduced possible relativistic effects. Fadeev calculations.
doi: 10.1103/PhysRevLett.81.57
1996FE05 Yad.Fiz. 59, No 9, 1551 (1996); Phys.Atomic Nuclei 59, 1492 (1996) X.Feng, M.H.Holzscheiter, M.Charlton, F.Cverna, T.Ichioka, N.S.P.King, R.A.Lewis, G.L.Morgan, J.Rochet, Y.Yamazaki Ultralow-Energy Antiprotons for Antihydrogen Spectroscopy and Antimatter Gravity
1994CA50 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.40 (1994) A.D.Carlson, W.E.Parker, P.W.Lisowski, G.L.Morgan, S.J.Seestrom, N.W.Hill, K.Meggers Measurements of the fission cross section of 237Np NUCLEAR REACTIONS 237Np(n, f), E=5.171 eV-5.1 keV; measured product s; deduced σ, σ(E). Data were imported from EXFOR entry 14035. Data from this article have been entered in the EXFOR database. For more information, access X4 dataset14035. 1994PA02 Phys.Rev. C49, 672 (1994) W.E.Parker, J.E.Lynn, G.L.Morgan, P.W.Lisowski, A.D.Carlson, N.W.Hill Intermediate Structure in the Neutron-Induced Fission Cross Section of 236U NUCLEAR REACTIONS 236U(n, F), E=5 eV-100 keV; measured fission σ, resonance fission widths; deduced intermediate resonance structure. 237U deduced fission barrier parameters.
doi: 10.1103/PhysRevC.49.672
1993AM06 Nucl.Sci.Eng. 115, 1 (1993) W.B.Amian, R.C.Byrd, D.A.Clark, C.A.Goulding, M.M.Meier, G.L.Morgan, C.E.Moss Differential Neutron Production Cross Sections for 597-MeV Protons NUCLEAR REACTIONS C, 27Al, Fe, Pb, Ni, B, O, 238U(p, xn), E=597 MeV; measured σ(θn, En). Intranuclear cascade evaporation model.
doi: 10.13182/NSE93-A35517
1993FI01 Phys.Rev. C47, 237 (1993) R.W.Finlay, W.P.Abfalterer, G.Fink, E.Montei, T.Adami, P.W.Lisowski, G.L.Morgan, R.C.Haight Neutron Total Cross Sections at Intermediate Energies NUCLEAR REACTIONS 9Be, C, N, O, 27Al, Si, 40Ca, Cu, 90Zr, 93Nb, Sn, Ta, 208Pb, 209Bi(n, X), E ≤ 600 MeV; measured transmission vs neutron energy; deduced total σ(E), neutron mean free path. Enriched 40Ca, 90Zr, 208Pb targets.
doi: 10.1103/PhysRevC.47.237
1992AM03 Nucl.Instrum.Methods Phys.Res. A313, 452 (1992) W.B.Amian, M.M.Meier, R.C.Byrd, C.A.Goulding, G.L.Morgan, C.E.Moss Efficiency Calibration of a Cylindrical BC418 Neutron Detector at Neutron Energies between 135 and 800 MeV NUCLEAR REACTIONS Pb, 7Li(p, n), E ≤ 800 MeV; measured neutron detection efficiency for E=135-800 MeV; Fe(n, n), E=110-725 MeV; measured total σ. Cylindrical BC418 neutron detector, efficiency calibration.
doi: 10.1016/0168-9002(92)90823-M
1992AM07 Nucl.Sci.Eng. 112, 78 (1992) W.B.Amian, R.C.Byrd, C.A.Goulding, M.M.Meier, G.L.Morgan, C.E.Moss, D.A.Clark Differential Neutron Production Cross Sections for 800-MeV Protons NUCLEAR REACTIONS U, B, C, N, O, 27Al, Fe, Cd, W, Pb, 9Be(p, xn), E=800 MeV; measured σ(θ, En). Model comparison, tof.
doi: 10.13182/NSE92-A23953
1992ME04 Nucl.Sci.Eng. 110, 289 (1992) M.M.Meier, W.B.Amian, C.A.Goulding, G.L.Morgan, C.E.Moss Differential Neutron Production Cross Sections for 256-MeV Protons NUCLEAR REACTIONS 9Be, C, O, 27Al, Fe, Pb, 238U(p, xn), E=256 MeV; measured σ(θ, En). Tof technique, intranuclear cascade evaporation. Model comparison.
doi: 10.13182/NSE92-A23901
1992ME05 Nucl.Sci.Eng. 110, 299 (1992) M.M.Meier, W.B.Amian, C.A.Goulding, G.L.Morgan, C.E.Moss Neutron Yields from Stopping-Length Targets for 256-MeV Protons NUCLEAR REACTIONS 9Be, C, 27Al, Fe(p, xn), E=256 MeV; measured absolute neutron yields; deduced neutron production mechanism. Tof techniques, intranuclear cascade evaporation-model calculations.
