NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Nilsson Found 47 matches. 1995RO06 J.Phys.(London) G21, L1 (1995) H.A.Roth, S.E.Arnell, J.Blomqvist, D.Foltescu, T.Kuroyanagi, S.Mitarai, A.Nilsson, J.Nyberg, O.Skeppstedt First Observation of the Neutron-Deficient Nucleus 93Rh NUCLEAR REACTIONS 58Ni(40Ca, 2n3p), E=187 MeV; measured Eγ, Iγ, (particle)γ-, γγ-coin. 93Rh deduced high-spin levels, J, π. Enriched target, Ge detector array, particle-multiplicity filter.
doi: 10.1088/0954-3899/21/2/001
1994AR33 Phys.Rev. C49, 51 (1994) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, J.Blomqvist, A.Nilsson, T.Kuroyanagi, S.Mitarai, J.Nyberg Yrast Level Structure of the Neutron Deficient N = 49 Isotones 92Tc, 93Ru, 94Rh, and 95Pd up to High Angular Momentum NUCLEAR REACTIONS 58Ni(40Ca, X), E=180 MeV; measured γγ-coin, Eγ, Iγ. 92Tc, 93Ru, 94Rh, 95Pd deduced high-spin levels, J, π, band structure, configuration.
doi: 10.1103/PhysRevC.49.51
1994RO08 Phys.Rev. C50, 1330 (1994) H.A.Roth, S.E.Arnell, D.Foltescu, O.Skeppstedt, J.Blomqvist, A.Nilsson, T.Kuroyanagi, S.Mitarai, J.Nyberg Gaps in the Yrast Level Structure of the N = 50 Isotones 93Tc, 94Ru, and 95Rh at High Angular Momentum NUCLEAR REACTIONS 58Ni(40Ca, X), E=180 MeV; measured Eγ, Iγ, γ(θ). 93Tc, 94Ru, 95Rh deduced high-spin levels, J, π, T1/2. Multidetector array NORDBALL including particle selection. Shell model comparison.
doi: 10.1103/PhysRevC.50.1330
1993AR01 Phys.Scr. 47, 142 (1993) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg High-Spin States of the Neutron Deficient Isotope 91Tc NUCLEAR REACTIONS 58Ni(40Ca, 3pα), E=180, 187 MeV; measured Eγ, Iγ, γγ-coin, γ anisotropy. 91Tc deduced levels, J, π. Shell model comparison.
doi: 10.1088/0031-8949/47/2/003
1993AR02 Phys.Scr. 47, 355 (1993) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg First Information About the Level Structure of 91Ru NUCLEAR REACTIONS 58Ni(40Ca, n2pα), E=187 MeV; measured γγ-coin, Iγ(θ), Eγ, Iγ. 91Ru deduced levels, J, π, configuration. Shell model.
doi: 10.1088/0031-8949/47/3/005
1993AR07 Nucl.Phys. A557, 477c (1993) S.E.Arnell, D.Foltescu, T.Kuroyanagi, S.Mitarai, A.Nilsson, H.A.Roth, O.Skeppstedt In-Beam Gamma Ray Study of Neutron Deficient Nuclei with A ≈ 90 NUCLEAR REACTIONS 58Ni(40Ca, X), E=147-187 MeV; measured γ spectra. 91Tc, 92Ru deduced levels. Shell model. In-beam study. NUCLEAR STRUCTURE 90Mo, 91Tc, 92Ru; calculated levels. Shell model.
doi: 10.1016/0375-9474(93)90564-E
1993AR08 Z.Phys. A346, 111 (1993) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg The Level Structure of 92Ru Up to High Spin Values NUCLEAR REACTIONS 58Ni(40Ca, 2pα), E=147, 187 MeV; measured Eγ, Iγ, γγ-coin, γ(θ). 92Ru deduced levels, J, π. Shell model.
doi: 10.1007/BF01294626
1992AR15 Phys.Scr. 46, 389 (1992) S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt, A.Nilsson, S.Mitarai, J.Nyberg Nuclear Structure of the Neutron Deficient Isotope 90Mo NUCLEAR REACTIONS 58Ni(40Ca, 4pα), E=180, 187 MeV; measured γγ-coin, γ-anisotropy, Iγ, Eγ. 90Mo deduced levels, possible J, π.
