NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = H.D.Holmgren Found 76 matches. 1988SI01 Phys.Rev. C37, 158 (1988) J.D.Silk, H.D.Holmgren, D.L.Hendrie, T.J.M.Symons, G.D.Westfall, P.H.Stelson, S.Raman, R.L.Auble, J.R.Wu, K.Van Bibber Fragmentation of 16O Projectiles at 100 MeV per Nucleon NUCLEAR REACTIONS 27Al(16O, 12CX), E=100 MeV/nucleon; measured invariant σ vs rapidity. 27Al(16O, X), E=100 MeV/nucleon; measured σ(fragment θ), σ vs fragment mass for X=7,9,10Be, 10,11,12B, 10,11,12,13,14C, 13,14,15N; deduced reaction mechanism.
doi: 10.1103/PhysRevC.37.158
1984CI03 Phys.Rev. C29, 1289 (1984) G.Ciangaru, C.C.Chang, H.D.Holmgren, A.Nadasen, P.G.Roos Three-Body Approach to the Multiple Scattering Direct Reactions: Pragmatic application to the 58Ni(p, 2p)57Co continuum NUCLEAR REACTIONS 58Ni(p, 2p), E=198 MeV; calculated σ(θ1, θ2, E1), σ(θ1, θ2, E1, E2). Multi-step direct process, three-body approach.
doi: 10.1103/PhysRevC.29.1289
1984CI04 Phys.Rev. C29, 2017 (1984) G.Ciangaru, C.C.Chang, J.R.Wu, R.W.Koontz, H.D.Holmgren Nuclear States of 28Si and 28Al from (α, t) and (α, h) Reactions at 80 MeV NUCLEAR REACTIONS 27Al(α, t), (α, 3He), E=80 MeV; measured σ(θ), σ(Et), σ(E(3He)); deduced optical model parameters. 28Si, 28Al levels deduced L, spectroscopic factors. Finite-range DWBA, shell model wave functions.
doi: 10.1103/PhysRevC.29.2017
1983AU06 Phys.Rev. C28, 1552 (1983) R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, C.Y.Wong, D.L.Hendrie, H.D.Holmgren, J.D.Silk Light Ion Emission from Reactions Induced by 0.8-2.4 GeV 16O Projectiles NUCLEAR REACTIONS Ni(16O, X), E=0.8, 1.6, 2.4 GeV; Au(16O, X), E=1.6, 2.4 GeV; Al, Sn(16O, X), E=1.6 GeV; measured σ(E, θ) for X=p, d, t, 3He, 4He; deduced model parameters.
doi: 10.1103/PhysRevC.28.1552
1983CI02 Phys.Rev. C27, 1360 (1983) G.Ciangaru, C.C.Chang, H.D.Holmgren, A.Nadasen, P.G.Roos, A.A.Cowley, S.Mills, P.P.Singh, M.K.Saber, J.R.Hall Continuum Spectrum in the Quasifree (p, 2p) Scattering NUCLEAR REACTIONS 58Ni(p, 2p), E=198 MeV; measured σ(θ1, E2, θ2, E2); deduced reaction mechanism. DWIA calculations, quasifree particle rescattering effect.
doi: 10.1103/PhysRevC.27.1360
1983KA13 Phys.Rev. C28, 105 (1983) A.M.Kalenda, B.D.Anderson, A.R.Baldwin, R.Madey, J.W.Watson, C.C.Chang, H.D.Holmgren, R.W.Koontz, J.R.Wu, H.Machner Energy and Angular Distributions of Neutrons from 90 MeV Proton and 140 MeV Alpha-Particle Bombardment of Nuclei NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, n), E=90 MeV; 27Al, 58Ni, 90Zr, 209Bi(α, n), E=140 MeV; measured σ(θ, En); deduced reaction mechanisms. Plane wave impulse approximation, quasifree scattering, preequilibrium exciton, intranuclear cascade, geometry dependent hybrid models, (p, p') data comparison.
