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NSR database version of May 24, 2024.

Search: Author = J.F.Bruandet

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1999DO19      Nucl.Phys. A656, 259 (1999)

L.Donadille, E.Liatard, B.Benoit, F.Hanappe, L.Stuttge, G.Rudolf, E.M.Kozulin, Yu.A.Lazarev, P.Desesquelles, L.A.Litnevsky, B.Bilwes, J.-F.Bruandet, G.J.Costa, O.Dorvaux, F.Farget, J.Fayot, G.Guillaume, A.Huck, I.Itkis, M.G.Itkis, S.Jokic, N.A.Kondratev, F.-R.Lecolley, J.-F.Lecolley, Yu.Ts.Oganessian, G.Perrin, D.Santos, F.Schussler, S.Tomasevic, J.-B.Viano, B.Vignon

Fission Dynamics for Capture Reactions in 58, 64Ni + 208Pb Systems: New results in terms of thermal energy and neutron multiplicity correlated distributions

NUCLEAR REACTIONS 208Pb(58Ni, F), E=6.5-8.9 MeV/nucleon; 208Pb(64Ni, F), E=5.9-7.4 MeV/nucleon; measured fission fragments mass, kinetic energy distributions, neutron multiplicity; deduced friction coefficient, fission time, pre-, post-scission neutron distributions. Combined dynamical and statistical model.

doi: 10.1016/S0375-9474(99)00306-1
Citations: PlumX Metrics


1990AZ04      Phys.Rev.Lett. 65, 305 (1990)

F.Azaiez, M.M.Aleonard, S.Andriamonje, J.F.Chemin, J.N.Scheurer, D.W.Spooner, J.P.Thibaud, J.F.Bruandet, E.Liatard, F.Beck, G.Costa

Observation of Characteristic X Rays Emitted During Sequential Proton Evaporation by the 112Xe Compound Nucleus

NUCLEAR REACTIONS 54Fe(58Ni, X), E=4.1 MeV/nucleon; measured Doppler shifted (X-ray)(evaporation residue)-coin; deduced mean proton width. Evaporation of 3p from compound nucleus.

doi: 10.1103/PhysRevLett.65.305
Citations: PlumX Metrics


1990EL04      Nucl.Phys. A517, 340 (1990)

Y.El Masri, F.Hanappe, J.C.Steckmeyer, V.Martin, G.Bizard, B.Borderie, R.Brou, J.F.Bruandet, P.Duhamel, H.Fuchs, J.L.Laville, J.Peter, R.Regimbart, M.Rivet, B.Tamain, T.U.Chan

Gamma-Ray Multiplicity Measurements for the Determination of the Initial Angular Momentum Ranges in Normal and Fast Fission Processes

NUCLEAR REACTIONS 165Ho(40Ar, F), E=315 MeV; Re(20Ne, F), E=220 MeV; measured γ-multiplicity vs fission fragment mass, total kinetic energy; deduced fission mechanism, fragment mass distribution, critical angular momentum.

doi: 10.1016/0375-9474(90)90039-O
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1990LI39      Europhys.Lett. 13, 401 (1990)

E.Liatard, J.F.Bruandet, F.Glasser, S.Kox, T.U.Chan, G.J.Costa, C.Heitz, Y.El Masri, F.Hanappe, R.Bimbot, D.Guillemaud-Mueller, A.C.Mueller

Matter Distribution in Neutron-Rich Light Nuclei and Total Reaction Cross-Section

NUCLEAR STRUCTURE 6,7,8,9,11Li, 9,10,11,12,14Be, 10,11,12,13,14,15,17B; analyzed data; deduced rms radii.

doi: 10.1209/0295-5075/13/5/004
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1989AZ02      Nucl.Phys. A501, 401 (1989)

F.Azaiez, S.Andriamonje, J.F.Chemin, M.Fidah, J.N.Scheurer, M.M.Aleonard, G.Bastin, J.P.Thibaud, G.Costa, F.Beck, J.F.Bruandet, E.Liatard