doi: 10.13182/NSE92-A23902
1990ME04 Nucl.Sci.Eng. 104, 339 (1990) M.M.Meier, C.A.Goulding, G.L.Morgan, J.L.Ullmann Neutron Yields from Stopping- and Near-Stopping-Length Targets for 256-MeV Protons NUCLEAR REACTIONS, MECPD C, 27Al, Fe, U(p, xn), E=256 MeV; measured absolute neutron yields. Model calculations.
doi: 10.13182/NSE90-A23733
1989ME08 Nucl.Sci.Eng. 102, 310 (1989) M.M.Meier, D.A.Clark, C.A.Goulding, J.B.McClelland, G.L.Morgan, C.E.Moss, W.B.Amian Differential Neutron Production Cross Sections and Neutron Yields from Stopping-Length Targets for 113-MeV Protons NUCLEAR REACTIONS Be, C, 27Al, Fe, U, O, Pb, W(p, xn), E=113 MeV; measured σ(θn, En). Thin elemental targets.
doi: 10.13182/NSE89-A27480
1989RA09 Phys.Rev. C39, 1929 (1989) J.Rapaport, P.W.Lisowski, J.L.Ullmann, R.C.Byrd, T.A.Carey, J.B.McClelland, L.J.Rybarcyk, T.N.Taddeucci, R.C.Haight, N.S.P.King, G.L.Morgan, D.A.Clark, D.E.Ciskowski, D.A.Lind, R.Smythe, C.D.Zafiratos, D.Prout, E.R.Sugarbaker, D.Marchlenski, W.P.Alford, W.G.Love Fermi and Gamow-Teller Strength in p-Shell Nuclei from (p, n) Reactions at 492 and 590 MeV NUCLEAR REACTIONS 7Li, 11B, 12,13,14C(p, n), E=492 MeV; 13C, 11B(p, n), E=590 MeV; measured σ(θ, E); deduced unit σ(ratio).
doi: 10.1103/PhysRevC.39.1929
1988DE17 Nucl.Instrum.Methods Phys.Res. A268, 155 (1988) Magnetic Moments of Low-Energy Neutron Resonances in 161Dy NUCLEAR REACTIONS 161Dy(n, X), E=low; measured transmission spectra. 162Dy deduced resonances, μ. Polarized target, tof.
doi: 10.1016/0168-9002(88)90601-8
1988HI12 Phys.Rev.Lett. 61, 1174 (1988) K.H.Hicks, R.Abegg, A.Celler, O.Hausser, R.S.Henderson, N.W.Hill, K.P.Jackson, R.G.Jeppesen, N.S.P.King, M.A.Kovash, R.Liljestrand, C.A.Miller, G.L.Morgan, J.R.Shepard, A.Trudel, M.Vetterli, S.Yen Spin-Dependent Observables for the 12C(p, p'γ) Reaction at 400 MeV NUCLEAR REACTIONS 12C(polarized p, p'γ), E=400 MeV; measured σ(θp', θγ), spin dependent observables. 12C level deduced spin-flip probability. Relativistic, nonrelativistic treatments, impulse approximation.
doi: 10.1103/PhysRevLett.61.1174
1988SC04 Phys.Lett. 203B, 22 (1988) R.L.Schutt, R.E.Shamu, P.W.Lisowski, M.S.Moore, G.L.Morgan Nucleon Scattering from 208Pb at Low and Intermediate Energies NUCLEAR REACTIONS 208Pb(n, n), E=2-250 MeV; analyzed σ(E). 208Pb(n, n), E=13.5-40 MeV; analyzed σ(θ); deduced model parameters. Phenomenological optical model.
doi: 10.1016/0370-2693(88)91562-6
1986KI12 Phys.Lett. 175B, 279 (1986) N.S.P.King, P.W.Lisowski, G.L.Morgan, P.N.Craig, R.G.Jeppesen, D.A.Lind, J.R.Shepard, J.L.Ullmann, C.D.Zafiratos, C.D.Goodman, C.A.Goulding Observation of Fermi and Gamow-Teller Strength in the 800 MeV (p, n) Reaction NUCLEAR REACTIONS 6Li, 12,13C, 15N(p, n), E=800 MeV; measured σ(θ), σ(θ) vs neutron momentum. 12,13N, 15O, 6Be deduced Gamow-Teller, Fermi transition strengths.
