NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = R.J.Slobodrian Found 79 matches. 1995BA24 Can.J.Phys. 73, 74 (1995) D.Baddou, C.Rioux, R.J.Slobodrian, J.M.Nelson Analysing Power and Differential Cross Sections of (3He, p) Reactions on 6Li and 7Li at Low Energy NUCLEAR REACTIONS 6,7Li(polarized 3He, p), E=4.6 MeV; measured σ(θ), analyzing power vs θ. DWBA analysis.
doi: 10.1139/p95-012
1990SL03 Nuovo Cim. 103A, 1523 (1990) Uncertainties in Proton-Proton Scattering at Low Energies NUCLEAR REACTIONS 1H(p, pγ), E=low; 1H(p, p), E=0-30 MeV; analyzed data analyses; deduced uncertainties.
doi: 10.1007/BF02820298
1989SL01 Phys.Rev. C39, 1052 (1989) Three- and N-Body Systems: An approach in terms of relative coordinates and momenta ATOMIC PHYSICS, Mesic-Atoms 3He; calculated kaonic, antiprotonic atom binding energies. NUCLEAR STRUCTURE 3He; calculated kaonic, antiprotonic atom binding energies.
doi: 10.1103/PhysRevC.39.1052
1988DO02 Phys.Rev. C37, 927 (1988) P.Doleschall, H.Kroger, R.J.Slobodrian Coulomb Faddeev Calculation of d + p → p + p + n Spectra near Threshold and Three-Body Effects NUCLEAR REACTIONS 1n, 1H(d, d), E=7.4; calculated σ(θ). 1H(d, 2p), E=7.4 MeV; 1n(d, np), E=7.4 MeV; calculated σ(θ1, θ2, E1, E2).
doi: 10.1103/PhysRevC.37.927
1986BR15 Phys.Rev. C34, 330 (1986) P.Bricault, R.J.Slobodrian, J.Pouliot, R.Roy Strong Anomaly in the d-p Bremsstrahlung NUCLEAR REACTIONS 1H(d, γ), E=6.3-7.1 MeV; measured σ(θp, θd); deduced bremsstrahlung σ(E).
doi: 10.1103/PhysRevC.34.330
1986KR05 Phys.Rev. C33, 1208 (1986) H.Kroger, A.M.Nachabe, R.J.Slobodrian Deuteron-Proton Breakup Reaction at E(d) = 7.4 MeV NUCLEAR REACTIONS 2H(p, np), E=7.4 MeV; calculated kinematically complete breakup σ(θ1, θ2) vs Ep. Coulomb effects.
doi: 10.1103/PhysRevC.33.1208
1986NA12 J.Phys.(Paris) 47, 1141 (1986) A.M.Nachabe, R.J.Slobodrian, B.K.Sinha, R.Roy, H.Kroger Mise en Evidence de la Force a Trois Corps dans la Reaction d + p → p + p + n pres du Seuil de Cassure NUCLEAR REACTIONS 1H(d, 2p), E=7.4 MeV; measured σ(θ1, θ2) vs arc length; deduced two-pion exchange three-body force role in breakup.
doi: 10.1051/jphys:019860047070114100
1985KR08 Phys.Rev. C32, 628 (1985) H.Kroger, A.M.Nachabe, R.J.Slobodrian Peaks in the Low Energy d + p Breakup Cross Section and the Repulsive Coulomb Force NUCLEAR REACTIONS 2H(p, pn), E=7.4 MeV; measured σ(θ1, θ2) vs energy along kinematical arc. Kinematically complete experiment, repulsive Coulomb force.
doi: 10.1103/PhysRevC.32.628
1985PO17 Can.J.Phys. 63, 951 (1985) L.Potvin, R.Roy, P.Bricault, R.Larue, C.Rioux, R.J.Slobodrian Reaction (3He, α): Validite du modele optique dans la description de la voie 3He-noyau NUCLEAR REACTIONS 17O, 29Si, 53Cr(3He, α), E=14 MeV; measured σ(θ); deduced optical model parameters. DWBA analysis.