doi: 10.1103/PhysRevC.28.105
1982AU07 Phys.Rev.Lett. 49, 441 (1982) R.L.Auble, J.B.Ball, F.E.Bertrand, C.B.Fulmer, D.C.Hensley, I.Y.Lee, R.L.Robinson, P.H.Stelson, D.L.Hendrie, H.D.Holmgren, J.D.Silk, H.Breuer Target-A Dependence of Light-Ion Emission from Reactions Induced by 100-MeV/u 16O NUCLEAR REACTIONS Al, Ni, Sn, Au(16O, p), (16O, d), (16O, t), (16O, 3He), (16O, α), E=100 MeV/nucleon; measured σ(θ, Ep), σ(θ, Ed), σ(θ, Et), σ(θ, E(3He)), σ(θ, Eα), inclusive reactions; deduced reaction mechanism, moving source parameters, target mass effects.
doi: 10.1103/PhysRevLett.49.441
1981AN01 Phys.Rev.Lett. 46, 226 (1981) B.D.Anderson, A.R.Baldwin, A.M.Kalenda, R.Madey, J.W.Watson, C.C.Chang, H.D.Holmgren, R.W.Koontz, J.R.Wu Proton and Neutron Inclusive Spectra and the Importance of the Single Nucleon-Nucleon Scattering Process NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, pX), (p, nX), E=90 MeV; measured σ(En, θ), σ(Ep, θ); deduced nucleon-nucleon scattering mechanism dominance. PWIA, quasifree scattering calculation.
doi: 10.1103/PhysRevLett.46.226
1980CO17 Phys.Rev. C22, 2633 (1980) A.A.Cowley, C.C.Chang, H.D.Holmgren Forward-Angle Proton Spectra in the Continuum from the 58Ni(p, xp) Reaction at 100 MeV NUCLEAR REACTIONS 58Ni(p, xp), E=100 MeV; measured σ(θ, Ep); deduced quasi-free nucleon-nucleon scattering effects.
doi: 10.1103/PhysRevC.22.2633
1980CO19 Phys.Rev.Lett. 45, 1930 (1980) A.A.Cowley, C.C.Chang, H.D.Holmgren, J.D.Silk, D.L.Hendrie, R.W.Koontz, P.G.Roos, C.Samanta, J.R.Wu Energy Dissipation Process for 100-MeV Protons and the Nucleon-Nucleon Interactions in Nuclei NUCLEAR REACTIONS 58Ni(p, 2p), E=100 MeV; measured pp-coin, σ(Ep1, Ep2, θ1, θ2); deduced reaction mechanism, energy dissipation process. DWIA analysis, quasifree scattering.
doi: 10.1103/PhysRevLett.45.1930
1979KO32 Phys.Rev.Lett. 43, 1862 (1979) R.W.Koontz, C.C.Chang, H.D.Holmgren, J.R.Wu Projectile Fragmentation Processes in 35-MeV/amu (α, xy) Reactions NUCLEAR REACTIONS 90Zr(α, pt), (α, 2d), (α, pX), E=35 MeV/nucleon; measured fragment-fragment (θ), (fragment)(fragment)-coin; deduced reaction mechanism.
doi: 10.1103/PhysRevLett.43.1862
1979WA11 Phys.Rev. C20, 1079 (1979) N.S.Wall, J.R.Wu, C.C.Chang, H.D.Holmgren Medium Energy Nuclear Reactions: 'Quasi-Two-Body Scaling' and 'Hot Spots' NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(p, p), (p, d), (p, t), (p, α), E=90 MeV; 27Al, 58Ni, 90Zr, 209Bi(α, p), (α, d), (α, t), (α, α), E=140 MeV; calculated energy spectra; deduced characteristic parameter. Quasi two-body scaling, hot spot interpretation.
doi: 10.1103/PhysRevC.20.1079
1979WU02 Phys.Rev. C19, 370 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren Charged-Particle Spectra: 80 MeV Deuterons on 27Al and 58Ni and 70 MeV Deuterons on 90Zr, 208Pb, and 232Th NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 208Pb, 232Th(d, pX), (d, dX), (d, tX), (d, 3HeX), (d, αX), E=70, 80 MeV; measured σ(θp, Ep), σ(θd, Ed), σ(θt, Et), σ(θ(3He), E(3He)), σ(θα, Eα); deduced σ(E). Comparison with preequilibrium exciton, compound nuclear evaporation, deuteron breakup model.
