NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = C.A.Goulding Found 45 matches. 2001AU02 Phys.Rev. C63, 034322 (2001) S.M.Austin, E.Adamides, A.Galonsky, T.Nees, W.A.Sterrenburg, D.E.Bainum, J.Rapaport, E.Sugarbaker, C.C.Foster, C.D.Goodman, D.J.Horen, C.A.Goulding, M.B.Greenfield Splitting of the Dipole and Spin-Dipole Resonances NUCLEAR REACTIONS 90,92,94Zr(p, n), E=79.2, 119.4 MeV; measured σ(E, θ); deduced splitting between GDR and spin-dipole resonance. NUCLEAR STRUCTURE 90,92,94Zr, 112,116,124Sn, 208Pb; calculated resonance energies, dipole-spin-dipole splitting.
doi: 10.1103/PhysRevC.63.034322
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
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
1990RA08 Phys.Rev. C41, 1920 (1990) J.Rapaport, C.C.Foster, C.D.Goodman, C.A.Goulding, T.N.Taddeucci, D.J.Horen, E.R.Sugarbaker, C.Gaarde, J.Larsen, J.A.Carr, F.Petrovich, M.J.Threapleton (p, n) Reaction on Li Isotopes for E(p) = 60-200 MeV NUCLEAR REACTIONS 7,6Li(p, n), (polarized p, n), E=60-200 MeV; measured σ(θ). 6Be deduced Gamow-Teller transition strength. 7Be deduced branching ratio, Gamow-Teller transition strength. DWIA analysis.
doi: 10.1103/PhysRevC.41.1920
1990TA11 Phys.Rev. C41, 2548 (1990) T.N.Taddeucci, W.P.Alford, M.Barlett, R.C.Byrd, T.A.Carey, D.E.Ciskowski, C.C.Foster, C.Gaarde, C.D.Goodman, C.A.Goulding, E.Gulmez, W.Huang, D.J.Horen, J.Larsen, D.Marchlenski, J.B.McClelland, D.Prout, J.Rapaport, L.J.Rybarcyk, W.C.Sailor, E.Sugarbaker, C.A.Whitten, Jr. Zero-Degree Cross Sections for the 7Li(p, n)7Be(g.s.+0.43-MeV) Reaction in the Energy Range 80-795 MeV NUCLEAR REACTIONS 7Li(p, n), E=80-795 MeV; measured σ(θ).
doi: 10.1103/PhysRevC.41.2548
1989AM03 Nucl.Instrum.Methods Phys.Res. A281, 353 (1989) W.B.Amian, M.M.Meier, R.C.Byrd, C.A.Goulding, C.E.Moss Efficiency Calibration of a Cylindrical BC418 Neutron Detector at Neutron Energies between 30 and 200 MeV NUCLEAR REACTIONS 7Li(p, n), E not given; measured neutron spectra; deduced detector efficiency. Tof, BC418 detector.
doi: 10.1016/0168-9002(89)91333-8
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
1987RA15 Phys.Rev. C36, 500 (1987) J.Rapaport, D.Wang, J.A.Carr, F.Petrovich, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, T.N.Taddeucci, D.Horen, E.Sugarbaker (p(pol), n) Reaction on Carbon Isotopes at E(p) = 160 MeV NUCLEAR REACTIONS 12,13,14C(polarized p, n), E=160 MeV; measured σ(θ), σ(θ, En), analyzing power. 15N(polarized p, n), E=160 MeV; analyzed data. 12,13,14N, 15O levels deduced Gamow-Teller transition strength.
doi: 10.1103/PhysRevC.36.500
1987TA13 Nucl.Phys. A469, 125 (1987) T.N.Taddeucci, C.A.Goulding, T.A.Carey, R.C.Byrd, C.D.Goodman, C.Gaarde, J.Larsen, D.Horen, J.Rapaport, E.Sugarbaker The (p, n) Reaction as a Probe of Beta Decay Strength NUCLEAR REACTIONS 12,14C, 42Ca, 28Si, 90Zr, 208Pb, 7Li, 54Fe(p, n), E=50-200 MeV; measured σ(Ep, θ=0°). 12,14N, 42Sc, 28P, 90Nb, 208Bi, 7Be, 54Co deduced reaction population, B(GT) proportionality.
