NSR Query Results

Output year order : Descending
Format : Normal

NSR database version of April 26, 2024.

Search: Author = E.Hammaren

Found 39 matches.

Back to query form

2000HJ01      Eur.Phys.J. A 7, 201 (2000)

T.Hjelt, K.W.Schmid, E.Hammaren, A.Faessler

Unrestricted Symmetry-Projected Hartree-Fock-Bogoliubov Calculations for Some PF-Shell Nuclei

NUCLEAR STRUCTURE ⁴⁶Ti, ⁵⁰Cr, ⁶²Zn; calculated levels, J, π, binding energy. Unrestricted HFB calculation, comparison with truncated shell model.

doi: 10.1007/s100500050382
Citations: PlumX Metrics

1998HA52      Eur.Phys.J. A 2, 371 (1998)

E.Hammaren, K.W.Schmid, A.Faessler

Unrestricted Symmetry-Projected Hartree-Fock-Bogoliubov Calculations for SD-Shell Nuclei

NUCLEAR STRUCTURE ²⁴Mg, ²⁸Si, ^26,27Al; calculated levels, J, π. Symmetry-projected HFB calculations with unrestricted vacua, comparisons with complete shell-model diagonalizations.

doi: 10.1007/s100500050133
Citations: PlumX Metrics

1993SU02      Phys.Rev. C47, 757 (1993)

J.Suhonen, E.Hammaren

Massive Neutrinos and Right-Handed Weak Currents in Double Beta Decay

RADIOACTIVITY ⁷⁶Ge(2β); analyzed T_1/2 data; deduced effective right-handed coupling upper limit, two scenarios for massive neutrinos.

doi: 10.1103/PhysRevC.47.757
Citations: PlumX Metrics

1992HA16      Nucl.Phys. A541, 226 (1992)

E.Hammaren, P.Heikkinen, K.W.Schmid, A.Faessler

Microscopic and Phenomenological Analysis of the Alaga Rule for Dipole States

NUCLEAR STRUCTURE ¹⁵⁶Gd, ¹⁶⁴Dy; calculated B(M1), γ-branching ratio for dipole excitations. Microscopic approach. Alaga rule phenomenological analysis.

doi: 10.1016/0375-9474(92)90095-2
Citations: PlumX Metrics

1992PE11      Nucl.Phys. A549, 352 (1992)

A.Petrovici, E.Hammaren, K.W.Schmid, F.Grummer, A.Faessler

Shape Coexistence in the A ≈ 70 Region Including Neutron-Proton Interaction and Unnatural-Parity Correlations in the Mean Field

NUCLEAR STRUCTURE ⁷²Ge, ⁷²Kr; calculated levels. ⁶⁸Ge; calculated levels, B(λ), spectroscopic quadrupole moments. Neutron-proton interaction, unnatural parity correlations, mean field approach.

doi: 10.1016/0375-9474(92)90084-W
Citations: PlumX Metrics

1987LI11      Nucl.Phys. A469, 348 (1987)

P.O.Lipas, P.Toivonen, E.Hammaren

IBA-1 Calculations of E2/M1 Mixing Ratios

NUCLEAR STRUCTURE ^{146,148,150,152}Sm, ^152,154,156Gd, ¹⁶²Dy, ^{162,164,166,168}Er, ¹⁷²Yb, ¹⁹⁰Os; calculated levels, δ(E2/M1). Interacting boson approximation.

doi: 10.1016/0375-9474(87)90115-1
Citations: PlumX Metrics

1986HA11      Phys.Lett. 171B, 347 (1986)

E.Hammaren, K.W.Schmid, A.Faessler, F.Grummer

Microscopic Prediction of the M1 Strength Distributions in Medium Heavy Nuclei

NUCLEAR STRUCTURE ^{128,130,132,134}Ce, ^126,128,130Ba; calculated B(M1); deduced branching state dependence.

doi: 10.1016/0370-2693(86)91418-8
Citations: PlumX Metrics

1986HA14      Nucl.Phys. A454, 301 (1986)

E.Hammaren, K.W.Schmid, F.Grummer, A.Faessler, B.Fladt

Microscopic Description of Even-Even Nuclei in the Mass A = 130 Region

NUCLEAR STRUCTURE ^{128,130,132,134}Ce, ^126,128,130Ba, ^120,124,126Xe; calculated levels, yrast sequence, transition energies, B(E2). ^{124,126,128,130,132}Ba; calculated two-quasiparticle contributions to ground band energies. ¹²⁸Ba; calculated static, electric quadrupole moments vs spin. ^126,130Ba; calculated g vs spin. Self-consistent HFB mean field, microscopic treatment.

