NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = C.J.Herrlander Found 45 matches. 1986FA04 Nucl.Phys. A453, 77 (1986) B.Fant, T.Weckstrom, V.Rahkonen, C.J.Herrlander, A.Kallberg High-Spin and Isomeric States in 203Po NUCLEAR REACTIONS 204Pb(α, 5n), E=63 MeV; measured Eγ, Iγ, γ(θ), γ(t), γγ(t), I(ce). 203Po deduced levels, J, π, T1/2, B(λ), configurations. Enriched targets, Ge, Ge(Li), Si(Li) detectors. Shell model.
doi: 10.1016/0375-9474(86)90030-8
1986HO03 Nucl.Phys. A451, 141 (1986) K.Honkanen, C.J.Herrlander, B.Fant, T.Lonnroth Yrast Levels in 198Pb and the Structure of Neutron-Deficient Pb Isotopes NUCLEAR STRUCTURE 198,190,202,208Pb; calculated levels; deduced configurations, energy-deformation curves, shapes. Shell-model, Hartree-Fock calculations. NUCLEAR REACTIONS 192Os(12C, 6n), E=100-106 MeV; measured Iγ, γ(θ), γγ-coin, Iγ(t), I(ce). 198Pb deduced levels, J, π, ICC, T1/2, transition rates. Enriched targets, Ge, Ge(Li), Si(Li) detectors.
doi: 10.1016/0375-9474(86)90248-4
1986RA24 Phys.Scr. 34, 720 (1986) V.Rahkonen, B.Fant, C.J.Herrlander On the Yrast Structure of 206Po NUCLEAR REACTIONS 206Pb(α, 4n), E=51-55 MeV; 207Pb(α, 5n), E=59 MeV; 206Pb(3He, 3n), E=27 MeV; measured σ(E), γ(θ), Eγ, Iγ, I(ce), γγ-coin. 206Po deduced levels, J, π, T1/2, γ-multipolarity, ICC. Enriched target, Ge(Li) detectors, electron lens. Shell model.
doi: 10.1088/0031-8949/34/6A/030
1985RA18 Nucl.Phys. A441, 11 (1985) V.Rahkonen, B.Fant, C.J.Herrlander, K.Honkanen, A.Kallberg, T.Weckstrom An Investigation of the Yrast States in 205,207Po NUCLEAR REACTIONS 204,206,207,208Pb(α, xn), E=40-63 MeV; 207Pb(3He, 3n), E=27 MeV; measured Eγ, Iγ, γ(θ), γ(t), γγ(t), I(ce). 205,207Po deduced levels J, π, T1/2, ICC, γ-multipolarity, B(λ), configurations. Ge, Ge(Li), Si-Li detectors, enriched targets. Shell-model.
doi: 10.1016/0375-9474(85)90165-4
1985WE05 Z.Phys. A321, 231 (1985) T.Weckstrom, B.Fant, T.Lonnroth, V.Rahkonen, A.Kallberg, C.-J.Herrlander In-Beam Study of High-Spin States in 199,200,201Po and Systematical Features of Z = 84 Polonium Isotopes NUCLEAR REACTIONS 194Pt(12C, 7n), (12C, 6n), (12C, 5n), 195Pt(12C, 6n), E=100, 102, 106 MeV; measured Eγ, Iγ, γγ-, γγ(nn)-, γ(nn)-coin, γ yields, γ(X-ray)-coin. 199,201Po deduced levels, J, π, γ-branching. 200Po deduced levels, isomer T1/2, J, π, γ-branching, γ-multipolarity, configuration. Self-consistent Hartree-Fock calculations.
1984FA10 Nucl.Phys. A429, 296 (1984) B.Fant, T.Weckstrom, T.Lonnroth, C.J.Herrlander, K.Honkanen, A.Kallberg Study of the Three-Proton Three Neutron-Hole Nucleus 208At NUCLEAR REACTIONS 209Bi(α, 5n), E=51-60 MeV; measured Eγ, Iγ, γ(θ), γ(t), γγ(t), I(ce). 208At deduced levels J, π, T1/2, ICC, γ-multipolarity, B(λ), transition rates, configurations. Shell model considerations.
doi: 10.1016/0375-9474(84)90209-4
1982KL10 Nucl.Phys. A391, 184 (1982) W.Klamra, J.Bialkowski, C.J.Herrlander, L.Hildingsson, D.Jerrestam, A.Johnson, A.Kerek, J.Kownacki, A.Kallberg, Th.Lindblad, C.G.Linden, T.Vertse Gamma-Gamma Energy Correlations and Moment of Inertia in Light Xe Isotopes NUCLEAR REACTIONS 114,116Cd(12C, xn), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectra. 118,120,122Xe deduced moment of inertia.
