NSR Query Results
Output year order : Descending NSR database version of May 10, 2024. Search: Author = R.Freeman Found 89 matches. 2006SZ06 Nucl.Phys. A779, 21 (2006) S.Szilner, F.Haas, Z.Basrak, R.M.Freeman, A.Morsad, M.P.Nicoli Competition between direct and dissipative processes in the binary channels of the 16O + 12C and 18O + 12C reactions NUCLEAR REACTIONS 12C(16O, 16O'), (16O, 15O), (16O, 14N), E=62-124 MeV; 12C(18O, 18O'), (18O, 17O), (18O, 16O), (18O, 15N), (18O, 19F), (18O, 20Ne), E=66-120 MeV; measured particle spectra, σ(E, θ), σ; deduced reaction mechanism features.
doi: 10.1016/j.nuclphysa.2006.09.007
2005AU04 Int.J.Mod.Phys. E14, 239 (2005) L.Auditore, R.Barna, D.De Pasquale, A.Italiano, A.Trifiro, M.Trimarchi, V.Rauch, C.Beck, T.Bellot, C.Bhattacharya, D.Disdier, R.M.Freeman, F.Haas, R.Nouicer, P.Papka, M.Rousseau, A.Sanchez i Zafra, O.Stezowski, A.Strazzeri A semi-classical analysis of the proton sequential emission in 16O + 58Ni deep inelastic collisions NUCLEAR REACTIONS 58Ni(16O, pX), E=132 MeV; measured Ep, multiplicity, (fragment)p-coin; deduced non-equilibrium proton emission, related reaction mechanism features.
doi: 10.1142/S021830130500293X
2004MA26 Phys.Rev. C 69, 034616 (2004) D.Mahboub, C.Beck, B.Djerroud, R.M.Freeman, F.Haas, R.Nouicer, M.Rousseau, P.Papka, A.Sanchez i Zafra, Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.Sperduto, E.Berthoumieux, R.Dayras, R.Legrain, E.Pollacco, A.Hachem Light particle emission in 35Cl + 24Mg fusion reactions at high excitation energy and angular momentum NUCLEAR REACTIONS 24Mg(35Cl, xnypzα), E=260 MeV; measured En, Ep, Eα, in-plane and out-of-plane angular correlations, (residue)(particle)-coin. 59Cu deduced deformation and angular momentum effects in compound nucleus decay.
doi: 10.1103/PhysRevC.69.034616
2002BA97 Phys.Rev. C 66, 054607 (2002) R.Barna, D.De Pasquale, A.Italiano, A.Trifiro, M.Trimarchi, V.Rauch, C.Beck, T.Bellot, C.Bhattacharya, D.Disdier, R.M.Freeman, F.Haas, R.Nouicer, P.Papka, M.Rousseau, O.Stezowski, A.Strazzeri Comparison between α and proton sequential emission in 16O(132 MeV)+58Ni deep inelastic collisions NUCLEAR REACTIONS 58Ni(16O, X), E=132 MeV; measured Eα, Ep, projectile-like fragments spectra, angular correlations; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.66.054607
2002BH01 Phys.Rev. C65, 014611 (2002) C.Bhattacharya, M.Rousseau, C.Beck, V.Rauch, R.M.Freeman, D.Mahboub, R.Nouicer, P.Papka, O.Stezowski, A.Hachem, E.Martin, A.K.Dummer, S.J.Sanders, A.Szanto De Toledo Deformation Effects in 56Ni Nuclei Produced in 28Si + 28Si at 112 MeV NUCLEAR REACTIONS 28Si(28Si, X), E=112 MeV; measured Eα, Ep, light charged particles σ(θ), angular correlations; deduced deformation effects. 30Si(30Si, X), E=120 MeV; analyzed Eα, related data. Statistical model analysis.
doi: 10.1103/PhysRevC.65.014611
2002RO35 Phys.Rev. C66, 034612 (2002) M.Rousseau, C.Beck, C.Bhattacharya, V.Rauch, O.Dorvaux, K.Eddahbi, C.Enaux, R.M.Freeman, F.Haas, D.Mahboub, R.Nouicer, P.Papka, O.Stezowski, S.Szilner, A.Hachem, E.Martin, S.J.Sanders, A.K.Dummer, A.Szanto de Toledo Highly Deformed 40Ca Configurations in 28Si + 12C NUCLEAR REACTIONS 12C(28Si, X), E=112, 180 MeV; measured Ep, Eα, σ(θ), energy and angular correlations between light and heavy fragments. 40Ca deduced highly deformed configurations. Statistical model analysis.
doi: 10.1103/PhysRevC.66.034612
2001BA93 Phys.Rev. C64, 054601 (2001) R.Barna, D.De Pasquale, A.Italiano, A.Trifiro, M.Trimarchi, A.Strazzeri, V.Rauch, D.Disdier, C.Bhattacharya, C.Beck, T.Bellot, R.M.Freeman, R.Nouicer, M.Rousseau, O.Stezowski Semiclassical Approach to Sequential α Emission in (96 MeV) 16O + 58Ni and (133 MeV) 16O + 48Ti Deep Inelastic Collisions NUCLEAR REACTIONS 58Ni(16O, αX), E=96 MeV; 48Ti(16O, αX), E=133 MeV; measured fragments charge distributions, (fragment)α-coin, angular correlation; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.64.054601
2001BE01 Phys.Rev. C63, 014607 (2001) C.Beck, R.Nouicer, D.Disdier, G.Duchene, G.de France, R.M.Freeman, F.Haas, A.Hachem, D.Mahboub, V.Rauch, M.Rousseau, S.J.Sanders, A.Szanto de Toledo Molecular Resonance and Highly Deformed Fission Fragments in 28Si + 28Si NUCLEAR REACTIONS 28Si(28Si, X), E=111.6 MeV; measured Eγ, Iγ, excitation energy spectra, angular distributions, (fragment)(fragment)-, (fragment)γ-coin. 56Ni deduced quasimolecular resonance features. 28Si, 24Mg, 32S deduced transition intensities. Eurogam II array.
