NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = G.Morgan Found 65 matches. 2024LA01 Phys.Rev. C 109, 024309 (2024) S.Lalkovski, F.G.Kondev, K.Auranen, A.D.Ayangeakaa, M.P.Carpenter, J.A.Clark, P.Copp, N.P.Giha, D.J.Hartley, T.Lauritsen, S.Marley, G.E.Morgan, C.Muller-Gatermann, S.Nandi, W.Reviol, D.Santiago-Gonzalez, G.Savard, D.Seweryniak, Ir.B.Vasilev, J.Wu Structure of the high-spin, β-decaying state in the neutron-rich nucleus 146La
doi: 10.1103/PhysRevC.109.024309
2024LO03 Nucl.Instrum.Methods Phys.Res. A1062, 169228 (2024) S.Lopez-Caceres, S.T.Marley, M.P.Carpenter, G.Savard, F.G.Kondev, P.Copp, W.Reviol, C.Muller-Gatermann, D.Seweryniak, J.A.Clark, D.Santiago-Gonzalez, G.E.Morgan, A.J.Mitchell, G.L.Wilson, M.L.Smith The LSU-Argonne conversion electron spectrometer: A new detector for the X-Array and SATURN decay station RADIOACTIVITY 150Ce, 150Pr(β-); measured decay products, Eβ, Iβ, X-rays; deduced T1/2 via conversion electrons emission. Comparison with available data. The LSU-Argonne Conversion Electron Spectrometer (LACES), the ATLAS/CARIBU facility at Argonne National Laboratory.
doi: 10.1016/j.nima.2024.169228
2023GA11 Phys.Rev.Lett. 130, 192502 (2023) A.T.Gallant, N.D.Scielzo, G.Savard, J.A.Clark, M.Brodeur, F.Buchinger, D.P.Burdette, M.T.Burkey, S.Caldwell, J.E.Crawford, A.Czeszumska, C.M.Deibel, J.Greene, D.Heslop, T.Y.Hirsh, A.F.Levand, B.Longfellow, G.E.Morgan, P.Mueller, R.Orford, S.Padgett, N.Paul, A.Perez Galvan, A.Reimer, R.Segel, K.S.Sharma, K.Siegl, L.Varriano, B.J.Zabransky Angular Correlations in the β Decay of 8B: First Tensor-Current Limits from a Mirror-Nucleus Pair RADIOACTIVITY 8B(β+); measured decay products, Eβ, Iβ; deduced the α-β-ν angular correlation in the Gamow-Teller β+ decay. The Beta-decay Paul Trap.
doi: 10.1103/PhysRevLett.130.192502
2023HO14 Phys.Rev.Lett. 131, 262701 (2023) D.E.M.Hoff, K.Kolos, G.W.Misch, D.Ray, B.Liu, A.A.Valverde, M.Brodeur, D.P.Burdette, N.Callahan, J.A.Clark, A.T.Gallant, F.G.Kondev, G.E.Morgan, M.R.Mumpower, R.Orford, W.S.Porter, F.Rivero, G.Savard, N.D.Scielzo, K.S.Sharma, K.Sieja, T.M.Sprouse, L.Varriano Direct Mass Measurements to Inform the Behavior of 128mSb in Nucleosynthetic Environments ATOMIC MASSES 128,128mSb; measured cyclotron frequencies; deduced mass excesses, isomer excitation energy. Comparison with AME2020, NUBASE2020, state-of-the-art shell model calculations using the GCN5082 interaction. The phase-imaging ion-cyclotron resonance (PI-ICR) technique with the Canadian Penning Trap (CPT) mass spectrometer at the Californium Rare Isotope Breeder Upgrade facility.
doi: 10.1103/PhysRevLett.131.262701
2022BU16 Phys.Rev.Lett. 128, 202502 (2022) M.T.Burkey, G.Savard, A.T.Gallant, N.D.Scielzo, J.A.Clark, T.Y.Hirsh, L.Varriano, G.H.Sargsyan, K.D.Launey, M.Brodeur, D.P.Burdette, E.Heckmaier, K.Joerres, J.W.Klimes, K.Kolos, A.Laminack, K.G.Leach, A.F.Levand, B.Longfellow, B.Maass, S.T.Marley, G.E.Morgan, P.Mueller, R.Orford, S.W.Padgett, A.Perez Galvan, J.R.Pierce, D.Ray, R.Segel, K.Siegl, K.S.Sharma, B.S.Wang Improved Limit on Tensor Currents in the Weak Interaction from 8Li β Decay RADIOACTIVITY 8Li(β-); measured decay products, Eβ, Iβ; deduced tensor currents in the low-energy regime by examining the β-ν correlation of trapped 8Li ions with the Beta-decay Paul Trap. Comparison with the standard model prediction.
