NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = R.H.Stokes Found 25 matches. 1983PO11 Phys.Rev. C28, 2299 (1983) S.Pontoppidan, P.R.Christensen, O.Hansen, F.Videbaek, H.C.Britt, B.H.Erkkila, Y.Patin, R.H.Stokes, M.P.Webb, R.L.Ferguson, F.Plasil, G.R.Young Quasielastic Transfer Reactions Induced by 56Fe on 58Ni, 64Ni, and 122Sn NUCLEAR REACTIONS 58,64Ni, 122Sn(56Fe, X), E=320, 460 MeV; measured fragment yield vs mass, σ(fragment θ) vs (Q) for X=51,50V, 51,52,53,54,55Cr, 52,53,54,55,56Mn, 54,55,56,57,58,59,60Fe, 56,57,58,59,60Co, 57,58,59,60,61Ni; deduced reaction mechanism. DWBA analyses.
doi: 10.1103/PhysRevC.28.2299
1982BR22 Phys.Rev. C26, 1999 (1982) H.C.Britt, B.H.Erkkila, A.Gavron, Y.Patin, R.H.Stokes, M.P.Webb, P.R.Christensen, O.Hansen, S.Pontoppidan, F.Videbaek, R.L.Ferguson, F.Plasil, G.R.Young, J.Randrup Correlated Charge and Mass Distributions from Reactions of 56Fe with 58Ni, 64Ni, and 122Sn NUCLEAR REACTIONS 58Ni(56Fe, X), E=315, 461 MeV; 64Ni(56Fe, X), E=464 MeV; 122Sn(56Fe, X), E=320, 460 MeV; measured σ(fragment θ) vs energy loss, fragment distribution first, second moments; deduced reaction mechanism. Transport theory.
doi: 10.1103/PhysRevC.26.1999
1979BL01 Phys.Rev. C19, 1288 (1979) M.Blann, R.H.Stokes, B.Erkkila, H.C.Britt, P.D.Goldstone, R.L.Ferguson, F.Plasil, H.H.Gutbrod Final and Primary Yields and Dispersions for Strongly Damped Reaction Of 86Kr + 124Sn NUCLEAR REACTIONS 124Sn(86Kr, X), E=440, 720 MeV; measured distributions of fragment energy, mass vs atomic number; deduced primary distribution.
doi: 10.1103/PhysRevC.19.1288
1978PL02 Phys.Rev.Lett. 40, 1164 (1978) F.Plasil, R.L.Ferguson, H.C.Britt, R.H.Stokes, B.H.Erkkila, P.D.Goldstone, M.Blann, H.H.Gutbrod Measurement of the Energy Division Versus Mass in Highly Damped Reactions NUCLEAR REACTIONS 124Sn(86Kr, X), E=440, 720 MeV; measured σ(A, Z).
doi: 10.1103/PhysRevLett.40.1164
1978PL07 Phys.Rev. C18, 2603 (1978) F.Plasil, R.L.Ferguson, H.C.Britt, B.H.Erkkila, P.D.Goldstone, R.H.Stokes, H.H.Gutbrod Evaporation Residue Products from Reactions with 86Kr NUCLEAR REACTIONS 65Cu, 90Zr, 109Ag(86Kr, X), E=366-716 MeV; measured evaporation residue σ(θ). 65Cu(86Kr, X), E=366, 716 MeV; measured A, Z distributions of evaporation residue products.
doi: 10.1103/PhysRevC.18.2603
1977BR30 Phys.Rev.Lett. 39, 1458 (1977) H.C.Britt, B.H.Erkkila, P.D.Goldstone, R.H.Stokes, B.B.Back, F.Folkmann, O.Christensen, B.Fernandez, J.D.Garrett, G.B.Hagemann, B.Herskind, D.L.Hillis, F.Plasil, R.L.Ferguson, M.Blann, H.H.Gutbrod Angular Momentum Limits in Fusion Reactions Induced by Argon and Krypton Projectiles NUCLEAR REACTIONS 122,124Sn(40Ar, X), 76Ge(86Kr, X); measured γ-multiplicity. 70,74Ge(86Kr, X); measured σ(A, Z).
doi: 10.1103/PhysRevLett.39.1458
1976BR10 Phys.Rev. C13, 1483 (1976) H.C.Britt, B.H.Erkkila, R.H.Stokes, H.H.Gutbrod, F.Plasil, R.L.Ferguson, M.Blann Argon- and Krypton-Induced Reactions at Energies of 4-7 MeV/amu NUCLEAR REACTIONS 109Ag(40Ar, X), E=169-337 MeV; 121Sb(40Ar, X), E=282, 340 MeV; 65Cu(84Kr, X), E=494, 604 MeV; measured elastic scattering, evaporation residue, fission, fusion σ.
doi: 10.1103/PhysRevC.13.1483
1972WA07 Part.Nucl. 3, 1 (1972) Nuclear and Coulomb Pairing Energy Systematics in Light Nuclei
1971HO26 Phys.Rev.Lett. 27, 1086 (1971) H.H.Howard, R.H.Stokes, B.H.Erkkila Experimental Determination of the 12Be Ground-State Mass NUCLEAR REACTIONS 7Li(7Li, 2p), E=25, 30, 30.1 MeV; measured Q, σ(E(p1), E(p2)). 12Be deduced ground-state mass.
