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NSR database version of April 27, 2024.

Search: Author = D.Cutoiu

Found 18 matches.

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2004WI06      Phys.Rev. C 69, 044310 (2004)

H.-F.Wirth, G.Graw, S.Christen, D.Cutoiu, Y.Eisermann, C.Gunther, R.Hertenberger, J.Jolie, A.I.Levon, O.Moller, G.Thiamova, P.Thirolf, D.Tonev, N.V.Zamfir

0+ states in deformed actinide nuclei by the (p, t) reaction

NUCLEAR REACTIONS 230,232Th, 234U(p, t), E=25 MeV; measured σ(E, θ). 228,230Th, 232U deduced 0+ level energies, spectroscopic factors, transfer strengths. Comparison with model predictions.

doi: 10.1103/PhysRevC.69.044310
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0171. Data from this article have been entered in the XUNDL database. For more information, click here.

1998SA30      Nucl.Phys. A637, 491 (1998)

A.Savelius, S.Juutinen, K.Helariutta, P.Jones, R.Julin, P.Jamsen, M.Muikku, M.Piiparinen, J.Suhonen, S.Tormanen, R.Wyss, P.T.Greenlees, P.Simecek, D.Cutoiu

Coexisting Structures in 115Sn and 116Sn

NUCLEAR REACTIONS 104Ru(18O, 3nα), (18O, 2nα), E=65 MeV; measured Eγ, Iγ, γγ-coin, γγ(θ). 115,116Sn deduced high-spin levels, J, π. Enriched target, Compton suppressed Ge detectors, charged-particle Si detectors. Shell model, microscopic quasiparticle-phonon model, total Routhian surface calculations.

doi: 10.1016/S0375-9474(98)80004-3
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Data from this article have been entered in the XUNDL database. For more information, click here.

1997SA29      Acta Phys.Pol. B28, 173 (1997)

A.Savelius, K.Helariutta, P.M.Jones, R.Julin, S.Juutinen, P.Jamsen, M.Muikku, M.Piiparinen, S.Tormanen, P.Simecek, D.Cutoiu

Coexisting Structures in 116Sn from Weak Fusion-Evaporation Reactions

NUCLEAR REACTIONS 104Ru(18O, 2nα), E=65 MeV; measured Eγ, Iγ, γγ-, (particle)γ-coin. 116Sn deduced high-spin levels, J, π, configurations.

1996GI04      Phys.Rev. C53, 2770 (1996)

A.Giannatiempo, A.Nannini, A.Perego, P.Sona, D.Cutoiu

Spin-Parity Assignments and Evidence for Mixed-Symmetry States in 100Ru

RADIOACTIVITY 100Rh(β+), (EC) [from 100Ru(p, n)]; measured I(ce), Eγ, Iγ. 100Ru deduced levels, ICC, J, π, γ-branching ratio. Interacting boson model.

doi: 10.1103/PhysRevC.53.2770
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1995GI14      Phys.Rev. C52, 2969 (1995)

A.Giannatiempo, A.Nannini, P.Sona, D.Cutoiu

Full-Symmetry and Mixed-Symmetry States in Even Ruthenium Isotopes

NUCLEAR STRUCTURE 98,100,102,104,106,108,110,112,114Ru; calculated levels, B(λ), electric quadrupole moments, γ branching ratios, γ strength function. Interacting boson model approach.

doi: 10.1103/PhysRevC.52.2969
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1993CU07      Roum.J.Phys. 38, 877 (1993)

D.Cutoiu

Description of an Electron Spectrometer Built in the Institute of Physics and Nuclear Engineering

RADIOACTIVITY 133Ba(EC); 207Bi(EC), (β+); measured I(ce). Mini-orange spectrometer, off-beam, on-bean tests.

1993FA11      Z.Phys. A346, 21 (1993)

T.F.Fazzini, A.Giannatiempo, A.Nannini, A.Perego, D.Cutoiu

Search for the Lowest 2+ Mixed-Symmetry State in 102Ru

RADIOACTIVITY 102Rh(EC) [from 102Ru(p, n), E=6 MeV]; measured I(ce), Eγ, Iγ. 102Ru deduced level, J, π, K-shell ICC, B(λ) ratio.

doi: 10.1007/BF01290777
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1992KU01      Phys.Rev. C45, 640 (1992)

J.Kumpulainen, R.Julin, J.Kantele, A.Passoja, W.H.Trzaska, E.Verho, J.Vaaramaki, D.Cutoiu, M.Ivascu

Systematic Study of Low-Spin States in Even Cd Nuclei

NUCLEAR REACTIONS 106,108,110,112,116Cd(p, p'), E=7-9 MeV; 107,109Ag(p, 2n), E=12.3-17.4 MeV; 108,110Pd(α, 2n), E=17-20MeV; measured Eγ, Iγ, γγ-, pγ-coin, γ(θ). 106,108,110,112,116Cd deduced levels, J, π, ICC. Enriched targets, Ge, Si(Li) detectors.

RADIOACTIVITY 106,108,110In(EC), (β+); measured Eγ, Eβ. 106,108,110Cd deduced levels J, π, ICC, Ge, Si(Li) detectors.

doi: 10.1103/PhysRevC.45.640
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1990CA13      Z.Phys. A335, 271 (1990)

G.Cata, D.Bucurescu, D.Cutoiu, M.Ivascu, N.V.Zamfir

Effective Boson Number Calculations in Mo and Cd Isotopes

NUCLEAR STRUCTURE 96,98,100,102,104Mo, 106,108,110,112,114,116Cd; calculated levels, B(λ), γ-branching. Interacting boson model.

