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Search: Author = D.Lebrun

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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
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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
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1994JU03      Z.Phys. A347, 181 (1994)

J.Julien, M.Bolore, J.Gosset, J.M.Hisleur, A.Mougeot, G.S.Pappalardo, B.Saghai, G.Sanouillet, D.Ardouin, H.Dabrowski, B.Erazmus, C.Lebrun, V.Bellini, L.Sperduto, C.Cerruti, S.Leray, D.Lebrun, P.De Saintignon, T.Johansson, K.Kilian, L.Bimbot

Search for an Enhanced Production of Low Energy Pions in C(p, π+)X, Cu(p, π+)X, and Cu(p, π0)X Reactions for 300 MeV ≤ T(p) ≤ 400 MeV

NUCLEAR REACTIONS C, Cu(p, π+X), Cu(p, π0X), E=300-400 MeV; measured pion yield low to high energy ratio; deduced structure evidence.

doi: 10.1007/BF01292374
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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
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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
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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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1990BR25      Nucl.Phys. A519, 631 (1990)

M.Braeunig, W.von Oertzen, H.G.Bohlen, A.Miczaika, E.Stiliaris, M.Buenerd, C.Berat, J.Chauvin, D.Lebrun, J.Y.Hostachy, Ph.Martin, W.Mittig, J.Barrette, B.Berthier, B.Fernandez

Proton Stripping Induced by 13C at 50 MeV/Nucleon on 12C, 40Ca and 58Ni

NUCLEAR REACTIONS 12C, 40Ca, 58Ni(13C, 12B), E=50 MeV/nucleon; measured σ(θ). 13N, 41Sc, 59Cu levels deduced configurations, spectroscopic factors.

doi: 10.1016/0375-9474(90)90450-Z
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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.


1989BE50      Phys.Lett. 218, 299 (1989)

C.Berat, M.Buenerd, J.Chauvin, J.Y.Hostachy, D.Lebrun, P.Martin, J.Barrette, B.Berthier, B.Fernandez, A.Miczaika, W.Mittig, E.Stiliaris, W.von Oertzen, H.Lenske, H.H.Wolter

Heavy Ion Charge Exchange Reactions to Probe the Giant Electric Isovector Modes in Nuclei

NUCLEAR REACTIONS 12C, 40Ca, 58Ni(13C, 13N), E=50 MeV/nucleon; measured angle integrated spectra, σ(θ). 12B, 40K, 58Co deduced GDR analog.

doi: 10.1016/0370-2693(89)91585-2
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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-+ Measurement

NUCLEAR REACTIONS 232Th, 197Au, Ag, 58Ni, 27Al, 12C, 7Li(16O, X)π+-, E=93 MeV/nucleon; measured σ(θπ) vs pion momentum, (π-+) yield ratio; deduced pion production mechanism.

doi: 10.1016/0370-2693(89)90229-3
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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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1988HO18      Nucl.Phys. A490, 441 (1988)

J.Y.Hostachy, M.Buenerd, J.Chauvin, D.Lebrun, Ph.Martin, J.C.Lugol, L.Papineau, P.Roussel, N.Alamanos, J.Arvieux, C.Cerruti

Elastic and Inelastic Scattering of 12C Ions at Intermediate Energies

NUCLEAR REACTIONS 12C, 208Pb(12C, 12C), (12C, 12C'), E=1449, 2400 MeV; measured elastic, inelastic σ(θ); deduced optical-model parameters, transparency functions, reaction σ, sensitive region and energy dependence of the nuclear potentials. Near-side/far-side decomposition of the angular distributions. Glauber theory, including Fermi motion, Pauli blocking, finite size effects.

doi: 10.1016/0375-9474(88)90514-3
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1988JU02      Z.Phys. A330, 83 (1988)

J.Julien, M.Bolore, H.Dabrowski, J.M.Hisleur, V.Bellini, A.S.Figuera, R.Fonte, A.Insolia, G.F.Palama, G.V.Russo, M.L.Sperduto, J.Chauvin, P.De Saintignon, D.Lebrun, D.Rebreyend

Neutral Pion Production in Subthreshold Heavy Ion Collision with 16O(38 MeV/u) and 20Ne(200 MeV/u) Beams

NUCLEAR REACTIONS 27Al, 197Au(16O, π0X), E=38 MeV/nucleon; 27Al(20Ne, π0X), E=200 MeV/nucleon; measured σ(θ(π)), integrated σ vs E(π).