doi: 10.1088/0031-8949/46/5/002
1992DE30 Z.Phys. A343, 121 (1992) G.de Angelis, D.Bazzacco, S.Lunardi, M.A.Cardona, M.De Poli, Y.X.Guo, D.Ackermann, S.E.Arnell, A.Atac, S.Beghini, L.Corradi, A.D'Onofrio, D.Foltescu, E.Ideguchi, A.Nilsson, S.Mitarai, G.Montagnoli, H.Moreno, D.R.Napoli, V.Roca, H.A.Roth, F.Scarlassara, G.F.Segato, C.Signorini, O.Skeppstedt, P.Spolaore, A.M.Stefanini, F.Terrasi Identification of the N = 79 147Er Nucleus Through γ-Recoil Coincidences NUCLEAR REACTIONS 92Mo(58Ni, n2p), E=260 MeV; measured γ(recoil)-, γγ-coin. 147Er deduced levels, J, π, band structure.
doi: 10.1007/BF01291605
1988AR09 Z.Phys. A330, 69 (1988) S.E.Arnell, S.Mattsson, H.A.Roth, M.Rydehell, O.Skeppstedt, J.Nyberg, A.Johnson, A.Kerek, A.Nilsson, L.Westerberg Non-Equilibrium Neutron Emission in α-Induced Reactions on 124Sn NUCLEAR REACTIONS, ICPND 124Sn(α, 2n), (α, 3n), (α, 4n), (α, 5n), E=35-57 MeV; measured σ(E), γ-multiplicities vs E, γn-coin.
1988KR04 Z.Phys. A329, 235 (1988) A.Kreissl, A.D.Hancock, H.Koch, Th.Kohler, H.Poth, U.Raich, D.Rohmann, A.Wolf, L.Tauscher, A.Nilsson, M.Suffert, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, H.Plendl, G.Schmidt, J.J.Reidy First Direct Observation of Strong Interaction Spin-Orbit Effects in Antiprotonic Atoms ATOMIC PHYSICS 174Yb, 138Ba(p-bar, X), E not given; measured X-ray spectra; deduced strong interaction spin-orbit effects, energy shifts, widths.
1988SC13 Nucl.Phys. A486, 43 (1988) R.Schwengner, J.Doring, L.Funke, H.Rotter, G.Winter, A.Johnson, A.Nilsson High-Spin States and Band Structures in 79Br NUCLEAR REACTIONS 77Se(α, np), E=27 MeV; measured E(γ), I(γ), σ(E, E(γ), θ), γγ-, pγ-coin, DSA, recoil distance Doppler shift. 78Se(α, 2np), E=45 MeV; measured E(γ), I(γ), σ(E, E(γ), θ), γγ-coin, linear polarization, DSA. 79Br deduced levels, J, π, T1/2, B(λ). Enriched targets, Ge, Si detectors.
doi: 10.1016/0375-9474(88)90038-3
1988WI01 J.Phys.(London) G14, L13 (1988) G.Winter, J.Doring, L.Funke, H.Prade, H.Rotter, R.Schwengner, A.Johnson, A.Nilsson Transition Probabilities in the Band Crossing Region of 79Kr NUCLEAR REACTIONS 78Se(α, 3n), E=45 MeV; 77Se(α, 2n), E=27 MeV; measured Eγ, Iγ, γγ-coin. 79Kr deduced levels, J, π, T1/2, B(λ). In-beam γ-ray spectroscopy.
doi: 10.1088/0305-4616/14/1/003
1987AR19 Phys.Scr. 36, 214 (1987) S.E.Arnell, S.Mattsson, H.A.Roth, M.Rydehell, O.Skeppstedt, A.Johnson, J.Nyberg, A.Kerek, A.Nilsson Interpretation of the Residue Mass Distribution from 12C + 64Zn Collisions at E(12C) = 118 MeV NUCLEAR REACTIONS 64Zn(12C, X), E=118 MeV; measured (particle)γ-coin, ejectile spectra, γ multiplicities; deduced relative residue yield for X=Co-As.
doi: 10.1088/0031-8949/36/2/004
1987PO05 Nucl.Phys. A466, 667 (1987) H.Poth, H.Barth, G.Buche, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, U.Raich, D.Rohmann, A.Wolf, L.Tauscher, A.Nilsson, M.Suffert, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, H.S.Plendl, G.Schmidt, J.J.Reidy Measurement of Strong-Interaction Effects in Light Antiprotonic Atoms ATOMIC PHYSICS 6,7Li, 14N, 19F, 23Na(p-bar, X), E at 300 MeV/c; measured X-ray spectra. 7,6Li, 14N, 19F, 23Na deduced antiprotonic strong interaction level shifts, widths.
