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Search: Author = J.Delaunay

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1990CA23      Nucl.Phys. A513, 174 (1990)

Sl.Cavallaro, M.L.Sperduto, B.Delaunay, J.Delaunay, A.D'Onofrio, H.Dumont

Sub-Barrier Fusion Induced by ³⁵Cl and ³⁷Cl Beams on ^24,25,26Mg Isotopes

NUCLEAR REACTIONS, ICPND ^24,25,26Mg(³⁵Cl, X), (³⁷Cl, X), E(cm)=25-37 MeV; measured fusion σ(E); deduced barrier parameters. In beam γ-spectroscopy. Coupled channel calculations.

doi: 10.1016/0375-9474(90)90347-O
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1989DO01      Phys.Rev. C39, 834 (1989)

A.D'Onofrio, J.Gomez del Campo, B.Delaunay, J.Delaunay, H.Dumont, F.Andreozzi, A.Brondi, R.Moro, M.Romano, F.Terrasi

Preequilibrium Emission and Target-Projectile-Like Correlations for ²⁰Ne + ⁶⁰Ni at E(²⁰Ne) = 740 MeV

NUCLEAR REACTIONS ⁶⁰Ni(²⁰Ne, X), E=740 MeV; measured (particle)γ-coin; deduced preequilibrium contributions.

doi: 10.1103/PhysRevC.39.834
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1989SA47      Z.Phys. A334, 365 (1989)

M.G.Saint-Laurent, Sl.Cavallaro, M.L.Sperduto, B.Delaunay, J.Delaunay, H.Dumont

High Spin States of Some Nuclei Around the N = Z = 28 Double Closed Shell

NUCLEAR REACTIONS ³⁰Si(²⁸Si, n2p), (²⁸Si, 2np), E=54-85 MeV; ⁵⁴Fe(α, n), E=18-27 MeV; measured Eγ, Iγ, γ(θ), γγ(θ), oriented nuclei, σ(E), γγ-coin. ⁵⁷Ni deduced levels, T_1/2, B(λ), J, π. ⁵⁵Fe deduced levels, J, π, δ, γ-branching ratio. ⁵⁵Co deduced levels, possible J, T_1/2.

1987DO01      Phys.Rev. C35, 1167 (1987)

A.D'Onofrio, B.Delaunay, J.Delaunay, H.Dumont, J.Gomez del Campo, F.Andreozzi, A.Brondi, R.Moro, M.Romano, F.Terrasi, J.F.Bruandet

Heavy Residue Masses as Possible Indicators of the Impact Parameter in the Reaction ²⁰Ne + ⁶⁰Ni at 742 MeV

NUCLEAR REACTIONS ⁶⁰Ni(²⁰Ne, X), E=746 MeV; measured fragment σ(Z, A); deduced residue mass-impact parameter correlation. Massive transfer, participant spectator models.

doi: 10.1103/PhysRevC.35.1167
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1987DO02      Z.Phys. A326, 335 (1987)

A.d'Onofrio, B.Delaunay, J.Delaunay, H.Dumont, J.Gomez del Campo, A.Brondi, R.Moro, M.Romano, F.Terrasi, J.F.Bruandet

Evidence for Equilibration of Hot Nuclei

NUCLEAR REACTIONS ⁶⁰Ni(²⁰Ne, ⁷Li), E=742 MeV; measured γ(⁷Li)-coin; deduced ⁷Li production σ. Enriched target, high purity Ge detector. Hauser-Feshbach calculations.