doi: 10.1016/0375-9474(86)90271-X
Citations: PlumX Metrics

1986HA28      Nucl.Phys. A456, 317 (1986)

E.Hammaren, O.Hausser, H.R.Andrews, P.Taras, A.Larabee

¹³⁶Xe(¹³C, 4nγ) Reaction Study of ¹⁴⁵Nd

NUCLEAR REACTIONS ¹³⁶Xe(¹³C, 4nγ), E=49-60 MeV; measured E(γ), I(γ)(E), I(γ)(θ), γγ-, energy-coin. ¹⁴⁵Nd deduced levels, J, π. Pulsed beam, enriched solid ¹³⁶Xe target, Ge(Li) detectors.

doi: 10.1016/0375-9474(86)90396-9
Citations: PlumX Metrics

1986PA14      J.Phys.(London) G12, 1047 (1986)

A.Passoja, J.Kantele, M.Luontama, R.Julin, E.Hammaren, P.O.Lipas, P.Toivonen

Electromagnetic Decay of 0₂⁺ and O₃⁺ States in the N = 88-90 Nuclei of ^150,152Sm

RADIOACTIVITY ^152m,150mEu(EC), (β⁺), (β^-) [from ¹⁵⁰Sm(p, n), E=9.5 MeV; ¹⁵¹Eu(n, γ), E=thermal]; measured Iγ, Eγ, I(ce), I(ce)(X-ray)-coin. ^150,152Sm deduced levels, J, π, B(λ), E0 strength parameter. Enriched targets, Ge(Li) detectors, magnetic plus Si-Li conversion electron spectrometer. Interacting boson model.

doi: 10.1088/0305-4616/12/10/013
Citations: PlumX Metrics

1986SC19      Nucl.Phys. A456, 437 (1986)

K.W.Schmid, F.Grummer, E.Hammaren, M.Kyotoku, A.Faessler

Alignment and Electromagnetic Properties of the Yrast Bands in ¹²⁸Ba and ¹³⁰Ce: An analysis of the VAMPIR wave functions

NUCLEAR STRUCTURE ¹²⁸Ba, ¹³⁰Ce; calculated levels, yrast sequence, occupation probabilities, g, B(E2), static hexadecapole, dynamic quadrupole moments. HFB, angular momentum, particle number projection before variation.

doi: 10.1016/0375-9474(86)90404-5
Citations: PlumX Metrics

1985HA34      Nucl.Phys. A437, 1 (1985)

E.Hammaren, K.W.Schmid, F.Grummer, A.Faessler, B.Fladt

Microscopic Description of Odd-Mass Nuclei in the Mass A = 130 Region

NUCLEAR REACTIONS ^{130,132,134,136}Ba(d, p), E not given; calculated spectroscopic amplitudes. Microscopic model.

NUCLEAR STRUCTURE ^{127,129,131,133}Ce, ^{125,127,129,131}Ba, ^{123,125,127,129}Xe, ^127,129,131La, ^{123,125,127,129}Cs, ^{121,123,125,127}I; calculated levels, rotational parameters. ^132,134,136Ba; calculated one-neutron pickup spectroscopic amplitudes. ^{130,132,134,136}Ba; calculated one-proton stripping, one-proton pickup stripping spectroscopic amplitudes. Microscopic model.

doi: 10.1016/0375-9474(85)90225-8
Citations: PlumX Metrics

1985SC06      Nucl.Phys. A436, 417 (1985)

K.W.Schmid, F.Grummer, E.Hammaren, A.Faessler

VAMPIR Calculations for ¹²⁸Ba and ¹³⁰Ce: Two mechanisms of backbending

NUCLEAR STRUCTURE ¹²⁸Ba, ¹³⁰Ce; calculated yrast band, total binding energies, intrinsic pairing gap energy vs spin, quadrupole, hexadecapole moments, occupation numbers. HFB with spin, number projections before variation.

doi: 10.1016/0375-9474(85)90077-6
Citations: PlumX Metrics

1984KA12      Z.Phys. A316, 361 (1984)

R.Katajanheimo, R.Jaderholm, A.Siivola, T.Tuurnala, E.Hammaren, E.Liukkonen

Low-Lying Levels in the Nuclei ¹⁵¹Nd and ¹⁵⁵Sm

NUCLEAR REACTIONS ¹⁵⁰Nd, ¹⁵⁴Sm(d, pγ), E=10 MeV; measured γγ-coin. ¹⁵¹Nd deduced levels, tentative J, π, γ-branching. ¹⁵⁵Sm deduced levels, γ-branching. Axial particle-rotor model calculations.