doi: 10.1016/0375-9474(87)90462-3
1986KA08 Phys.Rev.Lett. 56, 2368 (1986) W.Kanert, F.J.Hartmann, H.Daniel, E.Moser, G.Schmidt, T.von Egidy, J.J.Reidy, M.Nicholas, M.Leon, H.Poth, G.Buche, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, U.Raich, D.Rohmann, M.Chardalas, S.Dedoussis, M.Suffert, A.Nilsson First Observation of the E2 Nuclear-Resonance Effect in Antiprotonic Atoms ATOMIC PHYSICS 92,94,95,98,100Mo(p-bar, X), E at 200, 300 MeV/c; measured antiprotonic X-ray spectra; deduced strong interaction widths, shifts, effective (p-bar)-nucleon scattering length, E2 nuclear resonance effect.
doi: 10.1103/PhysRevLett.56.2368
1986KO22 Phys.Lett. 176B, 327 (1986) Th.Kohler, P.Blum, G.Buche, A.D.Hancock, H.Koch, A.Kreissl, H.Poth, U.Raich, D.Rohmann, G.Backenstoss, Ch.Findeisen, J.Repond, L.Tauscher, A.Nilsson, S.Carius, M.Suffert, S.Charalambus, M.Chardalas, S.Dedoussis, H.Daniel, T.von Egidy, F.J.Hartmann, W.Kanert, G.Schmidt, J.J.Reidy, M.Nicholas, A.Wolf Precision Measurement of Strong Interaction Isotope Effects in Antiprotonic 16O, 17O, and 18O Atoms NUCLEAR REACTIONS 16,17,18O(p-bar, X), E=low; measured antiprotonic X-rays. ATOMIC PHYSICS 16,17,18O(p-bar, X), E=low; measured antiprotonic X-rays; deduced strong interaction shifts, widths.
doi: 10.1016/0370-2693(86)90173-5
1986RO23 Z.Phys. A325, 261 (1986) D.Rohmann, H.Barth, A.D.Hancock, H.Koch, Th.Kohler, A.Kreissl, H.Poth, U.Raich, A.Wolf, L.Tauscher, M.Suffert, M.Chardalas, S.Dedoussis, A.Nilsson, W.Kanert, T.von Egidy, F.J.Hartmann, G.Schmidt, J.J.Reidy Measurement of the 4f Strong Interaction Level Width in Light Antiprotonic Atoms NUCLEAR REACTIONS 14N, 16,17,18O, 19F, 23Na(p-bar, X), E=200, 300 MeV/c; measured antiprotomic X-ray spectra; deduced target atomic 4f level Γ; calculated antiprotonic transition intensities. Scintillation counters. Cascade model. ATOMIC PHYSICS 14N, 16,17,18O, 19F, 23Na(p-bar, X), E=200, 300 MeV/c; measured antiprotonic X-ray spectra. 14N, 16,17,18O, 19F, 23Na deduced 4f level Γ; calculated antiprotonic transition intensities. Scintillator counters. Cascade model.
1985BL16 Z.Phys. A322, 169 (1985) J.Blomqvist, S.A.Hjorth, A.Johnson, A.Kerek, W.Klamra, A.Nilsson, J.Nyberg, S.E.Arnell, S.Mattsson, H.Roth, O.Skeppstedt In-Beam γ-Ray Spectroscopy on 56Ni NUCLEAR REACTIONS 54Fe(α, 2n), E=35 MeV; measured γγ-coin. 56Ni deduced levels, J, π, configurations, yrast band. Shell model. NUCLEAR STRUCTURE 56Ni; calculated levels. Shell model.