doi: 10.1016/0375-9474(82)90226-3
1982LI05 Nucl.Phys. A378, 364 (1982) Th.Lindblad, L.Hildingsson, D.Jerrestam, A.Kallberg, A.Johnson, C.J.Herrlander, W.Klamra, A.Kerek, C.G.Linden, J.Kownacki, J.Bialkowski, T.Vertse On the Moment of Inertia in Deformed Ba-Xe Nuclei as Deduced from Gamma-Gamma Energy Correlation Experiments NUCLEAR REACTIONS 114,116,118,120,122Sn(12C, xn), (12C, αxn), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectra, moment of inertia.
doi: 10.1016/0375-9474(82)90599-1
1981BI02 Nucl.Phys. A357, 261 (1981) J.Bialkowski, B.Fant, C.J.Herrlander, L.Hildingsson, A.Johnson, W.Klamra, J.Kownacki, A.Kallberg, Th.Lindblad, C.G.Linden, T.Lonnroth, J.Sztarkier, T.Vertse, K.Wikstrom Gamma-Gamma Energy Correlations and Moment of Inertia in 130Ce NUCLEAR REACTIONS 124Te(12C, 6n), E=118 MeV; measured γγ-coin; deduced energy-energy correlation spectrum. 130Ce deduced collective moment of inertia.
doi: 10.1016/0375-9474(81)90638-2
1978BE39 Z.Phys. A287, 219 (1978) I.Bergstrom, J.Blomqvist, C.J.Herrlander, J.Hattula, O.Knuuttila, E.Liukkonen, V.Rahkonen On the Yrast Two Proton-Two Neutron Hole States in 208Po NUCLEAR REACTIONS 208Pb(α, 4nγ), E=41-51 MeV; measured γγ(t), Eγ, Iγ, γ(E), γ(θ), γγ-coin. 208Pb deduced levels, J, π, T1/2, λ, δ.
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
1977BL01 Phys.Rev.Lett. 38, 534 (1977) J.Blomqvist, I.Bergstrom, C.J.Herrlander, C.G.Linden, K.Wikstrom Quadrupole Interaction and High-Spin States in the Lead Region NUCLEAR STRUCTURE 204,205,207Pb, 208,209Po, 209,210At; calculated levels. 204,206,207Pb cores.
doi: 10.1103/PhysRevLett.38.534
1977HO17 Phys.Rev.Lett. 39, 389 (1977) D.Horn, O.Hausser, T.Faestermann, A.B.McDonald, T.K.Alexander, J.R.Beene, C.J.Herrlander Core-Excited High-Spin Isomers in 212Rn NUCLEAR REACTIONS 204Hg(13C, 5n), E=72-85 MeV; measured Iγ(E, t), γγ-coin, γ(θ), linear polarization. 212Rn deduced levels, J, π, T1/2, λ, δ, g.
doi: 10.1103/PhysRevLett.39.389
1976BE44 Z.Phys. A278, 257 (1976) I.Bergstrom, J.Blomqvist, C.J.Herrlander, C.G.Linden Evidence for a 3.6 Minute Isomeric 12- State of the πh-111/2 νi-113/2 Configuration in 206Tl and Effective Two-Particle Interactions NUCLEAR REACTIONS 204Hg(α, np), E=39-55 MeV; measured Eγ, Iγ, γ(t). 206Tl deduced levels, T1/2, J, π, B(λ).
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
1974BE74 Phys.Scr. 10, 287 (1974) I.Bergstrom, J.Blomqvist, C.J.Herrlander, K.Wikstrom, B.Fant Evidence for a Core-Excited Isomeric 31/2- State in 209Po NUCLEAR REACTIONS 208Pb(α, 3nγ), E=33-43 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t), γγ(t). 209Po deduced levels, T1/2, J, π, γ-mixing, ICC, λ.
1974WI20 Phys.Scr. 10, 292 (1974) K.Wikstrom, I.Bergstrom, J.Blomqvist, C.J.Herrlander, B.Fant, V.Rakhonen Evidence for Two-Nucleon Polarization in the π(h9/2i13/2)11-ν(j-2)0+ Level in 208Po NUCLEAR REACTIONS 208Pb(α, 4nγ), E=42-51 MeV; measured Eγ, Iγ, γ(t), γγ-coin, γγ(t). 208Po deduced levels, T1/2, J, π.
