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NSR database version of April 11, 2024.

Search: Author = K.G.Rensfelt

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2006JE02      Phys.Lett. B 635, 17 (2006)

H.B.Jeppesen, A.M.Moro, T.Nilsson, F.Ames, P.van den Bergh, U.C.Bergmann, G.Bollen, M.J.G.Borge, J.Cederkall, P.Van Duppen, S.Emhofer, O.Forstner, L.M.Fraile, H.O.U.Fynbo, J.Gomez-Camacho, D.Habs, R.von Hahn, G.Huber, M.Huyse, H.T.Johansson, B.Jonson, O.Kester, H.Lenske, L.Liljeby, M.Meister, G.Nyman, M.Oinonen, M.Pantea, H.Podlech, U.Ratzinger, K.Reisinger, K.G.Rensfelt, R.Repnow, K.Riisager, A.Richter, K.Rudolph, H.Scheit, A.Schempp, P.Schmidt, G.Schrieder, D.Schwalm, T.Sieber, H.Simon, O.Tengblad, E.Tengborn, M.Turrion, L.Weissman, F.Wenander, B.Wolf

Investigation of the 9Li + 2H → 8Li + t reaction at REX-ISOLDE

NUCLEAR REACTIONS 2H(9Li, 8Li), E=2.36 MeV/nucleon; measured particle spectra, σ(θ). 8Li levels deduced energies, spectroscopic factors. Comparison with optical model calculations, post-accelerated radioactive beam.

doi: 10.1016/j.physletb.2006.02.034
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1395.

2000HA68      Hyperfine Interactions 129, 43 (2000)

D.Habs, O.Kester, T.Sieber, H.Bongers, S.Emhofer, P.Reiter, P.G.Thirolf, G.Bollen, J.Aysto, O.Forstner, H.Ravn, T.Nilsson, M.Oinonen, H.Simon, J.Cederkall, F.Ames, P.Schmidt, G.Huber, L.Liljeby, O.Skeppstedt, K.G.Rensfelt, F.Wenander, B.Jonson, G.Nyman, R.von Hahn, H.Podlech, R.Repnow, C.Gund, D.Schwalm, A.Schempp, K.-U.Kuhnel, C.Welsch, U.Ratzinger, G.Walter, A.Huck, K.Kruglov, M.Huyse, P.Van den Bergh, P.Van Duppen, L.Weissman, A.C.Shotter, A.N.Ostrowski, T.Davinson, P.J.Woods, J.Cub, A.Richter, G.Schrieder, and the REX-ISOLDE Collaboration

The REX-ISOLDE project

doi: 10.1023/A:1012603025802
Citations: PlumX Metrics

1997HA11      Nucl.Phys. A616, 29c (1997)

D.Habs, O.Kester, G.Bollen, L.Liljeby, K.G.Rensfelt, D.Schwalm, R.von Hahn, G.Walter, P.Van Duppen, and the REX-ISOLDE Collaboration

The REX-ISOLDE Project

NUCLEAR REACTIONS, ICPND U(p, X)25Na/27Na/28Na/29Na/30Na/31Na/32Na/33Na/34Na, E=1 GeV; measured production yields for residual nuclei. Other aspects included, PS-ISOLDE setup, Uc2 target, surface ion source.

doi: 10.1016/S0375-9474(97)00071-7
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1052.

1997NO13      Nucl.Phys. A626, 511c (1997)

D.Novak, A.Kerek, W.Klamra, L.-O.Norlin, G.Zetterstrom, L.Bagge, A.Kallberg, A.Paal, K.G.Rensfelt, J.Gal, J.Molnar

Scraping the CRYRING Beam - A Simple Diagnostic Tool

doi: 10.1016/S0375-9474(97)00576-9
Citations: PlumX Metrics

1988KA04      Z.Phys. A329, 143 (1988)

L.Kaubler, W.Enghardt, H.Prade, P.Carle, L.O.Norlin, K.-G.Rensfelt, U.Rosengard

The Magnetic Moment of the 10+ Isomer in 140Ce and E1 Transitions in N = 82 Isotones Caused by Outer Subshell Configurations

NUCLEAR REACTIONS 138Ba(α, 2n), E=27, 32.5 MeV; measured γ(θ, H, t). 140Ce levels deduced g, J, π, T1/2, isomer decay, configuration. Shell model.

