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NSR database version of April 11, 2024.

Search: Author = S.E.Arnell

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2001RO15      Eur.Phys.J. A 10, 275 (2001)

H.A.Roth, S.E.Arnell, D.Foltescu, O.Skeppstedt, J.Blomqvist, G.de Angelis, D.Bazzacco, S.Lunardi

Yrast Level Structure of the Neutron-Deficient N = 80 Isotones 146Dy, 147Ho and 148Er up to High-Spin Values

NUCLEAR REACTIONS 92Mo(58Ni, 4p), (58Ni, 3p), (58Ni, 2p), E=260 MeV; measured Eγ, Iγ, (charged particle)γ-, (neutron)γ-, γγ-coin. 146Dy, 147Ho, 148Er deduced high-spin levels, J, π, configurations. Comparison with shell model predictions.

doi: 10.1007/s100500170113
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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
Citations: PlumX Metrics


1995SU27      J.Phys.Soc.Jpn. 64, 329 (1995)

M.Sugawara, S.Mitarai, T.Kuroyanagi, J.Mukai, H.Tomura, T.Morikawa, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, N.Gjorup, A.Virtanen, S.-E.Arnell, O.Skeppstedt, H.A.Roth, D.Foltescu

High Spin States in 79Rb

NUCLEAR REACTIONS 58Ni(28Si, 3pα), E=128 MeV; measured γγ-coin. 79Rb deduced high-spin levels, J, π, band structure.

doi: 10.1143/JPSJ.64.329
Citations: PlumX Metrics


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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1994MU02      Nucl.Phys. A568, 202 (1994)

J.Mukai, A.Odahara, H.Tomura, S.Suematsu, S.Mitarai, T.Kuroyanagi, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, S.E.Arnell, H.A.Roth, O.Skeppstedt

High-Spin States in the Odd-Odd Nucleus 82Y

NUCLEAR REACTIONS 58Ni(28Si, n3p), E=100, 102, 128 MeV; measured Eγ, Iγ, Iγ(θ), (particle)γ-, γγ-coin. 82Y deduced levels, J, π. Enriched target, Ge detector array, particle-multiplicity filter.

doi: 10.1016/0375-9474(94)90010-8
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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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1993AN05      Phys.Lett. 304B, 55 (1993)

R.Anne, S.E.Arnell, R.Bimbot, S.Dogny, H.Emling, H.Esbensen, D.Guillemaud-Mueller, P.G.Hansen, P.Hornshoj, F.Humbert, B.Jonson, M.Keim, M.Lewitowicz, P.Moller, A.C.Mueller, R.Neugart, T.Nilsson, G.Nyman, F.Pougheon, K.Riisager, M.-G.Saint-Laurent, G.Schrieder, O.Sorlin, O.Tengblad, K.Wilhelmsen Rolander, D.Wolski

Dissociation Reactions of the 11Be One-Neutron Halo. The Interplay between Structure and Reaction Mechanism

NUCLEAR REACTIONS 197Au, Ti, 9Be(11Be, X), E=41 MeV/nucleon; measured exclusive, inclusive σ(θ); deduced structure, reaction mechanism interplay.

doi: 10.1016/0370-2693(93)91399-8
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1993MI07      Z.Phys. A344, 405 (1993)

S.Mitarai, T.Kuroyanagi, A.Odahara, J.Mukai, H.Tomura, S.Suematsu, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, N.Gjorup, J.Jongman, S.E.Arnell, H.A.Roth, O.Skeppstedt

A Rotational Band in 82Zr

NUCLEAR REACTIONS 58Ni(28Si, 2n2p), E=128 MeV; measured γγ-coin. 82Zr deduced levels, J, π, band structure.

doi: 10.1007/BF01283195
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1993MI11      Nucl.Phys. A557, 381c (1993)

