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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 ^{186,188,190,192}Os, ¹⁹⁴Pt(⁴⁰Ca, ⁴⁰Ca'), (⁵⁸Ni, ⁵⁸Ni'), (¹³⁶Xe, ¹³⁶Xe'), (²⁰⁸Pb, ²⁰⁸Pb'), E=3.3-4.8 MeV/nucleon; measured Eγ, Iγ following Coulomb excitation. ^{186,188,190,192}Os, 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 ^{218,216,214,202,208}Po(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 T_1/2, 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 T_1/2, 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 T_1/2, 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 ^{112,114,116,118,120,122,124}Sn(¹⁶O, ¹⁶O'), E=48 MeV; measured Eγ, Iγ, γγ-coin, Coulomb excitation; ^{112,114,116,118,120,122,124}Sn(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). ^{112,114,116,118,120,122,124}Sn 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 ^{112,114,116,118,120,122,124}Sn(¹⁶O, ¹⁶O'γ), E=48 MeV; measured Eγ, Iγ, γγ-coin. ^{112,114,116,118,120,122,124}Sn(p, p'γ), E=6-8 MeV; measured Eγ, Iγ. ^{112,114,116,118,120,122,124}Sn 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), T_1/2, γγ-, e^-p-, γp-coin. ^112,114Cd levels deduced B(E2), T_1/2.

NUCLEAR REACTIONS Cd(¹⁶O, ¹⁶O'), E=44 MeV; measured double Coulomb excitation σ. ^112,114Cd levels deduced B(E2), T_1/2. 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 T_1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. ¹¹⁷Cd deduced levels, J, π, T_1/2, 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, T_1/2, 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 T_1/2, 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, T_1/2; 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, T_1/2, 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, T_1/2, 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 T_1/2, Eγ, Iγ, I(ce), γγ-coin, γγ-delay; deduced ICC, log ft. ¹¹⁹Cd deduced levels, J, π, T_1/2, 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 T_1/2, 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 T_1/2, 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, T_1/2, Iγ, γγ(t), I(ce). Deduced ICC, log ft. ^107mIn measured T_1/2, 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, T_1/2, 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 ^{114,116,118,120,122}Cd as Observed in the Beta Decay of Ag Isotopes

RADIOACTIVITY ^{114,116,118,120,122}Ag; measured Eγ, Iγ, γγ-coin, T_1/2, 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 T_1/2, 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, T_1/2, 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 T_1/2, 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, T_1/2, 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, T_1/2, 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, T_1/2, 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, T_1/2, 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, T_1/2, 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 T_1/2, 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, T_1/2, 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, T_1/2, 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 ^{168,170,172,174,176}Yb(d, d'), ^171,173Yb(d, p), (d, t), E=12 MeV; measured σ(Ed'), σ(Ep), σ(Et). ^{168,170,172,174,176}Yb 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, T_1/2, 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