doi: 10.1103/PhysRevC.63.014607
2001BH07 Pramana 57, 203 (2001) C.Bhattacharya, M.Rousseau, C.Beck, V.Rauch, R.M.Freeman, R.Nouicer, F.Haas, O.Dorvaux, K.Eddahbi, P.Papka, O.Stezowski, S.Szilner, D.Mahboub, A.Szanto de Toledo, A.Hachem, E.Martin, S.J.Sanders Deformation Effects in the 28Si + 12C and 28Si + 28Si Reactions NUCLEAR REACTIONS 12C, 28Si(28Si, X), E=112, 180 MeV; measured Eα, light charged particle and heavy fragment spectra; deduced di-nuclear system features, deformation effects. Statistical model calculations. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD6120. 2001SZ05 Phys.Rev. C64, 064614 (2001) S.Szilner, M.P.Nicoli, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, M.E.Brandan, G.R.Satchler Refractive Elastic Scattering of Carbon and Oxygen Nuclei: The mean field analysis and Airy structures NUCLEAR REACTIONS 12C(16O, 16O), E=62-124 MeV; 12C(18O, 18O), E=66-120 MeV; measured σ(θ); deduced potential features. Optical model analysis, Airy structures.
doi: 10.1103/PhysRevC.64.064614
2000NI03 Phys.Rev. C61, 034609 (2000) M.P.Nicoli, F.Haas, R.M.Freeman, S.Szilner, Z.Basrak, A.Morsad, G.R.Satchler, M.E.Brandan Detailed Study and Mean Field Interpretation of 16O + 12C Elastic Scattering at Seven Medium Energies NUCLEAR REACTIONS 12C(16O, 16O), E=62-124 MeV; measured σ(θ); deduced parameters. Optical model analysis, Woods-Saxon and folding-model potentials. Comparison with potentials at higher energies and for similar systems.
doi: 10.1103/PhysRevC.61.034609
1999BH08 Nucl.Phys. (Supplement) A654, 841c (1999) C.Bhattacharya, M.Rousseau, C.Beck, V.Rauch, R.Nouicer, R.M.Freeman, O.Stezowski, D.Mahboub, S.Belhabib, A.Hachem, E.Martin, A.Dummer, S.J.Sanders, A.Szanto de Toledo Role of Deformation in the Decay of 56Ni and 40Ca Di-Nuclei NUCLEAR REACTIONS 12C, 28Si(28Si, αX), E=112.6 MeV; measured Eα, Iα(θ); deduced deformation effects. Statistical model analysis, spin-dependent level density.
doi: 10.1016/S0375-9474(00)88558-9
1999FR07 Eur.Phys.J. A 4, 239 (1999) R.M.Freeman, F.Haas, M.-P.Nicoli, A.Morsad, Z.Basrak Recurring Angular Distribution Patterns in Resonant Heavy-Ion Reactions NUCLEAR REACTIONS 12C(12C, 8Be), E(cm)=32.5 MeV; 16O(14C, 15N), E(cm)=23.4, 27.4 MeV; 12C(18O, 16O), E(cm)=22.4, 23.4, 24.3 MeV; analyzed σ(θ); deduced resonance-like structures partial wave interference effects.
doi: 10.1007/s100500050226
1999LI25 Chem.Phys.Lett. 307, 198 (1999) N.Linden, H.Barjat, E.Kupce, R.Freeman How to Exchange Information between Two Coupled Nuclear Spins: The universal SWAP operation
doi: 10.1016/S0009-2614(99)00516-3
1999NI08 Phys.Rev. C60, 064608 (1999) M.P.Nicoli, F.Haas, R.M.Freeman, N.Aissaoui, C.Beck, A.Elanique, R.Nouicer, A.Morsad, S.Szilner, Z.Basrak, M.E.Brandan, G.R.Satchler Elastic Scattering of 16O + 16O at Energies E/A between 5 and 8 MeV NUCLEAR REACTIONS 16O(16O, 16O), E=75-124 MeV; measured σ(θ); deduced phenomenological and microscopic potentials. Optical model, interpretation in terms of Airy minima and the dispersion relation.
doi: 10.1103/PhysRevC.60.064608
1999NI14 Nucl.Phys. (Supplement) A654, 882c (1999) M.P.Nicoli, F.Haas, R.M.Freeman, N.Aissaoui, C.Beck, A.Elanique, R.Nouicer, A.Morsad, S.Szilner, Z.Basrak, M.E.Brandan Refractive Effects in the Elastic Scattering of Light Heavy Ions between 5 and 10 MeV/n: The 16O + 16O reaction NUCLEAR REACTIONS 16O(16O, 16O), E=75-124 MeV; measured σ(θ); deduced refractive effects. Optical model analysis.
doi: 10.1016/S0375-9474(00)88565-6
1999NO06 Phys.Rev. C60, 041303 (1999) R.Nouicer, C.Beck, R.M.Freeman, F.Haas, N.Aissaoui, T.Bellot, G.de France, D.Disdier, G.Duchene, A.Elanique, A.Hachem, F.Hoellinger, D.Mahboub, V.Rauch, S.J.Sanders, A.Dummer, F.W.Prosser, A.Szanto de Toledo, Sl.Cavallaro, E.Uegaki, Y.Abe Vanishing Spin Alignment: Experimental indication of a triaxial 28Si + 28Si Nuclear Molecule NUCLEAR REACTIONS 28Si(28Si, 28Si), (28Si, 28Si'), E=111.6 MeV; measured (fragment)γ-, (fragment)(fragment)-coin, σ(E, θ); deduced fragment spin correlations, molecular configuration.
doi: 10.1103/PhysRevC.60.041303
1999SZ01 J.Phys.(London) G25, 1927 (1999) S.Szilner, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, M.P.Nicoli, C.Beck Excitation Functions of Inelastic and Transfer Channels in 12C + 12C between Ec.m. = 30 and 60 MeV NUCLEAR REACTIONS 12C(12C, 12C'), (12C, 10B), (12C, 11B), E(cm)=30-60 MeV; measured σ(E); deduced intermediate structure resonances.
