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Search: Author = B.Cujec

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1993CU01      Nucl.Phys. A552, 267 (1993)

B.Cujec

Giant Resonances in Low-Energy Heavy-Ion Reactions

NUCLEAR REACTIONS ¹²C(¹³C, X), ¹¹B(¹⁴N, X), ⁹Be(⁹Be, X), ¹²C(¹²C, X), ²⁴Mg(α, α'), E ≈ resonance; analyzed fusion data; deduced GDR excitation.

doi: 10.1016/0375-9474(93)90466-B
Citations: PlumX Metrics

1993DA17      Nucl.Phys. A564, 314 (1993)

B.Dasmahapatra, B.Cujec, G.Kajrys, J.A.Cameron

Cross-Section Measurements for the ⁹Be + ⁹Be, ⁷Li + ¹¹B and α + ¹⁴C Reactions at Low Energies

NUCLEAR REACTIONS, ICPND ⁹Be(⁹Be, X), E=4.5-12.4 MeV; ¹¹B(⁷Li, X), E=4-11.2 MeV; ¹⁴C(α, X), E=20-30 MeV; measured σ(E) for γ transitions in ¹⁰Be, ¹²C, ¹³C, ¹⁶N, ¹⁷N, ¹⁶O. ¹⁸O deduced broad resonance. Enriched targets, Ge-detectors.

doi: 10.1016/0375-9474(93)90523-Z
Citations: PlumX Metrics

1993DA21      Nucl.Phys. A565, 657 (1993)

B.Dasmahapatra, B.Cujec

Measurement of Cross Sections for ¹²C + ¹⁴C Reaction at Subbarrier Energies

NUCLEAR REACTIONS ¹⁴C(¹²C, X), E(cm)=5-8 MeV; measured σ(E, Eγ) for transitions in ^24,25Mg, ^24,25Na, ^21,22Ne; deduced partial, total fusion σ. High purity Ge detector, heavy-ion detector, enriched target.

doi: 10.1016/0375-9474(93)90051-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1347.

1991BR15      Z.Phys. A339, 367 (1991)

W.Bruckner, B.Cujec, H.Dobbeling, K.Dworschak, H.Kneis, S.Majewski, M.Nomachi, S.Paul, B.Povh, R.D.Ransome, T.-A.Shibata, M.Treichel, Th.Walcher

Measurements of the Antiproton-Proton Elastic Cross Section in the Beam Momentum Range between 180 and 600 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, p-bar), E at 180-600 MeV/c; measured σ(θ); deduced s-, p-wave phase shifts.

1991BR16      Z.Phys. A339, 379 (1991)

W.Bruckner, B.Cujec, H.Dobbeling, K.Dworschak, H.Kneis, S.Majewski, M.Nomachi, S.Paul, B.Povh, R.D.Ransome, T.-A.Shibata, M.Treichel, Th.Walcher

Ranges of Interaction in p(p-bar) Scattering at Low Energies

NUCLEAR REACTIONS ¹H(p-bar, p-bar), E at 181-505 MeV/c; analyzed σ(θ); deduced annihilation range, proton size correlation.

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.

1990BR02      Z.Phys. A335, 217 (1990)

W.Bruckner, B.Cujec, H.Dobbeling, K.Dworschak, F.Guttner, H.Kneis, S.Majewski, M.Nomachi, S.Paul, B.Povh, R.D.Ransome, T.-A.Shibata, M.Treichel, Th.Walcher

Measurements of the Antiproton-Proton Annihilation Cross-Section in the Beam Momentum Range between 180 and 600 MeV/c

NUCLEAR REACTIONS ¹H(p-bar, X), E at 180-600 MeV/c; measured annihilation σ.

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.

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
Citations: PlumX Metrics

1988DA05      Nucl.Instrum.Methods Phys.Res. A265, 411 (1988)

B.Dasmahapatra, B.Cujec

Accurate Measurement of Target Thickness by Heavy Ion Elastic Scattering

NUCLEAR REACTIONS ¹²C(¹⁴N, ¹⁴N), E=10.2 MeV; ¹²C(¹³C, ¹³C), E=11 MeV; ¹³C(¹⁶O, ¹⁶O), E=13, 13.25 MeV; ¹¹B(¹⁴N, ¹⁴N), E=10 MeV; ⁹Be(⁹Be, ⁹Be), E=5.5 MeV; measured particle spectra.

