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NSR database version of April 27, 2024.

Search: Author = M.Conjeaud

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1994LI03      Phys.Rev. C49, 1214 (1994)

V.Lips, R.Barth, G.Klotz-Engmann, H.Oeschler, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, R.Legrain, E.C.Pollacco, C.Volant

Deep Inelastic Collisions in the System ⁴⁰Ar + ²³²Th at 31 MeV/nucleon

NUCLEAR REACTIONS ²³²Th(⁴⁰Ar, X), E=31 MeV/nucleon; measured fragment σ(θ, Z) vs velocity; deduced total kinentic energy loss, projectile fragment σ(θ).

doi: 10.1103/PhysRevC.49.1214
Citations: PlumX Metrics

1993PO12      Z.Phys. A346, 63 (1993)

E.C.Pollacco, C.Volant, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, R.Legrain, J.-E.Sauvestre

Fission Study for the System ⁸⁴Kr + ²³²Th at 25, 35 and 45 MeV/u

NUCLEAR REACTIONS ²³²Th(⁸⁴Kr, F), E=25-45 MeV/nucleon; measured fission (fragment)(fragment)(θ); deduced heavy residue recoil velocities, target plus projectile fusion evidence.

doi: 10.1007/BF01290782
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1989KL01      Nucl.Phys. A499, 392 (1989)

G.Klotz-Engmann, H.Oeschler, J.Stroth, E.Kankeleit, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, R.Legrain, E.C.Pollacco, C.Volant

Properties of Binary Fission and Multifragmentation in the Transition Regime

NUCLEAR REACTIONS ²³²Th(α, F), (¹⁴N, F), E=250, 800 MeV/nucleon; ¹⁹⁷Au, ¹⁶⁵Ho(α, F), E=70, 250, 800 MeV/nucleon; Ag(α, F), E=800 MeV/nucleon; ¹⁹⁷Au(¹⁴N, F), E=250 MeV/nucleon; measured fission σ, (fragment)(fragment)(θ), fragment velocities, fragment energy.

doi: 10.1016/0375-9474(89)90054-7
Citations: PlumX Metrics

1987KL02      Phys.Lett. 187B, 245 (1987)

G.Klotz-Engmann, H.Oeschler, E.Kankeleit, Y.Cassagnou, M.Conjeaud, R.Dayras, S.Harar, M.Mostefai, R.Legrain, E.C.Pollacco, C.Volant

Transition From Fission to Multifragmentation

NUCLEAR REACTIONS Ag, ¹⁶⁵Ho, ¹⁹⁷Au(α, X), E=70-800 MeV/nucleon; measured fragment mass spectra, relative velocities; deduced fission, multi-fragmentation characteristics. Tof telescopes.

doi: 10.1016/0370-2693(87)91089-6
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1987VO07      Phys.Lett. 195B, 22 (1987)

C.Volant, M.Conjeaud, S.Harar, M.Mostefai, E.C.Pollacco, Y.Cassagnou, R.Dayras, R.Legrain, G.Klotz-Engmann, H.Oeschler

Formation and Decay of Hot Nuclei

NUCLEAR REACTIONS ²³²Th(⁵⁸Ni, X), E=20, 25, 30 MeV/nucleon; measured (fragment)(fragment)-coin, σ(E), σ(E, θ₁, θ₂); deduced reaction mechanism. Exciton model calculations.

doi: 10.1016/0370-2693(87)90879-3
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1985CO19      Phys.Lett. 159B, 244 (1985)

M.Conjeaud, S.Harar, M.Mostefai, E.C.Pollacco, C.Volant, Y.Cassagnou, R.Dayras, R.Legrain, H.Oeschler, F.Saint-Laurent

Central Collisions in the Argon Induced Fission of Thorium in the Transition Energy Regime

NUCLEAR REACTIONS ²³²Th(⁴⁰Ar, F), E=31, 35, 44 MeV/nucleon; measured fission fragment σ(θ₁, θ₂), energies, masses, velocities; deduced collision energy dependence, large, small momentum transfer reaction σ(E).

doi: 10.1016/0370-2693(85)90243-6
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1984PO14      Phys.Lett. 146B, 29 (1984)