1986BO05      Nucl.Phys. A451, 171 (1986)

E.Bozek, D.M.De Castro-Rizzo, S.Cavallaro, B.Delaunay, J.Delaunay, H.Dumont, A.D'Onofrio, M.-G.Saint-Laurent, L.Sperduto, F.Terrasi

De-Excitation of ^58,60,62Ni Compound Nuclei Formed via Symmetric and Asymmetric Entrance Channels

NUCLEAR REACTIONS, ICPND ⁴⁶Ti(¹²C, X), E(cm)=17.21-45.05 MeV; ³⁰Si(²⁸Si, X), E(cm)=25.79-43.9 MeV; ⁴⁸Ti(¹²C, X), E(cm)=16.43-46.18 MeV; ³⁰Si(³⁰Si, X), E(cm)=27.18-47.43 MeV; ⁵⁰Ti(¹²C, X), E(cm)=17.23-47.27 MeV; ⁴⁴Ca(¹⁸O, X), E(cm)=19.44-42.25 MeV; measured absolute residue production σ for ^57,56,55,59Co, ^{56,55,54,57,58,59,53}Fe, ^58,57,60,59Ni, ^{55,54,53,52,51}Mn, ^51,49,50V.

doi: 10.1016/0375-9474(86)90250-2
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1986CA13      Nucl.Instrum.Methods Phys.Res. A245, 89 (1986)

Sl.Cavallaro, L.Y.Xiao, M.L.Sperduto, J.Delaunay

Determination of Sidefeeding Intensity by γ-γ Coincidence Data Analysis

NUCLEAR REACTIONS ³⁰Si(²⁸Si, pα), E=80 MeV; measured γγ-coin, γγ(θ, φ), oriented nuclei. ⁵³Mn levels deduced side feeding Iγ.

doi: 10.1016/0168-9002(86)90262-7
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1985DO08      Lett.Nuovo Cim. 42, 347 (1985)

A.D'Onofrio, H.Dumont, B.Delaunay, J.Delaunay, A.Brondi, R.Moro, M.Romano, F.Terrasi, S.Cavallaro, L.Sperduto, M.G.Saint-Laurent

Reaction Mechanism Study for the System: ²⁰Ne + ⁶⁰Ni at MeV/A

NUCLEAR REACTIONS ⁶⁰Ni(²²Ne, X), E=44 MeV/nucleon; measured Eγ, Iγ, γ(fragment)-coin, γ-multiplicites; deduced fragment mass distribution.

1985DU02      Nucl.Phys. A435, 301 (1985)

H.Dumont, B.Delaunay, J.Delaunay, D.M.De Castro Rizzo, A.Brondi, P.Cuzzocrea, A.D'Onofrio, R.Moro, M.Romano, F.Terrasi

Limitation to Complete Fusion in the Reactions ^12,13C + ⁴⁸Ti and ³⁰Si + ³⁰Si

NUCLEAR REACTIONS, ICPND ⁴⁸Ti(¹²C, X), (¹³C, X), E=20-60 MeV; ³⁰Si(³⁰Si, X), E=55-126 MeV; measured residue production σ(E). ⁴⁸Ti(¹²C, p), (¹²C, α), E=47.5 MeV; ⁴⁸Ti(¹³C, p), (¹³C, α), E=46 MeV; measured σ(fragment θ, E); deduced fusion σ(E). ⁴⁸Ti(¹³C, ¹³C), E=46 MeV; measured σ(θ). ⁴⁸Ti(¹³C, 2n), (¹³C, np), (¹³C, 3n), (¹³C, 2np), (¹³C, n2p), (¹³C, 4n), (¹³C, 3np), (¹³C, 2n3p), (¹³C, nα), (¹³C, 2nα), (¹³C, npα), (¹³C, 3nα), (¹³C, 2npα), (¹³C, n2α), E=46 MeV; ⁴⁸Ti(¹²C, 2n), (¹²C, np), (¹²C, 3n), (¹²C, 2np), (¹²C, n2p), (¹²C, 4n), (¹²C, 3np), (¹²C, 2n2p), (¹²C, pα), (¹²C, 2nα), (¹²C, npα), (¹²C, pα), (¹²C, npα), (¹²C, 2pα), (¹²C, 3nα), (¹²C, 2npα), (¹²C, 2α), (¹²C, n2α), E=47.5 MeV; measured σ.

