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NSR database version of April 11, 2024.

Search: Author = A.Backlin

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2006SR01      Nucl.Phys. A766, 25 (2006)

J.Srebrny, T.Czosnyka, Ch.Droste, S.G.Rohozinski, L.Prochniak, K.Zajac, K.Pomorski, D.Cline, C.Y.Wu, A.Backlin, L.Hasselgren, R.M.Diamond, D.Habs, H.J.Korner, F.S.Stephens, C.Baktash, R.P.Kostecki

Experimental and theoretical investigations of quadrupole collective degrees of freedom in 104Ru

NUCLEAR REACTIONS 104Ru(208Pb, 208Pb'), E=954 MeV; 104Ru(136Xe, 136Xe'), E=525 MeV; 104Ru(58Ni, 58Ni'), E=165, 190 MeV; measured Eγ, Iγ, (particle)γ -coin following Coulomb excitation. 104Ru deduced levels, J, π, E2 and M1 matrix elements, quadrupole collectivity. Comparison with model predictions.

doi: 10.1016/j.nuclphysa.2005.11.013
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1996WU07      Nucl.Phys. A607, 178 (1996)

C.Y.Wu, D.Cline, T.Czosnyka, A.Backlin, C.Baktash, R.M.Diamond, G.D.Dracoulis, L.Hasselgren, H.Kluge, B.Kotlinski, J.R.Leigh, J.O.Newton, W.R.Phillips, S.H.Sie, J.Srebrny, F.S.Stephens

Quadrupole Collectivity and Shapes of Os-Pt Nuclei

NUCLEAR REACTIONS 186,188,190,192Os, 194Pt(40Ca, 40Ca'), (58Ni, 58Ni'), (136Xe, 136Xe'), (208Pb, 208Pb'), E=3.3-4.8 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. 186,188,190,192Os, 194Pt deduced levels, J, π, E2, M1 matrix elements.

doi: 10.1016/0375-9474(96)00181-9
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1995FA18      Phys.Scr. T56, 243 (1995)

C.Fahlander, A.Atac, J.Blomqvist, A.Backlin, A.Hakansson, L.-O.Norlin, J.Nyberg, M.Piiparinen, D.Seweryniak

On the 2485 keV γ-Ray Line in 208Pb

NUCLEAR REACTIONS 208Pb(84Kr, 84Kr'), E=5 MeV/nucleon; measured γγ-coin; deduced evidence for 2.485 MeV γ-ray. 208Pb deduced no definitive evidence for transition.

doi: 10.1088/0031-8949/1995/T56/038
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1995KA29      Nucl.Phys. A593, 177 (1995)

A.E.Kavka, C.Fahlander, A.Backlin, D.Cline, T.Czosnyka, R.M.Diamond, D.Disdier, W.J.Kernan, L.Kraus, I.Linck, N.Schulz, J.Srebrny, F.S.Stephens, L.E.Svensson, B.Varnestig, E.G.Vogt, C.Y.Wu

Coulomb Excitation of 76,80,82Se

NUCLEAR REACTIONS 82Se(16O, 16O'), E=34 MeV; 48Ti(76Se, 76Se'), E=186 MeV; 48Ti(80Se, 80Se'), (82Se, 82Se'), E=195 MeV; 76Se(208Pb, 208Pb'), E=934 MeV; 208Pb(80Se, 80Se'), (82Se, 82Se'), E=312 MeV; measured (projectile)γ(θ), (projectile)(recoil)γ(θ) following Coulomb excitation. 76,80,82Se levels deduced B(E2), quadrupole moments. Enriched targets, Ge detectors, parallel-plate avalanche gas counters.

doi: 10.1016/0375-9474(95)00327-W
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1995SV01      Nucl.Phys. A584, 547 (1995)

L.E.Svensson, C.Fahlander, L.Hasselgren, A.Backlin, L.Westerberg, D.Cline, T.Czosnyka, C.Y.Wu, R.M.Diamond, H.Kluge

Multiphonon Vibrational States in 106,108Pd

NUCLEAR REACTIONS 106,108Pd(16O, 16O'), E=48 MeV; 106,108Pd(58Ni, 58Ni'), E=165.5 MeV; 106,108Pd(208Pb, 208Pb'), E=878 MeV; measured γγ-coin, pγ(θ), ppγ(θ) following Coulomb excitation; deduced 102-110Pd, 114Cd systematics. 106,108Pd deduced high-spin levels B(E2), quadrupole moments. Enriched targets.

doi: 10.1016/0375-9474(94)00514-N
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1992BA61      Nucl.Instrum.Methods Phys.Res. A317, 357 (1992)

P.Baltzer, K.G.Gorsten, A.Backlin

A Pulse-Counting Ionization Chamber for Measuring the Radon Concentration in Air

RADIOACTIVITY 218,216,214,202,208Po(α); 222Rn(α); measured Eα, Iα. Pulse counting ionization chamber for measuring radon concentration in air.