doi: 10.1139/p85-154
1985SI12 Z.Phys. A321, 381 (1985) B.K.Sinha, A.M.Nachabe, P.Bricault, J.Pouliot, L.Potvin, R.Roy, R.J.Slobodrian Production of High Energy Deuterons in the Reaction: 3He + 3He → 4He + 2He + e+ + ν NUCLEAR REACTIONS 3He(3He, α), E=13.6 MeV; measured σ(θ, Eα); deduced high energy deuteron production σ limit.
doi: 10.1007/BF01411968
1984KR19 Phys.Lett. 144B, 19 (1984) Coulomb Difference between p + d and n + d Breakup Amplitude very near the Threshold NUCLEAR REACTIONS 2H(p, 2p), E(cm)=0.275 MeV; calculated σ(θ1, θ2) vs energy along kinematic arc; deduced Coulomb effect role.
doi: 10.1016/0370-2693(84)90167-9
1984KR20 Phys.Rev. C30, 1390 (1984) Coulomb Scattering of Wave Packets NUCLEAR REACTIONS 1H(d, 2p), E=7.5, 7.402 MeV; calculated σ(θ1, θ2) vs kinematic curve. S-matrix, long-range Coulomb forces, wave packets.
doi: 10.1103/PhysRevC.30.1390
1984PO02 J.Phys.(Paris) 45, 71 (1984) J.Pouliot, P.Bricault, J.G.Dufour, L.Potvin, C.Rioux, R.Roy, R.J.Slobodrian Invariance par Renversement du Temps: Nouvelles mesures de polarisation dans la reaction 9Be(3He, p)11B NUCLEAR REACTIONS 9Be(3He, p), E=14 MeV; measured proton polarization vs θ; deduced time reversal invariance violation.
doi: 10.1051/jphys:0198400450107100
1984SL02 Phys.Lett. 135B, 17 (1984) Magnetic Dipole Effects on p-n-n Final States and Scattering Parameters NUCLEAR REACTIONS 2H(π-, γ), (n, 2n), E not given; analyzed scattering parameter from breakup data; deduced final state magnetic dipole effects.
doi: 10.1016/0370-2693(84)90444-1
1984SL04 Phys.Rev. C29, 2353 (1984) Scattering of Polarized Tritons near 10 MeV: Possible giant multipole resonance effects NUCLEAR REACTIONS 12C, 51V, 58Ni(polarized t, t), E ≈ 10 MeV; 27Al(polarized p, p), E not given; 58Ni(polarized 3He, 3He), E=33 MeV; analyzed data; deduced spin-orbit term excitation energy dependence. 15N, 28Si, 54Cr, 61Cu, 61Zn deduced possible GDR role.
doi: 10.1103/PhysRevC.29.2353
1983BR08 J.Phys.(Paris) 44, 461 (1983) P.Bricault, R.J.Slobodrian, C.Rioux, L.Potvin, R.Roy, R.Larue, B.Frois Rayonnement de Freinage dans l'Interaction 3He-2H pres du Seuil de Cassure du Deuton NUCLEAR REACTIONS 2H(3He, 3He), E=5.2-6 MeV; measured σ(θ, θγ) bremsstrahlung vs E.
doi: 10.1051/jphys:01983004404046100
1983PO13 Can.J.Phys. 61, 1609 (1983) J.Pouliot, R.Roy, P.Bricault, L.Potvin, R.J.Slobodrian Polarization et Mesures de Section Efficace dans la Reaction 9Be(3He, p)11B NUCLEAR REACTIONS 9Be(3He, p), E=13-14.2 MeV; measured σ(Ep), σ(θ), σ(θ) vs E.