doi: 10.1088/0954-3899/25/9/311
1998BE43 Eur.Phys.J. A 2, 281 (1998) C.Beck, R.Nouicer, D.Mahboub, B.Djerroud, R.M.Freeman, A.Hachem, T.Matsuse, Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto, R.Dayras, E.Berthoumieux, R.Legrain, E.Pollacco Study of the Fusion-Fission Process in the 35Cl + 24Mg Reaction NUCLEAR REACTIONS 24Mg(35Cl, X), E=8 MeV/nucleon; measured (fragment)(fragment)-coin, fragments energy, angular distributions, charge deficits; deduced no ternary processes. Statistical model calculations.
doi: 10.1007/s100500050121
1998CA02 Phys.Rev. C57, 731 (1998) Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto, R.Dayras, R.Legrain, E.Pollacco, C.Beck, B.Djerroud, R.M.Freeman, F.Haas, A.Hachem, B.Heusch, D.Mahboub, A.Morsad, R.Nouicer, S.J.Sanders Fusion and Binary-Decay Mechanisms in the 35Cl + 24Mg System at E/A ≈ 8 MeV NUCLEAR REACTIONS 24Mg(35Cl, X), E=282 MeV; measured fragments σ(E, Z, θ), fusion, binary mechanism σ; deduced partially-damped binary product decay times, reaction mechanism.
doi: 10.1103/PhysRevC.57.731
1997AI01 Phys.Rev. C55, 516 (1997) N.Aissaoui, F.Haas, R.M.Freeman, C.Beck, A.Morsad, B.Djerroud, R.Caplar, A.Hachem Binary Channels of the 19F-on-12C Reaction at 92 MeV NUCLEAR REACTIONS 12C(19F, X), E=92 MeV; measured σ(fragment, θ); deduced damped binary processes evidence. Statistical model calculations. Kinematic coincidence technique.
doi: 10.1103/PhysRevC.55.516
1997AI06 Z.Phys. A359, 271 (1997) N.Aissaoui, F.Haas, R.M.Freeman, C.Beck, A.Morsad, B.Djerroud, R.Caplar, G.A.Monnehan, A.Hachem Resonances and Fluctuations in the 16O + 15N and 12C + 19F Collisions NUCLEAR REACTIONS 16O(15N, X), E=30-70 MeV; measured Eγ, Iγ; 16O(15N, X), E=40-65 MeV; 12C(19F, X), E not given; measured fragment σ(θ), kinematic coincidences; deduced elastic, inelastic, transfer channels excitation functions, composite system quasimolecular resonances.
doi: 10.1007/s002180050402
1997HA63 Nuovo Cim. 110A, 989 (1997) F.Haas, A.Elanique, R.M.Freeman, C.Beck, R.Nouicer, D.L.Watson, C.Jones, R.Cowin, P.Lee, Z.Basrak Search for Electromagnetic Transitions between 12C-12C Cluster States in 24Mg NUCLEAR REACTIONS 12C(12C, 12C'), (12C, 8Be), (12C, α), E=32.9 MeV; measured Eγ, Iγ, γγ-, (fragment)γ-, (fragment)(fragment)-coin, Q-value spectra. 24Mg deduced resonance cluster configuration.
doi: 10.1007/BF03035936
1997SZ01 Phys.Rev. C55, 1312 (1997) S.Szilner, Z.Basrak, R.M.Freeman, F.Haas, A.Morsad, C.Beck Excitation Functions of Inelastic and Transfer Channels in 12C + 12C Around E(cm) = 32.5 MeV NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), (12C, 16O), E(cm)=30-35 MeV; measured σ(θ), σ(E); deduced intermediate structure.
doi: 10.1103/PhysRevC.55.1312
1996BE17 Phys.Rev. C54, 227 (1996) C.Beck, D.Mahboub, R.Nouicer, T.Matsuse, B.Djerroud, R.M.Freeman, F.Haas, A.Hachem, A.Morsad, M.Youlal, S.J.Sanders, R.Dayras, J.P.Wieleczko, E.Berthoumieux, R.Legrain, E.Pollacco, Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto 35Cl + 12C Asymmetrical Fission Excitation Functions NUCLEAR REACTIONS 12C(35Cl, F), E=150-280 MeV; measured σ(E, θ), fission (fragment)(fragment) correlations, missing charge distributions; deduced charge deficit systematics, fusion-fission σ(E). Extended Hauser-Feshbach method, transition-state formalism.
doi: 10.1103/PhysRevC.54.227
1996FA14 Phys.Rev. C54, 1249 (1996) K.A.Farrar, S.J.Sanders, A.K.Dummer, A.T.Hasan, F.W.Prosser, B.B.Back, I.G.Bearden, R.R.Betts, M.P.Carpenter, B.Crowell, M.Freer, D.J.Henderson, R.V.F.Janssens, T.L.Khoo, T.Lauritsen, Y.Liang, D.Nisius, A.H.Wuosmaa, C.Beck, R.M.Freeman, Sl.Cavallaro, A.Szanto de Toledo Fission Decay of 48Cr at E(*)(CN) ≈ 60 MeV NUCLEAR REACTIONS 12C(36Ar, X), 28Si(20Ne, X), 24Mg(24Mg, X), E(cm)=47, 45.5, 44.4 MeV; measured Eγ, Iγ, (particle)(particle)γ-coin; deduced σ(A) for fission, evaporation residues. 48Ca deduced spin distribution, fission decay features.
doi: 10.1103/PhysRevC.54.1249
1996NO08 Z.Phys. A356, 5 (1996) R.Nouicer, C.Beck, D.Mahboub, T.Matsuse, B.Djerroud, R.M.Freeman, A.Hachem, Sl.Cavallaro, E.De Filippo, G.Lanzano, A.Pagano, M.L.Sperduto, R.Dayras, E.Berthoumieux, R.Legrain, E.Pollacco Statistical Binary Decay of 35Cl + 24Mg at ≈ 8 MeV/nucleon NUCLEAR REACTIONS 24Mg(35Cl, X), E=8 MeV/nucleon; measured (fragment)(fragment)-coin; deduced production σ vs Z; deduced no ternary breakup events evidence. Extended Hauser-Feshbach method.