doi: 10.1016/0168-9002(92)90629-I
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1992FA01      Nucl.Phys. A537, 183 (1992)

C.Fahlander, I.Thorslund, B.Varnestig, A.Backlin, L.E.Svensson, D.Disdier, L.Kraus, I.Linck, N.Schulz, J.Pedersen, D.Cline

Triaxiality in 166Er

NUCLEAR REACTIONS 166Er(16O, 16O'), E=57 MeV; 166Er(32S, 32S'), E=115, 120 MeV; 166Er(58Ni, 58Ni'), E=221 MeV; measured pγ(θ) following Coulomb excitation. 166Er levels deduced B(E2), quadrupole moments. Enriched targets.

doi: 10.1016/0375-9474(92)90164-F
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1992FA05      Nucl.Phys. A541, 157 (1992)

C.Fahlander, B.Varnestig, A.Backlin, L.E.Svensson, D.Disdier, L.Kraus, I.Linck, N.Schulz, J.Pedersen

Coulomb Excitation of 172Yb

NUCLEAR REACTIONS 172Yb(16O, 16O'), E=57 MeV; 172Yb(32S, 32S'), E=115 MeV; 172Yb(58Ni, 58Ni'), E=224 MeV; measured (particle)γ(θ) following Coulomb excitation. 172Yb levels deduced B(E2), quadrupole moments. Enriched targets.

doi: 10.1016/0375-9474(92)90640-6
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1992TH04      Z.Phys. A342, 35 (1992)

I.Thorslund, C.Fahlander, A.Backlin, B.Kotlinski, D.Cline, A.T.Renalds, E.G.Vogt

Lifetime Measurements in 166Er

NUCLEAR REACTIONS 166Er(58Ni, 58Ni'), E=227 MeV; measured (particle)γ-coin, recoil distance. 166Er levels deduced T1/2, B(λ), γ-branching.

doi: 10.1007/BF01294486
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1990KO30      Nucl.Phys. A517, 365 (1990)

B.Kotlinski, D.Cline, A.Backlin, K.G.Helmer, A.E.Kavka, W.J.Kernan, E.G.Vogt, C.Y.Wu, R.M.Diamond, A.O.Macchiavelli, M.A.Deleplanque

Coulomb Excitation of 168Er

NUCLEAR REACTIONS 168Er(208Pb, 208Pb'), E=950 MeV; 168Er(58Ni, 58Ni'), E=220 MeV; 168Er(40Ca, 40Ca'), E=150 MeV; measured (particle)γ(θ), Eγ, Iγ, recoil distance following Coulomb excitation. 168Er levels deduced T1/2, δ, E2 matrix elements.

doi: 10.1016/0375-9474(90)90040-S
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1990KO38      Nucl.Phys. A519, 646 (1990)

B.Kotlinski, T.Czosnyka, D.Cline, J.Srebrny, C.Y.Wu, A.Backlin, L.Hasselgren, L.Westerberg, C.Baktash, S.G.Steadman

Heavy-Ion Coulomb Excitation of 72Ge

NUCLEAR REACTIONS 72Ge(16O, 16O'), E=35 MeV; 72Ge(58Ni, 58Ni'), E=155 MeV; 72Ge(208Pb, 208Pb'), E=270 MeV; measured Eγ, Iγ, (particle)γ-coin following Coulomb excitation. 72Ge levels deduced E2 matrix elements.

doi: 10.1016/0375-9474(90)90451-Q
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1989KO40      Nucl.Phys. A503, 575 (1989)

B.Kotlinski, D.Cline, A.Backlin, D.Clark

Lifetime Measurements of States in 110Pd

NUCLEAR REACTIONS 110Pd(58Ni, 58Ni'), E=190 MeV; measured recoil distance decay curves following Coulomb excitation, pγ-coin. 110Pd levels deduced T1/2, E2 matrix elements. Comparison with theory.

doi: 10.1016/0375-9474(89)90250-9
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1988FA07      Nucl.Phys. A485, 327 (1988)

C.Fahlander, A.Backlin, L.Hasselgren, A.Kavka, V.Mittal, L.E.Svensson, B.Varnestig, D.Cline, B.Kotlinski, H.Grein, E.Grosse, R.Kulessa, C.Michel, W.Spreng, H.J.Wollersheim, J.Stachel

Quadrupole Collective Properties of 114Cd

NUCLEAR REACTIONS 114Cd(16O, 16O'), E=45 MeV; 114Cd(40Ca, 40Ca'), E=122 MeV; 114Cd(58Ni, 58Ni'), E=184 MeV; 114Cd(208Pb, 208Pb'), E=916 MeV; measured ppγ(θ) following Coulomb excitation. 114Cd levels deduced B(E2), quadrupole moment. Enriched targets.

doi: 10.1016/0375-9474(88)90106-6
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1986GO02      Phys.Rev. C33, 793 (1986)

I.M.Govil, H.W.Fulbright, D.Cline, E.Wesolowski, B.Kotlinski, A.Backlin, K.Gridnev