doi: 10.1103/PhysRevC.19.370
1979WU03 Phys.Rev. C19, 659 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren Charged Particle Spectra: 140 MeV α Particle Bombardment of 27Al, 58Ni, 90Zr, 209Bi, and 232Th NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi, 232Th(α, pX), (α, dX), (α, 3HeX), (α, αX), E=140 MeV; measured σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(E(3He), θ(3He)), σ(Eα, θα); comparison with preequilibrium exciton, evaporation, projectile breakup models.
doi: 10.1103/PhysRevC.19.659
1979WU04 Phys.Rev. C19, 698 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren Charged-Particle Spectra: 90 MeV Protons on 27Al, 58Ni, 90Zr, and 209Bi NUCLEAR REACTIONS 27Al, 90Zr, 209Bi(p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), E=90 MeV; 58Ni(p, pX), (p, dX), (p, tX), (p, 3HeX), (p, αX), E=90, 100 MeV; measured σ(Ep, θp), σ(Ed, θd), σ(Et, θt), σ(E(3He), θ(3He)), σ(Eα, θα). Comparison with pre-equilibrium exciton, evaporation models.
doi: 10.1103/PhysRevC.19.698
1979WU09 Phys.Rev. C20, 1284 (1979) J.R.Wu, C.C.Chang, H.D.Holmgren, R.W.Koontz Alpha-Particle Breakup at Incident Energies of 20 and 40 MeV/Nucleon NUCLEAR REACTIONS 27Al, 58Ni, 90Zr, 209Bi(α, p), (α, d), (α, t), (α, 3He), E=80, 160 MeV; measured differential energy spectra; deduced α breakup yield, reaction mechanism. Plane wave model.
doi: 10.1103/PhysRevC.20.1284
1978WU02 Phys.Rev.Lett. 40, 1013 (1978) J.R.Wu, C.C.Chang, H.D.Holmgren Breakup of α Particles in the Fields of Nuclei NUCLEAR REACTIONS 209Bi, 58Ni, 90Zr, 120Sn, 232Th(α, p), (α, d), (α, t), (α, 3He), E=140 MeV; analyzed α-particle breakup.
doi: 10.1103/PhysRevLett.40.1013
1977CO07 Phys.Rev. C15, 1650 (1977) A.A.Cowley, P.G.Roos, N.S.Chant, R.Woody, III, H.D.Holmgren, D.A.Goldberg (p, d3He) Reaction as a Quasifree Reaction Process NUCLEAR REACTIONS 6,7Li, 9Be, 12C(p, d3He), E=100 MeV; measured σ(Ed, E(3He), θ); deduced absolute Sα for double quasifree angle pairs.
doi: 10.1103/PhysRevC.15.1650
1977RO02 Phys.Rev. C15, 69 (1977) P.G.Roos, N.S.Chant, A.A.Cowley, D.A.Goldberg, H.D.Holmgren, R.Woody, III Absolute Spectroscopic Factors from the (p, pα) Reaction at 100 MeV on 1p-Shell Nuclei NUCLEAR REACTIONS 6,7Li, 9Be, 12C(p, pα), E=100 MeV; measured σ(Ep, Eα, θ). 6,7Li, 9Be, 12C deduced Sα. Coplanar geometry, DWIA analysis.
doi: 10.1103/PhysRevC.15.69
1976BA38 Nucl.Phys. A268, 488 (1976) D.Bachelier, J.L.Boyard, T.Hennino, H.D.Holmgren, J.C.Jourdain, P.Radvanyi, P.G.Roos, M.Roy-Stephan Quasi-Free (p, pα) Scattering on 24Mg, 28Si, 40Ca and 58Ni at 157 MeV NUCLEAR REACTIONS 24Mg, 28Si, 40Ca, 58Ni(p, pα), E=157 MeV; measured σ(Eα, Ep, θ); deduced reaction mechanism. 24Mg, 28Si, 40Ca, 58Ni levels deduced S α.
