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NSR database version of May 24, 2024.

Search: Author = I.M.Szoghy

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1994SZ01      Phys.Rev. C49, 686 (1994)

J.Sziklai, J.A.Cameron, I.M.Szoghy, T.Vass

Multichannel Study on the Fragmentation of the (1g)9/2 Isobaric Analog Resonance in 53Mn

NUCLEAR REACTIONS 52Cr(p, p'), (p, p), E ≈ 4.1-4.25 MeV; measured σ(θ). 52Cr(p, γ), (p, p'γ), E ≈ 4-4.6 MeV; measured Eγ, Iγ, γ(θ). 53Mn deduced (1g)9/2 IAR fragmentation. Multi-channel study.

doi: 10.1103/PhysRevC.49.686
Citations: PlumX Metrics


1991DA05      Nucl.Phys. A526, 395 (1991)

B.Dasmahapatra, B.Cujec, I.M.Szoghy, J.A.Cameron

Cross Section Measurements for the 16O + 13C Reaction at Subbarrier Energies

NUCLEAR REACTIONS, ICPND 13C(16O, X), E(cm)=4.8-9.8 MeV; measured σ(E, Eγ); deduced partial σ for transitions in 24,25,27Mg, 21Ne, 24Na, 26,27,28Al, 27,28Si, 17O, total fusion σ. Hyperpure Ge detector, enriched target.

doi: 10.1016/0375-9474(91)90292-E
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1377.


1990DA03      Nucl.Phys. A509, 393 (1990)

B.Dasmahapatra, B.Cujec, F.Lahlou, I.M.Szoghy, S.C.Gujrathi, G.Kajrys, J.A.Cameron

Cross-Section Measurements for 7Li + 11B and 7Li + 13C Reactions at Low Energies

NUCLEAR REACTIONS 11B(7Li, X), E(cm)=1.45-6.10 MeV; measured σ(E, Eγ) for transitions in 10Be, 12,13C, 15,16,17N, 16O. 13C(7Li, X), E(cm)=1.47-6.48 MeV; measured σ(E, Eγ) for transitions in 12B, 15N, 17,18O, 18,19F. Statistical model analysis. Ge-detectors, enriched targets.

doi: 10.1016/0375-9474(90)90429-P
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1410.


1990SZ01      Phys.Rev. C41, 849 (1990)

J.Sziklai, T.Vass, J.A.Cameron, I.M.Szoghy

Fine Structure of the 1g9/2 Isobaric Analog Resonance in 61Cu

NUCLEAR REACTIONS 60Ni(p, γ), (p, p'γ), E=3.67-3.83 MeV; measured Iγ(θ), σ(Eγ, E). 61Cu deduced g9/2 IAS fine structure, B(M1), Γ.

doi: 10.1103/PhysRevC.41.849
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1989CU03      Phys.Rev. C39, 1326 (1989)

B.Cujec, I.Hunyadi, I.M.Szoghy

12C(12C, 8Be)16O Cross-Section Measurement at Sub-Barrier Energies

NUCLEAR REACTIONS, ICPND 12C(12C, 8Be), E(cm)=2.43-5.24 MeV; measured σ(E, θ); deduced reaction mechanism, σ(E).

doi: 10.1103/PhysRevC.39.1326
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1986SZ02      Nucl.Instrum.Methods Phys.Res. A242, 277 (1986)

I.M.Szoghy, Q.Haider, R.Ouellet

Monte Carlo Simulation of Multistep Reactions involving Three Particles in the Exit Channel

NUCLEAR REACTIONS 12C(12C, 8Be), (12C, 2α), E(cm)=2.43 MeV; calculated α-, 8Be yield vs θ. Three-body final state, Monte Carlo techniques.

doi: 10.1016/0168-9002(86)90221-4
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1984SZ01      ATOMKI Kozlem. 26, 67 (1984)

I.M.Szoghy, G.J.Costa, C.Gerardin, Ch.Heitz, R.Seltz

Emission of Prompt X-Rays following the Fusion of 35Cl and 59Co Nuclei

NUCLEAR REACTIONS 59Co(35Cl, X), E=100 MeV; measured E(X-ray), I(X-ray), γ(X-Ray)-coin; deduced Sr, Y, Zr, Nb, Mo relative yields. Evaporation following fusion.


1984SZ02      Phys.Rev. C30, 490 (1984)

J.Sziklai, J.A.Cameron, I.M.Szoghy

g9/2 Isobaric Analog Resonances in 51Mn

NUCLEAR REACTIONS 50Cr(p, γ), (p, p'γ), E=3.08-3.36 MeV; measured σ(Eγ, E); deduced Coulomb energy differences. 51Mn deduced IAR, J, π, Γp, Γp', proton reduced widths, spectroscopic factors. Enriched target, fine structure analysis.

doi: 10.1103/PhysRevC.30.490
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1982SZ01      Can.J.Phys. 60, 959 (1982)

I.M.Szoghy, C.Rangacharyulu

Isospin Impurity and Core Polarization of g9/2 IAR Fragments in 59Cu

NUCLEAR REACTIONS 58Ni(p, γ), E=2839, 3488, 3550 keV; measured γ(θ). 59Cu deduced resonance J, π, g9/2 IAR fragmentation, δ, Γγ, Γγ/Γ.