Multipole Collectivity in 168Er from Inelastic Scattering

NUCLEAR REACTIONS 168Er(α, α), (α, α'), E=36 MeV; 168Er(d, d), (d, d'), E=16 MeV; measured σ(θ), σ(Eα'); deduced optical model parameters. 168Er deduced octupole states, β4, β6 shape components, B(λ). Coupled-channels calculation, collective model form factors.

doi: 10.1103/PhysRevC.33.793
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1986LU06      Z.Phys. A324, 317 (1986)

M.Luontama, R.Julin, J.Kantele, A.Passoja, W.Trzaska, A.Backlin, N.-G.Jonsson, L.Westerberg

Electromagnetic Properties of Low-Spin States in 102,104Pd

NUCLEAR REACTIONS 102Pd(p, p'), (p, 2n), E=6-15 MeV; measured p'γ-coin, I(ce), γ(t). 102,104Pd(16O, 16O'), E=44 MeV; measured Eγ, Iγ following Coulomb excitation. 102,104Pd levels deduced B(λ), relative σ.


1986VA24      Nucl.Instrum.Methods Phys.Res. A248, 419 (1986)

B.Varnestig, A.Backlin, C.Fahlander, A.E.Kavka, T.Lenke, L.E.Svensson

A Position Sensitive Gas Detector System for Coulomb Excitation Experiments

NUCLEAR REACTIONS 208Pb(82Se, X), E=312 MeV; measured Eγ, Iγ. 172Yb(32S, 32S'), E=115 MeV; measured Eγ, Iγ following Coulomb excitation. 172Yb level deduced population angular dependence. Position sensitive gas detector.

doi: 10.1016/0168-9002(86)91027-2
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1982BA28      Nucl.Phys. A380, 189 (1982)

A.Backlin, G.Hedin, B.Fogelberg, M.Saraceno, R.C.Greenwood, C.W.Reich, H.R.Koch, H.A.Baader, H.D.Breitig, O.W.B.Schult, K.Schreckenbach, T.Von Egidy, W.Mampe

Levels in 156Gd Studied in the (n, γ) Reaction

NUCLEAR REACTIONS 155Gd(n, γ), E=thermal, resonance; measured Eγ, Iγ, I(ce). 156Gd deduced levels, J, π, ICC, B(λ), neutron binding energy. Ge(Li) detectors, curved-crystal spectrometer, magnetic electron-spectrometers, enriched targets.

doi: 10.1016/0375-9474(82)90104-X
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1981BA05      Nucl.Phys. A351, 490 (1981)

A.Backlin, N.G.Jonsson, R.Julin, J.Kantele, M.Luontama, A.Passoja, T.Poikolainen

0+ States and E0 and E2 Transition Rates in Even Sn Nuclei

NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(16O, 16O'), E=48 MeV; measured Eγ, Iγ, γγ-coin, Coulomb excitation; 112,114,116,118,120,122,124Sn(p, p'γ), E not given; measured Iγ, Eγ, I(ce), γp'-, (ce)p'-coin, γp(t), (ce)p(t), Coulomb excitation; 124Sn(p, 2n), E not given; measured Eγ, Iγ, I(ce). 112,114,116,118,120,122,124Sn deduced levels, J, π, ICC, B(E0), B(E2), sign of matrix product.

RADIOACTIVITY 116,118,120Sb; measured Iγ, I(ce), γγ(θ); 116,118In; measured Iγ, I(ce), βγ-coin. 116,118Sn deduced levels, J, π, B(λ). Ge(Li), annular NaI detectors, magnetic spectrometers, enriched targets.

doi: 10.1016/0375-9474(81)90184-6
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1981JO03      Nucl.Phys. A371, 333 (1981)

N.-G.Jonsson, A.Backlin, J.Kantele, R.Julin, M.Luontama, A.Passoja

Collective States in Even Sn Nuclei

NUCLEAR REACTIONS 112,114,116,118,120,122,124Sn(16O, 16O'γ), E=48 MeV; measured Eγ, Iγ, γγ-coin. 112,114,116,118,120,122,124Sn(p, p'γ), E=6-8 MeV; measured Eγ, Iγ. 112,114,116,118,120,122,124Sn deduced B(E2), B(E3), B(E1). Ge(Li), NaI detectors. Enriched targets.

RADIOACTIVITY 116Sb; measured Iγ. 116Sn deduced B(E2) ratio.

doi: 10.1016/0375-9474(81)90071-3
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1980JU05      Z.Phys. A296, 315 (1980)

R.Julin, J.Kantele, M.Luontama, A.Passoja, T.Poikolainen, A.Backlin, N.-G.Jonsson

Decay Characteristics of 0+2 and 0+3 States in 112Cd and 114Cd

RADIOACTIVITY 112Cd [from 111Cd(d, p), E=9 MeV; 112Cd(p, n)112In(β-decay)], 114Cd [from 113Cd(d, p), E=8 MeV]; measured Eγ, Iγ, I(ce), T1/2, γγ-, e-p-, γp-coin. 112,114Cd levels deduced B(E2), T1/2.

