NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = G.Perrin Found 49 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
1999LE09 Phys.Rev. C59, 1464 (1999) R.Legrain, J.F.Lecolley, F.R.Lecolley, N.Alamanos, L.Bianchi, Y.Cassagnou, H.Dabrowski, B.Erazmus, J.Julien, D.Lebrun, Ch.LeBrun, A.Mougeot, P.Hameau, G.Perrin, P.de Saintignon, J.L.Sida, J.P.Wieleczko Kaon Production in Nucleus-Nucleus Collisions at 92 MeV Per Nucleon NUCLEAR REACTIONS 12C, Ti, 181Ta(36Ar, K+X), E=92 MeV/nucleon; measured kaon production σ. Comparison with other meson production data.
doi: 10.1103/PhysRevC.59.1464
1995LE07 Nucl.Phys. A583, 379c (1995) F.R.Lecolley, N.Alamanos, L.Bianchi, Y.Cassagnou, H.Dabrowski, B.Erazmus, J.Julien, P.Hameau, D.Lebrun, C.Le Brun, J.F.Lecolley, R.Legrain, A.Mougeot, G.Perrin, P.de Saintignon, J.L.Sida, J.P.Wieleczko Kaon Production in Nucleus - Nucleus Collisions at 92 MeV per Nucleon NUCLEAR REACTIONS 12C, Ti, 181Ta(36Ar, X), E=92 MeV/nucleon; measured K+ production probability per participant nucleon vs total available energy.
doi: 10.1016/0375-9474(94)00690-O
1992ME02 Phys.Rev. C45, 1189 (1992) A.Menchaca-Rocha, E.Garcia-Solis, E.Belmont-Moreno, M.E.Brandan, M.Buenerd, J.Chauvin, P.DeSaintignon, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, J.Y.Hostachy Low-Energy Intermediate Mass Fragments in the 16O + 12C Reaction at 38 MeV/Nucleon NUCLEAR REACTIONS 12C(16O, X), E=708 MeV; measured σ(fragment θ, E) for X=6Li, 12C, σ(θ) for Z=3-9; deduced reaction residues yield mechanism. Cascade model.
doi: 10.1103/PhysRevC.45.1189
1992PE05 Z.Phys. A342, 199 (1992) G.Perrin, H.Dabrowski, G.Duhamel-Chretien, D.Lebrun, P.de Saintignon, R.Bougault, D.Durand, A.Genoux-Lubain, C.Le Brun, J.F.Lecolley, M.Louvel Pion Production in Heavy Ion Reactions Induced by 16O and 84Kr Beams at 60 MeV per Nucleon NUCLEAR REACTIONS 7Li, 12C, 27Al, 108Ag, 197Au(16O, π+), (16O, π-), E=65 MeV/nucleon; 7Li, 12C, 27Al, 108Ag, 197Au(84Kr, X), E=60 MeV/nucleon; measured pion production σ ratio vs pion momentum; deduced projectile-target mass scaling of σ regime change.
doi: 10.1007/BF01288470
1991DU01 Phys.Rev. C43, 1116 (1991) G.Duhamel-Chretien, G.Perrin, C.Perrin, V.Comparat, E.Gerlic, S.Gales, C.P.Massolo Neutron Hole States in 89Zr via the (p(pol), d) Reaction at 58 MeV NUCLEAR REACTIONS 90Zr(polarized p, d), E=58 MeV; measured σ(θ), vector analyzing power. 89Zr deduced levels, J, π, spectroscopic factors. DWBA analysis.
doi: 10.1103/PhysRevC.43.1116
1991JU04 Phys.Lett. 264B, 269 (1991) J.Julien, D.Lebrun, A.Mougeot, P.de Saintignon, N.Alamanos, Y.Cassagnou, C.Le Brun, J.F.Lecolley, R.Legrain, G.Perrin Subthreshold K+ Production in Heavy Ion Collisions NUCLEAR REACTIONS 48Ti(36Ar, K+), E=92 MeV/nucleon; measured kaon production σ. Muon detection following kaon decay.
doi: 10.1016/0370-2693(91)90347-S
1990LE02 Z.Phys. A335, 73 (1990) D.Lebrun, J.Chauvin, J.Julien, C.LeBrun, J.F.Lecolley, G.Perrin, D.Rebreyend, P.de Saintignon π- Production in 16O + 27Al at 38, 65 and 93 MeV/u NUCLEAR REACTIONS 27Al(16O, xπ-), E=38-93 MeV/nucleon; measured σ(θ(π), E(π)); deduced pion production mechanism.