doi: 10.1016/0370-2693(86)90856-7
1986ME18 Radiat.Eff. 96, 73 (1986) M.M.Meier, D.B.Holtkamp, G.L.Morgan, H.Robinson, G.J.Russell, E.R.Whitaker, W.Amian, N.Paul 318 and 800 MeV (p, xn) Cross Sections NUCLEAR REACTIONS C, 27Al, Pb, U(p, xn), E=800 MeV; Pb, U(p, xn), E=318 MeV; measured σ(E). Fast plastic scintillators, tof.
doi: 10.1080/00337578608211717
1986MO05 Phys.Rev. C33, 1224 (1986) G.L.Morgan, P.W.Lisowski, S.A.Wender, R.E.Brown, N.Jarmie, J.F.Wilkerson, D.M.Drake Measurement of the Branching Ratio 3H(d, γ)/3H(d, n) using Thick Tritium Gas Targets NUCLEAR REACTIONS, ICPND 3H(d, γ), (d, n), E=0.0-0.72 MeV; measured Eγ, Iγ, En, relative γ yield. 5He resonance deduced branching ratio.
doi: 10.1103/PhysRevC.33.1224
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
1981WI02 Nucl.Sci.Eng. 78, 147 (1981) R.R.Winters, N.W.Hill, R.L.Macklin, J.A.Harvey, D.K.Olsen, G.L.Morgan Uranium-238 Inelastic Neutron Scattering at 82 keV NUCLEAR REACTIONS 238U(n, n'), E=82 keV; measured σ(θ), integrated σ. Legendre polynomial analysis, statistical, optical model calculations.
doi: 10.13182/NSE81-A20100
1980LA13 Nucl.Sci.Eng. 75, 151 (1980) Measurement and Analysis of the 23Na(n, xγ) Reaction Cross Section for 0.2 ≤En ≤20 MeV NUCLEAR REACTIONS 23Na(n, γ), E=0.2-20 MeV; measured σ(θγ, E). NaI detector, multistep Hauser-Feshbach calculations.
doi: 10.13182/NSE80-A21304
1980OL06 Nucl.Sci.Eng. 74, 219 (1980) D.K.Olsen, G.L.Morgan, J.W.McConnell Measurement of the 7Li(n, n'γ)7Li' (0.478 MeV) Cross Section from 0.5 to 5.0 MeV NUCLEAR REACTIONS 7Li(n, n'γ), E=0.5-5 MeV; measured Eγ, Iγ, totalσ(Eγ). Ge(Li) detector.
doi: 10.13182/NSE80-A20124
1979MO09 Nucl.Sci.Eng. 70, 163 (1979) Cross Sections for the 14N(n, p0), (n, α0), and (n, α1) Reactions from 0.5 to 15 MeV NUCLEAR REACTIONS 14N(n, p), E=0.5-7.0 MeV; 14N(n, α), E=1-15 MeV; measured σ. Compared, current evaluated σ for 14N. Gaseous scintillator, nitrogen-xenon mixture.
doi: 10.13182/NSE79-A19649
1979MO24 Nucl.Sci.Eng. 72, 359 (1979) The Th(n, xγ) Reaction Cross Section for Neutrons of Energy between 0.3 and 20 MeV NUCLEAR REACTIONS Th(n, γ), E=0.3-20 MeV; measured σ(θγ, Eγ), total yield.
doi: 10.13182/NSE79-A20392
1977DI11 Nucl.Sci.Eng. 62, 515 (1977) J.K.Dickens, G.L.Morgan, G.T.Chapman, T.A.Love, E.Newman, F.G.Perey Cross Sections for Gamma-Ray Production by Fast Neutrons for 22 Elements between Z = 3 and Z = 82 NUCLEAR REACTIONS Li, C, N, F, Mg, Al, Si, Ca, V, Cr, Fe, Ni, Cu, Zn, Nb, Mo, Ag, Sn, Ta, W, Au, Pb(n, X), E=0.1-20.0 MeV; measured γ production σ.
doi: 10.13182/NSE77-A26989
1976MO13 Nucl.Sci.Eng. 60, 36 (1976) Production of Low-Energy Gamma Rays by Neutron Interactions with Fluorine for Incident Neutron Energies between 0.1 and 20 MeV NUCLEAR REACTIONS 19F(n, X), E=0.1-10.2 MeV; measured σ(E, Eγ). 19F, 19O, 16N deduced transitions.
doi: 10.13182/NSE76-A26855
1976MO29 Nucl.Sci.Eng. 61, 337 (1976) Cross Sections for the Al(n, xn) and Al(n, xγ) Reactions between 1 and 20 MeV NUCLEAR REACTIONS 27Al(n, xn), (n, γ), E=1-20 MeV; measured σ(E).