doi: 10.1007/BF01412031
1984GU06 Phys.Lett. 137B, 323 (1984) R.Guigas, P.Blum, H.Koch, M.Meyer, H.Poth, U.Raich, B.Richter, G.Backenstoss, P.Pavlopoulos, L.Tauscher, L.Adiels, K.Fransson, A.Nilsson, M.Suffert, K.Zioutas Strong Interaction Effects in Antiprotonic 6Li/7Li Atoms ATOMIC PHYSICS 6,7Li(p-bar, X), E at 600 MeV/c; measured E X-ray, I X-ray; deduced strong interaction shifts, widths. NUCLEAR REACTIONS 6,7Li(p-bar, X), E at 600 MeV/c; measured E X-ray, I X-ray; deduced strong interaction effects. Optical model comparison.
doi: 10.1016/0370-2693(84)91725-8
1983AR16 J.Phys.(London) G9, 1217 (1983) S.E.Arnell, C.Ekstrom, L.P.Ekstrom, A.Nilsson, I.Ragnarsson, P.J.Smith, E.Wallander Band Structure in 81Sr NUCLEAR REACTIONS 78Kr(α, nγ), E=14-18 MeV; 80Kr(α, 3nγ), E=45 MeV; measured Eγ, Iγ, γ(θ), linear polarization, DSA, γγ-coin. 81Sr deduced levels, J, π, δ, T1/2, γ-branching, B(λ), band structure. Particle-rotor model. Enriched solid, gas targets, Ge(Li) detectors.
doi: 10.1088/0305-4616/9/10/010
1981EK01 J.Phys.(London) G7, 85 (1981) L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, A.Nilsson, V.Paar, P.J.Twin, R.Wadsworth, E.Wallander, N.J.Ward Gamma-Ray Spectroscopy on 87Sr and the Energy-B(E2) Rule NUCLEAR REACTIONS 84Kr(α, nγ), E=11-17 MeV; measured γ(θ), γγ-coin, linear polarizations, DSA, σ(Eγ). 87Sr deduced levels, J, π, δ, T1/2, B(λ). Enriched target, Ge(Li) detectors. Generalized vibrator model.
doi: 10.1088/0305-4616/7/1/013
1981WA10 Nucl.Phys. A361, 387 (1981) E.Wallander, A.Nilsson, L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, H.G.Price, P.J.Twin, R.Wadsworth, N.J.Ward States in 89Sr Excited by the 86Kr(α, n)89Sr Reaction NUCLEAR REACTIONS 86Kr(α, nγ), E=12-16 MeV; measured Eγ, Iγ(E), Iγ(θγ), γγ-coin, linear polarization, DSA. 89Sr deduced levels, J, π, δ, T1/2, B(λ). Enriched solid 86Kr targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(81)90641-2
1980AR02 Nucl.Phys. A334, 71 (1980) S.E.Arnell, S.Sjoberg, O.Skeppstedt, E.Wallander, A.Nilsson, G.Finnas High Spin States of 83Sr NUCLEAR REACTIONS 80Kr(α, n), E=16-21 MeV; 82Kr(α, 3n), E=45 MeV; measured Eγ, Iγ(E, θγ), γγ-coin. 83Sr deduced levels, J, π. Enriched targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(80)90140-2
1980EK03 J.Phys.(London) G6, 1415 (1980) L.P.Ekstrom, G.D.Jones, F.Kearns, T.P.Morrison, A.Nilsson, P.J.Twin, R.Wadsworth, E.Wallander, N.J.Ward Lifetime and Linear Polarization Measurements with the 80Kr(α, nγ)83Sr and 82Kr(α, nγ)85Sr Reactions NUCLEAR REACTIONS 80Kr(α, nγ), 82Kr(α, 2nγ), 82Kr(α, nγ), E=14, 18 MeV; measured γ(θ), linear polarizations, DSA. 83,84,85Sr levels deduced J, π, δ, T1/2, transitions rates. Enriched solid 80,82Kr targets, Ge(Li)detectors.
doi: 10.1088/0305-4616/6/11/013
1978AR19 Z.Phys. A289, 89 (1978) S.E.Arnell, S.Sjoberg, O.Skeppstedt, E.Wallander, A.Nilsson, Z.P.Sawa, G.Finnas A Study of 87Zr by (α, xn) Reactions NUCLEAR REACTIONS 84Sr(α, nγ), (α, pγ), E=18, 21 MeV; 86Sr(α, 3nγ), (α, 2npγ), E=45, 51 MeV; measured Eγ, Iγ, γγ-coin, pγ-coin, DSA. 87Zr deduced levels, T1/2, J, π, δ, B(λ). Compared with core-cluster coupling model. 87Y levels deduced γ-branching.