S.Mitarai, T.Kuroyanagi, A.Odahara, J.Mukai, H.Tomura, S.Suematsu, T.Morikawa, D.Jerrestam, J.Nyberg, G.Sletten, A.Atac, M.Piiparinen, S.E.Arnell, D.Foltescu, H.A.Roth, O.Skeppstedt

Band Structures of Nuclei Around N, Z = 40 Selected by Charged Particle Detection

NUCLEAR REACTIONS 58Ni(28Si, 4p), E=128 MeV; 58Ni(32S, 4p), E=125 MeV; measured relative yield with respect to 1p, 2p, 3p exit channels. 58Ni(28Si, pα), E=100 MeV; 58Ni(32S, p2α), (32S, pα), E=120, 125 MeV; measured γγ-, pα-coin. 85Nb, 81Y deduced levels, J, π, yrast band dynamic moment of inertia. 58Ni(28Si, 2n2p), E=128 MeV; measured γ(particle)-coin. 82Zr deduced levels, J, π. 58Ni(32S, 2n2p), E=125 MeV; measured γγ-coin. 86Mo deduced possible yrast level transitions.

doi: 10.1016/0375-9474(93)90555-C
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1993MO29      Nucl.Instrum.Methods Phys.Res. A336, 587 (1993)

M.Moszynski, D.Wolski, T.Ludziejewski, S.E.Arnell, O.Skeppstedt, W.Klamra

Particle Identification by Digital Charge Comparison Method Applied to CsI(Tl) Crystal Coupled to Photodiode

RADIOACTIVITY 137Cs(β-); measured Eγ, Iγ. 232Th(α); measured α-spectra; deduced device particle identification capabilities. Digital charge comparison method, CsI(Tl)-photodiode assembly, proton spectra studied.

doi: 10.1016/0168-9002(93)91267-Q
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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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1992RI01      Nucl.Phys. A540, 365 (1992)

K.Riisager, R.Anne, S.E.Arnell, R.Bimbot, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, L.Johannsen, B.Jonson, A.Latimier, M.Lewitowicz, S.Mattsson, A.C.Mueller, R.Neugart, G.Nyman, F.Pougheon, A.Richard, A.Richter, M.G.Saint-Laurent, G.Schrieder, O.Sorlin, K.Wilhelmsen

Two-Neutron Removal Reactions for Very Neutron-Rich Nuclei

NUCLEAR REACTIONS 9Be, Ni, 197Au(11Li, 9Li), (14Be, 12Be), (8He, 6He), E=30 MeV/nucleon; measured σ(θ); deduced correlation with two-neutron separation energies, nn-distribution.

doi: 10.1016/0375-9474(92)90210-B
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1991AR08      Nucl.Instrum.Methods Phys.Res. A300, 303 (1991)

S.E.Arnell, H.A.Roth, O.Skeppstedt, J.Bialkowski, M.Moszynski, D.Wolski, J.Nyberg

A 2π Neutron and γ-Ray Multiplicity Filter for the NORDBALL Detection System

NUCLEAR REACTIONS 27Al(16O, X), E=63 MeV; measured Eγ, Iγ, neutron spectra. 58Ni(28Si, X), E=110 MeV; measured Eγ, Iγ. 2π neutron, γ-ray multiplicity filter.

doi: 10.1016/0168-9002(91)90441-R
Citations: PlumX Metrics


1990AN28      Phys.Lett. 250B, 19 (1990)

R.Anne, S.E.Arnell, R.Bimbot, H.Emling, D.Guillemaud-Mueller, P.G.Hansen, L.Johannsen, B.Jonson, M.Lewitowicz, S.Mattsson, A.C.Mueller, R.Neugart, G.Nyman, F.Pougheon, A.Richter, K.Riisager, M.G.Saint-Laurent, G.Schrieder, O.Sorlin, K.Wilhelmsen

Observation of Forward Neutrons from the Break-Up of the 11Li Neutron Halo

NUCLEAR REACTIONS 9Be, Ni, 197Au(11Li, 9Li), E=29 MeV/nucleon; measured σ(θ) following projectile breakup; deduced neutron halo radius.