doi: 10.1016/0375-9474(85)90316-1
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1984DE38      Nucl.Phys. A427, 151 (1984)

D.M.De Castro Rizzo, E.Bozek, S.Cavallaro, B.Delaunay, J.Delaunay, H.Dumont, M.G.Saint-Laurent, F.Terrasi

Fusion Excitation Functions near and below the Coulomb Barrier for Symmetric and Asymmetric Medium-Mass Systems

NUCLEAR REACTIONS, ICPND ^46,48,50Ti(¹²C, X), ⁴⁴Ca(¹⁸O, X), E(cm) ≈ 20-45 MeV; ^28,30Si(³⁰Si, X), E(cm) ≈ 25-45 MeV; measured fusion σ(E). ^48,50Ti(¹²C, ¹²C'), E=20-60 MeV; ⁴⁴Ca(¹⁸O, ¹⁸O'), E=30-60 MeV; measured inelastic σ(E); deduced barrier parameters. Hyperpure Ge, Ge(Li) detectors, in-beam γ-rays, rotating target. Zero-point motion, neck formation.

doi: 10.1016/0375-9474(84)90143-X
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1982DO03      Nucl.Phys. A378, 111 (1982)

A.D'Onofrio, H.Dumont, M.-G.Saint Laurent, B.Delaunay, F.Terrasi, J.Delaunay

Absolute Residue Cross Sections for ^46-50Ti + ¹³C Reactions at 36, 46 and 56 MeV

NUCLEAR REACTIONS, ICPND ^{46,47,48,49,50}Ti(¹³C, 2np), (¹³C, 2n2p), (¹³C, nα), (¹³C, 2nα), (¹³C, 2npα), (¹³C, n2α), (¹³C, 3α), (¹³C, ¹³C'), ⁴⁶Ti(¹³C, n3p), (¹³C, 2pα), (¹³C, p2α), ^46,47Ti(¹³C, pα), (¹³C, n2pα), (¹³C, 2α), (¹³C, np2α), ^47,48,49,50Ti(¹³C, 3np), (¹³C, 2n2α), (¹³C, 3n), ^48,49,50Ti(¹³C, 2n), (¹³C, 3nα), ^46,47,48,49Ti(¹³C, n2p), (¹³C, npα), ^49,50Ti(¹³C, 4n), (¹³C, 4np), E=36, 46, 56 MeV; ^46,47,48Ti(¹³C, np), ^47,48Ti(¹³C, 2p), E=36 MeV; measured σ for evaporation residues. In-beam techniques, enriched targets. Statistical particle evaporation calculations.

doi: 10.1016/0375-9474(82)90385-2
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1981CA17      Fizika(Zagreb) 13, Suppl.No.1, 52 (1981)

S.Cavallaro, L.Sperduto, H.Dumont, M.G.Saint-Laurent, B.Delaunay, J.Delaunay, A.D'Onofrio

Excitation Function of Evaporation Residues for the System ⁴⁶Ti + ¹²C in the Range 21-57 MeV(lab)

NUCLEAR REACTIONS ⁴⁶Ti(¹²C, X), E=21-57 MeV; measured production σ(E) for ⁵¹Cr, ⁴⁹V, ⁵⁵Fe, ⁵³Mn. In-beam spectroscopy. Statistical model.

1981DU21      Fizika(Zagreb) 13, Suppl.No.1, 64 (1981)

H.Dumont, E.Bozek, A.Brondi, B.Delaunay, J.Delaunay, A.D'Onofrio, D.Rizzo, M.G.Saint Laurent, F.Terrasi

Evidence for Massive Transfer Processes in the Reaction ⁴⁸Ti + ¹³C at 46 MeV

NUCLEAR REACTIONS ⁴⁸Ti(¹³C, X), E=46 MeV; measured (particle)γ-coin; deduced massive transfer process, production of ^52,51Cr, ⁵⁰V, ^49,48Ti, ^47,46Sc. ΔE-E telescopes.