NUCLEAR REACTIONS Cd(16O, 16O'), E=44 MeV; measured double Coulomb excitation σ. 112,114Cd levels deduced B(E2), T1/2. Metallic Cd target.

doi: 10.1007/BF01438525
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1979KA01      Z.Phys. A289, 157 (1979)

J.Kantele, R.Julin, M.Luontama, A.Passoja, T.Poikolainen, A.Backlin, N.-G.Jonsson

Absolute E0 and E2 Transition Rates and Collective States in 116Sn

NUCLEAR REACTIONS 116Sn(16O, 16O'), E=48 MeV; measured σ(Coulomb-excitation). 116Sn deduced absolute E0, E2 transition rates. Discussed deformed excited states.

doi: 10.1007/BF01435933
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1978GR14      Nucl.Phys. A304, 327 (1978)

R.C.Greenwood, C.W.Reich, H.A.Baader, H.R.Koch, D.Breitig, O.W.B.Schult, B.Fogelberg, A.Backlin, W.Mampe, T.von Egidy, E.Schreckenbach

Collective and Two-Quasiparticle States in 158Gd Observed Through Study of Radiative Neutron Capture in 157Gd

NUCLEAR REACTIONS 157Gd(n, γ), E=thermal, averaged-resonance; measured Eγ, Iγ, I(ce), γγ-coin. 158Gd deduced levels, J, π, ICC, B(λ), neutron binding energy. Ge(Li) detectors, curved-crystal spectrometer, magnetic-electron spectrometers. Enriched, natural targets.

doi: 10.1016/0375-9474(78)90242-7
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1978JO07      Nucl.Instrum.Methods 152, 485 (1978)

N.-G.Jonsson, J.Kantele, A.Backlin

A High-Efficiency Coincidence Method for Coulomb Excitation Studies of Weakly Populated Vibration-Like Levels

NUCLEAR REACTIONS 112,114Cd(16O, 16O'γ), E=44 MeV; 118Sn(16O, 16O'γ), E=48 MeV; measured Coulomb excitation. 112,114Cd, 118Sn levels deduced B(E2).

doi: 10.1016/0029-554X(78)90050-2
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1976BA32      Phys.Lett. 62B, 402 (1976)

A.Backlin, W.Dietrich, R.Julin, J.Kantele, M.Luontama, L.Westerberg

E0 Transitions in 114,116,118Sn

RADIOACTIVITY 118Sb; measured I(ce). 118Sn level deduced B(E0)/B(E2).

NUCLEAR REACTIONS 114,116,118Sn(p, p'), E=6.40-6.92 MeV; measured I(ce). 114,116Sn levels deduced B(E0)/B(E2).

doi: 10.1016/0370-2693(76)90668-7
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1976DI03      Z.Phys. A276, 133 (1976)

W.Dietrich, A.Backlin

Excited Levels of 111In and 113In

NUCLEAR REACTIONS 111,113Cd(p, nγ), E=6-11 MeV; measured σ(E, Eγ, θ), γγ-coin, I(ce). 111,113In deduced levels, ICC, J, π, λ.

doi: 10.1007/BF01437708
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1976FO10      Nucl.Phys. A267, 317 (1976)

B.Fogelberg, Y.Kawase, J.McDonald, A.Backlin

Levels in 117Cd Studied in the Decays of 117Ag and 117mAg

RADIOACTIVITY 117Ag [from 235U(n, F)]; measured T1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. 117Cd deduced levels, J, π, T1/2, γ-multipolarity, B(E1), B(E2), B(M1). Mass separated fission product. Ge(Li), Si(Li), NaI, plastic detectors.

doi: 10.1016/0375-9474(76)90663-1
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1976SV02      Nucl.Phys. A267, 190 (1976)

L.-G.Svensson, D.G.Sarantites, A.Backlin

Coulomb Excitation of 99Tc

NUCLEAR REACTIONS 99Tc(α, α'γ), E=10 MeV; 99Tc(16O, 16O'γ), E=28-42 MeV; measured relative σ(E, Eγ, θ), γγ-coin, DSA. 99Tc deduced levels, J, T1/2, δ, B(E2), B(M1).

doi: 10.1016/0375-9474(76)90653-9
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1976SV04      Phys.Scr. 14, 129 (1976)

L.-G.Svensson, O.Bergman, A.Backlin, N.-G.Jonsson, J.Lindskog

Transition Probabilities of the 9/2+ → 7/2+ Transitions in Odd-Mass Ag Isotopes

RADIOACTIVITY 105,107Cd, 111Pd; measured I(ce), γX-ray(t). 107,105,111Ag levels deduced T1/2, ICC, B(λ).

doi: 10.1088/0031-8949/14/4/001
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1975DI09      Phys.Scr. 12, 80 (1975)

W.Dietrich, B.Nyman, A.Johansson, A.Backlin

Excited States in 103Pd

RADIOACTIVITY 103Ag; measured Eγ, Iγ, γγ-coin, T1/2; deduced log ft. 103Pd deduced levels, J, π.