doi: 10.1016/0370-2693(90)91147-4
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1989CR03      Phys.Scr. 39, 547 (1989)

M.Cronqvist, S.Mattsson, M.Rydehell, O.Skeppstedt, S.E.Arnell, L.Westerberg

Neutron Emission Studied in Alpha Induced Reactions at 50 and 75 MeV on 124Sn

NUCLEAR REACTIONS 124Sn(α, xn), E=50, 75 MeV; measured neutron spectra. Two-source moving model, INDEX model analyses.

doi: 10.1088/0031-8949/39/5/002
Citations: PlumX Metrics


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.


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
Citations: PlumX Metrics


1986AR20      Phys.Scr. 34, 484 (1986)

S.E.Arnell, S.Mattsson, H.A.Roth, M.Rydehell, O.Skeppstedt, A.Johnson, J.Nyberg, L.Westerberg

Preequilibrium Reactions with 118 MeV 12C on 118Sn

NUCLEAR REACTIONS 118Sn(12C, Xγ), E=118 MeV; measured γ(particle)-coin, fragment spectra, σ(θ), X=4He, Li, 7,9,10Be, B, γ-multiplicities. 121,122,123Xe, 120Te deduced γ-multiplicity yrast transition dependence. Hyperpure Ge, NaI detectors. Sum rule calculations.

doi: 10.1088/0031-8949/34/6A/003
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1986NY01      Phys.Scr. 33, 206 (1986)

J.Nyberg, A.Johnson, S.A.Hjorth, A.Kerek, C.G.Linden, S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt

Angular Momentum Transfer in Reactions Induced by 14N Ions on 154Sm

NUCLEAR REACTIONS 154Sm(14N, 7np), (14N, 8np), (14N, 9np), (14N, xnd), (14N, xnp), (14N, xnt), E=151 MeV; measured proton spectra, (γ-multiplicity)(charged particle)-coin; deduced reaction mechanism. 158Er deduced <Mγ> vs spin.

doi: 10.1088/0031-8949/33/3/004
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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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1984NY03      ATOMKI Kozlem. 26, 68 (1984)

J.Nyberg, A.Johnson, S.A.Hjorth, A.Kerek, S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt

Angular Momentum Transfer in Partial Fusion Reactions Induced by 14N on 154Sm

NUCLEAR REACTIONS 154Sm(14N, 9np), (14N, 8nd), (14N, 7nt), E=154 MeV; measured γ-multiplicity, γp-, γd-, γt-coin; deduced partial fusion angular momentum transfer. Sum rule model.


1983AR14      Phys.Lett. 129B, 23 (1983)

S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt, S.A.Hjorth, A.Johnson, A.Kerek, J.Nyberg, L.Westerberg

Charge Particle Production in Peripheral Reactions Induced by 118 MeV 12C Ions on 118Sn

NUCLEAR REACTIONS 118Sn(12C, 3nα), (12C, 4nα), (12C, 5nα), (12C, 2n2α), E=118 MeV; measured γ-multiplicities, (particle)γ-coin; deduced fusion reaction mechanism.

doi: 10.1016/0370-2693(83)90720-7
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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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1983AR19      Phys.Scr. T5, 199 (1983)

S.E.Arnell, S.Mattsson, H.A.Roth, O.Skeppstedt, S.A.Hjorth, A.Johnson, Th.Lindblad, J.Nyberg, L.Westerberg

Incomplete-Fusion Reactions in the 12C + 118Sn System at E(12C) = 118 MeV

NUCLEAR REACTIONS 118Sn(12C, X), E=118 MeV; measured σ(fragment E), relative fragment production σ for X=He, Li, Be, B, γ(fragment)-coin; deduced reaction mechanism. Wilczynski sum rule model.