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
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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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1987HO03      Phys.Lett. 184B, 139 (1987)

J.Y.Hostachy, M.Buenerd, J.Chauvin, D.Lebrun, Ph.Martin, B.Bonin, G.Bruce, J.C.Lugol, L.Papineau, P.Roussel, J.Arvieux, C.Cerruti

Elastic Scattering of 12C on 12C at E/A = 120 MeV/u and 200 MeV/u

NUCLEAR REACTIONS 12C(12C, 12C), E=120, 200 MeV/nucleon; measured σ(θ); deduced surface transparency onset. Magnetic spectrometer. Optical model analyses.

doi: 10.1016/0370-2693(87)90557-0
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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
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1986MC04      Phys.Rev.Lett. 56, 2156 (1986)

P.L.McGaughey, K.D.Bol, M.R.Clover, R.M.DeVries, N.J.DiGiacomo, J.S.Kapustinsky, W.E.Sondheim, G.R.Smith, J.W.Sunier, Y.Yariv, M.Buenerd, J.Chauvin, D.Lebrun, P.Martin, J.C.Dousse

Dynamics of Low-Energy Antiproton Annihilation in Nuclei as Inferred from Inclusive Proton and Pion Measurements

NUCLEAR REACTIONS 12C, 89Y, 238U(p-bar, π+X), (p-bar, pX), E at 608 MeV/c; measured annihilation production σ for π+, p. Intranuclear cascade models.

doi: 10.1103/PhysRevLett.56.2156
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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.


1985CH03      J.Phys.(London) G11, 261 (1985)

J.Chauvin, D.Lebrun, F.Durand, M.Buenerd

Inelastic 12C(12C, 12C)12C Scattering via the Glauber Optical Potential at E/A=30 MeV and 85 MeV

NUCLEAR REACTIONS 12C(12C, 12C), E=30, 85 MeV/nucleon; calculated σ(θ). Glauber theory, optical limit.

doi: 10.1088/0305-4616/11/2/012
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1985DI01      Phys.Rev. C31, 292 (1985)

N.J.DiGiacomo, M.R.Clover, R.M.DeVries, J.C.Dousse, J.S.Kapustinsky, P.L.McGaughey, W.E.Sondheim, J.W.Sunier, M.Buenerd, D.Lebrun

Inclusive Pion Production in 330, 400 and 500 MeV Proton-Nucleus Collisions

NUCLEAR REACTIONS 12C, 238U(p, π+X), (p, π-X), E=330, 400, 500 MeV; measured σ(θ) vs pion momentum, σ; deduced π+ to π- production ratio.

doi: 10.1103/PhysRevC.31.292
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1984BE35      Nucl.Phys. A423, 511 (1984)

V.Bernard, J.Girard, J.Julien, R.Legrain, J.Poitou, A.Oskarsson, L.Carlen, H.-A.Gustafsson, B.Jakobsson, P.Kristiansson, B.Noren, I.Otterlund, H.Ryde, T.Johansson, G.Tibell, R.Bertholet, C.Guet, M.Maurel, H.Nifenecker, P.Perrin, F.Schussler, M.Buenerd, D.Lebrun, P.Martin, G.Lovhoiden, J.P.Bondorf, O.-B.Nielsen, A.Palmeri

Production of Charged Pions in Intermediate-Energy Heavy-Ion Collisions

NUCLEAR REACTIONS 7Li, 12C, 208Pb(12C, π+), E=60, 75, 85 MeV/nucleon; measured production σ(θ), σ(θ, E(π)); deduced (π-+) ratio.

doi: 10.1016/0375-9474(84)90038-1
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1984BL09      J.Phys.(Paris), Colloq.C4, 201 (1984); See 1984Bl23

Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, W.Von Oertzen, M.Buenerd, A.Gamp, D.Lebrun, Ph.Martin

High Excitation Energy Structures in Heavy Ion Collisions on a 208Pb Target


1984BL23      J.Phys.(Paris), Colloq.C-4, 201 (1984)

Y.Blumenfeld, Ph.Chomaz, N.Frascaria, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, W.von Oertzen, M.Buenerd, A.Gamp, D.Lebrun, Ph.Martin

High Excitation Energy Structures in Heavy Ion Collisions on a 208Pb Target

NUCLEAR REACTIONS 208Pb(36Ar, X), E=11 MeV/nucleon; 208Pb(20Ne, X), E=30 MeV/nucleon; measured fragment σ(θ), σ(EX, θX). Tof spectrometer.