1970BE37 Phys.Lett. 32B, 476 (1970) I.Bergstrom, B.Fant, C.J.Herrlander, P.Thieberger, K.Wikstrom, G.Astner On the (h9/2)3 Proton Configuration in 211At RADIOACTIVITY 211Rn; measured Eγ, Iγ, γγ-coin, I(ce). 211At deduced levels, J, π, ICC, γ-multipolarity. NUCLEAR REACTIONS 209Bi(α, 2nγ), E not given; measured Eγ, Iγ, γγ-coin, θ(γ), αγ-delay. 211At deduced levels, J, π, T1/2, γ-multipolarity.
doi: 10.1016/0370-2693(70)90389-8
1970BE53 Phys.Scr. 1, 243 (1970) I.Bergstrom, B.Fant, C.J.Herrlander, K.Wikstrom, J.Blomqvist Evidence for an Isomeric 22/2+ Level in 211At NUCLEAR REACTIONS 209Bi(α, 2nγ), E=26-43 MeV; measured σ(E;Eγ, θ(γ)), γγ-coin, αγ-delay. 211At deduced 29/2+ isomeric state, transitions, T1/2, γ-multipolarity, B(E3).
1970KE01 Phys.Lett. 31B, 10 (1970) A.Kerek, C.J.Herrlander, A.Luukko, M.Grecescu A 9/2- Isomeric State in 123Xe NUCLEAR REACTIONS 122Te(α, 3n), E=43 MeV; measured Eγ, Iγ, αγ-delay. 123Xe deduced isomeric state J, π, T1/2. Ge(Li) detector.
doi: 10.1016/0370-2693(70)90005-5
1970RE01 Nucl.Phys. A141, 130 (1970) I.Rezanka, A.Kerek, A.Luukko, C.J.Herrlander High-Spin States in Odd Xe Nuclei NUCLEAR REACTIONS 124,126,128Te(α, 3nγ), E=28-43 MeV; measured σ(Eγ, θ), σ(E;Eγ), αγ-delay. 125,127,129Xe deduced levels, J, π, γ-mixing. Enriched targets.
doi: 10.1016/0375-9474(70)90299-X
1969BE04 Nucl.Phys. A123, 99 (1969) I.Bergstrom, C.J.Herrlander, A.Kerek, A.Luukko Excited Nuclear Levels in Doubly Even Xe Isotopes Populated in (α, 2n) Reactions NUCLEAR REACTIONS Sn, Te(α, 2nγ), E=28 MeV; measured σ(Eγ, θ). 118,120,122,124,126Te, 124,126,128,130,132Xe deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90892-6
1969BE47 Phys.Rev. 181, 1642 (1969) I.Bergstrom, C.J.Herrlander, P.Thieberger, J.Blomqvist High-Spin Three-Particle States in 207Bi RADIOACTIVITY 207Bi [from 205Tl(α, 2n)]; measured T1/2, Eγ, Iγ. 207Bi deduced levels, J.
doi: 10.1103/PhysRev.181.1642
1969LU05 Nucl.Phys. A135, 49 (1969) A.Luukko, A.Kerek, I.Rezanka, C.J.Herrlander Levels in Doubly Even Tellurium Isotopes 114,116,118Te Populated in (α, 2n) Reactions NUCLEAR REACTIONS 112,114,116Sn(α, 2nγ), Eα = 28.9, 33.5, 39.1, 43.0 MeV; measured σ(Eγ, θ). 114,116,118Te deduced levels, J, π. Enriched targets.
doi: 10.1016/0375-9474(69)90146-8
1968JA11 Arkiv Fysik 37, 585 (1968) Decay Energy of 195Au and 175Hf RADIOACTIVITY 195Au, 175Hf; measured Eγ, Iγ, (X-ray)ce-coin; deduced K-capture probabilities, Q(EC). 175Hf deduced ICC, γ-branching.
1967ER01 Nucl.Phys. A92, 241 (1967) P.Erman, B.I.Deutch, C.J.Herrlander Nuclear Structure Effects in the 343 keV M1 Transition in 175Lu NUCLEAR STRUCTURE 175Hf; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0375-9474(67)90216-3
1966HE01 Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn. (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.515 (1966) L Subshell Measurements of Retarded Dipole Transitions
1965JA16 Res.Inst.For Phys., Stockholm, Annual Rept., p. 59 (1965) Measurements of K-Capture Probabilities NUCLEAR STRUCTURE 195Au, 175Hf; measured not abstracted; deduced nuclear properties.