1988RO08      Nucl.Phys. A482, 573 (1988)

U.Rosengard, P.Carle, A.Kallberg, L.O.Norlin, K.-G.Rensfelt, H.C.Jain, B.Fant, T.Weckstrom

Yrast Spectroscopy and g-Factor Measurements in 199Pb, 201Pb and 203Pb

NUCLEAR REACTIONS 198,200Hg(α, 2n), (α, 3n), E=41 MeV; 200,202Hg(α, 3n), (α, 4n), E=53 MeV; measured Eγ, Iγ, γ(θ), γ(θ, H, t), γγ(t). 199,201,203Pb deduced levels, J, π, T1/2, g, B(E2), configurations. Enriched thick targets, Ge, Ge(Li) detectors. Shell model.

NUCLEAR STRUCTURE 199,201,203Pb; calculated levels; deduced configurations. Shell model.

doi: 10.1016/0375-9474(88)90171-6
Citations: PlumX Metrics

1987CA23      Hyperfine Interactions 34, 77 (1987)

P.Carle, S.Egnell, L.O.Norlin, K.-G.Rensfelt, U.Rosengard, B.Fant, H.C.Jain, K.Johansson

Half-Lives and g-Factors of some Microsecond Isomers in the Lead Region

NUCLEAR REACTIONS 198Hg(α, 4n), (α, 3n), E=53 MeV; 209Bi(α, 3n), E=51 MeV; measured γ(θ, H, t). 198,199Pb, 210At deduced isomer T1/2, g.

1987FA15      Nucl.Phys. A475, 338 (1987)

B.Fant, T.Weckstrom, H.C.Jain, L.O.Norlin, K.-G.Rensfelt, P.Carle, U.Rosengard

Investigation of the High-Spin Structure of 200,202Pb

NUCLEAR REACTIONS 198Hg(α, 2n), E=41 MeV; 200,202Hg(α, 4n), E=53 MeV; measured E(γ), I(γ), γ(θ), γ(t), γγ(t). 200,202Pb deduced levels, J, π, T1/2, g, B(λ), configurations. Enriched targets, Ge, Ge(Li) detectors. Shell model.

doi: 10.1016/0375-9474(87)90170-9
Citations: PlumX Metrics

1987JA08      Hyperfine Interactions 34, 73 (1987)

H.C.Jain, L.O.Norlin, K.-G.Rensfelt, U.Rosengard, P.Carle, B.Fant, T.Weckstrom

The g-Factor of 19- Isomer in 202Pb

NUCLEAR REACTIONS 202Hg(α, 4n), E=53 MeV; measured γ(θ, H, t). 202Pb deduced isomer g, configuration, T1/2.

doi: 10.1007/BF02072682
Citations: PlumX Metrics

1987KA33      Hyperfine Interactions 34, 381 (1987)

L.Kaubler, W.Enghardt, H.Prade, F.Stary, P.Carle, L.O.Norlin, K.-G.Rensfelt, U.Rosengard

The Magnetic Moment of the 10+ Isomer in 140Ce and Temperature Dependence of the Paramagnetism for Ce Ions in BaO

RADIOACTIVITY 140mCe; measured γ(θ, H, t); deduced isomer g.