doi: 10.1139/p83-210
1983RI01 Nucl.Phys. A394, 428 (1983) C.Rioux, R.Roy, R.J.Slobodrian, H.E.Conzett Asymetrie Du Temps: Polarisation et pouvoir d'analyse dans les reactions Nucleaires NUCLEAR REACTIONS 2H, 7Li, 9Be(3He, p), E=14 MeV; measured polarization. 4He(polarized p, 3He), E=28.88, 29.77, 30.4 MeV; 9Be(polarized p, 3He), E=23.06 MeV; 11B(polarized p, 3He), E=22-23 MeV; measured A(θ). Natural, enriched targets.
doi: 10.1016/0375-9474(83)90116-1
1983RO21 Nucl.Phys. A411, 1 (1983) R.Roy, C.R.Lamontagne, R.J.Slobodrian, J.Arvieux, J.Birchall, H.E.Conzett Diffusion des Protons Polarises sur 24Mg, 27Al et 32S et Anomalies dans la Region des Resonances Geantes de l'25Al, du 28Si et du 33Cl NUCLEAR REACTIONS 24Mg, 27Al, 32S(polarized p, p), E=13-27 MeV; measured σ(θ), A(θ); deduced optical model parameters. Phase-shift analysis. Natural, enriched targets.
doi: 10.1016/0375-9474(83)90504-3
1982AB04 Can.J.Phys. 60, 1595 (1982) M.S.Abdel-Wahab, L.Potvin, R.Roy, P.Bricault, R.Larue, D.Pouliot, C.Rioux, R.J.Slobodrian Spin-Orbit Effects in Optical Model Analyses of 3He Elastic Scattering on Oxygen Isotopes NUCLEAR REACTIONS 16,17,18O(3He, 3He), E=14 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1139/p82-214
1982SL01 Z.Phys. A308, 15 (1982) The 4He(α, p)7Li, 7Li(0.478) Reaction near Threshold NUCLEAR REACTIONS, ICPND 4He(α, p), E=37-43 MeV; measured σ(θ) vs E, reaction σ, σ(Ep).
doi: 10.1007/BF01415844
1981SL01 J.Phys.(Paris) 42, 13 (1981) R.J.Slobodrian, S.S.Dasgupta, C.Rioux, F.Lahlou, R.Roy Deviations par Rapport a L'espace des Phases et Forces dans les Reactions p + d → p + p + n et d + p → p + p + n tres pres du Seuil NUCLEAR REACTIONS 1H(d, 2p), E=3.82, 4.02, 4.49, 5 MeV; measured σ(θp1, θp2, E); deduced three-body force effects. Gas target.
doi: 10.1051/jphys:0198100420101300
1981SL02 Phys.Lett. 101B, 1 (1981) Limited Success of Coulomb Corrected Faddeev Calculations of the p+d → p+p+n Spectra at very Low Energies NUCLEAR REACTIONS 2H(p, 2p), E=4.5, 7.405 MeV; analyzed σ(θp1, θp2, Ep2); deduced role of three body forces, charge exchange processes. Faddeev calculations, Coulomb effects.
doi: 10.1016/0370-2693(81)90476-7
1981SL03 Phys.Rev.Lett. 47, 1803 (1981) R.J.Slobodrian, C.Rioux, R.Roy, H.E.Conzett, P.von Rossen, F.Hinterberger Evidence of Time-Symmetry Violation in the Interaction of Nuclear Particles NUCLEAR REACTIONS 7Li, 9Be(3He, p), E=14 MeV; measured P(θ); deduced time-reversal invariance.
doi: 10.1103/PhysRevLett.47.1803
1980DA05 Phys.Lett. 91B, 32 (1980) S.S.Dasgupta, R.Roy, C.Rioux, F.Lahlou, R.J.Slobodrian The Reaction 2H(α, αp)n Near Threshold and Excited States of 6Li NUCLEAR REACTIONS 2H(α, pα), E=9.22-11.3 MeV; measured σ; deduced final-state interactions, three-body correlations. 6Li resonance deduced contribution. Kinematically complete experiment.