doi: 10.1016/0375-9474(87)90089-3
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
1984BO02 Phys.Rev. C29, 182 (1984) K.G.Boyer, W.J.Braithwaite, W.B.Cottingame, S.J.Greene, L.E.Smith, C.F.Moore, C.L.Morris, H.A.Thiessen, G.S.Blanpied, G.R.Burleson, J.F.Davis, J.S.McCarthy, R.C.Minehart, C.A.Goulding Pion Elastic and Inelastic Scattering from 40,42,44,48Ca and 54Fe NUCLEAR REACTIONS 40,42,44,48Ca, 54Fe(π+, π+'), (π-, π-'), E=116, 118, 292.5 MeV; measured σ(E(π)), σ(θ). 40,42,44,48Ca, 54Fe level deduced neutron density rms radii. DWIA analysis.
doi: 10.1103/PhysRevC.29.182
1984FA11 Phys.Rev. C30, 1622 (1984) J.A.Faucett, B.E.Wood, D.K.McDaniels, P.A.M.Gram, M.E.Hamm, M.A.Oothoudt, C.A.Goulding, L.W.Swenson, K.S.Krane, A.W.Stetz, H.S.Plendl, J.Norton, H.Funsten, D.Joyce Kinematically Complete Measurement of the (π±, π±p) Reaction on 12C at 220 MeV NUCLEAR REACTIONS 12C(π+, π+p), (π-, π-p), (π-, π-'), (π+, π+'), E=220 MeV; measured σ(θ(π), E(π)), σ(θ(π), θ(p), E(p)), σ(θ(π), θ(p), E(π)), σ(θ(π), θ(p)), σ(θ(π), θ(p)) vs missing mass; deduced reaction mechanism. Kinematically complete experiment.
doi: 10.1103/PhysRevC.30.1622
1984GA11 Nucl.Phys. A422, 189 (1984) C.Gaarde, J.S.Larsen, H.Sagawa, N.Ohtsuka, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, C.A.Goulding, D.Horen, T.Masterson, E.Sugarbaker Spin-Dipole Strength in 12N NUCLEAR REACTIONS 12C(p, n), E=120, 160, 200 MeV; measured σ(θ). 12N deduced levels, J, π, analogs.
doi: 10.1016/0375-9474(84)90513-X
1984SE12 Phys.Rev. C30, 270 (1984) S.J.Seestrom-Morris, M.A.Franey, D.Dehnhard, D.B.Holtkamp, R.L.Boudrie, J.F.Amann, G.C.Idzorek, C.A.Goulding 13C(p(pol), p')13C Reaction at T(p) = 547 MeV NUCLEAR REACTIONS 13C(polarized p, p'), E=547 MeV; measured σ(Ep'), σ(θ), analyzing power vs θ. DWIA analysis, shell model transition densities.
doi: 10.1103/PhysRevC.30.270
1983LE12 Phys.Rev. C28, 326 (1983) S.M.Levenson, D.F.Geesaman, E.P.Colton, R.J.Holt, H.E.Jackson, J.P.Schiffer, J.R.Specht, K.E.Stephenson, B.Zeidman, R.E.Segel, P.A.M.Gram, C.A.Goulding Inclusive Pion Scattering in the Δ(1232) Region NUCLEAR REACTIONS 4He, 12C, 58Ni, 208Pb(π+, π+'), E=100, 160, 220, 300 MeV; measured σ(θ, E), σ(E(π')), σ(θ); deduced reaction mechansim, σ(inelastic) vs mass.