High-Spin States in Neutron Deficient 106Sn and 108Sn Isotopes

NUCLEAR REACTIONS 54Fe(58Ni, 4p), (58Ni, 2pα), E=268 MeV; measured Eγ, Iγ, γγ-coin, linear polarization. 108Sn, 106Sn deduced levels J, π. Enriched target, Ge(Li) detectors.

doi: 10.1016/0375-9474(89)90299-6
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1989SA10      Z.Phys. A332, 457 (1989)

M.G.Saint-Laurent, R.Anne, D.Bazin, D.Guillemaud-Mueller, U.Jahnke, Jin Gen-Ming, A.C.Mueller, J.F.Bruandet, F.Glasser, S.Kox, E.Liatard, Tsan Ung Chan, G.J.Costa, C.Heitz, Y.El-Masri, F.Hanappe, R.Bimbot, E.Arnold, R.Neugart

Total Cross Sections of Reactions Induced by Neutron-Rich Light Nuclei

NUCLEAR REACTIONS Cu(X, X), E not given; measured reaction σ for projectile X=4,6He, 6,7,8,9,11Li, 7,9,10,11,12,14Be, 10,11,12,13,14,15,17B, 11,12,13,14,15,16,17,18,19C, 13,14,15,16,17,18,19N, 15,16,17,18,19,20,21O, 18,19,20,21F, 20,21Ne. Secondary beams, 4π γ method.


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.


1987KO12      Phys.Rev. C35, 1678 (1987)

S.Kox, A.Gamp, C.Perrin, J.Arvieux, R.Bertholet, J.F.Bruandet, M.Buenerd, R.Cherkaoui, A.J.Cole, Y.El-Masri, N.Longequeue, J.Menet, F.Merchez, J.B.Viano

Trends of Total Reaction Cross Sections for Heavy Ion Collisions in the Intermediate Energy Range

NUCLEAR REACTIONS, MECPD 12C(12C, X), E=9.33 MeV/nucleon; 12C, 27Al, 40Ca, 54,56,57Fe, Fe, 64,66,68Zn, Zn, 89Y, Ag(12C, X), E=30, 83, 200, 250, 300 MeV/nucleon; 27Al, 89Y(16O, X), E=30 MeV/nucleon; 12C, 27Al, 56Fe, 64Zn, Ag(20Ne, X), E=30, 100, 200, 300 MeV/nucleon; measured reaction σ. Tof. Model calculation.

doi: 10.1103/PhysRevC.35.1678
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1986LI27      Z.Phys. D2, 223 (1986)

E.Liatard, J.F.Bruandet, F.Glasser, Tsan Ung Chan, G.J.Costa, C.Gerardin, C.Heitz, M.Samri, R.Seltz

K-Shell Ionization Induced by 30 MeV/u Argon and Neon Beams

NUCLEAR REACTIONS 59Co, Cu, 89Y, 92Mo, Ag, Sm, 165Ho, 181Ta, Pt, 197Au, 209Bi, 232Th(20Ne, X), (40Ar, X), E=30 MeV/nucleon; measured X-ray spectra; deduced K-shell ionization σ ratio.

doi: 10.1007/BF01429077
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1985KO24      Phys.Lett. 159B, 15 (1985)

S.Kox, A.Gamp, C.Perrin, J.Arvieux, R.Bertholet, J.F.Bruandet, M.Buenerd, Y.El Masri, N.Longequeue, F.Merchez

Transparency Effects in Heavy-Ion Collisions over the Energy Range 100-300 MeV/Nucleon

NUCLEAR REACTIONS Zn, 27Al, 20Ne, Fe(12C, X), E ≈ 30-500 MeV/nucleon; 12C(12C, X), E ≈ 10-200 MeV/nucleon; measured reaction σ(E); deduced surface transparency role. Microscopic calculations.

doi: 10.1016/0370-2693(85)90110-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0775.