doi: 10.1007/s002180050138
1995CA06 Nucl.Phys. A583, 161c (1995) Sl.Cavallaro, C.Beck, E.Berthoumieux, R.Dayras, E.De Filippo, G.Di Natale, B.Djerroud, R.M.Freeman, A.Hachem, F.Haas, B.Heusch, G.Lanzano, R.Legrain, D.Mahboub, A.Morsad, A.Pagano, E.Pollacco, S.J.Sanders, M.L.Sperduto Origin and Decay-Properties of Binary Fragments Produced in the 35Cl + 24Mg Reaction at E/A ≈ 8 MeV/A NUCLEAR REACTIONS 24Mg(35Cl, X), E=260, 282.4 MeV; measured σ(fragment θ, E), (fragment)(fragment)(θ); deduced binary fragment origin, decay mechanisms.
doi: 10.1016/0375-9474(94)00725-3
1995FR14 Phys.Rev. C51, 3504 (1995) R.M.Freeman, F.Haas, A.Elanique, A.Morsad, C.Beck E(c.m.) = 32.5 MeV Resonance in 12C + 12C NUCLEAR REACTIONS 12C(12C, 16O), E=31.5-33.5 MeV; analyzed data. 24Mg deduced resonance chain state related feature.
doi: 10.1103/PhysRevC.51.3504
1994AI02 Z.Phys. A348, 237 (1994) N.Aissaoui, F.Haas, R.M.Freeman, C.Beck, A.Morsad, B.Djerroud, R.Caplar, G.A.Monnehan, A.Hachem, M.Youlal On the Resonant Behavior of the 16O + 15N Reaction NUCLEAR REACTIONS, ICPND 15N(16O, 16O), E(cm) ≈ 15-37.5 MeV; measured γ yield vs E, σ(θ); deduced σ(E); deduced resonance, L.
doi: 10.1007/BF01291924
1993BE15 Phys.Rev. C47, 2093 (1993) C.Beck, B.Djerroud, F.Haas, R.M.Freeman, A.Hachem, B.Heusch, A.Morsad, M.Vuillet-A-Cilles, S.J.Sanders Asymmetric Fission of 47V Induced by the 23Na + 24Mg Reaction NUCLEAR REACTIONS 24Mg(23Na, X), (23Na, F), E=89.1 MeV; measured fragment total kinetic energy, σ vs charge. 47V deduced no entrance channel effects in fission. Other reactions data analyzed.
doi: 10.1103/PhysRevC.47.2093
1992BE34 Z.Phys. A343, 309 (1992) C.Beck, B.Djerroud, F.Hass, R.M.Freeman, A.Hachem, B.Heusch, A.Morsad, M.Youlal, Y.Abe, R.Dayras, J.P.Wieleczko, T.Matsuse, S.M.Lee Competition between the Fusion-Fission and Deep-Inelastic Orbiting Mechanisms in the 35Cl + 12C Reaction NUCLEAR REACTIONS 12C(35Cl, X), E=180, 200 MeV; measured evaporation residue σ(θ), fission like yields charge distributions, σ(θ), fragment spectra, (fragment)(fragment)-coin damped yields σ(E) for X=B-Mg; deduced fusion-fission rather than orbiting process evidence.
doi: 10.1007/BF01291530
1992FR11 Z.Phys. A341, 175 (1992) R.M.Freeman, Z.Basrak, F.Haas, A.Hachem, G.A.Monnehan, M.Youlal The Resonant Behaviour of the Heavy-Ion Reaction 14C + 16O NUCLEAR REACTIONS, ICPND 16O(14C, 12C), (14C, 14C), (14C, 13C), E(cm)=21.05-32.1 MeV; measured σ(E), σ(θ); deduced resonances.
doi: 10.1007/BF01298477
1992FR13 Phys.Rev. C46, 589 (1992) R.M.Freeman, Z.Basrak, F.Haas, A.Hachem, G.A.Monnehan, M.Youlal Resonant and Nonresonant Behavior of the Heavy-Ion Reaction 14C + 12C NUCLEAR REACTIONS 12C(14C, 12C), (14C, 13C), (14C, 14C), (14C, 15N), (14C, 16O), (14C, 17O), (14C, 18O), (14C, 2α), E=42-54 MeV; measured binary channels σ(E, θ). 26Mg deduced resonances, J, π, rotational band moment of inertia.
doi: 10.1103/PhysRevC.46.589
1991MO03 Z.Phys. A338, 61 (1991) A.Morsad, F.Haas, C.Beck, R.M.Freeman Detailed Energy Dependence of the Elastic and Inelastic 12C + 12C Scattering between 5 and 10 MeV/nucleon NUCLEAR REACTIONS, ICPND 12C(12C, 12C), (12C, 12C'), E(cm)=30-60 MeV; measured σ(E); deduced structure.
doi: 10.1007/BF01279115
1989BE37 Z.Phys. A334, 521 (1989) C.Beck, B.Djerroud, B.Heusch, R.Dayras, R.M.Freeman, F.Haas, A.Hachem, J.P.Wieleczko, M.Youlal Fusion-Fission in the 35Cl + 12C Reaction at E(lab) = 180 MeV NUCLEAR REACTIONS 12C(35Cl, X), E=180 MeV; measured (fragment)(fragment)-coin, fragment production σ vs Z; deduced reaction mechanism. Kinematical coincidence technique.
1989FR04 Phys.Rev. C39, 1335 (1989) R.M.Freeman, F.Haas, A.Morsad, C.Beck Comparison of the 13C + 16O Reaction with 12C + 17O NUCLEAR REACTIONS, ICPND 13C(16O, 16O), (16O, 17O), E=42.4-66.5 MeV; measured σ(θ); deduced model parameters; deduced σ(E). Kinematic coincidences, enriched target. DWBA analysis.
doi: 10.1103/PhysRevC.39.1335
1988FR15 Phys.Rev. C38, 1081 (1988) R.M.Freeman, Z.Basrak, F.Haas, A.Hachem, G.A.Monnehan, A.Morsad, M.Youlal Origin of the 13C + 17O Resonant Structure NUCLEAR REACTIONS 13C(17O, 17O'), E=42.2-46.2 MeV; measured σ(θ, E). Kinematic coincidences.
doi: 10.1103/PhysRevC.38.1081
1987DA34 Fizika(Zagreb) 19, 445 (1987) S.Datta, N.Cindro, R.M.Freeman, C.Beck, F.Haas, A.Morsad Optical-Model Analysis of 13C(16O, 16O)13C in the Range E(cm) = 19-30 MeV NUCLEAR REACTIONS 13C(16O, 16O), E(cm)=19, 21.5, 22.4, 25.6, 28, 29.7 MeV; calculated σ(θ); deduced model parameters.