1989GE03 Phys.Rev. C39, 2190 (1989) E.Gerlic, J.Guillot, H.Langevin-Joliot, J.Van de Wiele, S.Gales, G.Duhamel, G.Perrin, C.P.Massolo, M.Sakai Stretched High-Spin Two-Neutron-Hole States in 206Pb and 114Sn via the (p, t) Reaction at 168 MeV NUCLEAR REACTIONS 116Sn, 208Pb(p, t), E=168 MeV; measured σ(θ), σ(Et). 114Sn, 206Pb deduced levels, J, π, configuration, two-neutron hole strengths. DWBA analysis.
doi: 10.1103/PhysRevC.39.2190
1989LE12 Phys.Lett. 223B, 139 (1989) D.Lebrun, J.Chauvin, D.Rebreyend, G.Perrin, P.De Saintignon, P.Martin, M.Buenerd, C.Le Brun, J.F.Lecolley, Y.Cassagnou, J.Julien, R.Legrain Heavy Ion Collision Geometry at 93 MeV/u from π-/π+ Measurement NUCLEAR REACTIONS 232Th, 197Au, Ag, 58Ni, 27Al, 12C, 7Li(16O, X)π+/π-, E=93 MeV/nucleon; measured σ(θπ) vs pion momentum, (π-/π+) yield ratio; deduced pion production mechanism.
doi: 10.1016/0370-2693(89)90229-3
1988BU21 Phys.Rev. C38, 2514 (1988) M.Buenerd, K.Bouhelal, Ph.Martin, J.Chauvin, D.Lebrun, G.Perrin, P.de Saintignon, G.Duhamel Quadrupole Transitions at Very Small Momentum Transfer in Nuclei NUCLEAR REACTIONS 58Ni, 92Mo, 120,124Sn, 140Ce, 208Pb(3He, 3He'), E=108.5 MeV; measured σ(θ). 58Ni, 92Mo, 120,124Sn, 140Ce, 208Pb deduced giant resonances excitation, deformation parameters, B(λ).
doi: 10.1103/PhysRevC.38.2514
1988DU17 Phys.Rev. C38, 2509 (1988) G.Duhamel, M.Buenerd, P.de Saintignon, J.Chauvin, D.Lebrun, Ph.Martin, G.Perrin Inelastic Alpha Scattering to the Giant Quadrupole and Monopole Resonances of 58Ni, 92Mo, and 120Sn at 152 MeV NUCLEAR REACTIONS 58Ni, 92Mo, 120Sn(α, α'), E=152 MeV; measured σ(θ). 58Ni, 92Mo, 120Sn deduced giant resonances, Γ, L, sum rule fraction.
doi: 10.1103/PhysRevC.38.2509
1988LA18 Phys.Rev. C38, 1168 (1988) H.Langevin-Joliot, V.Datar, E.Gerlic, J.Van de Wiele, F.Azaiez, S.Fortier, S.Gales, J.Guillot, J.M.Maison, C.P.Massolo, G.Duhamel, G.Perrin Highest Spin n-p States in Heavy Nuclei via the (α, d) Reaction at 218 MeV NUCLEAR REACTIONS 90Zr, 120Sn, 144Sm, 208Pb(α, d), E=218 MeV; measured σ(θ). 92Nb, 122Sb, 146Eu, 210Bi deduced levels, J, π. DWBA analysis.
doi: 10.1103/PhysRevC.38.1168
1988VO08 Nucl.Phys. A487, 195 (1988) W.von Oertzen, E.Adamides, M.Buenerd, J.Chauvin, D.Lebrun, J.Y.Hostachy, G.Duhamel, Ph.Martin, G.Perrin, P.de Saintignon Proton Transfer Induced by 13C at 30 MeV/u NUCLEAR REACTIONS 12C, 27Al, 58Ni, 90Zr(13C, 12B), (13C, 14N), E=30 MeV/nucleon; measured σ(θ). 11B, 89Y, 57Co, 91Nb, 59Cu levels deduced spectroscopic factors. DWBA analysis.