doi: 10.1016/0370-2693(80)90655-3
1980DA17 Phys.Rev. C22, 1815 (1980); Erratum Phys.Rev. C25, 1073 (1982) S.S.Dasgupta, R.J.Slobodrian, R.Roy, C.Rioux, F.Lahlou 2H(α, pα)n Reaction between 9.735 and 11.30 MeV NUCLEAR REACTIONS 2H(α, pα), E=9.735-11.3 MeV; measured σ(Ep, θp, θα). Gas target.
doi: 10.1103/PhysRevC.22.1815
1980LA08 Z.Phys. A295, 55 (1980) C.R.Lamontagne, B.Frois, R.J.Slobodrian, H.E.Conzett, C.Leemann The p-Si Elastic Scattering in the Region of Giant Multipole Resonances NUCLEAR REACTIONS 28Si(polarized p, p), E=17-29 MeV; measured σ(θ), A(θ); deduced optical model parameters.
doi: 10.1007/BF01414298
1980LA19 J.Phys.(Paris) 41, 485 (1980) F.Lahlou, R.J.Slobodrian, P.Bricault, S.S.Dasgupta, R.Roy, C.Rioux Variation des Dephasages de la Diffusion p-d pres du Seuil de Cassure du Deuton NUCLEAR REACTIONS 2H(p, p), E=3.14-3.74 MeV; measured σ(θ). Phase shift analysis.
doi: 10.1051/jphys:01980004106048500
1980SL02 Phys.Lett. B94, 9 (1980) Threshold and Coulomb Effects in p-d Bremsstrahlung NUCLEAR REACTIONS 1H(d, d), E=6.3-7.1 MeV; analyzed bremsstrahlung σ(E); deduced threshold, Coulomb effects.
doi: 10.1016/0370-2693(80)90812-6
1979PI11 Nuovo Cim. 52A, 387 (1979) The Search for High-Energy Deuterons in the 3He + 3He Reaction NUCLEAR REACTIONS 3He(3He, dα), E=11.5 MeV; measured production σ; discussed reaction mechanism, ν-production in sun.
doi: 10.1007/BF02770906
1979SL01 Nucl.Instrum.Methods 159, 413 (1979) R.J.Slobodrian, M.Irshad, R.Labrie, C.Rioux, R.Roy, R.Pigeon Facility for the Measurement of Proton Polarization in Nuclear Reactions NUCLEAR REACTIONS 14N(3He, p), E=9.6 MeV; measured σ(θ), P(θ).
doi: 10.1016/0029-554X(79)90669-4
1979SL02 Z.Phys. A291, 261 (1979) R.J.Slobodrian, R.Roy, C.Rioux, R.Pigeon, S.S.Dasgupta Proton Polarization in the 14N(3He, p)16O Reaction Near 10 MeV and Reaction Mechanisms NUCLEAR REACTIONS 14N(3He, p), E=9.8 MeV; measured P(E, θ), σ(E, θ). DWBA d-transfer analysis; deduced reaction mechanism.
doi: 10.1007/BF01409192
1978SL01 Phys.Lett. 78B, 55 (1978) R.J.Slobodrian, R.Roy, C.Rioux, B.Frois Anomaly in the p-d Bremsstrahlung Near the Break-up Threshold NUCLEAR REACTIONS 1H(d, pγ), E=6.3-7.1 MeV; measured bremsstrahlung spectrum, σ(E).
doi: 10.1016/0370-2693(78)90346-5
1978SL02 Phys.Lett. 78B, 539 (1978) α + α Scattering Phase Shifts and Values of the Reaction Cross Section Near Threshold of the 7Li + p and 7Be + n Channels NUCLEAR REACTIONS 7Li(p, X), 7Be(n, X); calculated σ.
