NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = O.M.Bilaniuk Found 29 matches. 1985DE49 Phys.Rev. C32, 1830 (1985) M.P.De Pascale, G.Giordano, G.Matone, D.Babusci, R.Bernabei, O.M.Bilaniuk, L.Casano, S.d'Angelo, M.Mattioli, P.Picozza, D.Prosperi, C.Schaerf, S.Frullani, B.Girolami Polarization Asymmetry in the Photodisintegration of the Deuteron NUCLEAR REACTIONS 2H(polarized γ, p), E=19.8, 29, 38.6, 60.8 MeV; measured photoneutron yield, azimuthal asymmetry factor; deduced polarization dependent, independent σ(θ).
doi: 10.1103/PhysRevC.32.1830
1982BI03 Yad.Fiz. 35, 549 (1982) O.-M.P.Bilanyuk, V.S.Bulkin, L.V.Dubar, O.F.Nemets, L.I.Slyusarenko, V.V.Tokarevsky Total Cross Sections for Interactions of Deuterons and α Particles with Nuclei (A ≈ 50) NUCLEAR REACTIONS, ICPND 45Sc, Ti, 51V, 52,53,54Cr(d, X), E=13.6 MeV; 45Sc, Ti, 51V, 52,53,54Cr(α, X), E=27.2 MeV; measured total reaction σ; deduced isotope-isotone effect, optical model parameters.
1981BI16 J.Phys.(London) G7, 1699 (1981) O.-M.P.Bilaniuk, V.V.Tokarevskii, V.S.Bulkin, L.V.Dubar, O.F.Nemets, L.I.Slyusarenko Deuteron and Alpha-Particle Total Reaction Cross Sections for Nuclei with A ≈ 50 NUCLEAR REACTIONS 45Sc, 48Ti, 51V, 52,53,54Cr(d, d), E=13.6 MeV; 45Sc, 48Ti, 51V, 52,53,54Cr(α, α), E=27.2 MeV; measured σ(θ), total σ(reaction); deduced nuclear density diffuseness parameter relation to isotopic-isotonic effect. Optical model. Transmission charge collection method.
doi: 10.1088/0305-4616/7/12/020
1979FO01 Phys.Rev. C19, 5 (1979) H.T.Fortune, O.M.Bilaniuk, G.Stephans, R.Middleton Mechanism of 14N(t, p) to the Ground State Quadruplet in 16N NUCLEAR REACTIONS 14N(t, p), E=15 MeV; measured σ(θ). 16N levels deduced L, reaction mechanism. DWBA analysis. Comparison with shell model.
doi: 10.1103/PhysRevC.19.5
1978BI10 Nucl.Phys. A305, 63 (1978) O.M.Bilaniuk, H.T.Fortune, R.Middleton Investigation of 16O Excited States via the 14N(3He, p) Reaction NUCLEAR REACTIONS 14N(3He, p), E=15.0 MeV; measured σ(Ep, θ). 16O deduced levels, L, J, π. DWBA analysis, comparison with ZMB wave functions. Gas target.
doi: 10.1016/0375-9474(78)90164-1
1978FO19 J.Phys.(London) G4, L181 (1978) H.T.Fortune, R.Middleton, O.M.Bilaniuk T = 0 Pairing Vibrations in 16O NUCLEAR REACTIONS 14N(3He, p), E=15.0 MeV; measured σ(Ep, θ). 16O deduced levels, L, J, π, configuration. DWBA analysis. Comparison with 16O(3He, p). Gas target.
doi: 10.1088/0305-4616/4/7/006
1978FO27 Phys.Rev. C18, 1920 (1978) H.T.Fortune, R.Middleton, O.M.Bilaniuk Two-Nucleon Transfer to T-Mixed States in 16O NUCLEAR REACTIONS 14N(t, p), 14N(3He, p), E=15.0 MeV; measured σ(Ep, θ); deduced T mixing effect on reaction mechanism.
doi: 10.1103/PhysRevC.18.1920
1977BI04 Phys.Rev. C16, 55 (1977) O.M.Bilaniuk, D.J.Crozier, H.T.Fortune, R.Middleton 34Cl via the 32S(3He, p) Reaction NUCLEAR REACTIONS 32S(3He, p), E=18 MeV; measured σ(Ep, θ). 34Cl deduced levels, L, J, π. H2S gas target.
doi: 10.1103/PhysRevC.16.55
1974DU03 Nucl.Phys. A224, 77 (1974) J.L.Durand, O.M.Bilaniuk, C.Perrin The 2H+p Break-up Reaction Off the Energy Shell at 58.5 MeV NUCLEAR REACTIONS 2H(p, 2p), E=58.5 MeV; measured σ(Ep), pp(θ). Analysis based on the coupled-equation code.