doi: 10.1016/0375-9474(88)90136-4
1987AD07 Nucl.Phys. A475, 598 (1987) E.Adamides, H.G.Bohlen, W.von Oertzen, M.Buenerd, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, G.Perrin, P.de Saintignon Three-Body Continuum in (13C, 13N) and (13C, 14N) Reactions NUCLEAR REACTIONS 12C, 27Al, 58Ni, 90Zr(13C, 13N), (13C, 14N), E=390 MeV; measured σ(θ); deduced reaction mecanism. Three-body continuum treatment. Enriched targets. Magnetic spectrometer.
doi: 10.1016/0375-9474(87)90081-9
1987AR30 Few-Body Systems 3, 27 (1987) J.Arvieux, A.Boudard, G.Gaillard, Nguyen Van Sen, G.Perrin, Ye.Yanlin, Y.Koike Vector and Tensor Analyzing Powers in Deuteron-Proton Elastic Scattering at E(d) = 70 MeV NUCLEAR REACTIONS 1H(polarized d, d), E=70 MeV; measured σ(θ), vector analyzing power vs θ. Faddeev formalism.
doi: 10.1007/BF01080942
1986BR25 Phys.Rev. C34, 1484 (1986) M.E.Brandan, A.Menchaca-Rocha, M.Buenerd, J.Chauvin, P.DeSaintignon, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, J.Y.Hostachy Elastic and Inelastic 16O + 12C Scattering at 38 MeV/Nucleon NUCLEAR REACTIONS 12C(16O, 16O), (16O, 16O'), E=608 MeV; measured σ(θ); deduced reaction σ. Magnetic spectrometer. Optical model, DWBA analyses.
doi: 10.1103/PhysRevC.34.1484
1986BU03 Phys.Lett. 167B, 379 (1986) M.Buenerd, J.Chauvin, G.Duhamel, J.Y.Hostachy, D.Lebrun, P.Martin, P.O.Pellegrin, G.Perrin, P.De Saintignon Search for High Excitation Energy Structures in the 20Ne + 208Pb System at E/A = 30 MeV NUCLEAR REACTIONS 208Pb(20Ne, 20Ne), (20Ne, 20Ne'), E=600 MeV; measured σ(E(20Ne)), σ(θ). 208Pb deduced giant resonance excitation. DWBA analysis.
doi: 10.1016/0370-2693(86)91284-0
1986VO02 Z.Phys. A323, 373 (1986) W.von Oertzen, M.Buenerd, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, G.Perrin, P.De Saintignon Charge Exchange Reactions (13C, 13N) and (13C, 13B) on 12C NUCLEAR REACTIONS 12C(13C, 13N), (13C, 13B), E=30 MeV/nucleon; measured σ(E(13N)), σ(E(13B)). 12B, 12N deduced GDR excitation.
1982GA17 Nucl.Phys. A381, 40 (1982) S.Gales, E.Gerlic, G.Duhamel, G.Perrin, C.Perrin, V.Comparat Spin of Deep-Hole States in 111Sn via the 112Sn(d(pol), t) Reaction NUCLEAR REACTIONS 112Sn(polarized d, t), E=40 MeV; measured σ(Et), σ(θ), A(θ); deduced valence, inner-hole components. 111Sn deduced levels, L, J, π, C2S. Enriched target, polarized beam, magnetic spectrometer. DWBA analysis.
doi: 10.1016/0375-9474(82)90499-7
1982GE06 Phys.Lett. 117B, 20 (1982) E.Gerlic, J.Guillot, H.Langevin-Joliot, S.Gales, M.Sakai, J.Van de Wiele, G.Duhamel, G.Perrin High Lying Two-Neutron Hole States in 206Pb and 114Sn Observed via the (α, 6He) Reaction at 218 MeV NUCLEAR REACTIONS 208Pb, 116Sn(α, 6He), E=218 MeV; measured σ(E(6He)), σ(θ); deduced reaction mechanism. 114Sn, 206Pb deduced levels, J, π, L, configuration. Zero-range DWBA analysis.