1981RI13      Fizika(Zagreb) 13, Suppl.No.1, 53 (1981)

D.Rizzo, E.Bozek, B.Delaunay, J.Delaunay, A.D'Onofrio, H.Dumont, M.G.Saint Laurent, F.Terrasi

Excitation Functions of the Neutron Transfer and Inelastic Scattering for ¹³C on ⁴⁸Ti (25-60 MeV lab)

NUCLEAR REACTIONS ⁴⁸Ti(¹³C, ¹²C), (¹³C, ¹³C'), E=25-60 MeV; measured σ(E). In-beam γ-spectroscopy.

1979HE07      Phys.Lett. 85B, 34 (1979)

H.P.Hellmeister, U.Kaup, J.Keinonen, K.P.Lieb, R.Rascher, R.Ballini, J.Delaunay, H.Dumont

Band Structure of ⁷⁸Kr

NUCLEAR REACTIONS ⁶⁵Cu(¹⁶O, 2np), E=42-58 MeV; measured Eγ, Iγ, γ(θ), γγ-coin, DSA. ⁷⁸Kr deduced levels, J, π, T_1/2, γ branching, B(E2). Neutron-proton boson model.

doi: 10.1016/0370-2693(79)90771-8
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1979HE18      Nucl.Phys. A332, 241 (1979)

H.P.Hellmeister, J.Keinonen, K.P.Lieb, U.Kaup, R.Rascher, R.Ballini, J.Delaunay, H.Dumont

Study of High Spin States in ⁷⁸Kr

NUCLEAR REACTIONS ⁶⁵Cu(¹⁶O, 2np), E=42-58 MeV; ⁶⁵Cu(¹⁹F, 2nα), E=55 MeV; ⁶⁴Ni(¹⁶O, 2n), E=47 MeV; ⁶⁸Zn(¹²C, 2n), E=30-36 MeV; ⁶⁵Cu(¹⁶O, 3n), E=54 MeV; measured Eγ, Iγ(θ), DSA, RDM. ⁷⁸Kr deduced levels, J, π, T_1/2. Enriched target.

doi: 10.1016/0375-9474(79)90107-6
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1979MO06      Nucl.Phys. A318, 236 (1979)

G.Moyat, B.Delaunay, J.Delaunay, J.Eberth, V.Zobel, L.Cleemann

Lifetimes and Parities of the Yrast States of ⁶⁰Ni

NUCLEAR REACTIONS ⁵¹V(¹²C, 2np), E ≈ 36 MeV; measured recoil distance line-shape analysis. ⁶⁰Ni levels deduced T_1/2, π. Monoisotopic target; 3 Ge(Li) polarimeter, resolution 1.8 keV at 1.33 MeV.

doi: 10.1016/0375-9474(79)90481-0
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1978HE22      Fizika, Suppl. 10, 13 (1978)

H.P.Hellmeister, J.Keinonen, K.P.Lieb, R.Rascher, R.Ballini, J.Delaunay, H.Dumont

Band Structure of ⁷⁸Kr

NUCLEAR REACTIONS ⁶⁵Cu(¹⁶O, 2np), E=42, 53, 54, 58 MeV; measured γγ-coin, γ(θ), σ(Eγ), DSA. ⁷⁸Kr deduced levels, T_1/2, J, π, band structure.

1978NO07      Nucl.Phys. A305, 262 (1978)

T.Nomura, J.Delaunay, C.Tosello, N.Bendjaballah

Partial Breakdown of the Evaporation Model and Possible Preequilibrium α-Particle Emission in Heavy-Ion Fusion Reactions

NUCLEAR REACTIONS ⁵²Cr(¹²C, X), E=56.0 MeV; ⁴⁸Ti(¹⁶O, X), E=57.7 MeV; measured Eγ, Iγ; deduced product cross sections. Enriched targets. Compared with evaporation model.

doi: 10.1016/0375-9474(78)90177-X
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1977BE16      Nucl.Phys. A280, 228 (1977)