doi: 10.1103/PhysRevC.28.326
1983RA30 Nucl.Phys. A410, 371 (1983) J.Rapaport, T.Taddeucci, T.P.Welch, C.Gaarde, J.Larsen, D.J.Horen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Giant Spin-Isospin Multipole Vibrations in 54,56Fe and 58,60Ni NUCLEAR REACTIONS 58Ni(p, n), E=120 MeV; 54,56Fe, 58,60Ni(p, n), E=160 MeV; measured σ(θ, En), θ < 6°, σ(θ). 58Cu, 54,56Co deduced L=0 transition strengths, Gamow-Teller state strengths. Shell model.
doi: 10.1016/0375-9474(83)90632-2
1983TA16 Phys.Rev. C28, 2511 (1983) T.N.Taddeucci, J.Rapaport, C.C.Foster, C.D.Goodman, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Spin Excitations in 40C(p, n) NUCLEAR REACTIONS 40Ca(p, n), E=59.3, 118.3, 159.3 MeV; measured σ(θ), σ(En). 40Sc level deduced Gamow-Teller transition strength. 42Ca(p, n), E=159.3 MeV; measured σ(θ). DWIA analyses.
doi: 10.1103/PhysRevC.28.2511
1982RA30 Phys.Lett. 119B, 61 (1982) J.Rapaport, T.Taddeucci, T.P.Welch, D.J.Horen, J.B.McGrory, C.Gaarde, J.Larsen, E.Sugarbaker, P.Koncz, C.C.Foster, C.D.Goodman, C.A.Goulding, T.Masterson Excitation of Gamow-Teller Resonances in A = 58 Nuclei NUCLEAR REACTIONS 58Ni(p, n), E=120, 160 MeV; measured σ(En, θ=0°). 58Cu deduced levels, isovector Gamow-Teller transition strength.
doi: 10.1016/0370-2693(82)90243-X
1982TA03 Phys.Rev. C25, 1094 (1982) T.N.Taddeucci, J.Rapaport, D.E.Bainum, C.D.Goodman, C.C.Foster, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, E.Sugarbaker Energy Dependence of the Ratio of Isovector Effective Interaction Strengths [J(στ)/J(τ)] from 0° (p, n) Cross Sections NUCLEAR REACTIONS 7Li, 13,14C, 26Mg, 37Cl, 42Ca(p, n), E=60-200 MeV; measured σ(θ=0°); deduced isovector effective interaction strength ratio. 7Be, 13,14N, 26Al, 37Ar, 42Sc levels deduced Gamow-Teller transition strengths.
doi: 10.1103/PhysRevC.25.1094
1982WA02 Phys.Rev. C25, 762 (1982) T.E.Ward, C.C.Foster, G.E.Walker, J.Rapaport, C.A.Goulding 1/E Dependence of the 7Li(p, n)7Be(g.s.+0.43 MeV) Total Reaction Cross Section NUCLEAR REACTIONS, ICPND 7Li(p, n), E=60-200 MeV; measured total reaction σ vs E. Activation technique. DWIA analysis.
doi: 10.1103/PhysRevC.25.762
1981BO26 Phys.Rev. C24, 598 (1981) K.G.Boyer, W.B.Cottingame, L.E.Smith, S.J.Greene, C.F.Moore, J.S.McCarthy, R.C.Minehart, J.F.Davis, G.R.Burleson, G.Blanpied, C.A.Goulding, H.A.Thiessen, C.L.Morris Pion Inelastic Scattering to the Low-Lying States in 42,44,48Ca: Determination of the neutron and proton multipole matrix elements NUCLEAR REACTIONS 42,44,48Ca(π+, π+), (π+, π+'), (π-, π-), (π-, π-'), E=180 MeV; measured σ(θ). 40,42,48Ca levels deduced neutron, proton multipole matrix elements, M(E2), M(E3). DWIA analysis, collective, microscopic model from factors.
doi: 10.1103/PhysRevC.24.598
1981GA26 Nucl.Phys. A369, 258 (1981) C.Gaarde, J.Rapaport, T.N.Taddeucci, C.D.Goodman, C.C.Foster, D.E.Bainum, C.A.Goulding, M.B.Greenfield, D.J.Horen, E.Sugarbaker Excitation of Giant Spin-Isospin Multipole Vibrations NUCLEAR REACTIONS 40Ca, 90Zr, 112,124Sn, 208Pb, 169Tm(p, n), E=200 MeV; measured σ(En, θ). 40Sc, 90Nb, 112,124Sb, 169Yb, 208Bi deduced resonances, L, Gamow-Teller resonance characteristics, giant spin-isospin multipole vibrations. Enriched targets, time-compensated large volume detectors.
