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Search: Author = C.J.Herrlander

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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


1968JA11      Arkiv Fysik 37, 585 (1968)

A.Jasinski, C.J.Herrlander

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
Citations: PlumX Metrics


1966HE01      Proc.Intern.Conf.Internal Conversion Process, Nashville, Tenn. (1965), J.H.Hamilton, Ed., Academic Press, Inc., New York, p.515 (1966)

C.J.Herrlander, G.T.Ewan

L Subshell Measurements of Retarded Dipole Transitions


1965JA16      Res.Inst.For Phys., Stockholm, Annual Rept., p. 59 (1965)

A.Jasinski, C.J.Herrlander

Measurements of K-Capture Probabilities

NUCLEAR STRUCTURE 195Au, 175Hf; measured not abstracted; deduced nuclear properties.


1964HE19      Nucl.Phys. 58, 544 (1964)

C.J.Herrlander, R.L.Graham

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
Citations: PlumX Metrics


1963EW03      Bull.Am.Phys.Soc. 8, No.4, 333, J16 (1963)

G.T.Ewan, C.J.Herrlander

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)

B.Wirhed, C.J.Herrlander

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)

C.J.Herrlander, R.L.Graham

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)

C.J.Herrlander, R.L.Graham

Internal-Conversion Measurements of γ-Rays in Tl203

NUCLEAR STRUCTURE 203Pb; measured not abstracted; deduced nuclear properties.


1962HE12      AECL-1659, p.25 (1962)

C.J.Herrlander, R.L.Graham

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)

C.J.Herrlander

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)

H.Ryde, C.J.Herrlander

Gamma Transitions in the Decay of La142


1957HE43      Nuclear Phys. 3, 161 (1957)

C.J.Herrlander, T.R.Gerholm

Excited Levels in Hg200 Studied from the Decay of Tl200

doi: 10.1016/0029-5582(57)90103-7
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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