doi: 10.1016/S0168-9002(98)90007-9
Citations: PlumX Metrics

1988LA25      Nucl.Phys. A486, 189 (1988)

F.Lahlou, B.Cujec, B.Dasmahapatra

Cross Section Measurements for the ⁹Be + ⁹Be System at Subbarrier Energies

NUCLEAR REACTIONS, ICPND ⁹Be(⁹Be, X), (⁹Be, ⁹Be), E(cm)=1.4-3.4 MeV; measured elastic σ(θ), total reaction σ(E), σ(E, E(γ)) for transitions in ¹³C, ¹⁶O, ¹⁶N, ¹⁰Be, ¹⁷N. Optical model, statistical model and DWBA analysis. NaI and Ge detectors.

doi: 10.1016/0375-9474(88)90046-2
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1272.

1986CU02      Nucl.Phys. A453, 505 (1986)

B.Cujec, B.Dasmahapatra, Q.Haider, F.Lahlou, R.A.Dayras

Reactions with ⁹Be at Subbarrier Energies

NUCLEAR REACTIONS, ICPND ¹⁰B(⁹Be, X), (⁹Be, nα), (⁹Be, ⁸Be), ⁹Be(⁹Be, X), (⁹Be, 2n), (⁹Be, np), (⁹Be, p), (⁹Be, ⁵He), E(cm) ≈ 1.25-3 MeV; ¹³C(⁹Be, ⁵He), (⁹Be, X)²⁰Ne/²¹Ne/¹⁷O, E(cm) ≈ 2-5 MeV; measured Eγ, Iγ, γ, residual production σ(E). ^21,20Ne, ¹⁷O deduced transitions. Statistical model, α-transfer, DWBA analyses. Enriched targets, Ge detectors.

doi: 10.1016/0375-9474(86)90450-1
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1591.

1985PO02      Nucl.Phys. A433, 550 (1985)

L.Potvin, B.Cujec

Measurement of the ¹¹B(¹¹B, ¹⁰Be)¹²C Proton Transfer Reaction at Low Energies

NUCLEAR REACTIONS, ICPND ¹¹B(¹¹B, ¹⁰Be), E(cm)=5.5 MeV; measured σ(θ); ¹¹B(¹¹B, ¹⁰Be), E(cm)=2.66-3.64 MeV; measured γ yields; deduced σ(E).

doi: 10.1016/0375-9474(85)90281-7
Citations: PlumX Metrics

1984DA17      Nucl.Phys. A427, 186 (1984)

B.Dasmahapatra, B.Cujec, F.Lahlou

Total Reaction and Transfer Cross Sections for ¹¹B + ⁹Be and ¹³C + ⁹Be Reactions at Low Energies

NUCLEAR REACTIONS, ICPND ¹¹B(⁹Be, X), (⁹Be, ⁸Be), E=1.4-4.4 MeV; ¹³C(⁹Be, X), (⁹Be, ⁸Be), (⁹Be, αn), E=1.2-5.2 MeV; measured σ(E), γ yields; deduced evidence for α-transfer reaction. NaI, hyperpure Ge, surface barrier detectors, enriched targets. Optical model analysis.

doi: 10.1016/0375-9474(84)90145-3
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1289.

1984HA43      Nucl.Phys. A429, 116 (1984)

Q.Haider, B.Cujec

Description of Sub-Barrier Fusion Cross Sections by the Proximity Potential

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, ¹²C), (¹²C, X), E=3-9 MeV; ¹⁶O(¹⁶O, ¹⁶O), (¹⁶O, X), E=7-15 MeV; calculated σ(θ), σ factor vs E; deduced model parameters. Subbarrier fusion, proximity potential.

doi: 10.1016/0375-9474(84)90152-0
Citations: PlumX Metrics

1983DA02      Nucl.Phys. A394, 301 (1983)

B.Dasmahapatra, B.Cujec, F.Lahlou

Fusion Cross Sections for ¹⁶O + ¹³C at Low Energies

NUCLEAR REACTIONS, ICPND ¹³C(¹⁶O, X), E(cm)=4.6-9.1 MeV; measured fusion σ(E). NaI and surface barrier detectors, enriched targets. Optical model analysis.

doi: 10.1016/0375-9474(83)90175-6
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1375.