doi: 10.1016/0375-9474(81)90019-1
1981GO18 Phys.Lett. 107B, 406 (1981) C.D.Goodman, C.C.Foster, D.E.Bainum, S.D.Bloom, C.Gaarde, J.Larsen, C.A.Goulding, D.J.Horen, T.Masterson, S.Grimes, J.Rapaport, T.N.Taddeucci, E.Sugarbaker Missing Gamow-Teller Strength in Mass 42 NUCLEAR REACTIONS 42Ca(p, n), E=160 MeV; measured σ(θ, En). 42Sc deduced Gamow-Teller transition strength distribution. Shell model.
doi: 10.1016/0370-2693(81)91217-X
1981HO03 Phys.Lett. 99B, 383 (1981) D.J.Horen, C.D.Goodman, D.E.Bainum, C.C.Foster, C.Gaarde, C.A.Goulding, M.B.Greenfield, J.Rapaport, T.N.Taddeucci, E.Sugarbaker, T.Masterson, S.M.Austin, A.Galonsky, W.Sterrenburg Energy Systematics of the Giant Gamow-Teller Resonance and a Charge-Exchange Dipole Spin-Flip Resonance NUCLEAR REACTIONS 90,92,94Zr, 112,116,124Sn, 169Tm, 208Pb(p, n), E=120, 160, 200 MeV; measured σ(En, θ). 90,92,94Nb, 112,116,124Sb, 169Yb, 208Bi deduced giant Gamow-Teller, charge exchange dipole spin-flip resonance energy systematics. Tof.
doi: 10.1016/0370-2693(81)90553-0
1981LE12 Phys.Rev.Lett. 47, 479 (1981) S.M.Levenson, D.F.Geesaman, E.P.Colton, R.J.Holt, H.E.Jackson, J.P.Schiffer, J.R.Specht, K.E.Stephenson, B.Zeidman, R.E.Segal, P.A.M.Gram, C.A.Goulding Inclusive Pion Scattering in the (3, 3) Resonance Region NUCLEAR REACTIONS 4He, 12C, 58Ni, 208Pb(π+, X), E=100, 160, 220 MeV; measured σ(inclusive), σ(reaction).
doi: 10.1103/PhysRevLett.47.479
1981MC07 Phys.Rev. C23, 2349 (1981) R.E.McAdams, V.G.Lind, O.H.Otteson, W.F.Denig, C.A.Goulding, M.Greenfield, H.S.Plendl, B.J.Lieb, C.E.Stronach, P.A.M.Gram, T.Sharma Evidence for the Peripheral Quasifree Nature of Single-Nucleon Removal from 27Al by 190-MeV π± NUCLEAR REACTIONS 27Al(π+, π+'), (π-, π-'), (π+, π+p), (π-, π-p), (π+, π+n), (π-, π-n), (π+, π+np), (π-, π-np), (π+, π+2np), (π-, π-2np), (π+, π+2n2p), (π-, π-2n2p), (π+, π+3n3p), (π-, π-3n3p), E=190 MeV; measured π+γ-, π-γ-coin, σ(θ) for nucleon removal; deduced evidence for one-step quasifree π-nucleon scattering.
doi: 10.1103/PhysRevC.23.2349
1981RA12 Phys.Rev. C24, 335 (1981) J.Rapaport, T.Taddeucci, C.Gaarde, C.D.Goodman, C.C.Foster, C.A.Goulding, D.Horen, E.Sugarbaker, T.G.Masterson, D.Lind 12C(p, n)12N Reaction at 120, 160, and 200 MeV NUCLEAR REACTIONS 12C(p, n), E=120, 160, 200 MeV; measured σ(En, θ); deduced energy independence of effective interaction spin-isospin term. Tof. Microscopic DWIA calculations.