doi: 10.1016/0375-9474(76)90545-5
1976BH02 Phys.Rev. C13, 2105 (1976) R.K.Bhowmik, C.C.Chang, J.-P.Didelez, H.D.Holmgren (p, 2p) Reaction on 7Li and 12C at 100 MeV NUCLEAR REACTIONS 7Li, 12C(p, 2p), E=100 MeV; measured σ(Ep), pp(θ); deduced distorted recoil momentum distributions. Separation energy resolution 0.8 MeV; DWIA analysis.
doi: 10.1103/PhysRevC.13.2105
1976DI05 Phys.Rev. C13, 1388 (1976) J.-P.Didelez, C.C.Chang, N.S.Chant, H.D.Holmgren, R.I.Steinberg, J.R.Wu Analysis of the 12C(d, 3He)11B(g.s.) Reaction at 80 MeV NUCLEAR REACTIONS 12C(d, 3He), E=80 MeV; calculated σ(θ). 11B deduced S. DWBA.
doi: 10.1103/PhysRevC.13.1388
1976LE05 Phys.Lett. 61B, 47 (1976) Y.Le Bornec, B.Tatischeff, L.Bimbot, I.Brissaud, H.D.Holmgren, J.Kallne, F.Reide, N.Willis Pion Production Near Threshold on 40Ca: Energy Dependence and Angular Distribution NUCLEAR REACTIONS 40Ca(p, π+), E=149-154 MeV; measured σ(E, Eπ+, θ).
doi: 10.1016/0370-2693(76)90558-X
1975BA75 J.Phys.(Paris), Colloq. 36, C5-127 (1975) D.Bachelier, J.L.Boyard, T.Hennino, H.D.Holmgren, J.C.Jourdain, P.Radvanyi, P.G.Roos, M.Roy-Stephan Diffusion Quasi Libre (p, pα) sur les Noyaux Pair-Pair 24Mg, 28Si, 40Ca et 58Ni NUCLEAR REACTIONS 24Mg, 28Si, 40Ca, 58Ni(p, pα), E=157 MeV; measured σ. 20Ne, 36Ar deduced α-S.
1975LE25 J.Phys.(Paris), Colloq. 36, C5-133 (1975) Y.Le Bornec, B.Tatischeff, L.Bimbot, I.Brissaud, H.D.Holmgren, F.Reide, N.Willis Reaction de Production de Pions Pres du Seuil NUCLEAR REACTIONS 40Ca(p, π+), E=149-154 MeV; measured σ(E).
1974BH03 Nucl.Phys. A226, 365 (1974) R.K.Bhowmik, C.C.Chang, P.G.Roos, H.D.Holmgren The 6Li(p, 2p)5He Reaction at 100 MeV NUCLEAR REACTIONS 6Li(p, 2p), E=100 MeV; measured σ(E1, E2, θ(1), θ(2)). Enriched target.
doi: 10.1016/0375-9474(74)90489-8
1974LE12 Phys.Lett. 49B, 434 (1974) Y.Le Bornec, B.Tatischeff, L.Bimbot, I.Brissaud, J.P.Garron, H.D.Holmgren, F.Reide, N.Willis Positive Pion Production at Threshold on a 10B Target NUCLEAR REACTIONS 10B(p, π), E=154 MeV; measured σ(Eπ, θ).
doi: 10.1016/0370-2693(74)90628-5
1970JA17 Nucl.Phys. A153, 49 (1970) M.Jain, P.G.Roos, H.G.Pugh, H.D.Holmgren The (p, pα) and (α, 2α) Reactions on 6Li and 7Li at 60 MeV NUCLEAR REACTIONS 6,7Li(p, pα), E=57 MeV; 6,7Li(α, 2α), E=64 MeV; measured σ(Ep, Eα, θ(p), θ(α)), σ(Eα1, Eα2, θ(1), θ(α2)). Enriched targets.
doi: 10.1016/0375-9474(70)90756-6
1969EP01 Phys.Rev. 178, 1698 (1969) M.Epstein, H.D.Holmgren, M.Jain, H.G.Pugh, P.G.Roos, N.S.Wall, C.D.Goodman, C.A.Ludemann Study of the C12(p, pα)Be8 Reaction and Excited States of C12 NUCLEAR REACTIONS 12C(p, pα)8Be 12C(p, 2p), E=57 MeV; measured σ(Ep, Eα); deduced reaction mechanism. 12C deduced levels, J, π, proton decay, T.