1984TS02      Phys.Rev. C29, 441 (1984)

Tsan Ung Chan, C.Morand, F.Azgui, M.Agard, J.F.Bruandet, B.Chambon, A.Dauchy, D.Drain, A.Giorni, F.Glasser

Level Structure of 60Ni from the 58Ni(α, 2pγ) Reaction

NUCLEAR REACTIONS 58Ni(α, 2p), E=23-40 MeV; measured Eγ, Iγ(θ), γγ-coin, DSA. 60Ni deduced levels, J, π, configuration, γ-branching ratios, yrast band, B(λ).

doi: 10.1103/PhysRevC.29.441
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1982TS04      Phys.Rev. C26, 424 (1982)

Tsan Ung Chan, M.Agard, J.F.Bruandet, B.Chambon, A.Dauchy, D.Drain, A.Giorni, F.Glasser, C.Morand

High-Spin States in 60Cu

NUCLEAR REACTIONS 58Ni(α, pn), E=24-40 MeV: measured Eγ, Iγ(θ), γγ-coin, DSA. 60Cu deduced high-spin levels, J, π, T1/2, E1, E2 transition strength, γ-branching.

doi: 10.1103/PhysRevC.26.424
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1980CH28      Nucl.Phys. A348, 179 (1980)

Tsan Ung Chan, J.F.Bruandet, B.Chambon, A.Dauchy, D.Drain, A.Giorni, F.Glasser, C.Morand

Niveaux de Spin Eleve dans le 63Cu Etat Isomerique Yrast 17/2+

NUCLEAR REACTIONS 61Ni(α, np), E=21-35 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 63Cu deduced levels J, π, γ-branching, T1/2. Isotopic target.

doi: 10.1016/0375-9474(80)90333-4
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1979CH01      Phys.Rev. C19, 244 (1979)

T.U.Chan, M.Agard, J.F.Bruandet, C.Morand

Crude Shell-Model Location of Two-Particle High-Spin States Corresponding to a Maximum Spin Coupling Configuration

NUCLEAR STRUCTURE 26Mg, 30Si, 34S, 38Ar, 42Ca, 60,62,64Cu, 66,68Zn, 68,70,72Ge; calculated energies of two-nucleon high spin states, coupling to maximum spin of two nucleons. Simple shell model.

doi: 10.1103/PhysRevC.19.244
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1979MO01      Nucl.Phys. A313, 45 (1979)

C.Morand, J.F.Bruandet, B.Chambon, A.Dauchy, D.Drain, A.Giorni, Tsan Ung Chan

Niveaux de Spin Eleve du 72Ge Atteints par la Reaction 70Zn(α, 2nγ) A E = 30 MeV

NUCLEAR REACTIONS 70Zn(α, 2nγ), E=22-35 MeV; measured σ(E, Eγ, θ), γγ-coin, γγ(θ), γ(t), DSA, Iγ. 72Ge deduced levels, J, π, T1/2, γ-branching, B(E2).

doi: 10.1016/0375-9474(79)90567-0
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1978CH34      Fizika, Suppl. 10, 7 (1978)

T.-U.Chan, M.Agard, J.F.Bruandet, A.Dauchy, A.Giorni, F.Glasser, J.E.Koops, C.Morand, B.Chambon, D.Drain

High-Spin States in 60Cu and a Simple Shell-Model Description of the Jπ = 6- and 9+ States in the Odd-Odd Cu Isotopes

NUCLEAR REACTIONS 58Ni(α, np), E=32 MeV; measured γγ-coin, γ(θ), σ(Eγ). 60Cu deduced levels, J, π, configurations.


1978MO21      Nucl.Phys. A308, 103 (1978)

C.Morand, M.Agard, J.F.Bruandet, A.Dauchy, A.Giorni, F.Glasser, Tsan Ung Chan

Etats de Spin Eleve du 66Ga

NUCLEAR REACTIONS 64Zn(α, npγ), E=22-40 MeV; 63Cu(α, nγ), E=18 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 66Ga deduced levels, J, π, γ-branching. Isotopic targets.

doi: 10.1016/0375-9474(78)90444-X
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1977CH31      Nucl.Phys. A293, 207 (1977)

Tsan Ung Chan, M.Agard, J.F.Bruandet, A.Giorni, F.Glasser, J.P.Longequeue, C.Morand