doi: 10.1016/0370-2693(78)90634-2
1977AS04 Phys.Rev. C16, 1762 (1977) J.Asai, C.Rioux, M.Irshad, R.Pigeon, R.J.Slobodrian Deuteron Transfer and p-8Be Optical Model Parameters in the 6Li(3He, p)8Be Reaction NUCLEAR REACTIONS 6Li(3He, p), E=14 MeV; calculated polarization, σ.
doi: 10.1103/PhysRevC.16.1762
1977GO16 Can.J.Phys. 55, 2113 (1977) G.Goulard, R.Roy, R.J.Slobodrian Reactopms 3He + 9Be, d + 10B → 3α et Excitation du 12C dans la Region 29-34 MeV NUCLEAR REACTIONS 9Be(3He, 2α), E=9.44, 9.94, 4.4, 4.96, 5.6 MeV; 10B(d, 2α), E=5.3, 5.77, 6.3 MeV; measured αα correlated spectra; deduced reaction mechanism. 12C deduced structure.
doi: 10.1139/p77-254
1977IR01 Nucl.Phys. A286, 483 (1977) M.Irshad, C.Rioux, J.Asai, R.Pigeon, R.J.Slobodrian Proton Polarization and Differential Cross Section for the (3He, p) Reaction on 6Li and 9Be at 14 MeV NUCLEAR REACTIONS 6Li, 9Be(3He, p), E=14 MeV; measured σ(θ), proton polarization. Enriched 6Li target.
doi: 10.1016/0375-9474(77)90597-8
1976AS05 Phys.Lett. 64B, 257 (1976) Deuteron Transfer in the 3He(3He, p)5Li Reaction NUCLEAR REACTIONS 3He(3He, p), E=13.5 MeV; analyzed polarization data; deduced reaction mechanism.
doi: 10.1016/0370-2693(76)90194-5
1976IR02 Nucl.Phys. A265, 349 (1976) M.Irshad, J.Asai, S.Sen, R.Pigeon, R.J.Slobodrian Polarization Effects in (3He, p) Reactions on 3He and 7Li at 14 MeV NUCLEAR REACTIONS 3He, 7Li(3He, p), E=14 MeV; measured σ(θ), proton polarization. Enriched 3He target.
doi: 10.1016/0375-9474(76)90359-6
1976SL02 Phys.Lett. 63B, 5 (1976) α + α Reaction Near Threshold of the 7Li + p and 7Be + n Channels NUCLEAR REACTIONS 7Li(n, X), E=near threshold; calculated σ.
doi: 10.1016/0370-2693(76)90453-6
1976SL05 Nucl.Instrum.Methods 136, 525 (1976) R.J.Slobodrian, B.Frois, J.Birchall, R.Roy New Method for the Measurement of Angular Distributions of Cross Sections and Polarizations NUCLEAR REACTIONS 1H(p, p), E=4.21 MeV; measured simultaneous σ(θ), polarization. Gaseous target.
doi: 10.1016/0029-554X(76)90375-X
1975RO09 Nucl.Phys. A245, 87 (1975) R.Roy, J.Birchall, B.Frois, U.Von Moellendorff, C.R.Lamontagne, R.J.Slobodrian Final State Interaction and Direct Features of the 9Be(τ, α)αα and 10B(d, α)αα Reactions NUCLEAR REACTIONS 9Be(3He, α), 10B(d, α), E=2.9-10 MeV; measured σ(E, Eα, θ), αα-coin, αα(θ, t). DWBA analysis, natural, enriched targets.
doi: 10.1016/0375-9474(75)90083-4
1975SL01 Phys.Rev.Lett. 35, 19 (1975) R.J.Slobodrian, R.Pigeon, M.Irshad Production of High-Energy Deuterons in the 3He + 3He Reaction and the Solar Neutrino Problem NUCLEAR REACTIONS 3He(3He, dα), E=13.6 MeV; measured σ.
