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NSR database version of April 27, 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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Data from this article have been entered in the XUNDL database. For more information, click here.

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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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, T_1/2. 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
Citations: PlumX Metrics

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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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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1646.

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
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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, T_1/2, 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, T_1/2, 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
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, T_1/2, 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, T_1/2.

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, T_1/2. 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, T_1/2.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
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
Citations: PlumX Metrics

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(β⁺)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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