doi: 10.1007/BF01439909
Citations: PlumX Metrics

1984KA35      Z.Phys. A319, 91 (1984)

R.Katajanheimo, H.Liljavirta, A.Siivola, E.Hammaren, E.Liukkonen

Low-Energy Rotational Bands in the Nucleus ¹⁵⁵Eu

NUCLEAR REACTIONS ¹⁵⁴Sm(³He, np), E=22, 27 MeV; measured Eγ, Iγ, γγ-coin. ¹⁵⁵Eu deduced levels, J, π, γ-branching, rotational parameters. Particle-rotor model.

doi: 10.1007/BF01429772
Citations: PlumX Metrics

1984KR02      J.Phys.(London) G10, 571 (1984)

T.I.Kracikova, M.Finger, V.N.Pavlov, V.A.Deryuga, P.O.Lipas, E.Hammaren, P.Toivonen

Nuclear Orientation Study of the Decay of ¹⁴⁶Eu

RADIOACTIVITY ¹⁴⁶Eu(EC), (β⁺) [from Er(p, X), E=660 MeV]; measured γ(θ), oriented nuclei; deduced orientation coefficients. ¹⁴⁶Sm deduced levels, J, π, δ, B(λ), X(E0/E2). Interacting boson approximation model.

doi: 10.1088/0305-4616/10/4/017
Citations: PlumX Metrics

1984KR09      J.Phys.(London) G10, 667 (1984)

T.I.Kracikova, M.Finger, J.Konicek, N.A.Lebedev, V.A.Deryuga, P.O.Lipas, E.Hammaren, P.Toivonen

Nuclear Orientation Study of the Decay of ¹⁴⁸Eu

NUCLEAR STRUCTURE ¹⁴⁸Sm; calculated levels, δ, B(E2), X(E0/E2), quasirotational band structure. Interacting boson model.

RADIOACTIVITY ¹⁴⁸Eu(EC), (β⁺), (α) [from Er(p, X), E=660 MeV]; measured γ(θ), oriented nuclei. ¹⁴⁸Sm deduced levels, J, π, δ, X(E0/E2). Interacting boson model.

doi: 10.1088/0305-4616/10/5/010
Citations: PlumX Metrics

1984KR14      J.Phys.(London) G10, 1115 (1984)

T.I.Kracikova, S.Davaa, M.Finger, M.I.Fominykh, W.D.Hamilton, P.O.Lipas, E.Hammaren, P.Toivonen

Nuclear Orientation Study of the Decay of ¹⁷²Lu

RADIOACTIVITY ¹⁷²Lu(EC) [from Ta(p, X)¹⁷²Hf(EC-decay)]; measured Eγ, Iγ, γ(θ), oriented nuclei. ¹⁷²Yb levels deduced J, π, γ-branching, δ, X(E0/E2), monopole transition density. Mass separated source implantation in Gd, Fe, ³He-⁴He dilution refrigerator, Ge(Li) detectors. Interacting boson model.

doi: 10.1088/0305-4616/10/8/016
Citations: PlumX Metrics

1984LI06      Phys.Lett. 139B, 10 (1984)

P.O.Lipas, E.Hammaren, P.Toivonen

IBA-1 Calculation of E2/M1 Mixing Ratios in ¹⁵⁴Gd

NUCLEAR STRUCTURE ¹⁵⁴Gd; calculated reduced (E2/M1) mixing ratio. Generalized interacting boson approximation.

doi: 10.1016/0370-2693(84)90023-6
Citations: PlumX Metrics

1984RA03      Nucl.Phys. A414, 269 (1984)

T.Ramsoy, J.Rekstad, A.Henriquez, F.Ingebretsen, M.Guttormsen, E.Hammaren, T.F.Thorsteinsen

Deep-Lying νh_11/2 Hole States in ¹⁴⁵Nd

NUCLEAR REACTIONS ¹⁴⁶Nd(³He, α), E=26 MeV; measured σ(Eγ, θ), Eγ, Iγ, γα-coin. ¹⁴⁵Nd deduced levels, γ-ray multiplicity, level density, spectroscopic strength. Enriched target, Ge(Li), NaI(Tl), Si detectors. Fermi gas model analysis.

doi: 10.1016/0375-9474(84)90644-4
Citations: PlumX Metrics

1984RE04      Nucl.Phys. A417, 376 (1984)