E.C.Pollacco, M.Conjeaud, S.Harar, C.Volant, Y.Cassagnou, R.Dayras, R.Legrain, M.S.Nguyen, H.Oeschler, F.Saint-Laurent

High Momentum and Energy Transfer Induced by 1760 MeV ⁴⁰Ar on ¹⁹⁷Au and ²³²Th Targets

NUCLEAR REACTIONS ¹⁹⁷Au, ²³²Th(⁴⁰Ar, F), E=1760 MeV; measured fission (fragment)(fragment)(θ), masses, velocities, energies; deduced mass transfer process dominance.

doi: 10.1016/0370-2693(84)90636-1
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1984SA15      Nucl.Phys. A422, 307 (1984)

F.Saint-Laurent, M.Conjeaud, R.Dayras, S.Harar, H.Oeschler, C.Volant

Momentum Transfer in Light-Ion-Induced Fission Reactions

NUCLEAR REACTIONS, ICPND ²³²Th(p, F), E=140-1000 MeV; ²³²Th(d, F), E=70-1000 MeV; ²³²Th(α, F), E=280, 1000 MeV; ¹⁹⁷Au(α, F), E=280 MeV; measured fission σ, σ(fragment θ), (fragment)(fragment)(θ). ^233,234Pu, ²³⁶U deduced spins, linear momentum transfer. Intranuclear cascade model.

doi: 10.1016/0375-9474(84)90519-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0647.

1982SA08      Phys.Lett. 110B, 372 (1982)

F.Saint Laurent, M.Conjeaud, R.Dayras, S.Harar, H.Oeschler, C.Volant

Momentum Transfer with Light Ions at Energies from 70 MeV to 1000 MeV

NUCLEAR REACTIONS, Fission ²³²Th(p, F), E=140, 250, 500, 1000 MeV; ²³²Th(d, F), E=70, 140, 500, 1000 MeV; ²³²Th(α, F), E=69.2, 140, 280, 1000 MeV; measured (fragment)(fragment)(θ); deduced dominating processes, corresponding regions. ^233,234Pa, ²³⁶U deduced forward momentum transfer during fission.

doi: 10.1016/0370-2693(82)91275-8
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0011.

1980WI09      Phys.Lett. 93B, 35 (1980)

J.P.Wieleczko, S.Harar, M.Conjeaud, F.Saint-Laurent

Entrance Channel Versus Compound Nucleus Limitations in the Fusion Process of 1p and 2s-1d Shell Nuclei

NUCLEAR REACTIONS ¹²C(¹⁴N, X), ¹⁰B, ¹²C, ¹⁶O(¹⁷O, X), E(cm)=12-30 MeV; measured fusion σ(E); deduced entrance channel, compound nucleus effects.

doi: 10.1016/0370-2693(80)90089-1
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1979SA26      Nucl.Phys. A327, 517 (1979)

F.Saint-Laurent, M.Conjeaud, S.Harar, J.M.Loiseaux, J.Menet, J.B.Viano

Formation and Deexcitation of the ³²S Compound Nucleus via the ²⁰Ne + ¹²C and ¹⁶O + ¹⁶O Entrance Channels

NUCLEAR REACTIONS ¹²C(²⁰Ne, X), E=67.1, 81, 92.3, 135, 157 MeV; ¹⁶O(¹⁶O, X), E=119, 141 MeV; measured σ for residual elements with Z=5-15; deduced limiting angular momenta for fusion, reaction mechanism.

doi: 10.1016/0375-9474(79)90272-0
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1978CO20      Nucl.Phys. A309, 515 (1978)

M.Conjeaud, S.Gary, S.Harar, J.P.Wieleczko

Complete Fusion of the ¹²C + ¹²C, ¹⁴N + ¹²C and ¹⁵N + ¹²C Systems

NUCLEAR REACTIONS ¹²C(¹²C, X), ¹²C(¹⁴N, X), ¹²C(¹⁵N, X), E=27-60 MeV; measured σ for residual elements for Z=6-13; deduced limiting angular momenta for fusion. Statistical model analysis of evaporation residues cross sections. Entrance, compound nucleus effects discussed.