doi: 10.1103/PhysRev.178.1698
1969RO04 Phys.Rev.Letters 22, 242(1969) P.G.Roos, H.Him, M.Jain, H.D.Holmgren Test of the Cluster-Knockout Model Using the Reaction Li6(p, pα)d NUCLEAR REACTIONS 6Li(p, pα), E=61.5 MeV; measured σ(Ep, θ(p), θ(α));deduced reaction mechanism.
doi: 10.1103/PhysRevLett.22.242
1968JA07 Phys.Rev. 172, 1015 (1968) The C13(He3, Be8(g.s.))Be8(g.s.) Reaction NUCLEAR REACTIONS 13C(3He, 8Be), E=2.5-5.75 MeV; measured σ(E;θ). 16O deduced resonances, J, π.
doi: 10.1103/PhysRev.172.1015
1968MO05 Phys.Rev. 166, 977 (1968) Angular Correlations for the Reaction Be9(He3, α)Be8(16.92)→α+α NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.166.977
1968RO19 Phys.Rev. 176, 1246(1968) P.G.Roos, H.G.Pugh, M.Jain, H.D.Holmgren, M.Epstein, C.A.Ludemann Be9(p, pα)He5 Reaction at 57 MeV NUCLEAR REACTIONS 9Be(p, pα), E = 57 MeV; measured σ(Ep, Eα, θ(p), θ(α)); deduced quasifree scattering contribution.
doi: 10.1103/PhysRev.176.1246
1966WA16 Nucl.Phys. 88, 81(1966) M.A.Waggoner, J.E.Etter, H.D.Holmgren, C.Moazed A Study of the Reaction 10B(3He, Pααα) NUCLEAR REACTIONS 10B(3He, p3α), E = 2.45, 6.0 MeV. Measured σ(Ep, Eα, θ(pd), θ(αα)). 12C, 9B deduced levels J, π. Enriched target.
doi: 10.1016/0029-5582(66)90454-8
1965DA11 Phys.Rev. 137, B315 (1965) P.Darriulat, G.Igo, H.G.Pugh, H.D.Holmgren Elastic Scattering of Alpha Particles by Helium Between 53 and 120 MeV NUCLEAR REACTIONS 4He(α, α), E=53-120 MeV; measured reaction products, Eα, Iα; deduced σ(θ), the real and imaginary parts of phase shifts, parameters, single-level dispersion theory fits.
doi: 10.1103/PhysRev.137.B315
1964DA12 Phys.Letters 11, 326 (1964) P.Darriulat, G.Igo, H.G.Pugh, H.D.Holmgren Elastic Alpha-Helium Scattering up to 120 MeV NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90349-X
1964ET01 Bull.Am.Phys.Soc. 9, No.4, 407, CA6 (1964) J.E.Etter, H.D.Holmgren, A.A.Jaffe, C.Moazed, M.A.Waggoner 10B(3He, pα)8Be Reaction NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
1964ET02 Phys.Letters 12, 42 (1964) J.E.Etter, M.A.Waggoner, H.D.Holmgren, C.Moazed, A.A.Jaffe The B10(He3, pα)2He4 Reaction NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)91169-2
1964MO05 Bull.Am.Phys.Soc. 9, No.4, 407, CA5 (1964) C.Moazed, J.E.Etter, H.D.Holmgren 9Be(3He, α)24He reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1964MO19 Phys.Letters 12, 45 (1964) C.Moazed, J.E.Etter, H.D.Holmgren, M.A.Waggoner The Be9(He3, α)2He4 Reaction NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)91170-9
1964SC09 Phys.Rev. 134, B577 (1964) R.B.Schwartz, H.D.Holmgren, L.M.Cameron, A.R.Knudson Differential Cross Sections of Triton-Induced Reactions on N14 NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.134.B577
1963HO01 Bull.Am.Phys.Soc. 8, No.1, 26, F12 (1963) F19(p, t)F17 and F19(p, α)O16 Reactions NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