doi: 10.1103/PhysRevC.24.335
1981RA19 Phys.Rev.Lett. 47, 1518 (1981) J.Rapaport, T.Taddeucci, P.Welch, C.Gaarde, J.Larsen, C.Goodman, C.C.Foster, C.A.Goulding, D.Horen, E.Sugarbaker, T.Masterson Empirical Evaluation of Gamow-Teller Strength Function for 37Cl → 37Ar and Its Implication in the Cross Section for Solar Neutrino Absorption by 37Cl NUCLEAR REACTIONS 37Cl(p, n), E=120 MeV; measured σ(En), σ(θ). 37Ar level deduced Gamow-Teller transition strengths, log ft. Tof.
doi: 10.1103/PhysRevLett.47.1518
1980BA16 Phys.Rev.Lett. 44, 1751 (1980) D.E.Bainum, J.Rapaport, C.D.Goodman, D.J.Horen, C.C.Foster, M.B.Greenfield, C.A.Goulding Observation of Giant Particle-Hole Resonances in 90Zr(p, n)90Nb NUCLEAR REACTIONS 90Zr(p, n), E=120 MeV; measured σ(En, θn). 90Nb deduced T=4, 5 components of Gamow-Teller strength, E1 resonance. Tof, macroscopic DWBA analysis.
doi: 10.1103/PhysRevLett.44.1751
1980GO07 Phys.Rev.Lett. 44, 1755 (1980) C.D.Goodman, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, C.C.Foster, W.G.Love, F.Petrovich Gamow-Teller Matrix Elements from 0°(p, n) Cross Sections NUCLEAR REACTIONS 7Li, 12,13C, 25,26Mg, 27Al, 28Si, 90Zr(p, n), E=120 MeV; measured σ(θ=0°). 7Be, 12,13N, 25,26Al, 27Si, 28P, 90Nb deduced Gamow-Teller matrix elements.
doi: 10.1103/PhysRevLett.44.1755
1980HO21 Phys.Lett. B95, 27 (1980) D.J.Horen, C.D.Goodman, C.C.Foster, C.A.Goulding, M.B.Greenfield, J.Rapaport, D.E.Bainum, E.Sugarbaker, T.G.Masterson, F.Petrovich, W.G.Love Search for Isobaric Analogues of M1 States and Giant Spinflip Resonance NUCLEAR REACTIONS 208Pb(p, n), E=120, 160 MeV; measured σ(θ, En). 209Bi deduced resonances, Γ, J, π, analog M1 states, giant spinflip resonance. Tof, enriched target.
doi: 10.1016/0370-2693(80)90391-3
1980RO18 Phys.Rev. C22, 2512 (1980) J.G.Rogers, J.L.Beveridge, D.P.GuRd, H.W.Fearing, A.N.Anderson, J.M.Cameron, L.G.Greeniaus, C.A.Goulding, C.A.Smith, A.W.Stetz, J.R.Richardson, R.Frascaria Proton-Proton Bremsstrahlung at 200 MeV NUCLEAR REACTIONS 1H(p, 2p), E=200 MeV; measured σ(θγ, bremsstrahlung). Soft photon, realstic potential calculations.
doi: 10.1103/PhysRevC.22.2512
1979DA16 Phys.Rev. C20, 1946 (1979) J.Davis, J.Kallne, J.S.McCarthy, R.C.Minehart, C.L.Morris, H.A.Thiessen, G.Blanpied, G.R.Burleson, K.Boyer, W.Cottingame, C.F.Moore, C.A.Goulding Pion Double Charge Exchange Reactions in 12C and 40,44,48Ca NUCLEAR REACTIONS 12C, 40,44,48Ca(π-, π+), (π+, π-), E=290 MeV; measured σ(E(π')).
