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Search: Author = G.Perrin

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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, 64}Ni + 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

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0386.

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0680.

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
Citations: PlumX Metrics

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1846.

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
Citations: PlumX Metrics

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
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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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1517.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1824.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1844.

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1835.

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1825.

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 ^{100,98,96,94,92}Mo(³He, ³He'), E=110 MeV; measured σ(E, θ). ^{100,98,96,94,92}Mo deduced E, Γ, strength of GQR.

doi: 10.1103/PhysRevC.20.1593
Citations: PlumX Metrics

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
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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
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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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0234.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1831.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1560.

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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0261.

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
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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
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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
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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
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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
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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
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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.