1987FR11 Fizika(Zagreb) Supplement 1, 13 (1987) R.M.Freeman, F.Haas, G.Monnehan, V.Barci, Z.Basrak, C.Beck, R.Caplar, A.Hachem, A.Morsad, M.Youlal The 12C + 15N Reaction: Example of a coupled-channel resonance NUCLEAR REACTIONS, ICPND 12C(15N, 15N), (15N, 15N'γ), E=51-62 MeV; measured σ(E), γ yield vs E; deduced resonance structure. 15N level deduced resonant role.
1986CI01 Phys.Rev. C33, 1280 (1986) Experimental Evidence and the Landau-Zener Promotion in Nucleus-Nucleus Collisions NUCLEAR REACTIONS, ICPND 12,13C(17O, 17O'), E(cm) ≈ 8-28 MeV; calculated γ-yield, σ(E). 12C(17O, 12C), E=41, 44.5, 49.5 MeV; 13C(16O, 12C), E=46.2 MeV; measured σ(θ); deduced potential parameters, Landau-Zener promotion evidence.
doi: 10.1103/PhysRevC.33.1280
1986FR04 Phys.Rev. C33, 1275 (1986) R.M.Freeman, C.Beck, F.Haas, A.Morsad, N.Cindro 12C + 17O Reaction NUCLEAR REACTIONS, ICPND 12C(17O, 17O), (17O, 17O'), (17O, 16O), E=40-70 MeV; measured σ(θ), σ(E), kinematic coincidences. DWBA analysis.
doi: 10.1103/PhysRevC.33.1275
1986RU02 Phys.Rev.Lett. 56, 2356 (1986) A.Ruckelshausen, R.D.Fischer, W.Kuhn, V.Metag, R.Muhlhans, R.Novotny, T.L.Khoo, R.V.F.Janssens, H.Groger, D.Habs, H.W.Heyng, R.Repnow, D.Schwalm, G.Duchene, R.M.Freeman, B.Haas, F.Haas, S.Hlavac, R.S.Simon Unexpected Entrance-Channel Effects in the Decay of the Compound Nucleus 156Er NUCLEAR REACTIONS 92Zr(64Ni, 4n), (64Ni, 3n), (64Ni, 2n), (64Ni, 2np), (64Ni, nα), (64Ni, 2nα), E=239 MeV; 144Sm(12C, 2n), (12C, 3n), (12C, 4n), (12C, nα), (12C, 2nα), (12C, 2np), E=73.5 MeV; measured evaporation residue yield vs spin. 156Er deduced entrance channel effects in decay.
doi: 10.1103/PhysRevLett.56.2356
1985BE37 Nucl.Phys. A443, 157 (1985) C.Beck, R.M.Freeman, F.Haas, B.Heusch, J.J.Kolata Role of the Valence Neutron in the 12C + 17O and 13C + 16O Collisions NUCLEAR REACTIONS, ICPND 12C(17O, X), 13C(16O, X), E=20-70 MeV; measured γ-ray yields of reaction products; deduced resonant behavior, Landau-Zener effect. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(85)90326-4
1985BE40 Nucl.Phys. A442, 320 (1985) C.Beck, F.Haas, R.M.Freeman, B.Heusch, J.P.Coffin, G.Guillaume, F.Rami, P.Wagner Comparison of Cross Sections for C + O Reactions in the Second Regime of Complete Fusion NUCLEAR REACTIONS, ICPND 12C(18O, X), E=32-140 MeV; 13C(17O, X), E=54-140 MeV; 12C(16O, X), E=62-150 MeV; 16O(12C, X), E=46.5-112.5 MeV; measured σ(fragment θ, E) for fragment Z=3-14, fusion σ(E); deduced critical, grazing angular momenta. 28Si deduced possible superdeformation. Statistical, complete fusion model predictions.
doi: 10.1016/0375-9474(85)90148-4
1984BE22 Phys.Rev. C29, 1942 (1984) C.Beck, F.Haas, R.M.Freeman, B.Heusch, J.P.Coffin, G.Guillaume, F.Rami, P.Wagner Fusion Cross Sections of the 12C + 16O Reaction at E(16O) up to 150 MeV NUCLEAR REACTIONS, ICPND 12C(16O, X), 16O(12C, X), E(cm)=26.6, 34.3, 42.9, 53.6, 64.3 MeV; measured evaporation residue yields; deduced fusion σ(E), critical, grazing (L).
doi: 10.1103/PhysRevC.29.1942
1983FR16 J.Phys.(Paris), Lett. 44, L-429 (1983) R.M.Freeman, F.Haas, C.Beck, A.Niemesken Low Lying Yrast States of 32S NUCLEAR REACTIONS 29Si(α, nγ), E=12 MeV; measured nγ(θ), γγ-coin. 32S deduced yrast levels, J, π.
doi: 10.1051/jphyslet:019830044011042900
1983FR17 Phys.Rev. C28, 437 (1983) R.M.Freeman, C.Beck, F.Haas, B.Heusch, J.J.Kolata Resonant Effects in the 13C + 17O Reaction NUCLEAR REACTIONS, ICPND 13C(17O, 17O'), E=35-60 MeV; measured γ yield vs E. 17O transition deduced single particle character. Nuclear Landau-Zener effect.