doi: 10.1103/PhysRevLett.27.1086
1971ST05 Phys.Rev. C3, 984 (1971) Search for Excited States of 6He NUCLEAR REACTIONS 7Li(t, α), 4He(t, p), 6Li(t, 3He) , E < 22 MeV; 7Li(d, 3He), E=17, 22 MeV; measured σ(θ). 6He level deduced J, π. 6He deduced no levels > 1.80 MeV.
doi: 10.1103/PhysRevC.3.984
1971YO04 Phys.Rev. C4, 1597 (1971) New States in 9Li from the Reaction 7Li(t, p)9Li NUCLEAR REACTIONS 7Li(t, p), E=15, 19 MeV; measured σ(Ep, θ). 9Li deduced levels, level-width, J, π.
doi: 10.1103/PhysRevC.4.1597
1969ST02 Phys.Rev. 178, 2024 (1969) Further Results on 7He NUCLEAR REACTIONS 7Li(t, 3He), E = 22 MeV; measured Q, σ(E(3He), θ). 7He deduced ground-state level-width.
doi: 10.1103/PhysRev.178.2024
1969ST07 Phys.Rev. 178, 1789 (1969) 18N and 22F Ground States, 22F Excited States, and T = 2 Analogs in 22Ne NUCLEAR REACTIONS 18O, 22Ne(t, 3He), E=22 MeV; measured Q, σ(E(3He)). 22F deduced levels. 22Ne(p, p'), (d, d'), (t, t'), E=22 MeV; measured σ(Ep'), σ(Ed'), σ(Et'). 22Ne deduced levels, isobaric analog.
doi: 10.1103/PhysRev.178.1789
1968OH04 Phys.Rev. 176, 1163 (1968) G.G.Ohlsen, R.H.Stokes, P.G.Young Search for States in the Three-Neutron and Triton Systems NUCLEAR REACTIONS 3He(t, 3He), 3H(t, 3He), E=22.25 MeV; measured reaction products, 3He spectra; analyzed evidence for 3n and 3H resonances; deduced a weak evidence for existence of a trineutron unbound by 1 to 1.5 MeV.
doi: 10.1103/PhysRev.176.1163
1968ST08 Bull.Am.Phys.Soc. 13, No.4, 652, GF6 (1968) Ground and Excited States of 22F NUCLEAR STRUCTURE 22F; measured not abstracted; deduced nuclear properties.
1968YO06 Phys.Rev. 173, 949 (1968) P.G.Young, R.H.Stokes, G.G.Ohlsen Search for the Ground State of 5H by Means of the 3H(t, p) Reaction NUCLEAR STRUCTURE 5H, 3H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.173.949
1967JA07 Phys.Rev. 161, 1050(1967) N.Jarmie, R.H.Stokes, G.G.Ohlsen, R.W.Newsome, Jr. Experimental Study of Excited 4H, 4He, and 4Li Nuclear Systems NUCLEAR STRUCTURE 4H, 3H, 3He, 4He, 4Li, 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.161.1050
1967ST04 Phys.Rev.Letters 18, 611(1967) New Isotope of Helium: 7He NUCLEAR STRUCTURE 7He, 7Li; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.18.611
1965BR40 Phys.Rev. 139, B354 (1965) H.C.Britt, W.R.Gibbs, J.J.Griffin, R.H.Stokes (d, p-f) Angular-Correlation Study of Fission-Barrier Transition States: Energy Gap of a Highly Deformed Nucleus NUCLEAR REACTIONS, Fission 233U, 239Pu(d, pF), E=14.9 MeV; measured σ(Ep, θ(p), θ(fragment)). 234U, 240Pu deduced fission-barrier transition states.
doi: 10.1103/PhysRev.139.B354
1965JA01 Bull.Am.Phys.Soc. 10, No.1, 51, DC5 (1965) M.Jakobson, J.H.Manley, R.H.Stokes He3 + d → T + 2p Reaction NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1965JA08 Nucl.Phys. 70, 97 (1965) M.Jakobson, J.H.Manley, R.H.Stokes The He3+d→t+2p Reaction NUCLEAR REACTIONS 2H(3He, t), E = 21 MeV; 3He(d, t), E = 11.7, 14.0 MeV; measured σ(Et, θ). Enriched targets.
doi: 10.1016/0029-5582(65)90226-9
1964RO08 Phys.Letters 8, 320 (1964) A Search for H4, Protons from H3(d, p) NUCLEAR STRUCTURE 4H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/S0031-9163(64)80016-0
1962CA33 Nucl.Phys. 36, 511 (1962) R.F.Carlson, R.M.Eisberg, R.H.Stokes, T.H.Short Total proton reaction cross section of copper NUCLEAR REACTIONS Cu(p, X), E=8.9 MeV; measured products; deduced σ, σ(E). Data were imported from EXFOR entry C0067.
doi: 10.1016/0029-5582(62)90474-1
1961CA08 Bull.Am.Phys.Soc. 6, No.5, 441, P11 (1961) R.F.Carlson, R.M.Bisberg, R.H.Stokes, T.H.Short Total Proton Reaction Cross Section for Copper at 9 MeV NUCLEAR STRUCTURE Cu; measured not abstracted; deduced nuclear properties.
1961ST03 Phys.Rev. 121, 613 (1961) (d, p) Reaction on Heavy Elements at Low Deuteron Energies NUCLEAR STRUCTURE 210Bi, 207Pb; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.121.613
Back to query form |