NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = S.Harar Found 37 matches. 1998BE14 Phys.Rev. C57, 1788 (1998) E.Berthoumieux, E.C.Pollacco, C.Volant, B.Berthier, Y.Cassagnou, J.L.Charvet, M.Colonna, R.Dayras, R.Legrain, C.Mazur, E.De Filippo, A.Cunsolo, A.Foti, G.Lanzano, A.Pagano, S.Urso, Sl.Cavallaro, R.Barth, V.Lips, H.Oeschler, S.Harar, E.Norbeck Heavy Fragment Production in 40Ar + 232Th Reactions at 27A, 44A, and 77A MeV NUCLEAR REACTIONS 232Th(40Ar, X), E=27, 44, 77 MeV/nucleon; measured light, intermediate, heavy fragments σ(E, θ); deduced fragment production mechanism.
doi: 10.1103/PhysRevC.57.1788
1995PO05 Nucl.Phys. A583, 441c (1995) E.C.Pollacco, E.Berthoumieux, E.De Filippo, C.Volant, R.Barth, B.Berthier, Y.Cassagnou, Sl.Cavallaro, J.L.Charvet, A.Cunsolo, M.Colonna, R.Dayras, D.Durand, A.Foti, S.Harar, G.Lanzano, R.Legrain, V.Lips, C.Mazur, E.Norbeck, H.Oeschler, A.Pagano, S.Urso Production of Heavy Fragments in the Reaction 40Ar + 232Th NUCLEAR REACTIONS 232Th(40Ar, X), (40Ar, F), E=44, 77 MeV/nucleon; measured fission, other fragment velocity vs mass, singles, coincidence modes; deduced heavy fragment production mechanism. Boltzmann-Nordheim-Vlasov approach.
doi: 10.1016/0375-9474(94)00701-N
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
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
1993YE01 Phys.Rev. C48, 1092 (1993) S.J.Yennello, K.Kwiatkowski, E.C.Pollacco, C.Volant, Y.Cassagnou, R.Dayras, D.E.Fields, S.Harar, E.Hourani, R.Legrain, E.Norbeck, R.Planeta, J.L.Wile, N.R.Yoder, V.E.Viola Studies of Intermediate-Mass Fragment Emission in the 3He + (nat)Ag, 197Au Reactions between 0.48 and 3.6 GeV NUCLEAR REACTIONS Ag, 197Au(3He, X), E=0.48-3.6 GeV; measured σ(fragment θ, E) for fragment Z=4-9; deduced energy dissipation, emitting source expansion features. Models comparison.
doi: 10.1103/PhysRevC.48.1092
1990PO10 Nucl.Phys. A519, 197c (1990) E.C.Pollacco, C.Volant, R.Dayras, Y.Cassagnou, S.Harar, R.Legrain, C.Mazur, S.J.Yennello, K.Kwiatkowski, N.R.Yoder, V.E.Viola, R.Planeta, J.L.Wile, D.E.Fields, E.Hourani, E.Norbeck Search for the Onset of Multifragmentation in the Reaction 3He + (nat)Ag NUCLEAR REACTIONS Ag(3He, X), E=0.48-3.6 GeV; measured σ(fragment θ, E).
doi: 10.1016/0375-9474(90)90626-W
1990YE05 Phys.Lett. 246B, 26 (1990) S.J.Yennello, K.Kwiatkowski, D.E.Fields, R.Planeta, V.E.Viola, Jr., E.C.Pollacco, C.Volant, R.Dayras, R.Legrain, Y.Cassagnou, S.Harar, E.Hourani Complex Fragment Emission from the 3He + (nat)Ag System between 0.48 and 3.6 GeV NUCLEAR REACTIONS Ag(3He, X), E=0.48-3.6 GeV; measured σ(fragment θ, E); deduced reaction mechanisms energy dependence.
doi: 10.1016/0370-2693(90)91302-R
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
1987HA28 Nucl.Phys. A471, 205c (1987) Entrance Channel Influence on the Formation and Decay of Hot Nuclei NUCLEAR REACTIONS, MECPD 232Th(58Ni, X), E=20, 25, 30 MeV/nucleon; 232Th(40Ar, X), E=31, 35, 39, 44 MeV/nucleon; 232Th, 165Ho(14N, X), E=60 MeV/nucleon; 165Ho(40Ar, X), E=31, 44 MeV/nucleon; measured fusion fragment σ(θ1, θ2); deduced entrance channel role, hot nuclei formation, decay mechanisms.
doi: 10.1016/0375-9474(87)90252-1
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
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
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
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
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
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
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
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
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
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
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
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
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
1973CO33 Nucl.Phys. A215, 383 (1973) M.Conjeaud, S.Harar, M.Caballero, N.Cindro The (t, α) Reaction on Even Tellurium Nuclei NUCLEAR REACTIONS 122,124,126,128Te(t, α), E=12 MeV; measured σ(Eα, θ). 121,123,125,127,129Sb deduced levels, L(p), π, J, S. Enriched targets.
doi: 10.1016/0375-9474(73)90662-3
1972CA41 An.Fis. 68, 155 (1972) C.Caballero, J.Casanova, S.Harar Estudio de la Estructura de los Isotopos del Sb Mediante las Reacciones A52(t, α)A-151Sb y A-Te(t, t)A-Te NUCLEAR REACTIONS 122,124,126,128,130Te(t, α);E=11.8 MeV; measured σ(Eα, θ); 126Te(t, t);E=11.8 MeV; measured σ(θ). 121,123,125,127,129Sb deduced levels.
1972HA09 Nucl.Phys. A183, 161 (1972) Study of the Level Scheme of 117In via Proton Transfer Reactions NUCLEAR REACTIONS 116Cd(3He, d), E=27 MeV; 116Cd(α, t), E=25.5 MeV; measured σ(Ed, θ), σ(Et). 117In deduced levels, J, π, L(p), S. Enriched 116Cd target.
doi: 10.1016/0375-9474(72)90936-0
1972PA16 Phys.Rev. C5, 1995 (1972) A.D.Panagiotou, H.E.Gove, S.Harar High-Spin States in 20Ne and their Possible Classification into Rotational Bands NUCLEAR REACTIONS 12C(12C, α);E=50, 51 MeV; measured αα(θ). 20Ne levels deduced J, π, γ-branching.
doi: 10.1103/PhysRevC.5.1995
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 112,114,116,118,120,122Sn(d, 3He), Ed=22 MeV; measured σ(E(3He), θ), Q. 111,113,115,117,119,121In deduced levels, J, π, L(p), S. Enriched targets.
doi: 10.1016/0375-9474(69)90905-1
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 112,114,116,118,120,122,124Sn(3He, d), E=18 MeV; measured σ(Ed, θ), Q. 113,115,117,119,121,123,125Sb deduced levels, J, π, L(p), S. Enriched targets.
doi: 10.1016/0375-9474(68)90855-5
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
1966CO25 Phys.Letters 23, 104 (1966) 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
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
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
Back to query form |