doi: 10.1088/0031-8949/1983/T5/040
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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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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
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1978BA37      Phys.Rev. C18, 119 (1978)

J.H.Barker, D.G.Sarantites, O.Skeppstedt, E.Wallander, G.Alenius, S.-E.Arnell

Multiplicity of the γ Cascades in the 61Cu Continuum: Dependence on Excitation Energy of the Entry States

NUCLEAR REACTIONS 58Ni(α, pγ), E=17.0, 19.5 MeV; measured γ-multiplicities for cascades, side feeding in 61Cu continuum as function of excitation energy.

doi: 10.1103/PhysRevC.18.119
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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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1975AL25      Nuovo Cim. 27A, 249 (1975)

N.G.Alenius, S.E.Arnell, E.Selin, O.Stankiewicz

Structure of 54Mn from the 54Cr(p, nγ)54Mn and 51V(α, nγ)54Mn Reactions

NUCLEAR REACTIONS 54Cr(p, nγ), E=3.0-4.3 MeV; 51V(α, nγ), E=7-15 MeV; measured σ(E, Eγ, θ), γγ-coin. 54Mn deduced levels, J, π, T1/2.

doi: 10.1007/BF02785345
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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
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1974AL13      Phys.Scr. 10, 43 (1974)

G.Alenius, S.E.Arnell, O.Stankiewicz

High Spin States in 39K from the 36Ar(α, pγ)39K Reaction

NUCLEAR REACTIONS 36Ar(α, pγ), E=10, 12, 14 MeV; measured Eγ, Iγ, DSA, γγ-coin, γ(θ). 39K deduced levels, J, π, γ-mixing, T1/2.

doi: 10.1088/0031-8949/10/1-2/003
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0666.


1973AR14      Phys.Scr. 8, 191 (1973)

S.E.Arnell, E.Selin

A Study of Excited States in 44Sc by Means of the 41K(α, nγ)44Sc Reaction

NUCLEAR REACTIONS 41K(α, nγ), E=10, 12, 14 MeV; measured σ(E, Eγ), γγ-coin. 44Sc deduced levels, J, π.

doi: 10.1088/0031-8949/8/5/004
Citations: PlumX Metrics


1972AL12      Nuovo Cim. 8A, 147 (1972)

N.G.Alenius, S.E.Arnell, O.Skeppstedt, E.Wallander, Z.P.Sawa

Structure of 43Ca from the 40Ar(α, nγ)43Ca Reaction

NUCLEAR REACTIONS 40Ar(α, nγ), E=13.5 MeV; measured Eγ, Iγ, γγ-coin, Iγ(θ), σ(E;Eγ, θ(γ)). 43Ca deduced levels, J, π, γ-branching. Ge(Li) detectors.

doi: 10.1007/BF02728760
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1972AL19      Nucl.Phys. A186, 209 (1972)

G.Alenius, S.E.Arnell, C.Schale, E.Wallander

Thermal-Neutron Capture Investigation of the N = 107 Isotones of 177Yb And 179Hf

NUCLEAR REACTIONS 176Yb(n, γ), 178Hf(n, γ), E=th; measured Eγ, Iγ, Q. 177Yb, 179Hf deduced levels, J, π. Enriched targets. Ge(Li) detector.

doi: 10.1016/0375-9474(72)90136-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20224.


1972AR37      Phys.Scr. 6, 222 (1972)

S.E.Arnell, C.G.Mattsson, O.Skeppstedt

High Spin States in 51Ti

NUCLEAR REACTIONS 48Ca(α, xnγ); E=10, 12, 14 MeV. Measured σ(E, Eγ, θ), P(Eγ). 51Ti deduced levels, J, π.

doi: 10.1088/0031-8949/6/5-6/003
Citations: PlumX Metrics


1972MA42      Phys.Scr. 5, 58 (1972)