1963HO19 Nucl.Phys. 48, 1 (1963) H.D.Holmgren, L.M.Cameron, R.L.Johnston Triton Induced Reactions on B10 NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90138-X
1963HO24 Phys.Rev. 132, 2644 (1963) F19(p, t)F17 and F19(p, α)O16 Reactions at 22.8 MeV NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.132.2644
1963LU01 Bull.Am.Phys.Soc. 8, No.1, 12, BA10 (1963) C.A.Ludemann, H.D.Holmgren, W.F.Hornyak C12(He3, pγ)N14 Angular Correlations NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1963LU05 Bull.Am.Phys.Soc. 8, No.4, 303, D6 (1963) C.A.Ludemann, H.D.Holmgren, J.E.Etter C12(He3, α0)C11 Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1963PU05 Bull.Am.Phys.Soc. 8, No.8, 612, N11 (1963) H.G.Pugh, P.Darriulat, H.D.Holmgren, G.Igo Elastic Scattering of α Particles from Helium at Energies between 52 and 120 MeV NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1962GU01 Phys.Rev. 125, 648 (1962) G.D.Gutsche, H.D.Holmgren, L.M.Cameron, R.L.Johnston Differential Cross Sections for Tritium-Induced Reactions on C12 NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.125.648
1962HO13 Nuclear Phys. 38, 489 (1962) Angular Correlations for the C13(He3, αγ)C12 Reaction NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)91060-X
1962SC05 Bull.Am.Phys.Soc. 7, No.4, 286, FB9 (1962) R.B.Schwartz, L.M.Cameron, H.D.Holmgren Cross Sections for the N14(t, p)N16 and N14(t, d0)N15 Reactions NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1961CA10 Bull.Am.Phys.Soc. 6, No.5, 416, B9 (1961) L.M.Cameron, H.D.Holmgren, R.B.Schwartz Differential Cross Sections of the N14(t, α)C13 Reactions NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1961HO01 Bull.Am.Phys.Soc. 6, No.1, 36, MA2 (1961) Tritium Induced Reactions in Light Nuclei NUCLEAR STRUCTURE 10B, 7Li, 11B, 6Li; measured not abstracted; deduced nuclear properties.
1961HO21 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Id., Academic Press Inc., New York, p.531 (1961) The 6Li(t, d)7Li and 10B(t, d)11B Reactions NUCLEAR STRUCTURE 10B, 6Li; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1458. 1961HO22 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.535 (1961) H.D.Holmgren, L.M.Cameron, G.Gutsche The 12C(t, α)11B Reaction NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1961HO23 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.537 (1961) The 7Li(t, α)6He Reaction NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1526. 1961HO24 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.539 (1961) The 13C(3He, αγ)12C Reaction NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
1961SC13 Bull.Am.Phys.Soc. 6, No.5, 416, B8 (1961) R.B.Schwartz, L.M.Cameron, H.D.Holmgren Differential Cross Sections of the N14(t, d0)N15 Reaction NUCLEAR REACTIONS 14N(t, d), E = 1-2 MeV; measured reaction products; deduced σ(θ), yields. The Nucleonics Division 2-Mv Van de Graaff accelerator.