doi: 10.1103/PhysRevLett.128.202502
2022HU21 Phys.Rev. C 106, L061301 (2022) T.Huang, D.Seweryniak, B.B.Back, P.C.Bender, M.P.Carpenter, P.Chowdhury, R.M.Clark, P.A.Copp, X.-T.He, R.D.Herzberg, D.E.M.Hoff, H.Jayatissa, T.L.Khoo, F.G.Kondev, G.Morgan, C.Morse, A.Korichi, T.Lauritsen, C.Muller-Gatermann, D.H.Potterveld, W.Reviol, A.M.Rogers, S.Saha, G.Savard, K.Sharma, S.Stolze, S.Waniganeththi, G.L.Wilson, J.Wu, Y.-F.Xu, S.Zhu Discovery of the new isotope 251Lr: Impact of the hexacontetrapole deformation on single-proton orbital energies near the Z=100 deformed shell gap NUCLEAR REACTIONS 203Tl(50Ti, 2n)251Lr, 205Tl(50Ti, 2n)253Lr, E=237 MeV; measured reaction products, α-decay of the reaction products, Eα, Iα. 251,253Lr; deduced levels J, π, α-decay width. 251,253,255Lr; calculated single-proton levels near the Fermi surface. Calculations with particle-number conserving cranked shell model. Beam delivered to target by ATLAS linear accelerator and recoiling reaction products were separated in the Argonne Gas-Filled Analyzer (AGFA) at (ANL). Decay of the implanted reaction products was measured in pixelized double-sided Si strip detector (DSSD). RADIOACTIVITY 251,253Lr(α)[from 203,205Tl(50Ti, 2n), E=237 MeV]; measured Eα, Iα; deduced T1/2, Q-value, α-decay branchings and widths. Comparison to other experimental data. and predictions of theoretical models.
doi: 10.1103/PhysRevC.106.L061301
2020CZ01 Phys.Rev. C 101, 024312 (2020) A.Czeszumska, N.D.Scielzo, S.A.Caldwell, J.A.Clark, G.Savard, B.S.Wang, A.Aprahamian, M.T.Burkey, C.J.Chiara, J.Harker, A.F.Levand, S.T.Marley, G.Morgan, J.M.Munson, E.B.Norman, A.Nystrom, R.Orford, S.W.Padgett, A.Perez Galvan, K.S.Sharma, K.Siegl, S.Y.Strauss β-delayed neutron emission studies of 137,138I and 144,145Cs performed with trapped ions RADIOACTIVITY 137,138I, 144,145Cs(β-), (β-n)[252Cf(SF) CARIBU facility and mass scans of radioactive beams with the Canadian Penning Trap (CPT) mass spectrometer at Argonne National Laboratory]; measured recoil ions, Eβ, Eγ, (recoil ions)β- and βγ-coin using Beta-decay Paul Trap with two plastic-scintillator ΔE-E telescopes, two MCP detectors, and two HPGe detectors; deduced beta-delayed neutron spectra, beta-delayed neutron-emission probabilities (%β-n or Pn). Comparison with previous experimental results.
doi: 10.1103/PhysRevC.101.024312
2020OR02 Nucl.Instrum.Methods Phys.Res. B463, 491 (2020) R.Orford, J.A.Clark, G.Savard, A.Aprahamian, F.Buchinger, M.T.Burkey, D.A.Gorelov, J.W.Klimes, G.E.Morgan, A.Nystrom, W.S.Porter, D.Ray, K.S.Sharma Improving the measurement sensitivity of the Canadian Penning Trap mass spectrometer through PI-ICR ATOMIC MASSES 142I, 146La, 163Gd; measured frequencies; deduced mass excesses.