doi: 10.1007/BF01408500
1978PO02 Nucl.Phys. A294, 435 (1978) H.Poth, G.Backenstoss, I.Bergstrom, P.Blum, J.Egger, W.Fetscher, R.Guigas, R.Hagelberg, N.Hassler, C.J.Herrlander, M.Izycki, H.Koch, A.Nilsson, P.Pavlopoulos, H.P.Povel, K.Rolli, I.Sick, L.Simons, A.Schwitter, J.Sztarkier, L.Tauscher Study on Antiprotonic Atoms of Light Nuclei and Isotopes ATOMIC PHYSICS N, 16,18O, S; measured antiprotonic X-rays; deduced strong interaction effects, chemical effects.
doi: 10.1016/0375-9474(78)90229-4
1977AR04 Nucl.Phys. A280, 72 (1977) S.E.Arnell, S.Sjoberg, O.Skeppstedt, E.Wallander, A.Nilsson, G.Finnas High-Spin States of 85Sr NUCLEAR REACTIONS 82Kr(α, n), E=14-21 MeV; 84Kr(α, 3n), E=35-45 MeV; measured Eγ, Iγ(Eα, θ(γ)), γγ-coin, Doppler shift attenuation. 85Sr deduced levels, J, π, T1/2, δ. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(77)90294-9
1975AR06 Nucl.Phys. A241, 109 (1975) S.E.Arnell, A.Nilsson, O.Stankiewicz States of High Spin in 87Sr, 88Sr and 89Sr NUCLEAR REACTIONS 86Kr(α, n), (α, 2n), (α, 3n), E=11-40 MeV; 84Kr(α, n), E=10-14 MeV; measured Eγ, Iγ, σ(E, Eγ, θ), γγ-coin, DSA. 87,88,89Sr deduced levels, J, π, T1/2. Enriched targets, Ge(Li) detectors.
doi: 10.1016/0375-9474(75)90367-X
1975FR23 Nucl.Instrum.Methods 131, 511 (1975) K.Fransson, A.Nilsson, J.de Raedt, L.Tauscher Precise Energy Determination of the First Excited State in 137Cs for Absolute Energy Calibration in Muonic Atoms RADIOACTIVITY 137Xe, 138Cs; measured Eγ. 137Cs, 138Ba deduced transition energies.
doi: 10.1016/0029-554X(75)90442-5
1974FO12 Phys.Scr. 10, 51 (1974) K.Forssten, A.Hasselgren, P.Monseu, A.Nilsson, Z.P.Sawa On Positive Parity Levels of High Angular Momentum in 69,71,73Ge NUCLEAR REACTIONS 66,68,70Zn(α, nγ), E=10, 12, 14.2 MeV; measured σ(Eγ, θ), γγ-coin, Pγ. 69,71,73Ge deduced levels, J, π, γ-mixing.
doi: 10.1088/0031-8949/10/1-2/004
1974NI01 Phys.Scr. 9, 83 (1974) On 1f2p Nuclei. Gamma Ray Spectroscopy on States in 65Zn and 67Zn Using 62,64Ni(α, n) Reactions NUCLEAR REACTIONS 62,64Ni(α, nγ), E < 14 MeV; Cu(α, np), E=24, 31 MeV; measured σ(Eα;Eγ, θ), linear polarized(γ), γγ-coin. 65,67Zn deduced levels, J, π, γ-mixing.
doi: 10.1088/0031-8949/9/2/004
1973GR31 Nucl.Phys. A212, 429 (1973) M.Grecescu, A.Nilsson, L.Harms-Ringdahl High-Spin States in the N = 50 Isotones 91Nb and 93Tc Populated in (α, p2nγ) Reactions NUCLEAR REACTIONS 90Zr, 92Mo(α, p2nγ), Eα=37-43 MeV; measured Eγ, Iγ(Eα, θ), αγ-delay, pγ-coin, γγ-coin. 91Nb, 93Tc deduced levels, J, π, T1/2, γ-mixing. Enriched targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(73)90816-6
1973NI04 Nucl.Phys. A212, 448 (1973) High-Spin States in the Isotones 89Zr, 91Mo and 93Ru Populated in α-Particle-Induced Reactions NUCLEAR REACTIONS 90Zr, 92Mo(α, 3nγ), (α, α'nγ), Eα=37-43 MeV; measured Eγ, Iγ, σ(Eα; Eγ, θ), αγ-delay, γγ-coin. 88Sr(α, 3nγ), Eα=41 MeV; measured Eγ, Iγ. 89Zr, 91Mo, 93Ru deduced levels, J, π, T1/2. Enriched targets. Ge(Li) detectors.