1983DA10      Can.J.Phys. 61, 657 (1983)

B.Dasmahapatra, B.Cujec, F.Lahlou

Fusion Cross Sections for ¹⁴N + ¹¹B at Low Energies

NUCLEAR REACTIONS, ICPND ¹¹B(¹⁴N, X), E(cm)=2.85-8.53 MeV; measured total γ yields; deduced fusion σ(E).

doi: 10.1139/p83-083
Citations: PlumX Metrics

1983DA20      Nucl.Phys. A408, 192 (1983)

B.Dasmahapatra, B.Cujec, F.Lahlou

Fusion and Neutron-Transfer Cross Sections for ¹³C + ¹⁰B and ¹³C + ¹¹B Reactions at Subbarrier Energies

NUCLEAR REACTIONS, ICPND ¹⁰B(¹³C, X), (¹³C, ¹²C), (¹³C, np), E=2.4-5.8 MeV; ¹¹B(¹³C, X), (¹³C, np), E=2.3-6.4 MeV; measured σ(E), γ-yields. Surface barrier, NaI detectors, enriched targets. Optical model analysis.

doi: 10.1016/0375-9474(83)90356-1
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1373.

1982DA16      Nucl.Phys. A384, 257 (1982)

B.Dasmahapatra, B.Cujec, F.Lahlou

Fusion Cross Sections for ¹²C + ¹²C, ¹²C + ¹³C and ¹³C + ¹³C at Low Energies

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, X), E=4.2-7 MeV; ¹³C(¹²C, X), E=3.1-6.7 MeV; measured fusion σ vs E. ²⁴Mg deduced resonance. NaI, surface barrier detectors, natural, enriched targets. Optical model analysis.

doi: 10.1016/0375-9474(82)90316-5
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1371.

1982DA28      Lett.Nuovo Cim. 35, 345 (1982)

B.Dasmahapatra, B.Cujec, F.Lahlou

The ¹²C + ¹²C Resonances between E(c.m.) = 4.5 and 6 MeV

NUCLEAR REACTIONS, ICPND ¹²C(¹²C, X), (¹²C, α), E=9.1-11.85 MeV; measured Eγ, Iγ, γ yield, total σ vs E, σ(θα). ²⁴Mg deduced resonances, J, π. Legendre polynomial analysis.

doi: 10.1007/BF02754703
Citations: PlumX Metrics

1981CU10      Can.J.Phys. 59, 1233 (1981)

B.Cujec, A.J.Ferguson, O.Hausser, D.Horn, R.E.Warner

Cross Sections for the ¹⁶O(¹⁶O, ⁸Be(g.s.))²⁴Mg Reaction and Mechanisms of α-Rearrangement Reactions

NUCLEAR REACTIONS ¹⁶O(¹⁶O, ⁸Be), E=53 MeV; measured ²⁴Mg(α)-coin; deduced reaction mechanism. ΔE-E heavy-ion telescope.

1980CH01      Nucl.Phys. A333, 273 (1980)

M.L.Chatterjee, L.Potvin, B.Cujec

Fusion Cross Section for ¹³C + ¹³C at Low Energies

NUCLEAR REACTIONS ¹³C(¹³C, X), E(cm)=3.05-6.88 MeV; measured total σ; ¹³C(¹³C, ²⁴Mg), E(cm)=3.17, 6.88 MeV; measured total σ. NaI detectors. Optical-model analysis.

doi: 10.1016/0375-9474(80)90233-X
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC1372.

1979CH22      Nucl.Phys. A323, 461 (1979)

M.L.Chatterjee, H.C.Cheung, B.Cujec

Total Reaction Cross Section for the ⁹Be + ¹⁰B System at Sub-Coulomb Energies

NUCLEAR REACTIONS ¹⁰B(⁹Be, X), E(cm)=1.04-4.94 MeV. ¹⁰B(⁹Be, αn), E(cm)=2.08-4.94 MeV; measured σ. ¹¹B levels deduced evidence for neutron transfer reaction. NaI detectors. Optical-model analysis.

doi: 10.1016/0375-9474(79)90120-9
Citations: PlumX Metrics

1978CH02      Nucl.Phys. A296, 333 (1978)

H.C.Cheung, M.D.High, B.Cujec

Fusion and Neutron Transfer Cross Sections for ⁹Be + ¹²C at Sub-Coulomb Energies

NUCLEAR REACTIONS ⁹Be(¹²C, X), E(cm)=2.8-6.3 MeV; measured fusion σ. ⁹Be(¹²C, ¹³C), E(cm)=1.0-5.8 MeV; measured total transfer σ to excited states in ¹³C. NaI, Ge(Li) detectors. Optical model analysis.