NUCLEAR REACTIONS 103Rh(p, nγ), E=6.3-12 MeV; measured σ(E, Eγ, θ), I(ce), γγ-coin, γ(t). 103Pd deduced levels, J, π, T1/2, ICC, λ.

doi: 10.1088/0031-8949/12/1-2/009
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1975DI12      Nucl.Phys. A253, 429 (1975)

W.Dietrich, A.Backlin, C.O.Lannergard, I.Ragnarsson

Possible Rotational States in Odd In Nuclei

NUCLEAR REACTIONS 106,108Cd(d, nγ), E=5-11 MeV; measured σ(E, Eγ, θ), γγ(t), nγ-coin, I(ce). 107,109In deduced levels, J, π, λ, ICC. Enriched targets.

doi: 10.1016/0375-9474(75)90490-X
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1975DI15      Phys.Scr. 12, 271 (1975)

W.Dietrich, G.C.Madueme, L.Westerberg, A.Backlin

Search for Low-Spin Negative Parity States in 97Mo and 99Mo

NUCLEAR REACTIONS 96,98Mo(d, pγ), E=4-12 MeV; measured Eγ, Iγ, I(ce), γγ-coin, pγ-coin, γ(θ, t). 97,99Mo deduced levels, J, π, T1/2, λ.

doi: 10.1088/0031-8949/12/5/004
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1975KA09      Nucl.Phys. A241, 237 (1975)

Y.Kawase, B.Fogelberg, J.McDonald, A.Backlin

States in 119Cd Studied in the Decay of 119Ag

RADIOACTIVITY 119Ag [from 235U(n, F)]; measured T1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. 119Cd deduced levels, J, π, T1/2, γ-multipolarity, B(E1), B(E2), B(M1). Mass separated fission product. Ge(Li), Si(Li), NaI, plastic detectors.

doi: 10.1016/0375-9474(75)90315-2
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1974BE24      Nucl.Phys. A223, 342 (1974)

C.Bergman, B.Svahn, L.-G.Svensson, A.Backlin, J.Lindskog

Transition Rates in 97Tc

RADIOACTIVITY 97Ru [from Rh(p, xnyp)]; measured I(ce), Auger-ce delay. 97Tc levels deduced T1/2, E2/M1 mixing ratios, B(M1), B(E2).

doi: 10.1016/0375-9474(74)90418-7
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1974MC09      Nucl.Phys. A224, 13 (1974); Erratum Nucl.Phys. A239, 530 (1975)

J.McDonald, B.Fogelberg, A.Backlin, Y.Kawase

The Decays of 2.6 min 119gCd and 1.9 min 119mCd to 119In

RADIOACTIVITY 119gCd, 119mCd [from 235U(n, F)]; measured T1/2, Eγ, Iγ, E(ce), I(ce), γγ coin, βγ, γγ delay, deduced multipolarities. 119In deduced levels, J, π, B(E1), B(E2). Isotopically separated 119Cd sources. Ge(Li), Si(Li), NaI(Tl), plastic detectors. Ge(Li)-Ge(Li) coin.

doi: 10.1016/0375-9474(74)90159-6
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1973NY03      Phys.Scr. 7, 265 (1973)

B.Nyman, A.Johansson, W.Dietrich, A.Backlin, H.Pettersson, B.Svahn, C.O.Lannergard

The Level Scheme of 107Cd Studied Through the 107Ag(p, nγ) and 106Cd(d, pγ) Reactions and the 107In Decay

RADIOACTIVITY 107In; measured Eγ, T1/2, Iγ, γγ(t), I(ce). Deduced ICC, log ft. 107mIn measured T1/2, Eγ, Iγ, I(ce). Deduced ICC. 107In deduced transitions, γ-multipolarity. 107Cd deduced levels, J, π, γ-multipolarities.

NUCLEAR REACTIONS 106Cd(d, pγ), E=6-11 MeV; 107Ag(p, nγ), E=3-12 MeV; measured Eγ, γγ-coin, Iγ, I(ce). Deduced ICC. 107Cd deduced levels, J, π, γ-multipolarities.

doi: 10.1088/0031-8949/7/6/004
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1972BA21      Nucl.Phys. A181, 76 (1972)

A.Backlin, G.Hedin, V.Berg, S.G.Malmskog

E2 and M1 Transition Probabilities between Low-Energy States in 189Ir

RADIOACTIVITY 189Pt; measured Eγ, Iγ, E(ce), I(ce), cece-delay. 189Ir deduced γ-mixing, γ-branching, T1/2, B(λ). Isotope-separated sources.

doi: 10.1016/0375-9474(72)90901-3
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1972HE05      Nucl.Phys. A184, 214 (1972)