C.G.Mattsson, S.E.Arnell, L.Jonsson

Thermal Neutron Capture in Natural Krypton

NUCLEAR REACTIONS Kr(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 84Kr deduced levels, J, π, γ-branching.

doi: 10.1088/0031-8949/5/1-2/009
Citations: PlumX Metrics


1971AL01      Nucl.Phys. A161, 209 (1971)

G.Alenius, S.E.Arnell, C.Schale, E.Wallander

Low Spin, Negative Parity States in the N = 103 Isotones of 171Er, 173Yb and 175Hf Identified by Thermal Neutron Capture Reactions

NUCLEAR REACTIONS 170Er(n, γ), 172Yb(n, γ), 174Hf(n, γ), E=th; measured Eγ, Iγ, Q. 171Er, 173Yb, 175Hf deduced levels, J, π. Enriched targets. Ge(Li) detectors.

doi: 10.1016/0375-9474(71)90329-0
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1971AL14      Phys.Scr. 3, 55 (1971)

G.Alenius, S.E.Arnell, C.Schale, E.Wallander

Thermal Neutron Capture Investigation of the 172Yb and 174Yb Level Structures

NUCLEAR REACTIONS 171,173Yb(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 172,174Yb deduced levels, J, π, K, γ-branching. Ge(Li) pair, anti-Compton spectrometer.

doi: 10.1088/0031-8949/3/2/002
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20244.


1971AL22      Phys.Scr. 3, 105 (1971)

G.Alenius, S.E.Arnell, C.Schale, E.Wallander

Low Spin States in 181Hf from the Thermal Neutron Capture Reaction

NUCLEAR REACTIONS 180Hf(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 181Hf deduced levels, J, π, Nilsson assignments.

doi: 10.1088/0031-8949/3/3-4/003
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20243.


1971AL27      Phys.Scr. 4, 35 (1971)

G.Alenius, S.E.Arnell, C.Schale, E.Wallander

Energy Levels in 175Yb from Primary Transitions in the Thermal Neutron Capture Reaction

NUCLEAR REACTIONS 174Yb(n, γ), E=thermal; measured Eγ, Iγ, Q. 175Yb deduced levels, J, π.

doi: 10.1088/0031-8949/4/1-2/006
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20246.


1971AR12      Nucl.Phys. A166, 241 (1971)

S.E.Arnell, H.Linusson, Z.Sawa

Energy Levels and Gamma Transitions in 70Ga

NUCLEAR REACTIONS 69Ga(d, p), 71Ga(d, t), Ed=12.1 MeV. 69Ga(d, pγ), Ed=7 MeV; 67Zn(α, pγ), Eα=14 MeV; 70Zn(p, nγ), Ep=1.4-4.0 MeV; 69Ga(n, γ), En=th; measured Eγ, γγ-coin, pγ-coin. 70Ga deduced levels, J, γ-branching. Enriched targets.

doi: 10.1016/0375-9474(71)90427-1
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1971AR39      Phys.Scr. 4, 89 (1971)

S.E.Arnell, R.Hardell, A.Hasselgren, C.-G.Mattsson, O.Skeppstedt

Thermal Neutron Capture in 50Ti and 64Ni

NUCLEAR REACTIONS 50Ti, 64Ni(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 51Ti, 65Ni deduced levels. Ge(Li) pair, anti-Compton spectrometer.

doi: 10.1088/0031-8949/4/3/001
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20247.


1970LI04      Ark.Fys. 40, 197 (1970)

H.Linusson, R.Hardell, S.E.Arnell

Low Lying Energy Levels in Ga70 and Ga72 Excited in Thermal Neutron Capture Reactions

NUCLEAR REACTIONS 69,71Ga(n, γ), E=thermal; measured Eγ, Iγ; deduced Q. 70,72Ga deduced levels.

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset20165.


1968JO09      Arkiv Fysik 35, 423 (1968)

L.Jonsson, R.Hardell, S.E.Arnell

Gamma Rays from Thermal Neutron Capture in Natural Neon

NUCLEAR STRUCTURE 21Ne, 20Ne, 23Ne; measured not abstracted; deduced nuclear properties.