1961WO08 Proc.Rutherford Jubilee Intern.Conf. Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.533 (1961) E.A.Wolicki, H.D.Holmgren, R.I.Johnston Angular Correlations in the Reaction 19B(3He, pγ)12C NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
1959BU05 Phys.Rev. 116, 1485 (1959) Radiative Proton Capture by O18
doi: 10.1103/PhysRev.116.1485
1959BU81 Phys.Rev. 113, 268 (1959) J.W.Butler, L.W.Fagg, H.D.Holmgren Energy Levels in F19 from the O18(d, nγ)F19 Reaction
doi: 10.1103/PhysRev.113.268
1959HO01 Phys.Rev. 114, 1281 (1959) H.D.Holmgren, E.A.Wolicki, R.L.Johnston B11(He3, p)C13 and B11(He3, d)C12 Reactions
doi: 10.1103/PhysRev.114.1281
1959HO03 Phys.Rev. 113, 1556 (1959) H3(α, γ)Li7 and He3(α, γ)Be7 Reactions
doi: 10.1103/PhysRev.113.1556
1959JO32 Bull.Am.Phys.Soc. 4, No.7, 403, C4 (1959) R.L.Johnston, H.D.Holmgren, G.D.Gutsche Differential Cross Sections for the O16(t, p)O18 and O16(t, α)N15 Reactions
1959WO53 Phys.Rev. 116, 1585 (1959) E.A.Wolicki, H.D.Holmgren, R.L.Holmgren, R.L.Johnston, E.G.Illsley Differential Cross Sections for the Be9(He3, p)B11 Reaction
doi: 10.1103/PhysRev.116.1585
1958BU12 Phys.Rev. 112, 461 (1958) Gamma-Ray Threshold Method and the O18(d, nγ)F19 Reaction
doi: 10.1103/PhysRev.112.461
1958HO72 Bull.Am.Phys.Soc. 3, No.1, 26, J2 (1958) He3(α, γ)Be7 Reaction
1958JO20 Phys.Rev. 109, 884 (1958) R.L.Johnston, H.D.Holmgren, E.A.Wolicki, E.G.Illsley Differential Cross Sections for the C12(He3, p)N14 Reaction
doi: 10.1103/PhysRev.109.884
1957HO61 Bull.Am.Phys.Soc. 2, No.4, 181, E7 (1957) H.D.Holmgren, E.A.Wolicki, R.L.Johnston B11(He3, p)C13, and B11(He3, d)C12 Angular Distributions at 4.5 MeV
1957HO62 Phys.Rev. 106, 102 (1957) H.D.Holmgren, E.H.Geer, R.L.Johnston, E.A.Wolicki C13(He3, α)C12 Angular Distributions at 4.5 MeV
doi: 10.1103/PhysRev.106.102
1957HO63 Phys.Rev. 106, 100 (1957) Differential Cross Section for the C13(He3, α)C12 Reaction at 2.00 MeV
doi: 10.1103/PhysRev.106.100
1957IL01 Phys.Rev. 107, 538 (1957) E.G.Illsley, H.D.Holmgren, R.L.Johnston, E.A.Wolicki Differential cross sections for the C13 (He3, p)N15 reaction NUCLEAR REACTIONS 13C(3He, p), E=1.8-4.5 MeV; measured products, 15N, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry C1361.
doi: 10.1103/PhysRev.107.538
1956HL01 Phys.Rev. 104, 1446 (1956) H.D.Holmgren, M.L.Bullock, W.E.Kunz Differential cross sections for the Be9(He3, p)B11 reaction NUCLEAR REACTIONS 9Be(3He, p), E=2 MeV; measured products, 11B, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry F0487.
doi: 10.1103/PhysRev.104.1446
1955HO28 Phys.Rev. 98, 241, R6 (1955) H.D.Holmgren, T.D.Hanscome, D.K.Willett Q Values for the O17(d, p)O18 and O18(d, p)O19 Reactions NUCLEAR REACTIONS 17,18O(d, p), E=1.390, 1.976 MeV; measured reaction products, Ep, Ip; deduced Q-values. Comparison with available data.
doi: 10.1103/PhysRev.98.220
1954BR05 Phys.Rev. 96, 80 (1954) R.J.S.Brown, K.F.Famularo, H.D.Holmgren, D.Rankin, T.F.Stratton Elastic Scattering of Deuterons by He3
doi: 10.1103/PhysRev.96.80
1954HO48 Phys.Rev. 95, 1544 (1954) H.D.Holmgren, J.M.Blair, B.E.Simmons, T.F.Stratton, R.V.Stuart Differential Cross Sections for the C12(d, p)C13 and C13(d, t)C12 Reactions
doi: 10.1103/PhysRev.95.1544
1952BR87 Phys.Rev. 88, 253 (1952) R.J.S.Brown, G.D.Frier, H.D.Holmgren, W.R.Stratton, J.L.Yarnell Differential Cross Section Measurements for the Scattering of Protons by Deuterons NUCLEAR REACTIONS 1H(d, d), E=960 keV-3.2 MeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry C0860.
doi: 10.1103/PhysRev.88.253
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