doi: 10.1016/0375-9474(78)90493-1
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1977LE17      Nucl.Phys. A289, 187 (1977)

A.Lepine, C.Volant, M.Conjeaud, S.Harar, E.F.da Silveira

¹⁶O Induced Reactions on ¹¹⁶Sn at 64 MeV

NUCLEAR REACTIONS ¹¹⁶Sn(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), (¹⁶O, ¹⁵N), (¹⁶O, ¹⁴C), E=64 MeV; measured σ(θ); deduced deformation, optical model parameters. ¹¹⁷Sb, ¹¹⁸Te levels deduced S. DWBA, CCBA analysis.

doi: 10.1016/0375-9474(77)90528-0
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0991.

1977VO08      J.Phys.(Paris) 38, 1179 (1977)

C.Volant, M.Conjeaud, S.Harar, E.F.da Silveira

Compound Nucleus Formation in the ¹⁴N + ¹⁶O System

NUCLEAR REACTIONS ¹⁶O(¹⁴N, X), E=20-60 MeV; measured σ(E).

doi: 10.1051/jphys:0197700380100117900
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1975CO15      Nucl.Phys. A250, 182 (1975)

M.Conjeaud, S.Harar, E.F.Da Silveira, C.Volant

Transfer Reactions Induced by ¹²C on ¹⁸O and ²⁶Mg at 46 MeV

NUCLEAR REACTIONS ¹⁸O(¹²C, ¹⁰Be), ²⁶Mg(¹²C, ¹¹B), (¹²C, ¹⁰Be), (¹²C, ⁹Be), E=46 MeV; measured σ(θ). ²⁶Mg(¹²C, ¹²C) deduced optical model parameters. ²⁰Ne, ²⁷Al, ²⁸Si, ²⁹Si levels deduced S. DWBA analysis with microscopic, cluster form factors. Enriched targets.

doi: 10.1016/0375-9474(75)90208-0
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1975CO25      J.Phys.(Paris), Colloq. 36, C5-111 (1975)

M.Conjeaud, S.Harar, A.Lepine, E.Da Silveira, C.Volant

Etude de Reactions Induites par des Projectiles ¹⁶O sur Une Cible ¹¹⁶Sn a 64 MeV

NUCLEAR REACTIONS ¹¹⁶Sn(¹⁶O, ¹⁶O), (¹⁶O, ¹⁶O'), (¹⁶O, ¹⁵N), (¹⁶O, ¹⁴C), E=64 MeV; measured σ(θ); deduced optical model parameters.

1975VO02      Nucl.Phys. A238, 120 (1975)

C.Volant, M.Conjeaud, S.Harar, S.M.Lee, A.Lepine, E.F.Da Silveira

Evidence for Critical Angular Momenta in the Formation of ²⁶Al via the ¹⁴N + ¹²C Channel

NUCLEAR REACTIONS ¹²C(¹⁴N, ⁶Li), E=20-60 MeV, measured σ(E;θ); ¹²C(¹⁴N, d), E=20-40 MeV, measured σ(E), σ(θ); ²⁰Ne, ²⁴Mg deduced levels.Hauser-Feshbach calculations, suggested critical angular momenta for the ²⁶Al compound nucleus formation.

doi: 10.1016/0375-9474(75)90343-7
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0504.

1973CO33      Nucl.Phys. A215, 383 (1973)

M.Conjeaud, S.Harar, M.Caballero, N.Cindro

The (t, α) Reaction on Even Tellurium Nuclei

NUCLEAR REACTIONS ^{122,124,126,128}Te(t, α), E=12 MeV; measured σ(Eα, θ). ^{121,123,125,127,129}Sb deduced levels, L(p), π, J, S. Enriched targets.

doi: 10.1016/0375-9474(73)90662-3
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1969CO03      Nucl.Phys. A129, 10 (1969)

M.Conjeaud, S.Harar, E.Thuriere

Reaction (d, ³He) sur les Isotopes Doublement Pair de l'Etain

NUCLEAR REACTIONS ^{112,114,116,118,120,122}Sn(d, ³He), Ed=22 MeV; measured σ(E(³He), θ), Q. ^{111,113,115,117,119,121}In deduced levels, J, π, L(p), S. Enriched targets.