N.Bendjaballah, B.Delaunay, J.Delaunay, T.Nomura

High Spin States in ⁵⁷Co

NUCLEAR REACTIONS ⁴⁸Ti(¹²C, 2np), E=26-48 MeV; ⁵⁴Fe(α, p)E=12-24 MeV; measured σ(E, Eγ, θ), γγ-coin, DSA. ⁵⁷Co deduced levels, J, T_1/2, δ. Enriched targets.

doi: 10.1016/0375-9474(77)90306-2
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1977BE27      Nucl.Phys. A284, 513 (1977)

N.Bendjaballah, J.Delaunay, A.Jaffrin, T.Nomura, K.Ogawa

The Level Structure of ⁵⁶Fe

NUCLEAR REACTIONS ⁵⁰Cr(¹²C, 2pα), E=26-58 MeV; ⁵⁴Fe(α, 2p), E=12-24 MeV; ⁵⁶Fe(α, α), E=12-24 MeV; measured σ(E, Eγ), γγ-coin, σ(E, Eγ, θ), T_1/2 by Doppler methods. ⁵⁶Fe deduced levels, spins, T_1/2, mixing ratios. Enriched targets.

doi: 10.1016/0375-9474(77)90400-6
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1977CA28      Nucl.Phys. A293, 125 (1977)

S.Cavallaro, J.Delaunay, R.Ballini, T.Nomura, N.Bendjaballah, C.Tosello

High Spin Levels in ⁵⁸Fe: Ground-State and Quasi-γ Bands

NUCLEAR REACTIONS ⁵⁵Mn(α, p), E=12-24 MeV; measured reaction products, Eγ, Iγ, γγ-coin, ⁵⁸Fe; deduced levels, J, σ(E, Eγ), σ(E, Eγ, θ), T_1/2, mixing ratios, B(E2), B(M1). Monoisotopic target. Doppler Shift Attenuation (DSA).

doi: 10.1016/0375-9474(77)90481-X
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1976BA10      Nucl.Phys. A258, 388 (1976)

R.Ballini, N.Bendjaballah, J.Delaunay, J.P.Fouan, V.Tokarevsky

High-Spin States in ⁵⁸Ni

NUCLEAR REACTIONS ⁴⁸Ti(¹²C, 2nγ), E=26-48 MeV; measured σ(E, Eγ, θ), γγ-coin. ⁵⁶Fe(α, 2nγ), E=18-24 MeV; measured σ(E, Eγ). ⁵⁸Ni deduced levels, J, δ. Enriched targets.

doi: 10.1016/0375-9474(76)90013-0
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1976BE26      Phys.Rev.Lett. 36, 1536 (1976)

N.Bendjaballah, J.Delaunay, T.Nomura, H.J.Kim

Possible Shape Transition in the Yrast Band of ⁵⁶Fe

NUCLEAR REACTIONS ⁵⁰Cr(¹²C, 2pαγ), E=26-58 MeV; ⁵⁴Fe(α, 2pγ), ⁵⁶Fe(α, α), E=12-24 MeV; measured σ(E, Eγ, θ), γγ-coin. ⁵⁴Fe(α, 2pγ), E=20, 24 MeV; measured DSA. ⁵⁶Fe deduced levels, J, π, T_1/2, B(λ).

doi: 10.1103/PhysRevLett.36.1536
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1976FO06      J.Phys.(London) G2, 365 (1976)

I.Fodor, I.Szentpetery, A.Schmiedekamp, K.Beckert, H.U.Gersch, J.Delaunay, B.Delaunay, R.Ballini

Analogue Resonances in the ⁶⁴Zn Nucleus

NUCLEAR REACTIONS ⁶³Cu(p, γ), E=3145-3275 keV; measured σ(E, Eγ). ⁶⁰Ni(α, p), E=7260-7450 keV; measured σ(E, Ep). ⁶⁴Zn deduced IAS, levels, J, π, Γγ, resonance strength.