doi: 10.1016/0370-2693(82)90865-6
1981DU13 J.Phys.(London) G7, 1415 (1981) G.Duhamel, G.Perrin, J.P.Didelez, E.Gerlic, H.Langevin-Joliot, J.Guillot, J.Van de Wiele Inner-Hole Excitations in 89Zr and 91Mo via the (3He, α) Reaction at 97 MeV NUCLEAR REACTIONS 90Zr, 92Mo(3He, α), E=97.3 MeV; measured σ(Eα), σ(θ). 89Zr, 91Mo deduced levels, L, J, π, C2S, IAS, valence, inner hole centroid energies. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1088/0305-4616/7/10/019
1981PE02 Nucl.Phys. A356, 61 (1981) G.Perrin, G.Duhamel, C.Perrin, E.Gerlic, S.Gales, V.Comparat Analyzing Powers of Valence and Inner Neutron-Hole States in 115Sn via the 116Sn(d(pol), t) Reaction NUCLEAR REACTIONS 116Sn(polarized d, t), E=40 MeV; measured σ(Et, θ), A(θ). 115Sn deduced valence and inner hole components. 115Sn levels deduced L, J, π, C2S. Enriched target, magnetic spectrometer. DWBA analysis.
doi: 10.1016/0375-9474(81)90118-4
1980GU03 Phys.Rev. C21, 879 (1980) J.Guillot, J.Van de Wiele, H.Langevin-Joliot, E.Gerlic, J.P.Didelez, G.Duhamel, G.Perrin, M.Buenerd, J.Chauvin Neutron Hole States in 207,206,205Pb Isotopes via the (3He, α) Reaction at 100 MeV NUCLEAR REACTIONS 208,207,206Pb(3He, α), E=101.75 MeV; measured σ(Eα, θ). 207,206,205Pb deduced levels, L, J, π, C2S. Enriched targets, magnetic spectrometer.
doi: 10.1103/PhysRevC.21.879
1980LE25 Phys.Lett. B97, 358 (1980) D.Lebrun, M.Buenerd, P.Martin, P.de Saintignon, G.Perrin Is there a Giant Monopole Resonance in Light Nuclei < Question > NUCLEAR REACTIONS 12C, 27Al, 40Ca, 56Fe, 58,60Ni(3He, 3He'), E=108.5 MeV; measured σ(E(3He), θ). 40Ca deduced weak giant monopole resonance. 12C, 27Al, 56Fe, 58,60Ni deduced monopole resonance, Γ, EWSR. DWBA analysis.
doi: 10.1016/0370-2693(80)90619-X
1979BU08 Phys.Lett. 84B, 305 (1979) M.Buenerd, C.Bonhomme, D.Lebrun, P.Martin, J.Chauin, G.Duhamel, G.Perrin, P.de Saintignon Inelastic Scattering of 108.5 MeV 3He Particles at Very Small Momentum Transfer to the Giant Monopole Resonance of 90Zr and 208Pb NUCLEAR REACTIONS 90Zr, 208Pb(3He, 3He'), E=105 MeV; measured σ(θ). 90Zr, 208Pb deduced giant M1 resonance. DWBA analysis.
doi: 10.1016/0370-2693(79)90045-5
1979GA13 Nucl.Phys. A327, 349 (1979) Y.R.Gaillard, P.Martin, G.Perrin, P.Desaintignon, M.Buenerd, J.M.Loiseaux, J.L.Escudie, A.Tarrats, H.V.Geramb Excitation Function of Giant Resonances as Doorway States in the 12C(P, P)12C Reaction between 19 and 23 MeV NUCLEAR REACTIONS 12C(p, p), E=19.15-23.34 MeV; measured σ(E, θ)A(E, θ). 13N deduced giant resonance strength distribution. Optical model, coupled channel, anti-symmetrized distorted-wave approximation.
doi: 10.1016/0375-9474(79)90264-1
1979MA06 Nucl.Phys. A315, 291 (1979) P.Martin, Y.Gaillard, P.de Saintignon, G.Perrin, J.Chauvin, G.Duhamel, J.M.Loiseaux Excitation of Low-Lying Levels and Giant Resonances in 90Zr via 57.5 MeV Polarized Proton Inelastic Scattering NUCLEAR REACTIONS 90Zr(polarized p, p'), E=57.5 MeV; measured σ(E(X), θ), Ay(E(X), θ), E=0-27 MeV. 90Zr deduced excitation of bound states, giant resonances. Collective, microscopic-model distorted-wave analysis. Enriched target.