1964HE19 Nucl.Phys. 58, 544 (1964) Penetration Effects in the K and L Internal Conversion Coefficients of the 279 keV Transition in Tl203 RADIOACTIVITY 203Pb[from Tl(p, n)]; measured ce, ICC, γ-mixing. Natural Tl target. 188Re, 192Ir, 198,199Au; measured ICC.
doi: 10.1016/0029-5582(64)90566-8
1963EW03 Bull.Am.Phys.Soc. 8, No.4, 333, J16 (1963) Penetration Matrix-Element Effects on Hindered E1 Transitions in Lu177 and Hf177 NUCLEAR STRUCTURE 175Yb, 177Yb, 177Lu; measured not abstracted; deduced nuclear properties.
1963WI04 Arkiv Fysik 23, 355 (1963) On the Decay of Pb200 NUCLEAR STRUCTURE 200Pb; measured not abstracted; deduced nuclear properties.
1962BE51 Arkiv Fysik 22, 395 (1962) I.Bergstrom, C.J.Herrlander, P.Thieberger, J.Uhler On Nuclear f5/2, p3/2 and p1/2 Level Spacings and Transition Probabilities in the Lead Region NUCLEAR STRUCTURE 201Hg, 201Pb, 203Pb, 205Pb; measured not abstracted; deduced nuclear properties.
1962HE07 Phys.Can. 18, No.3, 22, Abstr.4.11 (1962) The Decay of Hf181 NUCLEAR STRUCTURE 181Hf; measured not abstracted; deduced nuclear properties.
1962HE09 Bull.Am.Phys.Soc. 7, No.7, 491, QA5 (1962), Priv. Comm. (1962) Internal-Conversion Measurements of γ-Rays in Tl203 NUCLEAR STRUCTURE 203Pb; measured not abstracted; deduced nuclear properties.
1962HE12 AECL-1659, p.25 (1962) Studies of Relative L Subshell E2 Conversion Coefficients Correlated to the Penetration Matrix Element Effect in the 279 keV Gamma in Tl203 NUCLEAR STRUCTURE 203Pb; measured not abstracted; deduced nuclear properties.
1961BE29 Arkiv Fysik 20, 93 (1961) I.Bergstrom, C.J.Herrlander, P.Thieberger, J.Uhler On Nuclear f5/2, p3/2, p1/2 Level Spacings and Transition Probabilities in the Lead Region NUCLEAR STRUCTURE 205Bi, 203Bi, 201Pb, 201Bi, 201Tl; measured not abstracted; deduced nuclear properties.
1961HE15 Arkiv Fysik 20, 71 (1961) Coincidence Studies on the Decays of Bi206 and Bi205 NUCLEAR STRUCTURE 209Po, 205Bi, 206Bi; measured not abstracted; deduced nuclear properties.
1960HE03 Arkiv Fysik 16, 496A (1960) C.J.Herrlander, R.Stockendal, R.K.Gupta The Decay of Tl201 NUCLEAR STRUCTURE 201Tl; measured not abstracted; deduced nuclear properties.
1960HE05 Arkiv Fysik 17, 315 (1960) C.J.Herrlander, R.Stockendal, R.K.Gupta The Decay of Tl201 NUCLEAR STRUCTURE 201Tl; measured not abstracted; deduced nuclear properties.
1958RY76 Arkiv Fysik 13, 177 (1958) Gamma Transitions in the Decay of La142
1957HE43 Nuclear Phys. 3, 161 (1957) Excited Levels in Hg200 Studied from the Decay of Tl200
doi: 10.1016/0029-5582(57)90103-7
1957MC40 Nuclear Phys. 3, 513 (1957) J.A.McDonnell, R.Stockendal, C.J.Herrlander, I.Bergstrom Levels in Pb202 and Tl202 Populated from 3.62-h Pb202m
doi: 10.1016/0029-5582(57)90017-2
1956HE50 Nuclear Phys. 1, 643 (1956) C.J.Herrlander, R.Stockendal, J.A.McDonnell, I.Bergstrom The Isomer Pb204m
doi: 10.1016/0029-5582(56)90073-6
1955BE12 Phil.Mag. 46, 65 (1955) K.E.Bergkvist, I.Bergstrom, C.J.Herrlander, S.Hultberg, H.Slatis, E.Sokolowski, A.H.Wapstra, T.Wiedling Neutron Deficient Isotopes of Pb and Tl - II. Mass Numbers 204, 202, 201 and 200
doi: 10.1080/14786440108561195
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