1986JA13      Nucl.Phys. A458, 225 (1986)

H.C.Jain, P.Carle, A.Kallberg, L.O.Norlin, K.-G.Rensfelt, U.Rosengard, B.Fant

High-Spin Isomers in 202Pb

NUCLEAR REACTIONS 200,202Hg(α, xn), E=35-55 MeV; measured Eγ, Iγ, γ(t), γγ(t), I(ce). 202Pb deduced levels, J, π, T1/2, g, B(λ), configurations. Enriched targets, Ge, Ge(Li), Si(Li) detectors. Shell-model considerations.

doi: 10.1016/0375-9474(86)90354-4
Citations: PlumX Metrics

1986JA21      Phys.Scr. 34, 717 (1986)

H.C.Jain, L.O.Norlin, U.Rosengard, K.-G.Rensfelt, P.Carle

The g-Factor of the (21/2)+ Isomer in 203Pb

NUCLEAR REACTIONS 202Hg(α, 3n), E=41 MeV; measured γ(θ, H, t). 203Pb deduced levels, γ-branching, isomer g, configuration.

doi: 10.1088/0031-8949/34/6A/029
Citations: PlumX Metrics

1985BE22      Phys.Scr. 31, 333 (1985)

I.Bergstrom, J.Blomqvist, P.Carle, B.Fant, A.Kallberg, L.O.Norlin, K.-G.Rensfelt, U.Rosengard

On the Electromagnetic Properties of Core-Excited High-Spin States in 210Po and 211At

NUCLEAR REACTIONS 208Pb, 209Bi(α, 2n), E=35 MeV; measured I(ce), γ(t), γ(θ, H, t). 210Po, 211At deduced levels, T1/2, g, B(λ).

1985NO09      Z.Phys. A322, 463 (1985)

L.O.Norlin, I.Bergstrom, P.Carle, A.Kallberg, K.-G.Rensfelt, U.Rosengard, K.Johansson, B.Fant

The g-Factor of the 10- Isomeric Level in 208At

NUCLEAR REACTIONS 209Bi(α, 5n), E=cyclotron; measured γ(θ, H, t). 208At deduced isomer g, configuration.

doi: 10.1007/BF01412081
Citations: PlumX Metrics

1985RO07      Phys.Scr. 31, 122 (1985)

U.Rosengard, I.Bergstrom, J.Blomqvist, P.Carle, A.Kallberg, L.O.Norlin, K.-G.Rensfelt

The g-Factors of the (25/2)+ Level in 207Po and 11- Level in 208Po

NUCLEAR REACTIONS 206Pb(α, 3n), (α, 2n), E=44 MeV; measured γ(θ, H, t). 207,208Po levels deduced g.

1981KA10      Z.Phys. A299, 251 (1981)

L.Kaubler, H.Prade, F.Donau, U.Hagemann, F.Stary, K.-G.Rensfelt

Deformation Dependence of Magnetic Moments in the Odd Transitional Nuclei 117-125Te

NUCLEAR REACTIONS 115,119Sn(α, 2n), E=27 MeV; measured γ(θ, H, t). 117,121Te levels deduced μ, T1/2. Nilsson, soft rotor Coriolis, core-particle coupling models.

NUCLEAR STRUCTURE 119,123,125Te; calculated μ. Nilsson, soft rotor Coriolis, core-particle coupling models.

1979RO06      Nucl.Phys. A323, 495 (1979)

C.Roulet, G.Albouy, G.Auger, J.M.Lagrange, M.Pautrat, K.G.Rensfelt, H.Richel, H.Sergolle, J.Vanhorenbeeck

Properties of 192,190Pb: Behaviour of the Very Neutron-Deficient Even Lead Isotopes

NUCLEAR REACTIONS 156Gd(40Ar, 4nγ), E=190 MeV; 154Gd(40Ar, 4nγ), E=195 MeV; 156Gd(40Ar, 6nγ), E=225 MeV; 182W(16O, 6nγ), E=132 MeV; measured Eγ, Iγ, γγ(E, t), γX-coin. 192,190Pb deduced levels, γ-branching. 192Pb level deduced T1/2.

doi: 10.1016/0375-9474(79)90122-2
Citations: PlumX Metrics

1978RA03      Z.Phys. A284, 357 (1978)

V.Rahkonen, I.Bergstrom, J.Blomqvist, O.Knuuttila, K.-G.Rensfelt, J.Sztarkier, K.Westerberg

An Isomeric 19+ State of the πh29/2i13/2νg9/2(j-2)0+ Configuration in 210At and the Question of Isospin in the Two-Particle Core Polarization