doi: 10.1088/0305-4616/2/6/005
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1976PI05      Nucl.Phys. A264, 132 (1976)

M.Pichevar, J.Delaunay, B.Delaunay, H.J.Kim, Y.El Masri, J.Vervier

High-Spin States in ⁵⁹Ni

NUCLEAR REACTIONS ⁵⁰Cr(¹²C, n2pγ), E=26-58 MeV; ⁵⁶Fe(α, nγ), E=10, 15, 22.5 MeV; measured σ(E, Eγ, θ), γγ-coin. ⁵⁹Ni deduced levels, J, mixing ratios. Enriched ⁵⁰Cr target.

doi: 10.1016/0375-9474(76)90149-4
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1975BE22      Nucl.Phys. A244, 322 (1975)

N.Bendjaballah, J.Delaunay, H.J.Kim

High-Spin Yrast Cascade in ⁵⁶Co

NUCLEAR REACTIONS ⁵⁰Cr(¹²C, npαγ), E=26-58 MeV; measured σ(E, Eγ), γγ-coin, γγ(θ). ⁵⁶Co levels deduced J, δ. Ge(Li) detectors.

doi: 10.1016/0375-9474(75)90062-7
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1975KI16      Nucl.Phys. A250, 211 (1975)

H.J.Kim, R.Ballini, B.Delaunay, J.Delaunay, J.P.Fouan, M.Pichevar

Yrast Cascade in ⁶⁰Ni

NUCLEAR REACTIONS ⁵⁸Ni(α, 2pγ), E=15-25 MeV; ⁴⁶Ti(¹⁶O, 2pγ), E=30-60 MeV; measured σ(E, Eγ), γγ-coin. ⁵⁰Cr(¹²C, 2pγ), E=26-48 MeV; measured σ(E, Eγ, θ), γγ-coin. ⁶⁰Ni deduced levels, J.

doi: 10.1016/0375-9474(75)90209-2
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1975TU02      Acta Phys.Pol. B6, 123 (1975)

I.M.Turkiewicz, J.Delaunay, J.P.Fouan

The Study of ¹⁴N(α, d)¹⁶O Reaction at 21 MeV

NUCLEAR REACTIONS ¹⁴N(α, d), (α, α), E=21 MeV; measured σ(Ed, θ). ¹⁶O levels deduced L.

1974PI03      Nucl.Phys. A224, 34 (1974)

M.Pichevar, J.Delaunay, B.Delaunay

Lifetime Measurements in ⁵⁹Ni and ⁵⁷Ni

NUCLEAR REACTIONS ⁵⁶Fe(α, nγ), E=7.5-10.5 MeV; ⁵⁴Fe(α, nγ), E=9 MeV; measured Eγ, Doppler shift attenuation. ^57,59Ni levels deduced T_1/2. Ge(Li) detector, enriched targets.

doi: 10.1016/0375-9474(74)90160-2
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1973RO20      Nucl.Phys. A207, 577 (1973)

H.Ronsin, P.Beuzit, J.Delaunay, R.Ballini, I.Fodor, J.P.Fouan

Lifetimes and Decays of Energy Levels in ⁶⁰Ni

NUCLEAR REACTIONS ⁶⁰Ni(p, p'γ), E=12 MeV, measured Doppler shift attenuation. ⁶⁰Ni deduced levels, T_1/2, J, π, B(Eλ). ⁵⁹Co(³He, dγ), E=18 MeV, measured dγ coin. ⁶⁰Ni deduced levels, J, π. ⁵⁹Co natural target, ⁶⁰Ni enriched target, Ge(Li) detector.

doi: 10.1016/0375-9474(73)90863-4
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1971TE02      Phys.Lett. 34B, 131 (1971)

A.Tellez, J.Delaunay, H.Ronsin

M1, Δ T = 1 and Δ T = 0 Transitions from the (f₇/₂d₃/₂^-1) T = 1 and (p₃/₂d₃/₂^-1)0-, T=0 States in ⁴⁰Ca