G.Hedin, A.Backlin

Levels in 189Ir Studied in the Decay of 189Pt

RADIOACTIVITY 189Pt[from Pb(p, spallation)]; measured Eγ, Iγ, I(ce), γγ-coin; deduced log ft. 189Ir deduced levels, J, π, ICC, multipolarities. Isotope-separated sources. Ge(Li), Si(Li) detectors.

doi: 10.1016/0375-9474(72)90454-X
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1972MA05      Nucl.Phys. A179, 781 (1972); Erratum Nucl.Phys. A196, 636 (1972)

A.Marcinkowski, A.Backlin, I.Bergqvist

Levels in 115In Studied by Means of Inelastic Neutron Scattering

NUCLEAR REACTIONS 115In(n, n'γ), E=0.78-1.80 MeV; measured Eγ, Iγ, σ(E;Eγ). 115In deduced levels, J, π, γ-branching. Natural target, Ge(Li) detector.

doi: 10.1016/0375-9474(72)90619-7
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1971BA45      Nucl.Phys. A169, 122 (1971)

A.Backlin, G.Hedin, S.G.Malmskog

Levels in 191Ir

RADIOACTIVITY 191Pt[from Pb(p, 3pxn)]; measured Eγ, Iγ, E(ce), I(ce), γγ-coin; deduced log ft. 191Ir deduced levels, I, π, ICC, multipolarities. Isotope separated sources, Ge(Li) detector.

doi: 10.1016/0375-9474(71)90566-5
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1971FO12      Nucl.Phys. A171, 353 (1971)

B.Fogelberg, A.Backlin

Levels in 178Hf Studied in the (n, γ) Reaction

NUCLEAR REACTIONS 177Hf(n, γ), E=thermal;measuredeγ, Iγ, E(ce), I(ce), γγ-coin. 178Hf deduced levels, J, π, K, γ-multipolarity. Enriched target, Ge(Li) detectors.

doi: 10.1016/0375-9474(71)90028-5
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1971FO22      Phys.Lett. 36B, 334 (1971)

B.Fogelberg, A.Backlin, T.Nagarajan

Energy Levels in 114,116,118,120,122Cd as Observed in the Beta Decay of Ag Isotopes

RADIOACTIVITY 114,116,118,120,122Ag; measured Eγ, Iγ, γγ-coin, T1/2, I(ce), Iβ; deduced log ft. 114,116,118Ag, 120,122Ag deduced levels, J, π.

doi: 10.1016/0370-2693(71)90718-0
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1971HO04      Nucl.Phys. A163, 311 (1971)

A.Hoglund, S.G.Malmskog, A.Backlin, B.Fogelberg, B.Jonson

Transition Rates in 192Au

RADIOACTIVITY 192Hg[from Pb(p, 3pxn)]; measured E(ce), I(ce), cece-delay. 192Au levels deduced T1/2, γ-mixing, B(M1), B(E1), B(E2). Isotope separated sources.

doi: 10.1016/0375-9474(71)90539-2
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1971MA24      Nucl.Phys. A166, 573 (1971)

S.G.Malmskog, V.Berg, B.Fogelberg, A.Backlin

On the Low-Energy Band Structure in 187Os

RADIOACTIVITY 187Ir[from Pb(p, spallation)]; measured Eγ, Iγ, E(ce), I(ce), (ce)(ce)-delay. 187Os deduced levels, T1/2, J, π, ICC, multipolarities, partial half-lives. Isotope separated sources. Ge(Li) detectors.

doi: 10.1016/0375-9474(71)90907-9
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1971MC02      Nucl.Phys. A162, 365 (1971)

J.McDonald, A.Backlin, S.G.Malmskog

Transition Probabilities in 99Tc

RADIOACTIVITY 99Mo[from 98Mo(n, γ)]; measured I(ce), γce-, cece-delay. 99Tc deduced T1/2, ICC, Iγ, mixing ratios, B(E2), B(M1). Enriched target.

doi: 10.1016/0375-9474(71)90991-2
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1970AH05      Nucl.Phys. A154, 303 (1970)

B.Ahlesten, A.Backlin

Decay Properties of the 99 and 130 keV Levels in 195Pt

RADIOACTIVITY 195Au[from Pt(d, xn)]; measured I(ce), E(ce), Iγ. 195Pt transitions deduced ICC, γ-mixing, B(E2), B(M1).

doi: 10.1016/0375-9474(70)90158-2
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1970BA56      Nucl.Phys. A156, 647 (1970)

A.Backlin, V.Berg, S.G.Malmskog

Negative Parity States in Odd-Mass Ir and Au Nuclei

RADIOACTIVITY 193Os[from 192Os(n, γ)], 191,189Pt, 193Hg[from Pb(p, spallation)]; measured E(ce), I(ce), γγ-coin, cece-, γce-delay; deduced log ft. 193Au, 193,191,189Ir deduced levels, J, π, T1/2, γ-multipolarity.

doi: 10.1016/0375-9474(70)90260-5
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1970BE06      Nucl.Phys. A143, 177 (1970)