Etats de Grand Spin du 62Cu

NUCLEAR REACTIONS 60Ni(α, npγ), E=22-35 MeV; 63Cu(p, npγ), E=22-28 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 52Cr(14N, 2n2pγ), E=50-75 MeV; measured Iγ. 62Cu deduced levels J, π, γ-branching. Isotopic target.

doi: 10.1016/0375-9474(77)90487-0
Citations: PlumX Metrics


1977GI18      Nucl.Phys. A292, 213 (1977)

A.Giorni, F.Glasser, F.Brut, C.Morand, J.F.Bruandet, J.P.Longequeue, Tsan Ung Chan

Niveaux de Haut Spin du 50V Observes par la Reaction 48Ti(α, pnγ)

NUCLEAR REACTIONS 48Ti(α, np), E=21-35 MeV; measured σ(E, Eγ, θ), Eγ, Iγ, DSA, γγ-coin. 50V deduced levels, J, π, T1/2, γ-branching. Isotopic target.

doi: 10.1016/0375-9474(77)90369-4
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1977MO01      J.Phys.(Paris) 38, 105 (1977)

C.Morand, M.Agard, J.F.Bruandet, A.Giorni, J.P.Longequeue, Tsan Ung Chan

High Spin Levels in 70Ga via 68Zn(α, pnγ)70Ga

NUCLEAR REACTIONS 68Zn(α, npγ), E=23-40 MeV; measured σ(E, Eγ, θ), γγ(t). 70Ga deduced levels, J, π, T1/2, λ, γ-branching.

doi: 10.1051/jphys:01977003802010500
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1977MO20      J.Phys.(Paris) 38, 1319 (1977)

C.Morand, J.F.Bruandet, A.Giorni, Tsan Ung Chan

Mesure de Durees de Vie par DSAM au Moyen de la Reaction (α, 2nγ) a E = 30 MeV sur Cible Autoporteuse: Application Aux 70Ge, 68Ge et 66Zn

NUCLEAR REACTIONS 66,68Zn, 64Ni(α, 2nγ), E=30 MeV; measured DSA. 68,70Ge, 66Zn levels deduced T1/2, δ, λ.

doi: 10.1051/jphys:0197700380110131900
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1976BR12      J.Phys.(Paris), Lett. 37, L-63 (1976)

J.F.Bruandet, F.Glasser, M.Agard, A.Giorni, J.P.Longequeue, Tsan Ung Chan

Niveaux de Spin Eleve dans le Noyau 64Zn

NUCLEAR REACTIONS 62Ni(α, 2nγ), E=22-40 MeV; measured σ(E, Eγ, θ), γγ-coin. 54Fe(12C, 2pγ), E=36-48 MeV; measured σ(E, Eγ). 55Mn(12C, 2npγ), E=35 MeV; measured recoil distance. 64Zn deduced levels, J, π, T1/2.

doi: 10.1051/jphyslet:0197600370406300
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1976BR23      Phys.Rev. C14, 103 (1976)

J.F.Bruandet, B.Berthet, C.Morand, A.Giorni, J.P.Longequeue, Tsan Ung Chan

High-Spin States in 68Zn

NUCLEAR REACTIONS 65Cu(α, pγ), E=12-21 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 68Zn deduced levels, J, π, δ, T1/2 limit. Enriched target, Ge(Li) detectors.

doi: 10.1103/PhysRevC.14.103
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1976BR33      Z.Phys. A279, 69 (1976)

J.F.Bruandet, Tsan Ung Chan, M.Agard, J.P.Longequeue, C.Morand, A.Giorni

In Beam Gamma Spectroscopy of 62Zn

NUCLEAR REACTIONS 60Ni(α, 2nγ), E=28-35 MeV; 63Cu(p, 2nγ), E=22-31 MeV; measured Eγ, Iγ, γγ-coin, γ(θ, t). 62Zn deduced levels, J, π, T1/2, λ. Enriched target, Ge(Li) detectors.

doi: 10.1007/BF01409093
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1976CH17      J.Phys.(Paris), Lett. 37, L-237 (1976)

T.U.Chan, M.Agard, J.F.Bruandet, A.Giorni, F.Glaser, J.P.Longequeue, C.Morand

Ferromagnetic Effect and Spin Assignment for the 390 keV State in 62Cu

NUCLEAR REACTIONS 60Ni(α, npγ), E=32 MeV; measured γ(θ, t), Larmor precession. 63Cu(p, npγ); measured γ(t). 62Cu level deduced J, π, T1/2, g.