1968SK02      Arkiv Fysik 35, 527 (1968)

O.Skeppstedt, R.Hardell, S.E.Arnell

Gamma Rays from Thermal Neutron Capture in Natural Argon

NUCLEAR STRUCTURE 41Ar, 37Ar; measured not abstracted; deduced nuclear properties.


1967AR14      Nucl.Instr.Methods 54, 165 (1967)

S.E.Arnell, R.Hardell, A.Hasselgren, L.Jonsson, O.Skeppstedt

Thermal Neutron Capture Gammas Measured with Ge(Li)-Spectrometers and Internal Reactor Targets

NUCLEAR STRUCTURE 55Fe, 41Ar, 37Ar; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-554X(67)90618-0
Citations: PlumX Metrics


1967PE06      Arkiv Fysik 33, 371 (1967)

P.O.Persson, S.E.Arnell

Gamma Transitions in Co57

NUCLEAR STRUCTURE 57Co; measured not abstracted; deduced nuclear properties.


1966AR12      IAEA Panel Meeting, Vienna (June 1966)

S.E.Arnell, R.Hardell, A.Hasselgren, L.Jonsson, O.Skeppstedt

Neutron and Proton Capture Gammas Measured with Ge(Li) Spectrometers


1966JO08      Arkiv Fysik 32, 549 (1966)

L.Jonsson, O.Skeppstedt, S.E.Arnell

Gamma Decay of Proton Resonances in Mn54 and Mn55

NUCLEAR STRUCTURE 54Mn, 55Mn; measured not abstracted; deduced nuclear properties.


1966SK02      Arkiv Fysik 31, 83 (1966)

O.Skeppstedt, L.Jonsson, A.Hasselgren, S.E.Arnell

Inelastic Scattering of Protons by A36, A38 and A40

NUCLEAR STRUCTURE 41K, 39K, 37K; measured not abstracted; deduced nuclear properties.


1966ST10      Arkiv Fysik 31, 567 (1966)

S.Sterner, L.Jonsson, S.E.Arnell

Study of Levels in Mn51 and Mn53 Through the Radiative Capture of Protons by Cr50 and Cr52

NUCLEAR STRUCTURE 53Mn, 51Mn; measured not abstracted; deduced nuclear properties.


1966WE05      Arkiv Fysik 31, 113 (1966)

E.Wernbom-Selin, S.E.Arnell

Gamma Decay of Resonances in Na23

NUCLEAR STRUCTURE 23Na; measured not abstracted; deduced nuclear properties.


1965AR13      Arkiv Fysik 30, 397 (1965)

S.E.Arnell, A.Hasselgren

Anticoincidence Spectrometers for Nuclear Reaction Studies

NUCLEAR STRUCTURE 23Na, 9Be, 11B, 60Co, 28Si; measured not abstracted; deduced nuclear properties.


1965HA33      Arkiv.Fysik 30, 500 (1965)

R.Hardell, S.E.Arnell, P.Blichert-Toft

Thermal Neutron Capture Gammas of Fe55 and Argon Isotopes

NUCLEAR STRUCTURE Ar, 56Fe; measured not abstracted; deduced nuclear properties.


1964AR05      Arkiv Fysik 27, 1 (1964)

S.E.Arnell, E.Wernbom-Selin

Capture and Inelastic Scattering of Protons by Ne-21

NUCLEAR STRUCTURE 22Na; measured not abstracted; deduced nuclear properties.


1964AR06      Arkiv Fysik 27, 33 (1964)

S.E.Arnell, S.Sterner

A Search for Positron Branching in the Mn51+)Cr51 Transition

NUCLEAR STRUCTURE 51Mn; measured not abstracted; deduced nuclear properties.