doi: 10.1016/0375-9474(78)90077-5
Citations: PlumX Metrics

1977HI01      Nucl.Phys. A278, 149 (1977)

M.D.High, B.Cujec

Sub-Coulomb Energy ¹²C + ^10,11B and ¹⁴N + ¹⁰B Fusion Cross Sections

NUCLEAR REACTIONS ¹²C(¹⁰B, X), E(cm)=2.10-5.38 MeV; ¹²C(¹¹B, X), E(cm)=2.10-5.99 MeV; ¹⁰B(¹⁴N, X), E(cm)=2.64-5.97 MeV; measured total fusion σ(E), optical model analysis. ¹²C(¹⁰B, ¹⁰B), θ(cm)=90.4°, E(cm)=3.18-6.82 MeV; measured σ(θ), optical model analysis.

doi: 10.1016/0375-9474(77)90190-7
Citations: PlumX Metrics

1977HI04      Nucl.Phys. A282, 181 (1977)

M.D.High, B.Cujec

The ¹²C + ¹²C Sub-Coulomb Fusion Cross Section

NUCLEAR REACTIONS ¹²C(¹²C, X), (¹²C, p), (¹²C, α), E=4.9-12 MeV; measured γ-yields; deduced fusion σ(E).

doi: 10.1016/0375-9474(77)90179-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetB0144.

1976CU04      Nucl.Phys. A266, 461 (1976)

B.Cujec, C.A.Barnes

Total Reaction Cross Section for ¹²C + ¹⁶O below the Coulomb Barrier

NUCLEAR REACTIONS ¹²C(¹⁶O, X), E(cm)=4-11.78 MeV; measured total reaction σ, σ(E); deduced interaction potential. ²⁸Si levels deduced S.

doi: 10.1016/0375-9474(76)90370-5
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1976DA14      J.Phys.(Paris) 37, 819 (1976)

R.Dayras, B.Cujec, B.Heusch

Proprietes des Niveaux de ⁶¹Cu et ⁶³Cu par un Modele a Couplage Coeur-Particule

NUCLEAR STRUCTURE ^61,63Cu; calculated levels, S, T_1/2, γ-branching, δ, B(λ).

doi: 10.1051/jphys:01976003707-8081900
Citations: PlumX Metrics

1976HI05      Nucl.Phys. A259, 513 (1976)

M.D.High, B.Cujec

Boron+Boron Sub-Coulomb Energy Total Reaction Cross Sections

NUCLEAR REACTIONS ¹¹B(¹¹B, X), E(cm)=1.56-3.65 MeV; ¹¹B(¹⁰B, X), E(cm)=1.61-3.94 MeV; ¹⁰B(¹⁰B, X), E(cm)=1.84-3.66 MeV; measured total σ(E). Optical-model analysis. Enriched targets.

doi: 10.1016/0375-9474(76)90086-5
Citations: PlumX Metrics

1972DA06      Nucl.Phys. A186, 307 (1972)

R.Dayras, B.Cujec

Interpretation des Niveaux de ⁵⁷Co par l'Interaction Coeur-Particule

NUCLEAR STRUCTURE ⁵⁷Co; calculated levels, γ-mixing, S, B(λ). Particle-core coupling model.

doi: 10.1016/0375-9474(72)90048-6
Citations: PlumX Metrics

1972DE46      Nucl.Phys. A194, 577 (1972)

M.L.V.L.de Slobodrian, B.Cujec, R.Roy, R.J.Slobodrian

The ³He(tau, α)2p Reaction at 9.11, 7.88 and 6.9 MeV

NUCLEAR REACTIONS ³He(³He, α)2p, E=6.9, 7.88, 9.11 MeV; measured σ(Ep, Eα, θ); analyzed reaction mechanisms, final-state interactions.

doi: 10.1016/0375-9474(72)91004-4
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1063.