doi: 10.1103/PhysRevC.20.1946
1979GO16 Nucl.Phys. A331, 29 (1979) C.A.Goulding, M.B.Greenfield, C.C.Foster, T.E.Ward, J.Rapaport, D.E.Bainum, C.D.Goodman Comparison of the 12C(p, n)12N and 12C(p, p') Reactions at E = 62 and 120 MeV NUCLEAR REACTIONS 7Li(p, n), E=120 MeV; measured Eγ, Iγ, σ(θ); deduced production σ for 7Be. 12C(p, p'), E=62 MeV; measured σ(θ). 12C(p, n), E=62, 120 MeV; measured σ(θ).
doi: 10.1016/0375-9474(79)90298-7
1979KR14 Phys.Rev. C20, 1873 (1979) K.S.Krane, T.C.Sharma, L.W.Swenson, D.K.McDaniels, P.Varghese, B.E.Wood, R.R.Silbar, H.D.Wohlfahrt, C.A.Goulding Energetic Charged-Particle Spectrum Following μ- Capture by Nuclei NUCLEAR REACTIONS Al, Cu, Pb(μ-, X), E=0; measured charged-particle spectrum, σ(E).
doi: 10.1103/PhysRevC.20.1873
1978KA01 Phys.Rev.Lett. 40, 378 (1978) J.Kallne, H.A.Thiessen, C.L.Morris, S.L.Verbeck, G.R.Burleson, M.J.Devereaux, J.S.McCarthy, J.E.Bolger, C.F.Moore, C.A.Goulding Reactions 3He(π-, n)2H and 4He(π-, n)3H at Pion Energies of 100, 200, and 290 MeV NUCLEAR REACTIONS 4,3He(π-, n), E=100, 200, 290 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.40.378
1978LI16 Phys.Rev.Lett. 41, 1023 (1978) V.G.Lind, R.E.McAdams, O.H.Otteson, W.F.Denig, C.A.Goulding, M.Greenfield, H.S.Plendl, B.J.Lieb, C.E.Stronach, P.A.M.Gram, T.Sharma Gamma-Ray Spectrum in Coincidence with Scattered Pions from 190-MeV π- Reactions on 27Al NUCLEAR REACTIONS 27Al(π-, X), E=190 MeV; measured γ-spectra; deduced production σ, reaction mechanism.
doi: 10.1103/PhysRevLett.41.1023
1977ST30 Nucl.Phys. A290, 285 (1977) A.W.Stetz, J.M.Cameron, D.A.Hutcheon, R.H.McCamis, C.A.Miller, G.A.Moss, G.Roy, J.G.Rogers, C.A.Goulding, W.T.H.van Oers Elastic Proton Scattering from 4He in the Foward Direction at 200, 350 500 MeV NUCLEAR REACTIONS 4He(p, p), E=200, 350, 500 MeV; measured σ(θ), analyzing power.
doi: 10.1016/0375-9474(77)90437-7
1973GO38 Nucl.Phys. A215, 253 (1973) C.A.Goulding, P.Stoler, J.D.Seagrave 3He and 4He Total Neutron Cross Sections in the MeV Region NUCLEAR REACTIONS 3,4He(n, X), E approx 1-30 MeV; measured σ(E). Gaseous targets; 4He natural, 3He enriched.
doi: 10.1016/0375-9474(73)90654-4
1973HA17 Nucl.Sci.Eng. 50, 243 (1973) S.H.Hayes, P.Stoler, J.M.Clement, C.A.Goulding The Total Neutron Cross Sections of Uranium-238 from 0.8 to 30 MeV NUCLEAR REACTIONS 238U(n, X); E=0.8-30 MeV; measured σ(E).
doi: 10.13182/NSE73-A28977
1972CL04 Nucl.Phys. A183, 51 (1972) J.M.Clement, P.Stoler, C.A.Goulding, R.W.Fairchild Hydrogen and Deuterium Total Neutron Cross Sections in the MeV Region NUCLEAR REACTIONS 1H, 2H(n, X), E approx 1-20 MeV; measured σ(nt)(E). Gaseous targets; 1H natural, 2H enriched.
doi: 10.1016/0375-9474(72)90930-X
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