V.Berg, S.G.Malmskog, A.Backlin

The Level Structure in 193Ir

RADIOACTIVITY 193Os[from 192Os(n, γ)]; measured Eγ, Iγ, E(ce), I(ce), cece-delay; deduced log ft. 193Ir deduced levels, T1/2, J, π, ICC, γ-multipolarities, γ-mixing, B(M1), B(E2). Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(70)90689-5
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1970FO08      Nucl.Phys. A153, 301 (1970)

B.Fogelberg, A.Backlin, V.Berg, S.G.Malmskog

E2 and M1 Transition Probabilities in 193Au and 195Au

RADIOACTIVITY 193Hg, 195Hg[from Pb(p, 3pxn)]; measured Eγ, Iγ, E(ce), I(ce), cece-γce-delay. 193,195Au deduced levels, γ-mixing, γ-branching, T1/2, B(λ). Isotope separted sources.

doi: 10.1016/0375-9474(70)90773-6
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1970MA10      Nucl.Phys. A143, 160 (1970)

S.G.Malmskog, V.Berg, A.Backlin, G.Hedin

The Low-Energy Level Structure of 191Ir

RADIOACTIVITY 191Pt[from Pb(p, spallation)]; measured Eγ, Iγ, E(ce), I(ce), cece-delay. 191Ir deduced levels, T1/2, J, π, ICC, γ-multipolarities, γ-mixing, B(E2), B(M1), quadrupole moment. Isotope separated sources, Ge(Li) detector.

doi: 10.1016/0375-9474(70)90688-3
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1970MA37      Nucl.Phys. A153, 316 (1970)

S.G.Malmskog, V.Berg, A.Backlin

Transition Probabilities in 189Os

RADIOACTIVITY 189Ir[from Pb(p, spallation)]; measured Eγ, Iγ, E(ce), I(ce), cece-delay; deduced log ft. 189Os deduced levels, T1/2, J, π, ICC, multipolarities, mixing ratios, partial half-lives. Isotope separated sources, Si(Li), Ge(Li) detectors.

doi: 10.1016/0375-9474(70)90774-8
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1969BA11      Arkiv Fysik 39, 221 (1969)

A.Backlin, R.Boleu, B.Fogelberg

Gamma-Rays in the 1 MeV Region from the Reaction 161Dy(n, γ)162Dy

NUCLEAR REACTIONS 161Dy(n, γ), E = thermal; measured Eγ, Iγ. 162Dy deduced levels, K, J, π, branching ratio. Ge(Li) detector.


1969BA42      Nucl.Phys. A138, 429 (1969)

A.Backlin, F.Fogelberg, V.Berg, S.G.Malmskog

E2 and M1 Transition Probabilities in Odd-Mass Hg Nuclei

RADIOACTIVITY 193,195Hg; measured E(ce), I(ce), cece-delay. 193,195Hg levels deduced T1/2, ICC, γ-multipolarity, B(E2), B(M1).

doi: 10.1016/0375-9474(69)90347-9
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1969HE19      Arkiv Fysik 38, 593 (1969)

G.Hedin, A.Backlin

A Measurement of the K Conversion Coefficient of the 570 keV Transition in 207Pb

RADIOACTIVITY 207Bi; measured Eγ, Iγ, I(ce). 207Pb transitions deduced ICC, conversion line ratios.


1969MA07      Arkiv Fysik 39, 411 (1969)

S.G.Malmskog, A.Backlin

The Decay of 191Os

RADIOACTIVITY 191Os[from 190Os(n, γ)]; measured Eγ, Iγ, I(ce), cece-delay. 191Ir deduced levels, T1/2, γ-mixing, γ-branching.


1968FO07      NP-17722 (LF-23) (1968)

B.Fogelberg, A.Backlin

Precision Measurements in the Decay of 113Sn

RADIOACTIVITY 113Sn; measured Eγ, Iγ, I(ce). 113In transitions deduced γ-mixing, ICC.


1968HE19      Nucl.Instr.Methods 65, 31 (1968)

R.G.Helmer, A.Backlin

Numerical Construction of Level Schemes - 149Pm

RADIOACTIVITY 149Nd; measured Eγ. 149Pm deduced levels.

doi: 10.1016/0029-554X(68)90005-0
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1967BA17      Phys.Letters 24B, 389 (1967)

A.Backlin

E2/M1 Mixing Ratios of Transitions in 170Tm

NUCLEAR REACTIONS 169Tm(n, γ), E=thermal; measured I(ce), E(ce). 170Tm transitions deduced γ-mixing ratios.

doi: 10.1016/0370-2693(67)90299-7
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1967BA18      Nucl.Phys. A96, 539 (1967)

A.Backlin, B.Fogelberg, S.G.Malmskog

Possible Deformed States in 115In and 117In

RADIOACTIVITY 115Cd, 117Cd [from 114Cd, 116Cd(n, γ)]. Measured Eγ, Iγ, I(ce), βγ-, γce-delay. 115,117In deduced levels, T1/2, J, π, ICC, multipolarities, mixing ratios, partial half-lives. Enriched targets.

doi: 10.1016/0375-9474(67)90604-5
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1967BA21      Ark.Fys. 34, 459 (1967)

A.Backlin, S.G.Malmskog

Decay Properties of 147Nd

NUCLEAR REACTIONS 168,170,172,174,176Yb(d, d'), 171,173Yb(d, p), (d, t), E=12 MeV; measured σ(Ed'), σ(Ep), σ(Et). 168,170,172,174,176Yb deduced levels, J, π, K.