doi: 10.13182/NSE76-A26919
1974DI07 Nucl.Sci.Eng. 53, 277 (1974) J.K.Dickens, T.A.Love, G.L.Morgan Neutron-Induced Gamma-Ray Production in Calcium in the Energy Range 0.7 < E < 20 MeV NUCLEAR REACTIONS Ca(n, Xγ), E=0.7-20 MeV; measured σ(E, Eγ).
doi: 10.13182/NSE74-A23353
1974DI11 Phys.Rev. C10, 958 (1974) 28Si(n, n'γ) Photon Production Cross Sections for E = 1.78 MeV, 5.0 ≤ E ≤ 9.5 MeV NUCLEAR REACTIONS 28Si(n, n'γ), E=5-9.5 MeV; measured σ(E, Eγ).
doi: 10.1103/PhysRevC.10.958
1973DI07 Nucl.Sci.Eng. 50, 311 (1973) J.K.Dickens, G.L.Morgan, F.G.Perey Neutron-Induced Gamma-Ray Production in Iron for the Energy Range 0.8 < E < 20 MeV NUCLEAR REACTIONS 54,56Fe(n, Xγ), E=0.8-20 MeV; measured σ(E, Eγ, θ).
doi: 10.13182/NSE73-A26567
1971EV01 Can.J.Phys. 49, 402 (1971) F.Everling, G.L.Morgan, D.W.Miller, L.W.Seagondollar, P.W.Tillman, Jr. Energies of Some 25Al Levels from the 24Mg(p, γ)25Al Reaction and the Coulomb-Energy Differences of Analog Ratational Bands NUCLEAR REACTIONS 24Mg(p, γ), E=1201, 1485 keV; measured Q, Eγ. 25Al deduced levels, resonances.
doi: 10.1139/p71-050
1971HA27 Nucl.Phys. A167, 49 (1971) R.A.Hardekopf, C.E.Hollandsworth, R.L.Walter, J.M.Joyce, G.L.Morgan Remeasurement of the Neutron Polarization from the 7Li(p, n)7Be Reaction for 3 to 4 MeV Protons NUCLEAR REACTIONS 7Li(p, n0), 7Li(p, n1), E=3-4 MeV; measured neutron polarization(E;θ=50°).
doi: 10.1016/0375-9474(71)90579-3
1970MO13 Nucl.Phys. A148, 480 (1970) G.L.Morgan, D.R.Tilley, G.E.Mitchell, R.A.Hilko, N.R.Roberson Study of 18O Through 14C + α Reactions NUCLEAR REACTIONS 14C(α, α), E=3.5-16.5 MeV; measured σ(E, θ). 14C(α, n), E=4.9-8.5 MeV; measured σ(E). 18O deduced resonances J, π, level-width. Enriched target.
doi: 10.1016/0375-9474(70)90641-X
1970MO17 Phys.Lett. 32B, 353 (1970) G.L.Morgan, D.R.Tilley, G.E.Mitchell, R.A.Hilko, N.R.Roberson States in 18O Excited by the 14C(7Li, t) Reaction NUCLEAR REACTIONS 14C(7Li, t), E=20.4 MeV; measured σ(Et, θ). 18O deduced levels, rotational bands.
doi: 10.1016/0370-2693(70)90494-6
1970MO31 Phys.Rev. C2, 2034 (1970); Addendum to 68Ch35 Neutron-Helium Interaction. II. Angular Distributions and Phase Shifts from 0.2 to 7.0 MeV NUCLEAR REACTIONS 4He(n, n), E=0.2-7.0 MeV; measured σ(E;θ).
doi: 10.1103/PhysRevC.2.2034
1968MO26 Phys.Rev. 168, 1114 (1968) Neutron-Helium Interaction. II. Angular Distributions and Phase Shifts from 0.2 to 7.0 MeV NUCLEAR REACTIONS He(n, n), E=0.2-7.0 MeV; measured σ(E;Eα, θ(α)); deduced phase shifts. 5He deduced resonance parameters.
doi: 10.1103/PhysRev.168.1114
1968SA25 Phys.Rev. 168, 1102 (1968) J.R.Sawers, Jr., G.L.Morgan, L.A.Schaller, R.L.Walter Neutron-Helium Interaction. I. Scattering of Polarized Neutrons at 1.01 and 2.44 MeV NUCLEAR REACTIONS He(polarized n, n), E=1.015, 2.44 MeV; measured σ(Eα), P(θ); deduced phase shifts.
doi: 10.1103/PhysRev.168.1102
1966MO14 Phys.Rev. 150, 830 (1966) G.L.Morgan, R.L.Walter, C.S.Soltesz, T.R.Donoghue Polarization of Neutrons from C12 + d for Deuteron Energies from 3.9 to 5 MeV NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.150.830
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