doi: 10.1016/j.nimb.2019.04.016
2020WA04 Phys.Rev. C 101, 025806 (2020) B.S.Wang, S.A.Caldwell, N.D.Scielzo, A.Czeszumska, J.A.Clark, G.Savard, A.Aprahamian, M.T.Burkey, C.J.Chiara, J.Harker, A.F.Levand, S.T.Marley, G.E.Morgan, J.M.Munson, E.B.Norman, A.Nystrom, R.Orford, S.W.Padgett, A.Perez Galvan, K.S.Sharma, K.Siegl, S.Y.Strauss β-delayed-neutron studies of 135,136Sb and 140I performed with trapped ions RADIOACTIVITY 135,136Sb, 140I(β-), (β-n) [from 252Cf(SF) CARIBU facility and mass scans of radioactive beams with the Canadian Penning Trap (CPT) mass spectrometer at Argonne National Laboratory]; measured recoil ions, Eβ, Eγ, (recoil ions)β- and βγ-coin using Beta-decay Paul Trap with two plastic-scintillator ΔE-E telescopes, two MCP detectors, and two HPGe detectors; deduced beta-delayed neutron spectra, beta-delayed neutron-emission probabilities (%β-n or Pn). Comparison with earlier experimental results.
doi: 10.1103/PhysRevC.101.025806
2019BU23 Hyperfine Interactions 240, 36 (2019) M.T.Burkey, G.Savard, A.Gallant, N.D.Scielzo, J.A.Clark, T.Y.Hirsh, D.P.Burdette, E.Heckmaier, J.Klimes, K.Kolos, S.T.Marley, G.E.Morgan, R.Orford, S.Padgett, J.Pierce, R.Segel, Ku.S.Sharma, L.Varriano, B.S.Wang Precision β - ν correlation measurements with the Beta-decay Paul Trap RADIOACTIVITY 8Li(β-); measured decay products, Eβ, Iβ; deduced correlations. Comparison with simulations.
doi: 10.1007/s10751-019-1580-0
2018OR02 Phys.Rev.Lett. 120, 262702 (2018) R.Orford, N.Vassh, J.A.Clark, G.C.McLaughlin, M.R.Mumpower, G.Savard, R.Surman, A.Aprahamian, F.Buchinger, M.T.Burkey, D.A.Gorelov, T.Y.Hirsh, J.W.Klimes, G.E.Morgan, A.Nystrom, K.S.Sharma Precision Mass Measurements of Neutron-Rich Neodymium and Samarium Isotopes and Their Role in Understanding Rare-Earth Peak Formation ATOMIC MASSES 154,156,158,159,160Nd, 162,163,164Sm; measured cyclotron frequency ratios; deduced mass excess values. Comparison with AME16 evaluation.
doi: 10.1103/PhysRevLett.120.262702
2018SI07 Phys.Rev. C 97, 035504 (2018) K.Siegl, N.D.Scielzo, A.Czeszumska, J.A.Clark, G.Savard, A.Aprahamian, S.A.Caldwell, B.S.Alan, M.T.Burkey, C.J.Chiara, J.P.Greene, J.Harker, S.T.Marley, G.E.Morgan, J.M.Munson, E.B.Norman, R.Orford, S.Padgett, A.Perez Galvan, K.S.Sharma, S.Y.Strauss Recoil ions from the β decay of 134Sb confined in a Paul trap RADIOACTIVITY 134,134mSb(β-)[from 252Cf SF decay at CARIBU-ANL facility]; measured β, γ, singly-charged recoil ions, βγ-coin, β(ce)-coin, (recoils)β-coin, time-of-flight spectra for β(ion)-coin using Beta-decay Paul Trap (BPT); deduced charge-state distribution of the recoiling ions, mean electron loss, β-ν correlation coefficient (aβν), β-decay simulations, significant β-decay strength (17.2%) to high-lying excited states in 134Te to obtain an angular correlation consistent with expected value of unity for 0- to 0+ β transition. Comparison of the observed β-decay spectrum with that from the decay scheme in the ENSDF database or Nuclear Data Sheets for 134Sb g.s. decay. Comparison of mean atomic electron loss in 134Sb decay with that from the decays of noble gases 6He, 23Ne, 35Ar, 41Ar, 85Kr and 133Xe. 134,134mSb; half-lives used from literature and those determined at CARIBU-ANL facility (reference 23 in this work).
doi: 10.1103/PhysRevC.97.035504
2013VA12 Phys.Rev.Lett. 111, 061102 (2013) J.Van Schelt, D.Lascar, G.Savard, J.A.Clark, P.F.Bertone, S.Caldwell, A.Chaudhuri, A.F.Levand, G.Li, G.E.Morgan, R.Orford, R.E.Segel, K.S.Sharma, M.G.Sternberg First Results from the CARIBU Facility: Mass Measurements on the r-Process Path ATOMIC MASSES 130,131In, 130,131,132,133,134,135Sn, 131,132,133,134,135,136,137Sb, 133,135,136,137,138,139,140Te, 133,134,135,139,140,141I, 142,143,144,145,146Cs; measured TOF ion cyclotron resonances, cyclotron frequency; deduced mass excess. Comparison with theoretical calculations.