doi: 10.1016/0375-9474(79)90612-2
1979MO12 Phys.Rev. C20, 1593 (1979) A.Moalem, Y.Gaillard, A.M.Bemolle, M.Buenerd, J.Chauvin, G.Duhamel, D.Lebrun, P.Martin, G.Perrin, P.de Saintignon Isotopic Dependence of the Giant Quadrupole Resonance in the Stable Even-Mass Molybdenum Nuclei NUCLEAR REACTIONS 100,98,96,94,92Mo(3He, 3He'), E=110 MeV; measured σ(E, θ). 100,98,96,94,92Mo deduced E, Γ, strength of GQR.
doi: 10.1103/PhysRevC.20.1593
1978BU10 Phys.Rev.Lett. 40, 1482 (1978) M.Buenerd, D.Lebrun, J.Chauvin, Y.Gaillard, J.M.Loiseaux, P.Martin, G.Perrin, P.de Saintignon Heavy-Ion Inelastic Scattering to Giant Resonances NUCLEAR REACTIONS 90Zr, 208Pb(12C, 12C'), E=120 MeV; 40Ca, 90Zr, 197Au, 208Pb, 209Bi(14N, 14N'), E=161 MeV; measured spectra. 40Ca, 90Zr, 197Au, 208Pb, 209Bi deduced giant resonances.
doi: 10.1103/PhysRevLett.40.1482
1978DU11 Nucl.Phys. A306, 173 (1978) J.L.Durand, J.Chauvin, C.Perrin, G.Perrin, G.Duhamel, J.J.Benayoun, A.Laverne Measurements in a New Phase Space Region of the 2H(p, 2p)n Break-up Reaction NUCLEAR REACTIONS 2H(polarized p, 2p), E=15 MeV; measured σ(Ep1, Ep2).
doi: 10.1016/0375-9474(78)90320-2
1978DU13 Phys.Lett. 78B, 213 (1978) G.Duhamel, G.Perrin, J.Chauvin, M.Buenerd, E.Gerlic, J.Guillot, J.P.Didelez, H.Langevin-Joliot, J.Van de Wiele First Observation of T > = 45/2 Inner Hole States in 207Pb NUCLEAR REACTIONS 208Pb(3He, α), E=102 MeV; measured σ(Eα, θ). 207Pb deduced IAS, Γ, S. DWBA analysis.
doi: 10.1016/0370-2693(78)90008-4
1977PE07 Nucl.Phys. A282, 221 (1977) G.Perrin, Nguyen Van Sen, J.Arvieux, R.Darves-Blanc, J.L.Durand, A.Fiore, J.C.Gondrand, F.Merchez, C.Perrin A Systematic Study of Elastic Scattering of Polarized Deuterons Around 30 MeV by Complex Nuclei NUCLEAR REACTIONS 12C, 28Si, 40Ca, 56Fe, 58Ni, 64Zn, 90Zr, 118,120Sn, 208Pb(polarized d, d), E=30 MeV; measured σ(θ), vector polarization, tensor polarization; deduced optical model parameters. 12C, 28Si, 40Ca natural targets; enriched 56Fe, 58Ni, 64Zn, 90Zr, 118,120Sn, 208Pb targets.
doi: 10.1016/0375-9474(77)90213-5
1977PE09 Phys.Lett. 68B, 55 (1977) G.Perrin, D.Lebrun, J.Chauvin, P.Martin, P.De Saintignon, D.Eppel, H.V.Geramb, H.L.Yadav, V.A.Madsen The Octupole Giant Resonance Strength in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=42.5, 44.0, 49.3 MeV; measured σ(Ep', θ), A(θ). 16O deduced octupole strength.