J.Rekstad, B.Nordmoen, A.Henriques, F.Ingebretsen, S.Messelt, T.F.Thorsteinsen, E.Hammaren

The (³He, α) Strength Functions in Rare-Earth Nuclei

NUCLEAR REACTIONS ^156,157Gd, ¹⁷¹Yb(³He, α), E=26 MeV; measured σ(Eα, θ), αγ-coin. ^155,156Gd, ¹⁷⁰Yb levels deduced L, J, π, S. Enriched targets. DWBA calculations. Comparison to particle-plus-rotor model.

doi: 10.1016/0375-9474(84)90403-2
Citations: PlumX Metrics

1983LI06      Phys.Scr. 27, 8 (1983)

P.O.Lipas, J.Kumpulainen, E.Hammaren, T.Honkaranta, M.Finger, T.I.Kracikova, I.Prochazka, J.Ferencei

Study of Even Gd Nuclei by Decay of Oriented Tb, with Analysis by Simple Boson Models

NUCLEAR STRUCTURE ^{150,152,154,156,158,160}Gd; calculated levels, B(E2), monopole transition densities, B(E2)/B(E0). Interacting boson model.

RADIOACTIVITY ^150,152,154Tb(EC), (β⁺), ¹⁵⁶Tb(EC) [from Ta(p, X), E=660 MeV]; measured γ(θ), oriented nuclei. ^{150,152,154,156}Gd deduced levels, J, π, γ-multipolarity, δ, rotational band characteristics. TbGd samples, dilution refrigeration. Interacting boson model.

doi: 10.1088/0031-8949/27/1/002
Citations: PlumX Metrics

1983MA71      Nucl.Phys. A411, 125 (1983)

K.Maki-Kuutti, E.Hammaren

A Quasiparticle-Rotor Model with Variable Moments of Inertia: Application to ^149,151,153Sm and ¹⁰⁹Pd

NUCLEAR STRUCTURE ^149,151,153Sm, ¹⁰⁹Pd; calculated levels, rotational level characteristics. Quasiparticle-rotor model, variable moments of inertia.

doi: 10.1016/0375-9474(83)90511-0
Citations: PlumX Metrics

1983RE09      Phys.Scr. T5, 45 (1983)

J.Rekstad, A.Henriquez, F.Ingebretsen, G.Midttun, B.Skaali, R.Oyan, J.Wikne, T.Engeland, T.G.Thorsteinsen, E.Hammaren, E.Liukkonen

A Study of the Nuclear Structure at High Energy and Low Spin

NUCLEAR REACTIONS ^147,149Sm, ^155,157Gd, ^161,163Dy(³He, α), E=26 MeV; measured Eα, Iα, γα-coin, γ-multiplicity spectra; deduced structure change in deformed nuclei. ^146,148Sm, ¹⁵⁶Gd, ^160,162Dy deduced < Eγ > vs excitation energy. ¹⁵⁴Gd deduced < Eγ > vs excitation energy, γ-transition relative intensities.

doi: 10.1088/0031-8949/1983/T5/007
Citations: PlumX Metrics

1982HA17      Z.Phys. A305, 143 (1982)

E.Hammaren, D.G.Burke

Single-Proton States of ¹⁵⁹Ho Studied with the (p, α) Reaction. Spectroscopic Evidence for the Unusual Coriolis Strengths in ^159,161,163Ho Nuclei

NUCLEAR REACTIONS ^162,164Er(p, α), E=17 MeV; measured σ(Eα), σ(θ). ¹⁶¹Ho levels deduced normalization factors. ¹⁵⁹Ho deduced levels, J, π, S, rotational bands, Nilsson assignments. Enriched targets. Triton cluster transfer DWBA, Coriolis mixing calculations.

1982KA07      Nucl.Instrum.Methods 193, 495 (1982)

J.Kantele, E.Hammaren, D.G.Burke, J.C.Waddington

A Test of the Feasibility of γp-Coincidence Techniques in Conjunction with the (t, pγ) Reaction

NUCLEAR REACTIONS ¹⁵⁰Sm(t, pγ), E=15 MeV; measured Eγ, Iγ, pγ-coin. Ge(Li), Si-Au detectors.

doi: 10.1016/0029-554X(82)90241-5
Citations: PlumX Metrics

1982KA36      Phys.Scr. 26, 417 (1982)