doi: 10.1016/0375-9474(69)90905-1
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1968BA56      J.Phys.(Paris), Suppl.No.1, Colloq.C1-162 (1968)

G.Bassani, M.Conjeaud, S.Harar, J.Picard, G.Souchere

La Reaction (tau, d) sur les Noyaux ⁸⁸Sr, ⁹⁰Zr et ⁹²Mo

NUCLEAR REACTIONS ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo(³He, d), E=18 MeV; measured σ(θ). ⁸⁹Y, ⁹¹Nb, ⁹³Tc deduced levels, L(p), S.

1968BA57      J.Phys.(Paris), Suppl.No.1, Colloq.C1-163 (1968)

G.Bassani, M.Conjeaud, S.Harar, J.Picard, G.Souchere

Etats de Trou de Neutron dans les Noyaux N = 50

NUCLEAR REACTIONS ⁸⁸Sr, ⁹⁰Zr, ⁹²Mo(³He, α), E=18 MeV; measured σ(Eα, θ). ⁸⁷Sr, ⁸⁹Zr, ⁹¹Mo deduced levels, L(n), S.

1968BI15      J.Phys.(Paris), Suppl.No.1, Colloq.C1-168 (1968)

L.Bianchi, M.Conjeaud, S.Harar, J.Picard, C.Ellegaard, P.Vedelsby

Reactions ^115,113In(³He, d)^116,114Sn

NUCLEAR REACTIONS ^113,115In(³He, d), E=18 MeV; measured σ(Ed). ^114,116Sn deduced levels.

1968CO22      Nucl.Phys. A117, 449 (1968)

M.Conjeaud, S.Harar, Y.Cassagnou

(³He, d) Reactions on the Even Tin Isotopes

NUCLEAR REACTIONS ^{112,114,116,118,120,122,124}Sn(³He, d), E=18 MeV; measured σ(Ed, θ), Q. ^{113,115,117,119,121,123,125}Sb deduced levels, J, π, L(p), S. Enriched targets.

doi: 10.1016/0375-9474(68)90855-5
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1966BA25      Phys.Letters 22, 189 (1966)

G.Bassani, M.Conjeaud, J.Gastebois, S.Harar, J.M.Laget, J.Picard, Y.Cassagnou

(³He, d) Reactions on the Even Sn Isotopes

NUCLEAR STRUCTURE ¹²¹Sb, ¹²³Sb, ¹²⁵Sb, ¹¹⁷Sb, ¹¹³Sb, ¹¹⁹Sb, ¹¹⁵Sb; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90569-5
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1966CO25      Phys.Letters 23, 104 (1966)

M.Conjeaud, S.Harar, J.Picard

A Possible Process for Core Excitation in Even Single Closed Shell Nuclei

NUCLEAR STRUCTURE ¹¹⁶Sn; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0031-9163(66)90144-2
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1966CO35      CEA-N-621, p.10 (1966)

M.Conjeaud, B.Fernandez, S.Harar, J.Picard, G.Souchere

Reactions (d, p) et (d, t) sur les Isotopes Pairs de l'Etain

NUCLEAR STRUCTURE ¹¹¹Sn, ¹¹³Sn, ¹¹⁵Sn; measured not abstracted; deduced nuclear properties.

1965CO03      Nucl.Phys. 62, 225 (1965)

M.Conjeaud, B.Fernandez, S.Harar, J.Picard, G.Souchere

Diffusion de Neutrons de 14.6 MeV by le Soufre

NUCLEAR REACTIONS ³²S(n, n), (n, n'), E=14.6 MeV; measured σ(En', θ). ³²S deduced levels. Natural target.

doi: 10.1016/0029-5582(65)90865-5
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset21101.

1963SO05      J.Phys. 24, 822 (1963)

G.Souchere, S.Harar, B.Fernandez, J.Picard, M.Conjeaud

Diffusion Inelastique de Neutrons de 14 MeV sur le Soufre 32

NUCLEAR STRUCTURE ³²S; measured not abstracted; deduced nuclear properties.

doi: 10.1051/jphys:019630024011082201
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