doi: 10.1103/PhysRevLett.111.061102
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
1978LU01 Phys.Rev.Lett. 40, 104 (1978) A.H.Lumpkin, G.R.Morgan, J.D.Fox, K.W.Kemper Possible Identification of 10+ Levels in 24Mg at E(X) ≥ 20 MeV NUCLEAR REACTIONS 12C(16O, α), E=50-70 MeV; measured σ(E, Eα, Eγ). 24Mg deduced levels, J, π.
doi: 10.1103/PhysRevLett.40.104
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
1977GL05 Nucl.Phys. A286, 31 (1977) M.Glor, H.P.Nagele, G.Morgan, R.Neff, H.Rudin, F.Seiler The Reactions 6Li(d, p0)7Li, 6Li(d, p1)7Li* and 6Li(d, n1)7Be* between 0.6 and 1.0 MeV NUCLEAR REACTIONS 6Li(polarized d, p), E=0.6, 0.96 MeV; 6Li(polarized d, n), E=0.6, 0.8, 1.0 MeV; measured vector, tensor analyzing powers Ay(θ), A(θ). Enriched target.
doi: 10.1016/0375-9474(77)90005-7
1977LU05 Phys.Rev. C16, 220 (1977) A.H.Lumpkin, G.R.Morgan, K.W.Kemper Structure in the 12C(12C, d)22Na Reaction Near E(c.m.) = 14.3 MeV NUCLEAR REACTIONS 12C(12C, d), E(cm)=13-16.8 MeV; measured σ(Ed); deduced reaction mechanism.
doi: 10.1103/PhysRevC.16.220
1977MO06 Phys.Rev. C16, 167 (1977) (12C, 8Be) Reaction on Even Calcium Isotopes NUCLEAR REACTIONS 40Ca(12C, 8Be), E=35-46 MeV; measured σ(E). 40,42,44,48Ca(12C, 8Be), E=45 MeV; measured σ(θ). 44,48,46,52Ti deduced S.
doi: 10.1103/PhysRevC.16.167
1976FL05 Phys.Rev. C13, 1173 (1976) N.R.Fletcher, J.D.Fox, G.J.Kekelis, G.R.Morgan, G.A.Norton Resonant Structures in the 12C(12C, 8Be)16O Reaction, E(c.m.) = 9 to 20 MeV NUCLEAR REACTIONS 12C(12C, 8Be), E(cm)=9-20 MeV; measured σ(E, θ); deduced anomalies. 16O resonances deduced L.
doi: 10.1103/PhysRevC.13.1173
1976JA19 Nucl.Phys. A274, 177 (1976) D.R.James, G.R.Morgan, N.R.Fletcher, M.B.Greenfield A New Jπ = 12+ Resonance in the 12C + 16O System NUCLEAR REACTIONS 12C(16O, 8Be), E(cm)=18.5-20.5 MeV; measured σ(E, θ). 28Si deduced new resonances with J, π=12+, E(cm)=19.92 MeV.
doi: 10.1016/0375-9474(76)90235-9
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
1975MO33 Phys.Lett. 60B, 35 (1975) G.R.Morgan, N.R.Fletcher, G.A.Norton Alpha-Particle Transfer in the Reaction 40Ca(12C, 8Be)44Ti NUCLEAR REACTIONS 40Ca(12C, 8Be), E=45 MeV; measured σ(E(8Be), θ); deduced α-spectroscopic factors.
doi: 10.1016/0370-2693(75)90520-1
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
1971GR32 Helv.Phys.Acta 44, 662 (1971) H.Grunder, R.Gleyvod, G.Lietz, G.Morgan, H.Rudin, F.Seiler, A.Stricker Die T(d, n)4He-Reaktion mit polarisierten Deuteronen bei Energien oberhalb der 107-keV-Resonanz NUCLEAR REACTIONS 3H(polarized d, n), E=0.2, 0.6, 0.8, 1 MeV; measured analyzing power.
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
1964SA05 Bull.Am.Phys.Soc. 9, No.4, 445, FC16 (1964) J.R.Sawers, Jr., F.O.Purser, G.Morgan, R.L.Walter Scattering of 2.4- and 2.7-MeV Polarized Neutrons from Carbon NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
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