doi: 10.1103/PhysRevC.28.437
1982BA49 Phys.Rev. C26, 1774 (1982) Z.Basrak, R.Caplar, C.Beck, R.M.Freeman, F.Haas Correlation among Intermediate Structures in Binary and Fusion-Evaporation Channels of the 18O + 12C Reaction NUCLEAR REACTIONS, ICPND 12C(18O, X), (18O, 18O'), (18O, 16O)(18O, 17O), (18O, 14C), (18O, 15N), (18O, 13C), (18O, α), (18O, 2α), (18O, 5n), (18O, 5np), (18O, 5n2p), (18O, n2α), E=50-81 MeV; measured Eγ, Iγ; deduced σ(E), channel correlation effects. 30Si deduced structure in fusion evaporation, binary channel.
doi: 10.1103/PhysRevC.26.1774
1982FR15 Nucl.Phys. A385, 516 (1982) R.M.Freeman, P.A.DeYoung, L.J.Satkowiak, M.A.Xapsos, J.J.Kolata A New Level of 18F NUCLEAR REACTIONS 6Li(16O, α), E=24 MeV; measured Eγ, Iγ, αγ-coin, αγ(θ). 18F deduced level, T, T1/2, J, π. Enriched targets.
doi: 10.1016/0375-9474(82)90101-4
1982HE07 Phys.Rev. C26, 542 (1982) B.Heusch, C.Beck, J.P.Coffin, P.Engelstein, R.M.Freeman, G.Guillaume, F.Haas, P.Wagner Entrance Channel Effects for Complete Fusion of O + C Isotopes NUCLEAR REACTIONS, ICPND 12C(18O, 18O), (18O, X), E=32-140 MeV; 13C(17O, 17O), (17O, X), E=54-140 MeV; 14C(16O, 16O), (16O, X), E(cm)=10-60 MeV; measured σ(θ), evaporation σ vs E; deduced entrance channel effects, fusion evaporation. Tof fragment identification. Statistical, macroscopic models.
doi: 10.1103/PhysRevC.26.542
1981BA66 Fizika(Zagreb) 13, Suppl.No.1, 33 (1981) Z.Basrak, C.Beck, R.Caplar, R.M.Freeman, F.Haas Structure in the 12C + 18O Reaction Cross Sections NUCLEAR REACTIONS 12C(18O, γ), (18O, X), (18O, xn), E=50-81 MeV; measured production σ(E) for 17,18O, 13,14C, σ(fusion, E), σ(evaporation) vs E; deduced structure. Activation technique.
1981BE64 Fizika(Zagreb) 13, Suppl.No.1, 27 (1981) C.Beck, R.M.Freeman, F.Haas, B.Heusch, H.Bohn, K.A.Eberhard, U.Kaufl, H.Puchta, T.Senftleben, W.Trautmann Resonant Structure in the Reaction Channels of 14C + 14C NUCLEAR REACTIONS 14C(14C, 14C'), (14C, xn), (14C, xnα), E(cm)=12.5-32.5 MeV; measured σ(E), production σ(E) for 25Mg, 22Ne, Ne, 15C; deduced channel correlated structure. 28Mg deduced possible quasimolecular resonances.
1981FR23 Phys.Rev. C24, 2390 (1981) R.M.Freeman, C.Beck, F.Haas, B.Heusch, H.Bohn, U.Kaufl, K.A.Eberhard, H.Puchta, T.Senftleben, W.Trautmann Structure in the Reaction Channels of 14C + 14C NUCLEAR REACTIONS 14C(14C, 14C'), (14C, X), E(cm)=12.5-32.5 MeV; measured Eγ, Iγ; deduced production σ(E) for 15C, 21,22,23Ne, 25Mg, channel correlated resonance structure. Enriched target.
doi: 10.1103/PhysRevC.24.2390
1981HE08 Phys.Rev. C23, 1527 (1981) B.Heusch, C.Beck, J.P.Coffin, R.M.Freeman, A.Gallmann, F.Haas, F.Rami, P.Wagner, D.E.Alburger Systematics of Carbon + Carbon Fusion-Evaporation Reactions NUCLEAR REACTIONS 13C(13C, X), E=30-60 MeV; 12C, 13C, 14C(12C, X), E=40 MeV; measured σ(fragment θ, Z, mass), fusion-evaporation yields for 16,17,18O, 20,21,22Ne, 24,25Mg, 22,23,24Na, 19,20,21F. Enriched targets, tof fragment charge identification. Statistical particle evaporation calculations.
doi: 10.1103/PhysRevC.23.1527
1981KO07 Phys.Rev. C23, 1056 (1981) J.J.Kolata, C.Beck, R.M.Freeman, F.Haas, B.Heusch Structure in the 14C + 16O Reaction Cross Sections NUCLEAR REACTIONS 14C(16O, 22Ne), (16O, 18O), (16O, 17O), (16O, 15N), (16O, 14C), E(cm)=16.34 MeV; measured production σ; deduced resonance structure. 30Si deduced resonances, J, π, moment of inertia of crossing band.
doi: 10.1103/PhysRevC.23.1056
1981SP04 Phys.Lett. 102B, 6 (1981) K.-H.Speidel, G.J.Kumbartzki, W.Knauer, M.Knopp, V.Mertens, P.N.Tandon, J.Gerber, R.M.Freeman The g-Factor of the First Excited 2+ State in 26Mg from Transient Field Precession Measurements NUCLEAR REACTIONS 24Mg(α, α'), E=7.08 MeV; 26Mg(α, α'), E=8.01 MeV; measured γ(θ, H) in Fe, αγ(θ); deduced K-shell ion polarization effects. 26Mg level deduced g.
doi: 10.1016/0370-2693(81)90200-8
1980FR03 Phys.Lett. 90B, 229 (1980) R.M.Freeman, F.Haas, G.Korschinek Strong Resonant Behaviour of the 12C + 14C Reaction NUCLEAR REACTIONS 12C(14C, 14C'γ), (14C, 13C), (14C, 11B), (14C, 15N), E(cm)=18-26 MeV; measured σ(Eγ). 26Mg deduced strongly correlated resonances.
doi: 10.1016/0370-2693(80)90729-7
1980HE11 J.Phys.(Paris), Colloq.C-10, 229 (1980) B.Heusch, C.Beck, J.P.Coffin, R.M.Freeman, A.Gallmann, F.Haas, F.Rami, P.Wagner, D.E.Alburger The 18O + 12C Fusion-Evaporation Reaction NUCLEAR REACTIONS 12C(18O, X), E=32-100 MeV; 14C(16O, X), E=50 MeV; 12C(16O, X), E not given; measured σ(fragment mass, E); deduced production σ for Si, Al, Mg, Na, Ne. 30Si deduced no resonance structure in fusion channels. Statistical Hauser-Feshach calculations, Monte Carlo technique. Tof.