1967BA22      Ark.Fys. 34, 531 (1967)

A.Backlin, S.G.Malmskog

On the d5/2 - g7/2 Transitions in Odd Mass Pm Nuclei

NUCLEAR STRUCTURE 147Nd, 145Nd; measured not abstracted; deduced nuclear properties.


1967BA27      Arkiv Fysik 34, 495 (1967)

A.Backlin, S.G.Malmskog, H.Solhed

Transitions, Lifetimes and Levels in 149Pm

NUCLEAR STRUCTURE 147Nd, 147Pm, 141Pr, 141Ce, 199Hg, 199Au, 197Au, 197Hg, 203Hg, 203Tl, 170Tm, 165Ho, 165Dy, 161Tb, 161Dy, 152Sm, 152Eu, 149Nd, 170Yb; measured not abstracted; deduced nuclear properties.


1967BA34      Phys.Rev. 160, 1011 (1967)

A.Backlin, A.Suarez, O.W.B.Schult, B.P.K.Maier, U.Gruber, E.B.Shera, D.W.Hafemeister, W.N.Shelton, R.K.Sheline

Nuclear Levels of Dy162

NUCLEAR STRUCTURE 162Dy, 163Dy; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.160.1011
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1967BA45      Nucl.Phys. A103, 337 (1967)

A.Backlin, B.Fogelberg, S.G.Malmskog

Levels and Transition Rates in 199Au

RADIOACTIVITY 199Pt [from 198Pt(n, γ)]; measured Eγ, Iγ, E(ce), I(ce), βγ-, γγ-coin, βce-, cece-, ceγ-delay. 199Au deduced levels, T1/2, J, π, ICC, multipolarities, mixing ratios, partial half-lives. Enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(67)90257-6
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1967BA63      Arkiv Fysik 34, 59 (1967)

A.Backlin, S.G.Malmskog

On the Properties of the s1/2 → d3/2 Transition in 199Au

NUCLEAR STRUCTURE 199Pt, 197Pt; measured not abstracted; deduced nuclear properties.


1967BA76      Nucl.Instr.Methods 53, 177 (1967)

A.Backlin

A Computer Method for Deducing Nuclear Levels from Measured Transition Energies


1967MO05      Phys.Rev. 155, 1265 (1967)

H.T.Motz, E.T.Jurney, O.W.B.Schult, H.R.Koch, U.Gruber, B.P.Maier, H.Baader, G.L.Struble, J.Kern, R.K.Sheline, T.Von Egidy, T.Elze, E.Bieber, A.Backlin

Energy Levels of Ho166

NUCLEAR STRUCTURE 166Dy, 166Ho; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.155.1265
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1967SC05      Phys.Rev. 154, 1146 (1967)

O.W.B.Schult, M.E.Bunker, D.W.Hafemeister, E.B.Shera, E.T.Jurney, J.W.Starner, A.Backlin, B.Fogelberg, U.Gruber, B.P.K.Maier, H.R.Koch, W.N.Shelton, M.Minor, R.K.Sheline

Nuclear Levels in Dy163

NUCLEAR STRUCTURE 163Dy; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.154.1146
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1966BA10      Nucl.Phys. 80, 154 (1966)

A.Backlin, N.E.Holmberg, G.Backstrom

Internal Conversion Study of 113Cd(n, γ)114Cd

NUCLEAR REACTIONS 113Cd(n, γ), E = th; measured Eγ, I(ce). 114Cd deduced levels, J, π. Enriched target.

doi: 10.1016/0029-5582(66)90834-0
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1966BA46      Priv.Comm. (November 1966)

A.Backlin

NUCLEAR STRUCTURE 145Pm, 147Nd; measured not abstracted; deduced nuclear properties.


1966KO12      Nucl.Phys. 82, 561 (1966)

K.Korkman, A.Backlin

The High-Energy Transitions in 182W Following the Decay of 182Ta

RADIOACTIVITY 182Ta [from 181Ta(n, γ)]; measured Eγ, Iγ, I(ce). 182W deduced levels J, π, K. Natural target.

doi: 10.1016/0029-5582(66)90471-8
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1959BA09      Arkiv Fysik 15, 121 (1959)

G.Backstrom, J.Lindskog, O.Bergman, E.Bashandy, A.Backlin

Contributions to the Decay of Tb160 to Dy160


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