doi: 10.1016/0375-9474(74)90163-8
1973BA01 Phys.Rev. C7, 165 (1973) D.Bachelier, M.Bernas, O.M.Bilaniuk, J.L.Boyard, J.C.Jourdain, P.Radvanyi Quasifree (p, pα) Scattering on 6Li, 24Mg, 28Si, 40Ca, 140Ce, and 232Th at 156 MeV NUCLEAR REACTIONS 6Li, 24Mg, 28Si, 40Ca, 140Ce, 232Th(p, pα), E=156 MeV; measured σ(Ep, Eα, θ(p), θ(α)).
doi: 10.1103/PhysRevC.7.165
1972BI01 Nucl.Phys. A180, 69 (1972) O.M.Bilaniuk, H.T.Fortune, J.D.Garrett, R.Middleton, W.P.Alford The 14N(tau, p)16O(g.s.) Reaction between 7.9 and 18.0 MeV NUCLEAR REACTIONS 14N(3He, p)16O, E=7.9-18.0 MeV; measured σ(E(3He), θ); discussed reaction mechanisms.
doi: 10.1016/0375-9474(72)90156-X
1969BA18 Phys.Rev. 178, 1706 (1969) K.Bahr, T.Becker, O.M.Bilaniuk, R.Jahr Quasifree Knockout of Deuterons in the 6Li(α, αd)4He Reaction at 23.6 MeV NUCLEAR REACTIONS 6Li(α, αd)4He, E=23.6 MeV; measured σ(Ed, Eα, θ(dα)); deduced reaction mechanism.
doi: 10.1103/PhysRev.178.1706
1965FU16 Nucl.Phys. 70, 553 (1965) H.W.Fulbright, W.P.Alford, O.M.Bilaniuk, V.K.Deshpande, J.W.Verba A Comparison of the C12(He3, p) and (He3, n) Reactions Leading to Analogue States in N14 and O14 NUCLEAR REACTIONS 12C(3He, n), (3He, p), E = 6.5-11 MeV; measured σ(E, θ).
doi: 10.1016/0029-5582(65)90454-2
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
1964MA04 Phys.Rev. 133, B350 (1964) S.Mayo, J.Testoni, O.M.Bilaniuk Some (d, α) Reactions on Be9, F19, and Al27 at 27.5 MeV NUCLEAR STRUCTURE 19F, 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.133.B350
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
1963MA24 Phys.Rev. 130, 2373 (1963) Comparison of the C13(d, α)B11 and B11(He3, p)C13 Reactions NUCLEAR STRUCTURE 11B, 13C; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.130.2373
1962AL01 Bull.Am.Phys.Soc. 7, No.1, 60, R8 (1962) W.P.Alford, O.M.Bilaniuk, D.B.Marsh Angular Distributions in B10(He3, p)C12 and C13X(He3, p)N15 Reactions NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
1962BI01 Bull.Am.Phys.Soc. 7, No.1, 71, V1 (1962) N14(He3, p)O16(gd. st.) Excitation Functions and Angular Distributions NUCLEAR STRUCTURE 14N; measured not abstracted; deduced nuclear properties.
1962FU09 NYO-0034 (1962) H.W.Fulbright, W.P.Alford, O.M.Bilaniuk, V.K.Deshpande, J.W.Verba NUCLEAR STRUCTURE 12C; measured not abstracted; deduced nuclear properties.
1962MA08 Bull.Am.Phys.Soc. 7, No.4, 269, CB10 (1962) Comparison of (α, d) and (He3, p) Reactions on B11 NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
1961AL25 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed. Academic Press, New York, p.551 (1961) W.P.Alford, O.M.Bilaniuk, B.B.Marsh Double Pick-Up of Inequivalent Nucleons in C13(d, α)B11 NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
1960BI07 Nuclear Phys. 17, 435 (1960) s-Particle Doublets in Certain Light Nuclei NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(60)90137-1
1960BI08 Phys.Rev. 120, 211 (1960) B10(d, p)B11 Reaction and the Configurations of B11 NUCLEAR STRUCTURE 11B; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.211
1960RI07 Phys.Rev. 120, 527 (1960) L.H.T.Rietjens, O.M.Bilaniuk, M.H.Macfarlane Ti46,48(d, p)Ti47,49 Reactions and the 1f7/2n and 1f7/2n-12p Configurations NUCLEAR STRUCTURE 49Ti, 47Ti; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.120.527
1958BI31 Bull.Am.Phys.Soc. 3, No.3, 188, K8 (1958) Angular Distributions of Protons from B10(d, p)B11
1957BI80 Phys.Rev. 108, 305 (1957) Spin, Parity, and j-j Expansion Coefficients for States of Low Excitation in O18
doi: 10.1103/PhysRev.108.305
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