R.Katajanheimo, A.Siivola, E.Liukkonen, E.Hammaren

Remeasurement of the Lifetime of the Isomeric (9/2)⁺ State in ¹⁵⁵Dy

NUCLEAR REACTIONS ¹⁵⁵Gd(³He, 3n), E=27 MeV; measured γ(³He)(t), E(K X-ray), I(K X-ray). ¹⁵⁵Dy deduced isomer T_1/2, level decay characteristics, hindrance factors. Particle-rotor model.

doi: 10.1088/0031-8949/26/6/001
Citations: PlumX Metrics

1981BU03      Nucl.Phys. A359, 36 (1981)

D.G.Burke, E.Hammaren, G.Lovhoiden, J.A.Cizewski, E.R.Flynn, J.W.Sunier

The Nuclear Structure of ^161,163Ho Studied with the (t(pol), α) Reaction

NUCLEAR REACTIONS ^162,164Er(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). ^161,163Ho deduced levels, J, π, Nilsson assignments. Enriched targets.

doi: 10.1016/0375-9474(81)90210-4
Citations: PlumX Metrics

1981BU10      Nucl.Phys. A366, 202 (1981)

D.G.Burke, E.Hammaren, C.L.Swift, J.A.Cizewski, E.R.Flynn, J.W.Sunier, G.Lovhoiden

The ¹⁵⁹Tb(t, α)¹⁵⁸Gd Reaction with 17 MeV Polarized Tritons

NUCLEAR REACTIONS ¹⁵⁹Tb(polarized t, α), E=17 MeV; measured σ(Eα, θ), A(Eα, θ). ¹⁵⁸Gd deduced levels, J, π, two-quasiparticle Nilsson assignments.

doi: 10.1016/0375-9474(81)90284-0
Citations: PlumX Metrics

1981PI09      Z.Phys. A300, 133 (1981)

M.Piiparinen, R.Pengo, Y.Nagai, E.Hammaren, P.Kleinheinz, N.Roy, L.Carlen, H.Ryde, Th.Lindblad, A.Johnson, S.A.Hjorth, J.Blomqvist

High Spin Shell Model Excitations in ¹⁴⁹Gd

NUCLEAR REACTIONS ¹⁵⁰Sm(α, 5n), E=67 MeV; ¹⁴⁹Sm(α, 4n), E=51 MeV; ¹⁴⁸Sm(α, 3n), E=44 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, linear polarization, I(ce). ¹⁴⁹Gd deduced levels, J, π, configuration, ICC, γ-branching, T_1/2, B(E2). Shell model.

doi: 10.1007/BF01412290
Citations: PlumX Metrics

1980HA13      Nucl.Phys. A339, 465 (1980)

E.Hammaren, E.Liukkonen, R.Katajanheimo, T.Tuurnala

Nanosecond Lifetimes of the Low-Spin States in the Nucleus ¹⁴⁷Nd. A Particle-Rotor Model Interpretation of the Results

NUCLEAR REACTIONS ¹⁴⁶Nd(d, pγ), E=10 MeV; measured Eγ, Iγ, γγ-coin, γ(t). ¹⁴⁷Nd levels deduced T_1/2, B(λ). Enriched target. Intrinsic Ge, Ge(Li) detectors, pulsed beam. Rotational model interpretation.

doi: 10.1016/0375-9474(80)90027-5
Citations: PlumX Metrics

1980KO07      Nucl.Phys. A337, 464 (1980)

J.Kownacki, Z.Sujkowski, E.Hammaren, E.Liukkonen, M.Piiparinen, T.Lindblad, H.Ryde, V.Paar

Excited States in ¹⁴⁶Sm and ¹⁴⁷Sm

NUCLEAR REACTIONS ^144,146Nd(α, 2n), (α, 3n), E=20-43 MeV; ^146,148Nd(³He, 3n), (³He, 4n), E=19-27 MeV; measured Eγ, Iγ(E), Iγ(θ), γγ(t), αγ(t), I(ce). ^146,147Sm deduced levels, J, π, T_1/2, ICC. Enriched targets, Ge(Li), Ge detectors, solenoidal, double focusing electron spectrometers with Si(Li) detectors.

doi: 10.1016/0375-9474(80)90154-2
Citations: PlumX Metrics

1979HA19      Nucl.Phys. A321, 71 (1979)

E.Hammaren, E.Liukkonen, M.Piiparinen, J.Kownacki, Z.Sujkowski, T.Lindblad, H.Ryde