1979RA12      Can.J.Phys. 57, 733 (1979)

C.Rangacharyulu, I.M.Szoghy, C.St-Pierre, K.Ramavataram

g9/2 Isobaric Analogue Resonances in 64,66Zn(p, γ) Reactions

NUCLEAR REACTIONS 64,66Zn(p, γ), E=2.9-3.3 MeV; measured Eγ, Iγ, γ(θ). 65,67Ga deduced levels, J, π, fragmentation of 1g9/2 IAR, analog-antianalog M1 strengths. Compared with Aleshin model.

doi: 10.1139/p79-104
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1979RA13      Phys.Rev. C19, 1762 (1979)

C.Rangacharyulu, I.M.Szoghy, C.St-Pierre, K.Ramavataram

Gamma Decay of g9/2 Isobaric Analog Resonance in 57Co

NUCLEAR REACTIONS 56Fe(p, γ), E=3.7-3.8 MeV; measured Eγ, σ(Eγ, θ). 57Co levels deduced E1, M1 strengths, 9/2+ analog, antianalog states. Enriched target.

doi: 10.1103/PhysRevC.19.1762
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1978RA06      Phys.Rev. C17, 1583 (1978)

K.Ramavataram, C.Rangacharyulu, I.M.Szoghy, R.Hilko, C.St-Pierre

Isobaric Analog Resonances in the 68Zn(p, γ)69Ga Reaction

NUCLEAR REACTIONS 68Zn(p, γ), E=3.2-3.8 MeV; measured σ(E, Eγ). 69Ga deduced resonances, Γγ, M1 strength.

doi: 10.1103/PhysRevC.17.1583
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1976DA01      Nucl.Phys. A257, 118 (1976)

R.Dayras, B.Cujec, I.M.Szoghy

Etude du Noyau 63Cu par la Reaction 60Ni(α, pγ)63Cu

NUCLEAR REACTIONS 60Ni(α, pγ), E=11.7 MeV; measured σ(E;Ep, Eγ, θpγ). 63Cu deduced levels, J, π, δ, branching ratios. Isotopic 60Ni, self-supporting targets, Ge(Li) detector.

doi: 10.1016/0375-9474(76)90478-4
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1973SZ01      Nucl.Phys. A201, 433 (1973)

I.M.Szoghy, J.S.Forster, G.C.Ball

Mean Lives of States in 51Cr

NUCLEAR REACTIONS 48Ti(α, nγ), E=6.50, 7.50, 8.50 MeV; measured DSA. 51Cr deduced levels T1/2. Enriched target.

doi: 10.1016/0375-9474(73)90312-6
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1972HA07      Nucl.Phys. A179, 465 (1972)

O.Hausser, A.J.Ferguson, A.B.McDonald, I.M.Szoghy, T.K.Alexander, D.L.Disdier

High Spin States in 20Ne from 16O(α, α) Scattering

NUCLEAR REACTIONS 16O(α, α), E=5-11 MeV; measured σ(Eα, θ(α)). 20Ne deduced levels, J, π, α-widths. Natural targets.

doi: 10.1016/0375-9474(72)90383-1
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetT0232.


1971DA22      Nucl.Phys. A173, 49 (1971)

R.Dayras, M.Toulemonde, B.Cujec, B.Heusch, J.N.Mo, I.M.Szoghy

Mesures de Correlations Angulaires et de Vies Moyennes dans 57Co

NUCLEAR REACTIONS 54Fe(α, pγ), E=9.86, 10.02, 10.40 MeV; measured σ(E;Ep, Eγ, θ(pγ)), Iγ, Doppler-shift attenuation. 57Co deduced γ-branching, J, γ-mixing, mean T1/2. Enriched targets.

doi: 10.1016/0375-9474(71)90747-0
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1971HE14      Nucl.Phys. A169, 145 (1971)

B.Heusch, B.Cujec, R.Dayras, J.N.Mo, I.M.Szoghy

Etude du Noyau 61Cu par la Reaction 58Ni(α, pγ)61Cu

NUCLEAR REACTIONS 58Ni(α, pγ); measured σ(E;Ep, Eγ, θ(pγ)). 61Cu deduced levels, J, π, γ-mixing, branching ratios. Isotopic 58Ni, self-supporting targets, Ge(Li) detectors.

doi: 10.1016/0375-9474(71)90568-9
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1970MO12      Nucl.Phys. A147, 129 (1970)

J.N.Mo, B.Cujec, R.Dayras, I.M.Szoghy, M.Toulemonde

Level Structure of 55Co, 51V and 49V from γ-Decay

NUCLEAR REACTIONS 54Fe, 50Ti(3He, dγ), E(3He) = 10 MeV; 48Ti, 46Ti(α, pγ), Eα = 9.6-9.9 MeV; measured σ(Ed, Eγ), σ(E;Ep, Eγ). 55Co, 51V, 49V deduced levels γ-branching ratios.

doi: 10.1016/0375-9474(70)90515-4
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1970SZ02      Nucl.Phys. A153, 529 (1970)

I.M.Szoghy, B.Cujec, R.Dayras

Etude de 53Mn Suivant la Reaction (α, pγ)

NUCLEAR REACTIONS 50Cr(α, pγ), E=8-11 MeV; measured σ(E;Ep, Eγ, θ(pγ)). 53Mn deduced levels, J, π, γ-mixing, branching ratios. Enriched target. NaI(Tl) detectors.

doi: 10.1016/0375-9474(70)90790-6
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1969CU02      Phys.Rev. 179, 1060 (1969)

B.Cujec, I.M.Szoghy

Energy Levels in V47,49,51 and Mn51,53,55 from (He3, d) reactions

NUCLEAR REACTIONS 46,48,50Ti, 50,52,54Cr(3He, d), E=8-10 MeV; measured σ(Ed, θ). 47,49,51V, 51,53,55Mn deduced levels, J, π, L(p), S.

doi: 10.1103/PhysRev.179.1060
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