NUCLEAR REACTIONS 209Bi(α, 3nγ), E=35-52 MeV; measured Eγ, Iγ(E, θ, t), I(ce). 210At deduced levels, J, π, λ, T1/2, g.

doi: 10.1007/BF01422102
Citations: PlumX Metrics

1977RO15      Nucl.Phys. A285, 156 (1977)

C.Roulet, G.Albouy, G.Auger, J.M.Lagrange, M.Pautrat, K.G.Rensfelt, H.Richel, H.Sergolle, J.Vanhorenbeeck

Magnetic Moments of the 12+ Isomeric States in 194,196,198Pb

NUCLEAR REACTIONS W(16O, 4nγ), E=97 MeV; measured γ(θ, H, t). 194m,196m,198mPb deduced T1/2, g. Natural metallic target.

doi: 10.1016/0375-9474(77)90152-X
Citations: PlumX Metrics

1976LI09      Z.Phys. A277, 273 (1976)

C.G.Linden, I.Bergstrom, J.Blomqvist, K.-G.Rensfelt, H.Sergolle, K.Westerberg

High Spin States in 205Pb and a Precision Test of the Nuclear Shell Model for Three Nucleons

NUCLEAR REACTIONS 204Hg(α, 3nγ), E ≈ 40 MeV; measured Eγ, Iγ, γ(t), I(ce), γγ-coin, γ(θ, H). 205Pb deduced levels, J, π, T1/2, λ, ICC, B(λ), g.

1976RE12      Phys.Scr. 14, 95 (1976)

K.-G.Rensfelt, C.Roulet, K.Westerberg

The g-Factor of the 31/2--State in 209Po

NUCLEAR REACTIONS Pb(α, xnγ), E=45-51 MeV; measured γ(θ, H, t). 209Po level deduced g.

doi: 10.1088/0031-8949/14/3/005
Citations: PlumX Metrics

1975BE39      Z.Phys. A273, 291 (1975)

I.Bergstrom, C.J.Herrlander, T.Lindblad, V.Rahkonen, K.-G.Rensfelt, K.Westberg

Evidence for Two-Particle Core Polarization in the Isomeric 29/2+ and 21/2- States of the π(h29/2)8+ i13/2ν(j-2)0+ and π(h39/2)ν(j-2)0+ Configurations in 209At

NUCLEAR REACTIONS 209Bi(α, 4nγ), E=42-51 MeV; measured σ(Eγ, θ, t), γγ-coin, I(ce), ce(t). 209At deduced levels, J, π, ICC, g.

1975DI02      Phys.Lett. 55B, 293 (1975)

F.Dimmling, D.Riegel, K.-G.Rensfelt, C.-J.Herrlander

Quadrupole Moments of νh11/2 States in Sn-Isotopes and Electric Field Gradients at the Sn and Cd Sites in Cd, Sn and Sb Metal

NUCLEAR REACTIONS 113,114,116Cd(α, 4n), E=51 MeV; measured spin precession spectra. 113,114,116Sn levels deduced quadrupole moment. 118,119,120Sn, 111Cd levels deduced quadrupole moment.

doi: 10.1016/0370-2693(75)90603-6
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1974BL03      Phys.Scr. 9, 321 (1974)

J.Blomqvist, S.Borg, A.Kerek, K.-G.Rensfelt, J.Sztarkier

The Half-Life of the 6+ State in 134Te and the Effective 1g7/2 Proton Charge

RADIOACTIVITY 134Sb; measured γγ(t). 134Te level deduced T1/2.

doi: 10.1088/0031-8949/9/6/002
Citations: PlumX Metrics

1973AB09      Nucl.Instrum.Methods 111, 125 (1973)

K.Abrahamsson, A.Filevich, K.-G.Rensfelt, J.Sztarkier

A Fast Beam Pulsing System for the Stockholm 225-cm Cyclotron

NUCLEAR REACTIONS 208Pb(α, 3nγ); measured γγ(θ, H, t). 209Po levels deduced g.

doi: 10.1016/0029-554X(73)90103-1
Citations: PlumX Metrics

1973KL13      Phys.Scr. 7, 117 (1973)