Structural Connections between ¹⁴⁸Sm and ¹⁴⁹Sm Nuclei

NUCLEAR REACTIONS ¹⁴⁶Nd(α, 2n), ¹⁴⁸Nd(α, 3n), E=20-37 MeV; ¹⁴⁸Nd(³He, 3n), ¹⁵⁰Nd(³He, 4n), E=19-27 MeV; measured Eγ, Iγ(E), Iγ(θ), γγ-coin, αγ(t), Iγ(t), I(ce), I(ce)(t). ^148,149Sm deduced levels, J, π, T_1/2, ICC. Enriched targets. Ge(Li), Ge intrinsic detectors, solenoidal, double focussing electron spectrometers, Si(Li) detectors.

doi: 10.1016/0375-9474(79)90686-9
Citations: PlumX Metrics

1979KA11      Phys.Scr. 19, 497 (1979)

R.Katajanheimo, E.Hammaren

Particle-Rotor Model Study of the Transitional N = 89 and Some N = 91-95 Nuclei

NUCLEAR STRUCTURE ^161,163Er, ^155,157,161Dy, ^153,155,157Gd, ^151,153Sm, ¹⁴⁹Nd; calculated energy levels, relative Iγ; deduced Nilsson assignments. Particle-rotor model.

doi: 10.1088/0031-8949/19/5-6/002
Citations: PlumX Metrics

1979KA16      Phys.Scr. 20, 125 (1979)

R.Katajanheimo, A.Siivola, T.Tuurnala, E.Hammaren, E.Liukkonen

The Isomeric 9/2⁺ and the Lowest 7/2^- State in the Weakly Deformed N = 89 Nuclei

NUCLEAR REACTIONS ¹⁴⁸Nd(d, pγ), E=10 MeV; ¹⁵⁴Sm(³He, 4nγ), ¹⁵⁵Gd(³He, 3nγ), E=27 MeV; measured γγ(t), pγ(t), Eγ. ¹⁴⁹Nd, ¹⁵¹Sm, ¹⁵³Gd, ^155,157Dy, ^159,161Er deduced levels, T_1/2, J, π. Nilsson assignments, B(E1) particle-rotor model, nonspheroidal Woods-Saxon potential.

doi: 10.1088/0031-8949/20/1/023
Citations: PlumX Metrics

1979KO35      Nucl.Phys. A332, 422 (1979)

M.Kortelahti, A.Pakkanen, M.Piiparinen, E.Hammaren, T.Komppa, R.Komu

In-Beam Study and a Rotational Description of Low-Lying Levels in the N = 88 Nucleus ¹⁴⁹Pm

NUCLEAR REACTIONS ¹⁵⁰Nd(p, 2nγ), E=12.1-15.8 MeV; measured Eγ, Iγ(E), Iγ(θ), γγ-coin, pγ-delay. ¹⁴⁹Pm deduced levels, J, π, T_1/2. Enriched targets.

doi: 10.1016/0375-9474(79)90011-3
Citations: PlumX Metrics

1978KA16      Z.Phys. A286, 57 (1978)

R.Katajanheimo, T.Tuurnala, E.Hammaren

Level Structure of ¹⁷⁰Er Observed in the Decay of the 2.76 min ¹⁷⁰Ho

RADIOACTIVITY ¹⁷⁰Ho [from ¹⁷⁰Er(n, p)]; measured Eβ, T_1/2, Eγ, Iγ, γγ-coin, βγ-coin; deduced Q, log ft. ¹⁷⁰Er deduced levels, J, π, λ. ¹⁶⁹Ho; measured T_1/2.

doi: 10.1007/BF01434613
Citations: PlumX Metrics

1977TU01      Z.Phys. A280, 309 (1977)

T.Tuurnala, R.Katajanheimo, E.Hammaren

States of ¹⁶⁷Ho from the Decay of Neutron Rich Nuclide ¹⁶⁷Dy

RADIOACTIVITY ¹⁶⁷Dy; measured T_1/2, Eβ, γγ-, βγ-coin, Eγ, Iγ, γ(t), I(ce); deduced Q, ICC. ¹⁶⁷Ho deduced levels, K, J, π, λ, B(λ).

doi: 10.1007/BF01434358
Citations: PlumX Metrics

1975HA18      Z.Phys. A272, 341 (1975)

E.Hammaren, P.Puhakka, A.Siivola, T.Tuurnala

Low-Spin States in ¹⁵¹Gd

RADIOACTIVITY ¹⁵¹Tb; measured Eγ, Iγ, I(ce), γγ-coin; deduced ICC, log ft. ¹⁵¹Gd deduced levels, J, π, λ, β.