doi: 10.1103/PhysRevLett.35.19
1974FR13 Phys.Lett. 53B, 341 (1974) B.Frois, M.Irshad, C.R.Lamontagne, U.Von Moellendorff, R.Pigeon, R.Roy, R.J.Slobodrian Bremsstrahlung in the Proton-Proton Interaction at 6.92 MeV NUCLEAR REACTIONS 1,2H(p, p), E=6.92 MeV bremsstrahlung; measured pp-coin, σ.
doi: 10.1016/0370-2693(74)90397-9
1973DE27 Can.J.Phys. 51, 1293 (1973) R.de Swiniarski, H.E.Conzett, C.R.Lamontagne, B.Frois, R.J.Slobodrian Excitation of the Ground-State Rotational Band in 28Si by Inelastic Scattering of 25.25 MeV Polarized Protons NUCLEAR REACTIONS 28Si(polarized p, p'), E=25.25 MeV; measured σ(θ). Analyzing power. 28Si level deduced β2.
1973FR17 Phys.Rev. C8, 2132 (1973) B.Frois, J.Birchall, C.R.Lamontagne, U.von Moellendorff, R.Roy, R.J.Slobodrian Bremsstrahlung in the α-α and 3He-α Interactions NUCLEAR REACTIONS 4He(α, 2αγ), E=11.4-13.5 MeV; 4He(3He, 3Heαγ), E=7.4, 9.35 MeV; measured σ(Eγ).
doi: 10.1103/PhysRevC.8.2132
1973LA23 Phys.Lett. 45B, 465 (1973) C.R.Lamontagne, B.Frois, R.J.Slobodrian, H.E.Conzett, C.Leemann, R.De Swiniarski The Scattering of Polarized Protons from Si in the Giant Resonance Region of 29P NUCLEAR REACTIONS 28Si(p, p), E=17-29 MeV; measured σ(E;θ), A(θ).
doi: 10.1016/0370-2693(73)90645-X
1973RO28 Lett.Nuovo Cim. 6, 374 (1973) R.Roy, J.Birchall, B.Frois, R.J.Slobodrian Production Process Effects in Three-Body Final States; 10B(d, α)αα and 9Be(3He, α)αα NUCLEAR REACTIONS 10B(d, α), 9Be(3He, α), E=2.9-10.0 MeV; measured σ(E;θ).
doi: 10.1007/BF02745775
1972DE46 Nucl.Phys. A194, 577 (1972) M.L.V.L.de Slobodrian, B.Cujec, R.Roy, R.J.Slobodrian The 3He(tau, α)2p Reaction at 9.11, 7.88 and 6.9 MeV NUCLEAR REACTIONS 3He(3He, α)2p, E=6.9, 7.88, 9.11 MeV; measured σ(Ep, Eα, θ); analyzed reaction mechanisms, final-state interactions.
doi: 10.1016/0375-9474(72)91004-4
1972FR02 Phys.Rev.Lett. 28, 633 (1972) B.Frois, J.Birchall, R.Roy, R.J.Slobodrian Bremsstrahlung in α-α Scattering at 9.35 MeV NUCLEAR REACTIONS 4He(α, α'γ), E=9.35 MeV; measured bremsstrahlung σ.
doi: 10.1103/PhysRevLett.28.633
1971RO05 Phys.Lett. 34B, 491 (1971) R.Roy, J.Birchall, R.J.Slobodrian The Width of the 2.9 MeV State in 8Be from the 7Li(d, n)8Be Reaction NUCLEAR REACTIONS 7Li(d, n), E=3.72, 4.76 MeV; measured σ(En). 8Be resonance deduced level-width.
doi: 10.1016/0370-2693(71)90662-9
1970BA41 Nucl.Phys. A153, 409 (1970) A.D.Bacher, R.L.McGrath, J.Cerny, R.de Swiniarski, J.C.Hardy, R.J.Slobodrian The (3He, 6He) Reaction on 6Li and 7Li NUCLEAR REACTIONS 6,7Li(3He, 6He), E=53.2 MeV; measured σ(E(6He)) at θ=14.1°. 4Li deduced no T=2 states. Enriched target.