1984BU22      Nucl.Phys. A424, 313 (1984)

M.Buenerd, A.Lounis, J.Chauvin, D.Lebrun, P.Martin, G.Duhamel, J.C.Gondrand, P.De Saintignon

Elastic and Inelastic Scattering of Carbon Ions at Intermediate Energies

NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=360, 1016 MeV; 208Pb(13C, 13C), (13C, 13C'), E=390 MeV; measured σ(θ); deduced optical model parameters, transparency functions, reaction σ, inelastic σ(E).

doi: 10.1016/0375-9474(84)90186-6
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1519.


1984CH18      Z.Phys. A318, 41 (1984)

Ph.Chomaz, N.Frascaria, Y.Blumenfeld, J.P.Garron, J.C.Jacmart, J.C.Roynette, W.Bohne, A.Gamp, W.Von Oertzen, M.Buenerd, D.Lebrun, Ph.Martin

High Excitation Energy Structures in 208Pb

NUCLEAR REACTIONS 208Pb(36Ar, 36Ar'), E=11 MeV/nucleon; 208Pb(20Ne, 20Ne'), E=30 MeV/nucleon; measured σ(θ), σ(θ, E(36Ar')), σ(θ, E(20Ne')); deduced reaction mechanism. 208Pb deduced high excitation structures, excitation process, Γ. DWBA analysis.

doi: 10.1007/BF02117213
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1984JU02      Phys.Lett. 142B, 340 (1984)

J.Julien, M.Bolore, X.Charlot, J.M.Hisleur, J.Martino, G.S.Pappalardo, L.Roussel, B.Saghai, G.Sanouillet, L.Bimbot, D.Lebrun, F.F.Guber, A.B.Kurepin, A.I.Reshetin

Evidence for a Resonant Structure in Inclusive Cu(p, π+)X Reactions between 300 and 400 MeV

NUCLEAR REACTIONS Cu(p, π+X), E=300-400 MeV; measured σ(E(π), θ(π)); deduced resonant structure.

doi: 10.1016/0370-2693(84)91336-4
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1983CH38      Phys.Rev. C28, 1970 (1983)

J.Chauvin, D.Lebrun, A.Lounis, M.Buenerd

Low and Intermediate Energy Nucleus-Nucleus Elastic Scattering and the Optical Limit of Glauber Theory

NUCLEAR REACTIONS 12C(12C, 12C), E=20, 30, 85 MeV/nucleon; calculated σ(θ), reaction σ. 208Pb(13C, 13C), E=30 MeV/nucleon; calculated σ(θ). Glauber theory, optical limit.

doi: 10.1103/PhysRevC.28.1970
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1983ME22      Phys.Lett. 131B, 31 (1983)

A.Menchaca-Rocha, M.E.Brandan, M.Buenerd, J.Chauvin, D.Lebrun, P.Martin, P.de Saintignon, J.C.Gondrand, I.Dorion, A.Lounis

Measurement of Reactions Induced by 30 MeV/A 12C

NUCLEAR REACTIONS 12C, 58Ni(12C, α), (12C, 9Be), (12C, X), 197Au(12C, X), E=30 MeV/nucleon; measured σ(θ, Eα), σ(θ, E(9Be)), σ(fragment θ) for X=10C, 10B, 7Be, 6,7Li. Coalescence model analysis.

doi: 10.1016/0370-2693(83)91085-7
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1981BU08      Phys.Lett. 102B, 242 (1981)