doi: 10.1016/0370-2693(77)90033-8
1976LE16 Nucl.Phys. A265, 291 (1976) D.Lebrun, G.Perrin, P.Martin, P.de Saintignon, J.Arvieux, M.Buenerd, H.V.Geramb, K.A.Amos Evidence of an Isoscalar E3 Giant Resonance in 16O NUCLEAR REACTIONS 16O(polarized p, p'), E=31.7, 33.8, 35.8, 36.8, 39.9 MeV; measured σ(Ep', θ), A(θ). 16O deduced isoscalar resonance, E3 strengths. Distorted wave analyses include giant resonance effects.
doi: 10.1016/0375-9474(76)90355-9
1975AR16 Nucl.Phys. A247, 238 (1975) J.Arvieux, M.Buenerd, A.J.Cole, P.De Saintignon, G.Perrin, D.J.Horen Giant Resonances in f-p Shell Nuclei Studied by Inelastic Scattering Of 80 MeV 3He Ions NUCLEAR REACTIONS 48Ti, 56Fe, 59Co, 60Ni(3He, 3He'), E=80 MeV; measured σ(E(3He'), θ). 48Ti, 56Fe giant resonances deduced L.
doi: 10.1016/0375-9474(75)90634-X
1975HO05 Phys.Rev. C11, 1247 (1975) D.J.Horen, J.Arvieux, M.Buenerd, J.Cole, G.Perrin, P.de Saintignon Giant Resonance Region Observed in 3He Scattering by 144,154Sm, 159Tb, 165Ho, 169Tm, and 208Pb NUCLEAR REACTIONS 144,154Sm, 165Ho(3He, 3He'), E=80 MeV; measured σ(E, E(3He'), θ). 159Tb, 169Tm, 208Pb(3He, 3He'), E=80 MeV; measured σ(E(3He')). 144,154Sm, 159Tb, 165Ho, 169Tm, 208Pb deduced giant resonance character.
doi: 10.1103/PhysRevC.11.1247
1974AM05 Phys.Lett. 52B, 138 (1974) K.A.Amos, H.V.Geramb, R.Sprickmann, J.Arvieux, M.Buenerd, G.Perrin Resonance Effects in the 12C(p, p')12C*, 1+ Transition NUCLEAR REACTIONS 12C(polarized p, p'), E=22.3, 26.7, 30.5 MeV; measured σ(E, Ep', θ), A(E, θ). 12C deduced resonance coupling strengths.
doi: 10.1016/0370-2693(74)90071-9
1974DU10 Phys.Lett. 53B, 57 (1974) J.L.Durand, J.Arvieux, C.Perrin, G.Perrin Analyzing Power of the 6Li(p, pα)2H Reaction: a New Test for Reaction Mechanisms NUCLEAR REACTIONS 6Li(polarized p, pα), E=40 MeV; measured σ(θ), A(θ).
doi: 10.1016/0370-2693(74)90343-8
1974RO09 Nucl.Phys. A220, 381 (1974) R.Roche, N.Van Sen, G.Perrin, J.C.Gondrand, A.Fiore, H.Muller Evidence for the Deuteron-Nucleus Tensor Interaction NUCLEAR REACTIONS 40Ca, 56Fe(polarized d, d), E=30 MeV; 90Zr, 208Pb(polarized d, d), E=28.8 MeV; measured σ(θ), iT11(θ), T22-square root 3/2 T20; deduced optical-model parameters. Natural 40Ca, enriched 56Fe, 90Zr, 208Pb.
doi: 10.1016/0375-9474(74)90726-X
1973FI11 Phys.Rev. C8, 2019 (1973) A.Fiore, J.Arvieux, Nguyen Van Sen, G.Perrin, F.Merchez, J.C.Gondrand, C.Perrin, J.L.Durand, R.Darves-Blanc Vector and Tensor Analyzing Power Measurements in the Scattering of Polarized Deuterons by Protons and Comparison with Exact Three-Body Calculations NUCLEAR REACTIONS 1H(d, d), E=20.4, 25.1, 29.9 MeV; measured iT11(θ).