1989BU20      Phys.Lett. 229B, 321 (1989)

D.Bucurescu, G.Cata, D.Cutoiu, E.Dragulescu, M.Ivascu, N.V.Zamfir, A.Gizon, J.Gizon

Investigation of the Particle-Core Structure of Odd-Mass Nuclei in the N(p)N(n) Scheme

NUCLEAR STRUCTURE A ≈ 80-100; A ≈ 130; analyzed odd mass nuclei band structure; deduced particle-core structure. The N(p)N(n) scheme.

doi: 10.1016/0370-2693(89)90411-5
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1987IV05      Rev.Roum.Phys. 32, 937 (1987)

M.Ivascu, D.B.Ion, D.Bucurescu, G.Cata, D.Cutoiu, D.Galeriu, R.Ion-Mihai, N.V.Zamfir

Search for Spontaneous Emission of Mesons from 252Cf

RADIOACTIVITY 252Cf(SF); measured (light particle)(heavy particle)-coin; deduced meson decay branching upper limits.

1986BU10      Z.Phys. A324, 387 (1986); Erratum Z.Phys. A327, 241 (1987)

D.Bucurescu, G.Cata, D.Cutoiu, G.Constantinescu, M.Ivascu, N.V.Zamfir

An Extended IBA Consistent-Q Formalism Applied to Ru and Pd Isotopes

NUCLEAR STRUCTURE 98,100,102,104,106,108Ru, 102,104,106,108,110,112Pd; calculated levels, B(E2). Interacting boson approximation.

1985BU10      Rev.Roum.Phys. 30, 181 (1985)

D.Bucurescu, G.Cata, G.Constantinescu, D.Cutoiu, M.Ivascu, N.V.Zamfir

Interacting Boson and Interacting Boson-Fermion Calculations in the A ≈ 100 Transitional Region

NUCLEAR STRUCTURE 96,98,100,102,104,106Ru, 98,100,102,104,106,108Pd; calculated levels, band structure, B(E2), quadrupole moment. 97,99,101,103,105Rh; calculated levels, model parameter dependence. Interacting boson model.

1985BU11      Nucl.Phys. A443, 217 (1985)

D.Bucurescu, G.Cata, D.Cutoiu, G.Constantinescu, M.Ivascu, N.V.Zamfir

IBFA Description of High-Spin Positive-Parity States in Rh Isotopes

NUCLEAR STRUCTURE 96,98,100,102,104,106Ru, 99Rh; calculated levels, B(E2). 97,101,103,105,107Ru; calculated levels; deduced model parameters. Interacting boson-fermion approximation.

NUCLEAR REACTIONS 88Sr(14N, 3n), E=54 MeV; measured Eγ, Iγ, recoil. 99Rh deduced levels, T1/2, B(E2). Interacting boson-fermion approximation model comparison.

doi: 10.1016/0375-9474(85)90261-1
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1984BU26      J.Phys.(London) G10, 1189 (1984)

D.Bucurescu, G.Constantinescu, D.Cutoiu, M.Ivascu, N.V.Zamfir, A.A.Haliem

High-Spin States in 86Y

NUCLEAR REACTIONS, ICPND 76Ge(14N, 4n), E=38-56 MeV; 73Ge(16O, 2np), E=48-60 MeV; measured Eγ, Iγ, σ(E), σ(Eγ, θγ), (charged-particle)γ-, γγ-coin. 86Y deduced levels, J, π. Ge(Li) detectors, enriched targets.

doi: 10.1088/0305-4616/10/9/009
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1983BU09      Nucl.Phys. A401, 22 (1983)

D.Bucurescu, G.Cata, D.Cutoiu, G.Constantinescu, M.Ivascu, N.V.Zamfir

Description of the Neutron Deficient Sr and Zr Isotopes in the Interacting Boson Model

NUCLEAR STRUCTURE 78,80,82,84Sr; calculated levels, potential energy surfaces, backbending plots, B(E2) ratios. 80,82,84,86Zr; calculated levels, backbending plots, B(E2) ratios. 85Y, 83,81Sr; calculated levels, B(E2). Interacting boson model.

doi: 10.1016/0375-9474(83)90334-2
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1981BU05      J.Phys.(London) G7, 667 (1981)

D.Bucurescu, G.Constantinescu, M.Ivascu, N.V.Zamfir, M.Avrigeanu, D.Cutoiu

Evidence for a g9/2 Decoupled Band in 85Y

NUCLEAR REACTIONS 74Ge(14N, 3n), E=40-52 MeV; 72Ge(16O, 2np), E=45-64 MeV; 73Ge(16O, 3np), E=48-60 MeV; measured σ(Eγ, E), σ(Eγ, θ), pγ-, γγ-coin. 85Y deduced levels, J, π. Enriched targets, Ge(Li) detector.

doi: 10.1088/0305-4616/7/5/011
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1981BU06      J.Phys.(London) G7, L123 (1981)

D.Bucurescu, G.Constantinescu, D.Cutoiu, M.Ivascu, N.V.Zamfir

Possible Shape Phase Transition in the Heavy Kr Isotopes

NUCLEAR STRUCTURE 70,72,74,76,78,80,82,84,86,88,90,92,94,96Kr; calculated potential energy surfaces; deduced phase transition effects between N=58 and 60. Mascroscopic approach, shell, pairing effect microscopic corrections.

doi: 10.1088/0305-4616/7/1/016
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