doi: 10.1016/0375-9474(70)90779-7
1970RO37 Nucl.Instrum.Methods 87, 1 (1970) A proton-recoil spectrometer using solid-state detectors and particle identification NUCLEAR REACTIONS 7Li, 27Al(d, n), E ≈ 4.8 MeV; measured neutron spectra. Proton-recoil spectrometer.
doi: 10.1016/0029-554X(70)90875-X
1969BA29 Phys.Letters 29B, 573 (1969) A.D.Bacher, F.G.Resmini, R.J.Slobodrian, R.De Swiniarski, H.Meiner, W.M.Tivol Observation of the 3He(p, n)3p Reaction at 25 MeV NUCLEAR REACTIONS 3He(p, n)3p, E=25 MeV; measured σ(En).
doi: 10.1016/0370-2693(69)90300-1
1968MC01 Nucl.Phys. A108, 177(1968) J.S.C.McKee, A.U.Luccio, R.J.Slobodrian, W.F.Tivol Small-Angle Behaviour of the Polarization in p-d Elastic Scattering NUCLEAR REACTIONS 2H(p, p), E = 11.6 MeV; measured polarization (E, θ). Enriched 2H target.
doi: 10.1016/0375-9474(68)90152-8
1968SL02 Phys.Rev. 174, 1122 (1968) R.J.Slobodrian, H.E.Conzett, E.Shield, W.F.Tivol Proton-proton elastic scattering between 6 and 10 MeV NUCLEAR REACTIONS 1H(p, p), E=6.1-9.9 MeV; measured products, Eπ, Iπ; deduced σ(θ). Data were imported from EXFOR entry A1212.
doi: 10.1103/PhysRev.174.1122
1968TO01 Nucl.Phys. A111, 236(1968) The 3He(3He, T)3P Reaction at 44 MeV NUCLEAR REACTIONS 3He(3He, t)3p, E=44 MeV; measured σ(Et, θ); deduced no evidence for narrow 3p interaction.
doi: 10.1016/S0375-9474(68)91084-1
1967MC04 Phys.Letters 24B, 240 (1967) J.S.C.McKee, D.J.Clark, R.J.Slobodrian, W.F.Tivol Scattering of Polarized Protons by Deuterium in the Energy Region 10 to 20 MeV NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90474-1
1967SL01 Phys.Letters 25B, 19 (1967) R.J.Slobodrian, J.S.C.McKee, W.F.Tivol, D.J.Clark, T.A.Tombrello The 2p final-State Interaction in the 3He(3He, α)2p reaction NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0370-2693(67)90062-7
1967SL02 Phys.Rev.Letters 19, 704 (1967) R.J.Slobodrian, J.S.C.McKee, H.Bichsel, W.F.Tivol High-Precision Measurement of Proton-Proton Polarization Between 10 and 20 MeV NUCLEAR STRUCTURE 1H; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.19.704
1967SL03 Nucl.Phys. A101, 109 (1967) R.J.Slobodrian, J.S.C.McKee, D.J.Clark, W.F.Tivol, T.A.Tombrello A Search for Excited States of 3He NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(67)90290-4
1967SL04 Phys.Rev.Letters 19, 595 (1967) R.J.Slobodrian, H.Bichsel, J.S.C.McKee, W.F.Tivol High-Resolution Fast-Neutron Spectroscopy of the Reaction 9Be(p, n)9B at 20 MeV NUCLEAR STRUCTURE 9Be, 9B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRevLett.19.595
1964BI06 Nucl. Phys. 50, 585 (1964) The H3(d, p)He4 and He3(d, d)He3 Reactions at 23.2 to 27.0 MeV NUCLEAR STRUCTURE 3H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90230-5
1964CO20 Phys. Letters 11, 68 (1964) H.E.Conzett, H.S.Goldberg, E.Shield, R.J.Slobodrian, S.Yamabe Polarization of 40 MeV Protons Elastically Scattered from Deuterons NUCLEAR STRUCTURE 2H; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(64)90262-8