1980KO02 Phys.Rev. C21, 579 (1980) J.J.Kolata, R.M.Freeman, F.Hass, B.Heusch, A.Gallmann Reaction Cross Sections for 12C + 12C NUCLEAR REACTIONS 12C(12C, X), E(cm)=14-31 MeV; measured production σ(E) for 22,23Na, 19,20,21,22Ne, 18,19F, 16O, 12C; deduced fusion σ, inelastic σ, 3α evaporation σ. 24Mg deduced fusion L trajectory.
doi: 10.1103/PhysRevC.21.579
1979FR08 Phys.Rev. C20, 569 (1979) R.M.Freeman, F.Haas, B.Heusch, S.M.Lee Comparison of the γ-Ray Yield Functions for the 12C + 24Mg and 16O + 28Si Reactions NUCLEAR REACTIONS 12C(24Mg, X), E=45-71 MeV; 16O(28Si, X), E=55-96 MeV; measured Iγ(E), nγ-coin; deduced reaction mechanism. 34Cl, 34S, 31P, 28Si, 28Mg, 38Ar, 41,42Ca, 39K deduced production σ(E). Natural C, O targets.
doi: 10.1103/PhysRevC.20.569
1979KO03 Phys.Rev. C19, 408 (1979) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Reaction Cross Sections for 16O + 12C NUCLEAR REACTIONS 12C(16O, X), E(cm)=17-28 MeV; measured σ(E, production). Evaporation model analysis of nuclide distributions. Correlation analysis of fluctuations.
doi: 10.1103/PhysRevC.19.408
1979KO15 Phys.Rev. C19, 2237 (1979) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Gross and Intermediate-Width Structure in the Interaction of 16O with 16O NUCLEAR REACTIONS 16O(16O, X), E(cm)=12-40 MeV; measured production σ for 20Ne, 23Na, 27,28,29,30Si, 30,31P, 26,27Al, 24,26Mg; deduced total σ(fusion), barrier height, critical parameters, normalizations. Evaporation model, optical model analysis.
doi: 10.1103/PhysRevC.19.2237
1978BA76 Fizika, Suppl. 10, 11 (1978) P.Baumann, A.M.Bergdolt, G.Bergdolt, R.M.Freeman, F.Haas, B.Heusch, A.Huck, G.Walter Study of High Spin States in 30P and 32P NUCLEAR REACTIONS 16O(16O, np), E=42 MeV; 18O(16O, np), E=35 MeV; measured nγ-, γγ-coin, Eγ, Iγ. 27Al(α, n), E=14.6 MeV; measured RDM. 30P deduced levels, J, π, T1/2, B(λ). 32P deduced levels, J, π, T1/2.
1978FR05 Phys.Rev.Lett. 40, 927 (1978) Periodic Structure in the Heavy-Ion Reactions 18O + 12C and 18O + 16O NUCLEAR REACTIONS 12C(18O, 18O'), E=25-59 MeV; 16O(18O, 18O'), E=30-51 MeV; measured γ-spectra; deduced periodic structure.
doi: 10.1103/PhysRevLett.40.927
1977HA11 Nucl.Phys. A279, 237 (1977) F.Haas, R.M.Freeman, B.Heusch, A.Gallmann Structure en Bande du Noyau 22Na: le Premier Niveau Jπ = 6+ NUCLEAR REACTIONS 19F(α, n), E=7.825, 8.225 MeV; measured n-γ(θ), Doppler shift attenuation. 22Na levels deduced J, π, branching ratios, δ, T1/2, transition strengths.
doi: 10.1016/0375-9474(77)90226-3
1977HE04 Phys.Rev. C15, 1196 (1977) B.Heusch, F.Haas, R.M.Freeman, A.Gallmann Experimental Study of the 12C(3He, p)14N Reaction Mechanism between 11 And 20 MeV Bombarding Energy NUCLEAR REACTIONS 12C(3He, pγ), E=11-20 MeV; measured pγ(θ); deduced reaction mechanism, nuclear alignments.
doi: 10.1103/PhysRevC.15.1196
1977KO16 Phys.Rev. C16, 891 (1977) J.J.Kolata, R.C.Fuller, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Reaction Cross Sections for 16O + 16O NUCLEAR REACTIONS 16O(16O, X), E(cm)=12.5-30.5 MeV; measured σ(A) for production of A=16-31 reaction products; deduced broad shape resonances.
doi: 10.1103/PhysRevC.16.891
1976FR09 Nucl.Phys. A261, 471 (1976) R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Largeurs de Transitions Gamma du Niveau a 2788 keV de 21Ne NUCLEAR REACTIONS 18O(α, n), E=4.7 MeV; measured Iγ, γγ(θ), recoil distance. 21Ne deduced branching ratios, δ, T1/2, transition strengths.
doi: 10.1016/0375-9474(76)90160-3
1976FR19 Phys.Rev. C14, 2006 (1976) R.M.Freeman, F.Haas, B.Heusch, A.Gallmann Strong Isoscalar M2 Transition in 22Na NUCLEAR REACTIONS 19F(α, nγ), E=5.5 MeV; measured n, γ spectra. 22Na level deduced γ-branching.
doi: 10.1103/PhysRevC.14.2006
1976KO24 Phys.Lett. 65B, 333 (1976) J.J.Kolata, R.M.Freeman, F.Haas, B.Heusch, A.Gallmann On the Fusion Cross Section for 16O + 12C NUCLEAR REACTIONS 12C(16O, X), E=40-65 MeV; measured total fusion σ(E).