1964AR07      Phys. Letters 9, 319 (1964)

S.E.Arnell, S.Sterner

Tentative Level Schemes of Mn51 and Mn53

NUCLEAR STRUCTURE 51Mn, 53Mn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(64)90382-8
Citations: PlumX Metrics


1964AR12      Arkiv Fysik 26, 485 (1964)

S.E.Arnell, K.C.Tripathi

The A38(p, γ)K39 Reaction

NUCLEAR STRUCTURE 39K; measured not abstracted; deduced nuclear properties.


1964AR13      Arkiv Fysik 27, 41 (1964)

S.E.Arnell, P.O.Persson

Gamma Rays from Proton Bombardment of A40

NUCLEAR STRUCTURE 41K; measured not abstracted; deduced nuclear properties.


1964AR14      Arkiv Fysik 26, 423 (1964)

S.E.Arnell, S.Sterner

An Investigation of the Cr52(p, γ)Mn53 Reaction

NUCLEAR STRUCTURE 53Mn; measured not abstracted; deduced nuclear properties.


1964AR16      Arkiv Fysik 25, 531 (1964)

S.E.Arnell, S.Sterner

Deexcitation and Spin of the 3.56 MeV Level in Na21

NUCLEAR STRUCTURE 21Na; measured not abstracted; deduced nuclear properties.


1964AR17      Arkiv Fysik 26, 153 (1964)

S.E.Arnell

New Energy Levels in K37

NUCLEAR STRUCTURE 37K; measured not abstracted; deduced nuclear properties.


1964AR18      Arkiv Fysik 25, 389 (1964)

S.E.Arnell, E.Wernbom

Positron Branching Ratios in the Decays of F17, Na21, Al25, and Al26m

NUCLEAR STRUCTURE 21Na, 17F, 25Al, 26Al; measured not abstracted; deduced nuclear properties.


1964AR19      Arkiv Fysik 26, 309 (1964)

S.E.Arnell, S.Sterner

Energy Levels of Mn51

NUCLEAR STRUCTURE 51Mn; measured not abstracted; deduced nuclear properties.


1964AR20      Arkiv Fysik 26, 193 (1964)

S.E.Arnell, P.O.Persson

The Fe56(p, γ)Co57 Reaction

NUCLEAR STRUCTURE 57Co; measured not abstracted; deduced nuclear properties.


1963AR05      Arkiv Fysik 23, 301 (1963)

S.E.Arnell, E.Wernbom

Resonance Energies for Proton Capture in Ne21 and Ne22

NUCLEAR STRUCTURE 22Na, 23Na; measured not abstracted; deduced nuclear properties.


1963AR13      Nucl.Instr.Methods 24, 185 (1963)

S.E.Arnell, E.G.Nadjakov

Thermal Neutron Capture Gammas Measured with a Three Crystal Pair Spectrometer with Internal Target

doi: 10.1016/0029-554X(63)90308-2
Citations: PlumX Metrics


1962AR03      Arkiv Fysik 21, 177 (1962)

S.E.Arnell

Radiative Proton Capture by Cr50, Cr52, Cr53, and Cr54

NUCLEAR STRUCTURE 53Mn, 51Mn, 54Mn, 55Mn; measured not abstracted; deduced nuclear properties.


1962AR04      Arkiv Fysik 22, 391 (1962)

S.E.Arnell

Proton Capture in Some Isotopes of Argon and Neon

NUCLEAR STRUCTURE 41K, 37K, 23Na, 22Na; measured not abstracted; deduced nuclear properties.


1961AR10      Nuclear Phys. 24, 500 (1961)

S.E.Arnell

Proton Capture in A40

NUCLEAR STRUCTURE 41K; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(61)90418-7
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1958AR15      Nuclear Phys. 6, 196 (1958)

S.E.Arnell, J.Dubois, O.Almen

Half-Lives of the Positon Emitting Mirror Nuclides

doi: 10.1016/0029-5582(58)90099-3
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