NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = J.F.Bruandet Found 33 matches. 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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
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
Back to query form |