doi: 10.1103/PhysRevC.8.2019
1973PE06 Nucl.Phys. A206, 623 (1973) G.Perrin, Nguyen Van Sen, J.Arvieux, C.Perrin, R.Darves-Blanc, J.L.Durand, A.Fiore, J.C.Gondrand, F.Merchez Elastic and Inelastic Scattering of Polarized Deuterons by 120Sn at 28.6 MeV NUCLEAR REACTIONS 120Sn(polarized d, d), E=28.6 MeV; measured σ(θ), iT11(θ), T20(θ), T22(θ)-square root(3/2)T20(θ); 120Sn(polarized d, d'), E=28.6 MeV; measured σ(θ), iT11(θ); deduced optical-model parameters. 120Sn deduced deformations β2, β3. Enriched target.
doi: 10.1016/0375-9474(73)90091-2
1972DA08 Lett.Nuovo Cim. 4, 16 (1972) R.Darves-Blanc, N.Van Sen, J.Arvieux, A.Fiore, J.C.Gondrand, G.Perrin Elastic Scattering of Polarized Protons by 3H between 19 and 57 MeV NUCLEAR REACTIONS 3H(polarized p, p), E=19-57 MeV; measured σ(θ), P(θ). 3H(p, p), 3H(p, n), E=56.7 MeV; measured σ(θ).
doi: 10.1007/BF02756421
1972DA10 Nucl.Phys. A191, 353 (1972) R.Darves-Blanc, N.Van Sen, J.Arvieux, J.C.Gondrand, A.Fiore, G.Perrin Polarisation et Section Efficace de la Diffusion Elastique p + 3H a 19 et 30 MeV NUCLEAR REACTIONS 3H(polarized p, p), E=19, 30 MeV; measured σ(θ), pp(θ); 3He(polarized p, p), E=30 MeV; measured pp(θ); deduced phase shifts. Tritium-loaded target; 3He gas target.
doi: 10.1016/0375-9474(72)90520-9
1972PE09 Nucl.Instrum.Methods 101, 603 (1972) G.Perrin, Nguyen Van Sen, A.Fiore, J.Arvieux Absolute Calibration of a 12C Polarimeter for Deuterons between 20 and 30 MeV NUCLEAR REACTIONS 12C(polarized d, d), E=20.5, 25.2, 29.5 MeV; measured iT11(θ).
doi: 10.1016/0029-554X(72)90053-5
1972PE14 Lett.Nuovo Cim. 4, 381 (1972) G.Perrin, Nguyen Van Sen, J.Arvieux, C.Perrin, A.Fiore, J.L.Durand Octupole Excitation of the 6.88 Level of 28Si by Deuteron Inelastic Scattering at 29.5 MeV NUCLEAR REACTIONS 28Si(d, d'), E=29.5 MeV; measured σ(Ed', θ). 28Si level deduced deformation parameters β(L).
doi: 10.1007/BF02756540
1972PE15 Nucl.Phys. A193, 215 (1972) G.Perrin, Nguyen van Sen, J.Arvieux, A.Fiore, J.L.Durand, R.Darves-Blanc, J.C.Gondrand, F.Merchez, C.Perrin Diffusion Elastique des Deutons Polarises par 12C de 20 a 30 MeV NUCLEAR REACTIONS 12C(polarized d, d), E=20.5, 25.2, 29.5 MeV; measured vector polarization iT11(θ);E=20.5, 29.5 MeV; measured σ(θ); deduced optical model parameters.
doi: 10.1016/0375-9474(72)90247-3
1968CA01 Nucl.Phys. A107, 436 (1968) P.Carlos, J.Matuszek, A.Audias, B.P.Maier, H.Nifenecker, G.Perrin, R.Samama Capture Radiative de Neutrons Thermiques dans 48Ti NUCLEAR REACTIONS 48Ti(n, γ), E = th; measured σ(Eγ), γγ-coin, γγ-coin, γγ(θ). 49Ti levels deduced J, π, delta. Natural target.
doi: 10.1016/0375-9474(68)90631-3
1968IR02 Compt.Rend. 267B, 1358 (1968) J.-L.Irigaray, G.-Y.Petit, R.Samama, P.Carlos, J.Girard, G.Perrin Intensites et Energies des Raies γ dans la Reaction Rb(n, γ)Rb NUCLEAR REACTIONS 85Rb(n, γ), E=0.058 eV; measured Eγ, Iγ; deduced Q. 86Rb deduced levels, J, π. Ge(Li) detector, natural target.
Back to query form |