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 T_1/2. Enriched targets.

doi: 10.1016/0375-9474(71)90747-0
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1971HE17      Nucl.Phys. A172, 395 (1971)

B.Heusch, B.Cujec, R.Dayras

Mesures de Vies Moyennes dans le Noyau ⁶¹Cu

NUCLEAR REACTIONS ⁵⁸Ni(α, pγ), E=10.01 MeV; measured Doppler-shift attenuation. ⁶¹Cu deduced T_1/2, γ-width(M1), γ-width(E2). Enriched target.

doi: 10.1016/0375-9474(71)90721-4
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1969CU02      Phys.Rev. 179, 1060 (1969)

B.Cujec, I.M.Szoghy

Energy Levels in V^47,49,51 and Mn^51,53,55 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
Citations: PlumX Metrics

1969DA05      Nucl.Phys. A127, 545 (1969)

R.Dayras, B.Cujec

Etude des Niveaux de ⁵⁷Co Jusqu'a 1.90 MeV

NUCLEAR REACTIONS ⁵⁴Fe(α, p), E=10.23, 10.30 MeV; measured σ(E; Ep, Eγ, θ(pγ)), Eγ. ⁵⁷Co deduced levels, J, π, delta. Enriched target.

doi: 10.1016/0375-9474(69)91026-4
Citations: PlumX Metrics

1968BO03      Nucl.Phys. A108, 529 (1968)

N.Bouchard, B.Cujec

Energy Levels of ⁵⁷Co

NUCLEAR REACTIONS ⁵⁴Fe(α, p), E = 10.5, 11 MeV; measured σ(Ep, θ). ⁵⁷Co deduced levels. Enriched target.

doi: 10.1016/0375-9474(68)90321-7
Citations: PlumX Metrics

1968CU03      Bull.Am.Phys.Soc. 13, No.4, 723, KH6 (1968)

B.Cujec, R.Dayras, I.Szoghy

Spins of Excited States in Mn⁵³ and Co⁵⁷ from (α, pγ) Angular Correlation Measurements

NUCLEAR STRUCTURE ⁵⁷Co, ⁵³Mn; measured not abstracted; deduced nuclear properties.

1966CU01      Nucl.Phys. 81, 523(1966)

B.Cujec

New Levels in ⁴³Sc

NUCLEAR REACTIONS ⁴⁰Ca(α, p), E = 9, 10 MeV; measured σ(Ep, θ). ⁴³Sc deduced levels. Natural target.

doi: 10.1016/0029-5582(66)90227-6
Citations: PlumX Metrics

1965CL01      Bull.Am.Phys.Soc. 10, No.1, 25, BC3 (1965)

D.Cline, H.E.Gove, B.Cujec

Energy Levels of Sc⁴² from the Ca⁴⁰(He³, p)Sc⁴² Reaction

NUCLEAR STRUCTURE ⁴²Sc; measured not abstracted; deduced nuclear properties.

1965CU03      Phys.Letters 15, 266 (1965)

B.Cujec, W.G.Davies, W.K.Dawson, T.B.Grandy, G.C.Neilson, K.Ramavataram

The Si³⁰(d, n)P³¹ Reaction

NUCLEAR STRUCTURE ³¹P; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(65)91242-4
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1964CU05      Phys. Rev. 136, B1305 (1964)

B.Cujec

Studies of Mg²⁵, Mg²⁶, and Mg²⁷ Nuclei with (d, p) Reactions

NUCLEAR STRUCTURE ²⁷Mg, ²⁵Mg, ²⁶Mg; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.136.B1305
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1963CU02      Phys.Rev. 131, 735 (1963)

B.Cujec

Nuclear Structure Studies in the Palladium Isotopes with (d, p) and (d, t) Reactions

NUCLEAR STRUCTURE ¹⁰⁶Pd, ¹⁰⁵Pd, ¹⁰⁹Pd, ¹⁰⁷Pd, ¹⁰³Pd; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.131.735
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1962CU01      Bull.Am.Phys.Soc. 7, No.1, 59, R7 (1962)

B.Cujec

Photonuclear Effect with Be⁹

NUCLEAR STRUCTURE ⁹Be; measured not abstracted; deduced nuclear properties.

1962CU05      Nuclear Phys. 37, 396 (1962)

B.Cujec

Photonuclear Effect with Be⁹

NUCLEAR STRUCTURE ⁹Be; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(62)90273-0
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1962CU07      Phys.Rev. 128, 2303 (1962)

B.Cujec

Investigation of d-s Shell Nuclei with (d, He³) Reactions

NUCLEAR STRUCTURE ²⁶Mg, ⁸⁹Y, ¹⁹F, ³⁹K, ³¹P, ³⁰Si, ³⁶S, ³⁴S, ⁶²Ni, ⁵⁷Co, ¹⁶O; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRev.128.2303
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