doi: 10.1016/0375-9474(73)90817-8
1972ME03 Nucl.Phys. A181, 566 (1972) L.Mesko, A.Nilsson, S.A.Hjorth, M.Brenner, O.Holmlund High-Spin Levels in 95Mo and 97Mo from (α, xn) Reactions NUCLEAR REACTIONS 92,94Zr(α, n), Eα=14 MeV; 94Zr(α, 3n), Eα=35 MeV; measured Eγ, Iγ(θ), polarization, α-γdelay, γγ-coin. 95,97Mo deduced levels, J, π, mixing ratios. Enriched targets.
doi: 10.1016/0375-9474(72)90501-5
1971BR54 Comment.Phys.-Math. 41, 367 (1971) M.Brenner, K.Forssten, O.Holmlund, P.-E.Hagg, P.Lindblom, E.Still, A.Nilsson, S.A.Hjorth An Isomeric (g9/2)2 Proton State in 94Mo RADIOACTIVITY 94Tc; measured Xγ-delay; deduced log ft. 94Tc deduced J, π. 94mMo levels deduced configurations.
1970NI08 Phys.Scr. 1, 161 (1970) L.Nilsson, A.Nilsson, I.Bergqvist The Decay of Bound Isobaric Analogue States in 28Si and 32S Using (d, nγ) Reactions NUCLEAR REACTIONS 27Al, 31P(d, nγ), E=4.0 MeV; measured σ(En, Eγ), Eγ, Iγ. 28Si, 32S deduced levels, J, π, isobaric analogs.
doi: 10.1088/0031-8949/1/4/003
1962KJ02 Arkiv Fysik 20, 507 (1962) Neutron Angular Distributions from the Reaction Be9(α, n)C12 at 14.1 MeV NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1962KJ04 Arkiv Fysik 22, 277 (1962) Neutron Angular Distributions from the Be9(α, n)C12 Reaction at 12.7, 11.3 and 9.8 MeV NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0260. 1962KJ05 Arkiv Fysik 21, 169 (1962) J.Kjellman, A.Nilsson, S.Schwarz Angular Distributions of Neutrons from the Reaction Li7(α, n)B10 at 13.9 and 13.5 MeV NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1962KJ07 Arkiv Fysik 22, 418 (1962) J.Kjellman, A.Nilsson, S.Schwarz Neutron Angular Distributions from the Reaction Li7(α, n)B10 at 13.9 and 13.5 MeV NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1962NI02 Nuclear Phys. 32, 177 (1962) Neutron Angular Distributions from the Be9(α, n)C12 Reaction at 14.1, 13.9 and 13.5 MeV NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90333-4
1962NI04 Arkiv Fysik 21, 551 (1962) A Study of the Reaction C13(α, n)O16 at 14.1, 13.7 and 12.8 MeV NUCLEAR STRUCTURE 13C; measured not abstracted; deduced nuclear properties.
1962NI09 Arkiv Fysik 22, 426 (1962) Neutron Angular Distributions from the Be9(α, n)C12 Reaction at 14.1, 13.9 and 13.5 MeV NUCLEAR STRUCTURE 9Be; measured not abstracted; deduced nuclear properties.
1961KJ01 Proc.Rutherford Jubilee Intern.Conf., Manchester, England, J.B.Birks, Ed., Academic Press Inc., New York, p.605 (1961) J.Kjellman, A.Nilsson, S.Schwarz Angular Distributions of Neutrons from the Reaction Li7(α, n)B10 at 13.5 and 13.9 MeV NUCLEAR STRUCTURE 7Li; measured not abstracted; deduced nuclear properties.
1961NI04 Arkiv Fysik 19, 289 (1961) Angular Distribution of the Neutrons from the Reaction Li7(p, n)Be7 NUCLEAR STRUCTURE 7Be, 7Li; measured not abstracted; deduced nuclear properties.
1960NI01 Arkiv Fysik 16, 512A (1960) Angular Distribution Measurements on the Reaction Li7(p, n)Be7 NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
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