NUCLEAR REACTIONS ⁴⁰Ca(p, p'γ), E=12 MeV; ³⁹K(³He, dγ), E=18 MeV; measured Doppler shift attenuation, σ(Ep', Eγ), σ(Ed, Eγ). ⁴⁰Ca deduced levels, T_1/2, level-width.

doi: 10.1016/0370-2693(71)90687-3
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1970TE05      J.Phys.(Paris), 31, Colloq.C2-172 (1970)

A.Tellez, J.P.Fouan, R.Ballini, J.Cabe, J.Delaunay

Reactions induites par ⁷Li sur ³⁶Ar

NUCLEAR REACTIONS ³⁶Ar(⁷Li, t), (⁷Li, ⁶He), E=26.75 MeV; measured ³H, ⁶He spectra at 26-50 deg; deduced ⁴⁰Ca energy levels, J, π.

doi: 10.1051/jphyscol:1970256
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1970TU02      Nucl.Phys. A143, 641 (1970)

I.M.Turkiewicz, P.Beuzit, J.Delaunay, J.P.Fouan

Nuclear Structure Studies by the ^62-64Ni(d, p) Reaction

NUCLEAR REACTIONS ^62,64Ni(d, p), E=11.5 MeV; measured σ(Ep, θ). ^63,65Ni deduced levels, L, π, S. Enriched targets.

doi: 10.1016/0375-9474(70)90553-1
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1969BE18      Nucl.Phys. A137, 97 (1969)

P.Beuzit, J.Delaunay, J.P.Fouan, H.Ronsin

Study of Decay Schemes of ⁵⁸Ni Levels

NUCLEAR REACTIONS ⁵⁸Ni(p, p'γ), E = 12 MeV; measured σ(Ep', Eγ). ⁵⁸Ni deduced levels, branching ratios for some levels. NaI(Tl), Si(Li), Ge(Li) detectors. Enriched targets.

doi: 10.1016/0375-9474(69)90075-X
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1969BE20      Nucl.Phys. A128, 594 (1969)

P.Beuzit, J.Delaunay, J.P.Fouan, N.Cindro

Levels of ⁶²Ni and ⁶⁴Ni

NUCLEAR REACTIONS ^62,64Ni(p, p'γ), E=12 MeV; measured σ(Ep', θ(p')), σ(Ep, Eγ). ^62,64Ni deduced levels, γ-branching, L, deformation parameter β(L), reduced transition probabilities. Enriched targets.

doi: 10.1016/0375-9474(69)90425-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0458.

1969TE03      Nucl.Phys. A127, 438 (1969)

A.Tellez, R.Ballini, J.Delaunay, J.P.Fouan

Study of Excited States of ⁴⁰Ca and ⁴⁸Ca by the (p, p'γ) Reaction at E=12 MeV

NUCLEAR REACTIONS ^40,48Ca(p, p'γ), E=12 MeV; measured σ(Ep', θ) σ(Ep', Eγ). ^40,48Ca deduced levels, L, deformation parameters β(L), reduced transition probabilities, γ-ray branching. Enriched targets.

doi: 10.1016/0375-9474(69)90584-3
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0387.

1969TE05      Phys.Letters 29B, 655 (1969)

A.Tellez, R.Ballini, J.Delaunay, J.P.Fouan

Excitation and Gamma Decay of (f₇/₂³, d₃/₂^-1)T=1 and T=2 States in ⁴²Ca

NUCLEAR REACTIONS ⁴¹K(³He, dγ), E=18 MeV; ⁴²Ca(p, p'γ), E=12 MeV; measured σ(Ed, Eγ, θ(d)), σ(Ep', Eγ). ⁴²Ca deduced levels, T, γ-branching.

doi: 10.1016/0370-2693(69)90101-4
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1968BA05      Phys.Letters 26B, 215 (1968)