1976CH36      Nucl.Phys. A257, 413 (1976)

T.U.Chan, M.Agard, J.F.Bruandet, A.Giorni, J.P.Longequeue

Etude du 64Cu par la Reaction 62Ni(α, pnγ)

NUCLEAR REACTIONS 62Ni(α, npγ), E=25-40 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 65Cu(p, npγ), E=22 MeV; 61Ni(α, pγ), E=17.5 MeV; measured Iγ. 64Cu deduced levels, J, π, γ-branching. Isotopic target.

doi: 10.1016/0375-9474(76)90454-1
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1976MO15      Phys.Rev. C13, 2182 (1976)

C.Morand, M.Agard, J.F.Bruandet, A.Giorni, J.P.Longequeue, Tsan Ung Chan

70Ge High-Spin Levels via the 68Zn(α, 2nγ)70Ge Reaction

NUCLEAR REACTIONS 68Zn(α, 2nγ), E=24-40 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 70Ge deduced levels, J, π, T1/2, γ-branching.

doi: 10.1103/PhysRevC.13.2182
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1976MO22      Z.Phys. A278, 189 (1976)

C.Morand, B.Berthet, M.Agard, J.F.Bruandet, A.Giorni, F.Glasser, J.P.Longequeue, Tsan Ung Chan

High-Spin States in 68Ga

NUCLEAR REACTIONS 65Cu(α, nγ), E=12-21 MeV; 66Zn(α, npγ), E=25-40 MeV; measured σ(E, Eγ, θ), γγ(t), Eγ, Iγ. 68Ga deduced levels, J, π, γ-branching, λ, δ.

doi: 10.1007/BF01437775
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1976TS01      Nucl.Phys. A257, 413 (1976); see 76Ch36

Tsan Ung Chan, M.Agard, J.F.Bruandet, A.Giorni, J.P.Longequeue

Etude du 64Cu par la Reaction 62Ni(α, pnγ)

doi: 10.1016/0375-9474(76)90581-9
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1975BR25      Phys.Rev. C12, 1739 (1975)

J.F.Bruandet, M.Agard, A.Giorni, J.P.Longequeue, C.Morand, Tsan Ung Chan

High-Spin States in 66Zn

NUCLEAR REACTIONS 64Ni(α, 2nγ), 64Zn(α, 2nγ), E=22-40 MeV; measured σ(E, Eγ, θ), γγ-coin, γ(t). 63Cu(α, pγ), E=22 MeV; 65Cu(α, 2npγ), 68Zn(α, 2nαγ), 56Fe(12C, 2pγ), E=40 MeV; measured σ(Eγ). 66Zn deduced levels, J, π, L.

doi: 10.1103/PhysRevC.12.1739
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1972KO43      Nucl.Phys. A197, 568 (1972)

D.H.Kong-A-Siou, J.F.Bruandet, J.P.Longequeue, N.Longequeue, B.Vignon

Etude des Isotopes 44,46,48Ti par les Reactions 46,48,50Ti(p, t)

NUCLEAR REACTIONS 46,48,50Ti(p, t), E=40 MeV; measured σ(θ). 44,46,48Ti deduced levelsl, J, π, T. Enriched isotopic targets.

doi: 10.1016/0375-9474(72)91030-5
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1971BR52      Phys.Lett. 37B, 58 (1971)

J.F.Bruandet, N.Longequeue, J.P.Longequeue, B.Vignon

Spectroscopie du 48Cr Obtenue par Reaction 50Cr(p, t)48Cr

NUCLEAR REACTIONS 50Cr(p, t), E=40 MeV; measured σ(Et, θ). 48Cr deduced levels, J, π.

doi: 10.1016/0370-2693(71)90570-3
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