M.Buenerd, J.Pinston, J.Cole, C.Guet, D.Lebrun, J.M.Loiseaux, P.Martin, E.Monnand, J.Mougey, H.Nifenecker, R.Ost, P.Perrin, Ch.Ristori, P.de Saintignon, F.Schussler, L.Carlen, H.A.Gustafsson, B.Jakobsson, T.Johansson, G.Jonsson, J.Krumlinde, I.Otterlund, H.Ryde, B.Schroder, G.Tibell, J.B.Bondorf, O.B.Nielsen

Elastic and Inelastic Scattering of 1.03 GeV 12C Projectiles

NUCLEAR REACTIONS 12C, Ca, 89Y, 208Pb(12C, 12C), (12C, 12C'), E=86 MeV/nucleon; measured σ(θ); deduced optical model parameters. 40Ca deduced evidence for GQR. Natural Ca target. Optical model, DWBA analyses.

doi: 10.1016/0370-2693(81)90867-4
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1319.


1981BU11      Phys.Rev. C24, 1356 (1981)

M.Buenerd, D.Lebrun

Coulomb Excitation of the Giant Dipole Resonance with Helium Projectiles

NUCLEAR REACTIONS 208Pb(α, α'), E=96, 172.5, 480 MeV; calculated σ(θ), Coulomb excitation of giant multipole resonances. DWBA, nuclear, Coulomb form factors.

doi: 10.1103/PhysRevC.24.1356
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1981LE03      Phys.Rev. C23, 552 (1981)

D.Lebrun, M.Buenerd, M.Bini, B.G.Harvey, R.Legrain, J.Mahoney, T.J.M.Symons, K.Van Bibber

Inelastic Scattering of 9Be of 27 MeV/A to Giant Resonances

NUCLEAR REACTIONS 208Pb(9Be, 9Be'), E=245 MeV; measured σ(θ). 208Pb deduced excitation of GQR. DWBA analysis.

doi: 10.1103/PhysRevC.23.552
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1981MO20      Phys.Lett. 105B, 25 (1981)

J.Mougey, R.Ost, M.Buenerd, A.J.Cole, C.Guet, D.Lebrun, J.M.Loiseaux, P.Martin, M.Maurel, E.Monnand, H.Nifenecker, P.Perrin, J.Pinston, C.Ristori, P.de Saintignon, F.Schussler, L.Carlen, B.Jakobsson, A.Oskarsson, I.Otterlund, B.Schroder, H.A.Gustafsson, T.Johansson, H.Ryde, J.P.Bondorf, O.B.Nielsen, G.Tibell

Projectile Fragments from 86 MeV/Nucleon 12C Induced Reactions

NUCLEAR REACTIONS 12C, Ag, Au(12C, X), E=86 MeV/nucleon; measured σ(fragment E, θ); deduced production σ for 6,7,8,9Li, 7,9,10Be, 8,10,11B, 9,10,11C, 12B. Fragmentation model.

doi: 10.1016/0370-2693(81)90032-0
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1980BU16      Phys.Rev.Lett. 45, 1667 (1980)

M.Buenerd, D.Lebrun, Ph.Martin, P.de Saintignon, C.Perrin

Evidence for Deformation Effect on the Giant Monopole Resonance

NUCLEAR REACTIONS 140Ce, 144,150,152Sm, 159Tb, 165Ho, 169Tm, 181Ta, 197Au, 208Pb, 232Th(3He, 3He'), E=108.5 MeV; measured σ(E(3He), θ). 140Ce, 144,150,152Sm, 159Tb, 165Ho, 169Tm, 181Ta, 197Au, 208Pb, 232Th deduced giant monopole resonance, Γ, EWSR strengths, coupling to giant quadrupole vibrations.

doi: 10.1103/PhysRevLett.45.1667
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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
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1979AR01      Phys.Rev.Lett. 42, 753 (1979)

J.Arvieux, J.P.Albanese, M.Buenerd, D.Lebrun, E.Boschitz, C.H.Q.Ingram, J.Jansen

Giant-Resonance Studies via Inelastic Pion Scattering

NUCLEAR REACTIONS Ca(π+, π+'), E=163, 261 MeV; measured σ(Eπ+), σ(θ). 40Ca deduced giant quadrupole resonance energy, Γ.

doi: 10.1103/PhysRevLett.42.753
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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.


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
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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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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
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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
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