R.Ballini, N.Cindro, J.Delaunay, J.P.Fouan, O.Nathan, J.P.Passerieux

The Reaction ²⁰⁷Pb(d, pγ₀)²⁰⁸Pb at 10 MeV

NUCLEAR STRUCTURE ²⁰⁸Pb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0370-2693(68)90345-6
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1968BA14      Nucl.Phys. A111, 147 (1968)

R.Ballini, A.G.Blair, N.Cindro, J.Delaunay, J.P.Fouan

The Levels of ⁶⁰Ni

NUCLEAR REACTIONS ⁶⁰Ni(p, p'γ), E=13 MeV; measured σ(Ep', Eγ, θ p'). ⁵⁹Co(³He, dγ), E=18, 22 MeV; measured σ(Ed, Eγ, θ(d)). ⁶⁰Ni deduced levels, L(p), deformation parameters, S, transition probabilities. Enriched targets.

doi: 10.1016/S0375-9474(68)90620-9
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1968BA64      Izv.Akad.Nauk SSSR, Ser.Fiz. 32, 1653 (1968); Bull.Acad.Sci.USSR, Phys.Ser. 32, 1533 (1969)

R.Ballini, J.Delaunay, J.P.Fouan, A.G.Blair, N.Cindro

Single Particle-Hole and Collective Levels in ⁴⁰Ca and ⁶⁰Ni

NUCLEAR REACTIONS ³⁹K(³He, dγ), E = 18 MeV; ⁵⁹Co(³He, dγ), E = 22 MeV; measured σ(Ed, Eγ). ⁴⁰Ca, ⁶⁰Ni(p, p'γ), E = 13 MeV; measured σ(Ep', Eγ). ⁴⁰Ca, ⁶⁰Ni deduced levels, L(p), S, J, π.

1967BA02      Phys.Rev.Letters 18, 408 (1967)

R.Ballini, N.Cindro, J.Delaunay, J.P.Fouan, M.Loret, J.P.Passerieux

Excitation of Simple Configurations in the Outgoing Reaction Channel

NUCLEAR STRUCTURE ⁴⁰Ca; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.18.408
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1967BA19      Nucl.Phys. A97, 561(1967)

R.Ballini, N.Cindro, J.Delaunay, J.Fouan, M.Loret, J.P.Passerieux

Proton Spin-Flip in Inelastic Scattering ⁵²Cr and ⁵⁴Fe

NUCLEAR REACTIONS ⁵²Cr, ⁵⁴Fe(p, p'γ), E = 11 MeV; measured σ(Ep', Eγ, θ); deduced proton spin-flip probability for 2+ states. Enriched ⁵⁴Fe target.

doi: 10.1016/0375-9474(67)90520-9
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1967BE28      Phys.Rev.Letters 19, 94 (1967)

P.Beuzit, Y.Cassagnou, N.Cindro, E.Cotton, J.Delaunay, J.P.Fouan, L.Papineau

Search for 2p-1h Configurations in Mirror Nuclei ⁴¹Ca and ⁴¹Sc

NUCLEAR STRUCTURE ⁴¹Sc; measured not abstracted; deduced nuclear properties.

doi: 10.1103/PhysRevLett.19.94
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1966BA23      Phys.Letters 21, 708 (1966)

R.Ballini, N.Cindro, J.Delaunay, J.Fouan, M.Loret, J.P.Passerieux

Levels in ⁶⁰Ni and ⁶²Ni at High Excitation Energies

NUCLEAR STRUCTURE ⁶⁰Ni, ⁶²Ni; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90135-1
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1966BA50      CEA-N-621, p.18 (1966)

R.Ballini, N.Cindro, J.Delaunay, J.Fouan, M.Loret, J.P.Passerieux

Experiences (p, p') et (p, p'γ) sur ⁶⁰Ni et ⁶²Ni

NUCLEAR STRUCTURE ⁶⁰Ni, ⁶²Ni; measured not abstracted; deduced nuclear properties.