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NSR database version of April 11, 2024.

Search: Author = A.Nilsson

Found 47 matches.

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
Citations: PlumX Metrics


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1822.


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2158.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1974NI01      Phys.Scr. 9, 83 (1974)

A.Nilsson, Z.P.Sawa

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1973NI04      Nucl.Phys. A212, 448 (1973)

A.Nilsson, M.Grecescu

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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1962KJ02      Arkiv Fysik 20, 507 (1962)

J.Kjellman, A.Nilsson

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)

J.Kjellman, A.Nilsson

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)

A.Nilsson, J.Kjellman

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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0414.


1962NI04      Arkiv Fysik 21, 551 (1962)

A.Nilsson, J.Kjellman

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)

A.Nilsson, J.Kjellman

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)

A.Nilsson

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)

A.Nilsson

Angular Distribution Measurements on the Reaction Li7(p, n)Be7

NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.


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