W.Klamra, S.A.Hjorth, K.-G.Rensfelt

Properties of Rotational Excitations in 159Dy

NUCLEAR REACTIONS 158Gd(α, 3nγ), E=35 MeV; measured Eγ, γ(θ), γγ-coin. 159Dy deduced levels, J, π, γ-mixing, γ-branching. 159Dy levels calculated Nilsson configuration.

doi: 10.1088/0031-8949/7/3/004
Citations: PlumX Metrics

1972FI06      Nucl.Instrum.Methods 98, 601 (1972)

A.Filevich, K.-G.Rensfelt, J.Sztarkier

A Device for Melted Targets for in-Beam g-Factor Determinations

NUCLEAR REACTIONS 209Bi(α, 3nγ), E=43 MeV; measured αγ(θ, H, t).

doi: 10.1016/0029-554X(72)90251-0
Citations: PlumX Metrics

1972FI16      Phys.Scr. 5, 27 (1972)

A.Filevich, K.-G.Rensfelt, J.Sztarkier, K.Nakai, I.Bergstrom

The g-Factor of the 15- State in 210At

NUCLEAR REACTIONS 209Bi(α, 3nγ), E not given; measured αγ(θ, H, t). 210At level deduced g. Stroboscopic method.

doi: 10.1088/0031-8949/5/1-2/005
Citations: PlumX Metrics

1972NA08      Nucl.Phys. A189, 526 (1972)

K.Nakai, B.Herskind, J.Blomqvist, A.Filevich, K.-G.Rensfelt, J.Sztarkier, I.Bergstrom, S.Nagamiya

The g-Factor of the 12+ Isomeric State in 206Pb and the Effective Orbital g-Factor of the Neutron

NUCLEAR REACTIONS 204Hg(α, 2nγ), E=27 MeV; measured αγ(θ, H, t). 206mPb deduced g, neutron effective orbital g.

doi: 10.1016/0375-9474(72)90311-9
Citations: PlumX Metrics

1972WI19      Phys.Scr. 5, 126 (1972)

K.Wikstrom, B.Fant, A.Filevich, K.-G.Rensfelt, J.Sztarkier, I.Bergstrom

Evidence for 15- and 11+ Isomeric States of the πl(h9/2)2 i13/2l29/2+ν(p1/2)-1 and π(h9/2)321/2-ν(p1/2)-1 Configurations

NUCLEAR REACTIONS 209Bi(α, 3nγ), E=32-43 MeV; measured σ(E;Eγ, θ(γ)), αγ-delay. 210mAt deduced levels, J, π, g, T1/2, configurations.

1971BE37      Phys.Scr. 3, 11 (1971)

I.Bergstrom, J.Blomqvist, B.Fant, A.Filevich, G.Linden, K.-G.Rensfelt, J.Sztarkier, K.Wikstrom

E2 Core Polarization by Neutrons in the (i13/2)-2 Configuration in 206Pb

NUCLEAR REACTIONS 204Hg(α, 2nγ), E = 26 MeV; measured Eγ, Iγ, αγ-delay. 206Pb deduced levels, T1/2, B(EL), neutron E2 core polarization charge.

1971KO13      Phys.Lett. 35B, 153 (1971)

J.Kownacki, K.G.Rensfelt

An 880 ns Isomeric State in 144Sm

NUCLEAR REACTIONS 144Nd(α, 2nγ), E=31 MeV; measured αγ-delay, Eγ, Iγ. 144Sm level deduced T1/2.

doi: 10.1016/0370-2693(71)90244-9
Citations: PlumX Metrics

1970RE12      Nucl.Phys. A156, 529 (1970)

K.-G.Rensfelt, A.Johnson, S.A.Hjorth

The Rotational Spectrum of 161Ho

NUCLEAR REACTIONS 159Tb(α, 2n), Eα=30 MeV; measured Eγ, Iγ(θ), αγ-delay. 161Ho deduced levels, J, K, g, γ-mixing. Natural target.

doi: 10.1016/0375-9474(70)90249-6
Citations: PlumX Metrics

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