1964CO27 Bull. Am. Phys. Soc. 9, No. 7, 704, B5 (1964) H.E.Conzett, E.Shield, R.J.Slobodrian, S.Yamabe Complex Phase-Shift Analysis of the Elastic α-α Scattering Near 40 MeV NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1964SH19 Bull.Am.Phys.Soc. 9, No.7, 703, B4 (1964) E.Shield, H.E.Conzett, P.Darriulat, H.Pugh, R.J.Slobodrian Excitation Functions for α-He4 Scattering NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
1963BI01 Bull.Am.Phys.Soc. 8, No.1, 37, J7 (1963) He3(d, p)He4 and He3(d, d)He3 Reactions at 27 MeV NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
1963BI08 Phys.Letters 4, 209 (1963) Cylindrical Bessel Function Dependence in the Angular Distribution of the He3(d, p)He4 Stripping Reaction at 27 MeV NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90277-4
1963BI14 Phys.Letters 7, 77 (1963) Diproton and the He3(d, t)He2 Reaction NUCLEAR STRUCTURE 3He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0031-9163(63)90450-5
1963ER02 Nucl.Phys. 49, 65 (1963) Scattering and Stripping of Deuterons on He4 between 21 and 28 MeV NUCLEAR STRUCTURE 4He; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90074-9
1962ER03 Nuclear Phys. 34, 532 (1962) Scattering and Stripping of 27.0 MeV Deuterons on Nitrogen NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90002-0
1962SL02 Phys.Rev. 125, 1003 (1962) Elastic and Inelastic Scattering of 28-MeV Deuterons NUCLEAR STRUCTURE 12C, 2H, Li, 27Al; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.125.1003
1962SL03 Nuclear Phys. 32, 684 (1962) Scattering of 27.7 MeV Deuterons on Beryllium and Boron NUCLEAR STRUCTURE 11B, 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90370-X
1962SL04 Phys.Rev. 126, 1059 (1962) Stripping with 28-MeV Deuterons NUCLEAR STRUCTURE 10B, 12C, 7Li, 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.126.1059
1961SL06 Bol.Acad.Nac.Cienc.(Cordoba, Rep.Arg.) 42, 75 (1961); Phys.Abstr. 67, 1989, Abstr.22164 (1964) Scattering of 28.1 MeV Deuterons by Lithium NUCLEAR STRUCTURE 7Li, 6Li; measured not abstracted; deduced nuclear properties.
1961SL09 NP-10974 (1961); Nuclear Sci.Abstr. 16, 295, Abstr.2487 (1962) Dispersion de Deuterones de 28, 1 MeV Por Hidrogeno, Litio, Carbono y Aluminio. Informe No.54
1960CO04 Phys.Rev. 117, 1075 (1960) H.E.Conzett, G.Igo, H.C.Shaw, R.J.Slobodrian Alpha-Alpha Scattering in the Range 36.8 to 4.73 MeV NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.117.1075
1959LE37 Phys.Rev. 116, 1229 (1959) Excitation Function for the Al27(d, αp)Na24 Reaction Between 0 and 28.1 MeV NUCLEAR REACTIONS 27Al(d, pα), E=10.9-28.4 MeV; measured products, 24Na, 4He, Eπ, Iπ; deduced σ, σ(E). Data were imported from EXFOR entry P0124.
doi: 10.1103/PhysRev.116.1229
1957CO63 Bull.Am.Phys.Soc. 2, No.6, 305, E11 (1957) H.E.Conzett, G.Igo, H.C.Shaw, R.J.Slobodrian Elastic Scattering of 44.7-MeV Alpha Particles by Helium
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