doi: 10.1016/0370-2693(76)90235-5
1975FR11 Phys.Rev. C11, 1948 (1975) R.M.Freeman, F.Haas, A.R.Achari, R.Modjtahed-Zadeh High-Spin States of 28Al NUCLEAR REACTIONS 27Al(d, p), E=12.32 MeV; measured σ(Ep, θ). 27Al(d, pγ), E=3.14 MeV; measured pγ-coin, pγ(t). 28Al levels deduced γ-branching, T1/2.
doi: 10.1103/PhysRevC.11.1948
1975WA06 Phys.Rev. C11, 1459 (1975) P.Wagner, R.M.Freeman, A.Gallman, E.K.Warburton Decay of the 10Be 0+ 6.18-MeV Level NUCLEAR REACTIONS 11B(t, αγ); measured σ(Eγ), αγ-coin. 10Be deduced transitions, γ-branching ratios.
doi: 10.1103/PhysRevC.11.1459
1973FR18 Phys.Rev. C8, 2182 (1973) R.M.Freeman, F.Haas, B.Heusch, J.Fernandez Castillo, J.W.Olness, A.Gallmann Rotational Band Structure of 22Na. II. Neutron-Gamma Coincidence Measurements NUCLEAR REACTIONS 19F(α, nγ), E=11 MeV; measured nγ(θ, t), DSA, γγ(θ). 22Na levels deduced T1/2, quadrupole moment.
doi: 10.1103/PhysRevC.8.2182
1973HA40 Nucl.Phys. A211, 289 (1973) F.Haas, R.M.Freeman, B.Heusch, S.Kohmoto, A.Gallmann Vies Moyennes dans 14N NUCLEAR REACTIONS 12C(3He, pγ), E=5.54 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 14N deduced levels, T1/2. Natural 12C targets self-supporting or on Ni backing.
doi: 10.1016/0375-9474(73)90720-3
1973HA55 Phys.Rev. C8, 2169 (1973) F.Haas, R.M.Freeman, J.Fernandez Castillo, A.Gallmann Rotational Band Structure of 22Na. I. Electromagnetic Transitions for Levels of E(ex) < 4.0 MeV NUCLEAR REACTIONS 19F(α, nγ), E=5-8 MeV; measured DSA, recoil distance, Eγ. 22Na levels deduced T1/2, π, γ-branching.
doi: 10.1103/PhysRevC.8.2169
1972FR11 Nucl.Phys. A197, 529 (1972) R.M.Freeman, R.Faerber, M.Toulemonde, A.Gallmann Etude de Transitions γ dans le Noyau 35S NUCLEAR REACTIONS 34S(d, pγ), E=3.50, 4.00 MeV; measured Eγ, DSA, σ(Ep, Eγ, θ(pγ)). 35S deduced levels, γ-branching ratios, J, γ-mixing, T1/2. Enriched target.
doi: 10.1016/0375-9474(72)91027-5
1970FR10 Nucl.Phys. A156, 305 (1970) Etude de Transitions γ dans les Noyaux 40K et 28Al NUCLEAR REACTIONS 27Al(d, p), 39,41K(d, p), E=3.5, 3.7 MeV; measured Eγ, pγ-coin. 28Al, 40K deduced levels, γ-branching ratios. 42K deduced transitions. Natural targets.
doi: 10.1016/0375-9474(70)90143-0
1968MA38 Phys.Letters 28B, 106 (1968) P.J.Mathew, G.J.McCallum, R.M.Freeman New Isotope 82As RADIOACTIVITY 82As; measured T1/2, Eγ, Iγ.
doi: 10.1016/0370-2693(68)90142-1
1967GO07 Phys.Rev. 155, 1119 (1967) S.Gorodetzky, R.M.Freeman, A.Gallmann, F.Haas, B.Heusch Angular-Correlation Studies of the Reactions O16(He3, Pγ)F18 and O16(He3, αγ)O15 NUCLEAR STRUCTURE 18F, 16O, 15O; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.155.1119
1966GO15 Phys.Rev. 149, 801 (1966) S.Gorodetzky, R.M.Freeman, A.Gallman, F.Hass Angular-Correlation Studies of the Reactions O16(He3, αγ)O15, C12(He3, pγ)N14, and C12(d, pγ)C13 NUCLEAR STRUCTURE 12C, 15O, 13C, 16O, 14N; measured not abstracted; deduced nuclear properties.
doi: 10.1103/PhysRev.149.801
1965FR02 Proc.Phys.Soc.(London) 85, 267 (1965) Multi-Level Analysis of Resonances in 6Li(d, α)α and 7Li(p, α)α Reactions NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
doi: 10.1088/0370-1328/85/2/308
1965MA13 Proc.Phys.Soc. (London) 85, 281 (1965) G.S.Mani, R.M.Freeman, F.Picard, D.Redon, A.Sadeghi An Experimental Study of 6Li(d, α)α Reaction NUCLEAR STRUCTURE 8Be; measured not abstracted; deduced nuclear properties.
doi: 10.1088/0370-1328/85/2/309
1964FR03 Nucl.Phys. 51, 593 (1964) Levels in Na23 from the Alpha Bombardment of F19 NUCLEAR STRUCTURE 23Na; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(64)90297-4
1964MA51 Nucl.Phys. 60, 588(1964) G.S.Mani, R.Freeman, F.Picard, A.Sadeghi, D.Redon Study of the Reaction Li7(p, α)α up to 12 MeV Proton Energy NUCLEAR REACTIONS 7Li(p, α) E=1-12 MeV; measured σ(E; θ). 8Be deduced levels. Enriched target.
doi: 10.1016/0029-5582(64)90095-1
1963FR12 J.Phys. 24, 894 (1963) R.Freeman, J.M.F.Jeronymo, G.S.Mani, A.Sadeghi Niveaux d'Excitation de 23Na d'Apres les Reactions Induites par Particules Alpha sur 19F NUCLEAR STRUCTURE 19F, 23Na; measured not abstracted; deduced nuclear properties.
doi: 10.1051/jphys:019630024011089400
1962FR06 Nuclear Phys. 37, 215 (1962) Gamma-Ray Transitions in C11 from the B10(d, nγ)C11 Reaction NUCLEAR STRUCTURE 10B; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(62)90259-6
1961FR07 Nuclear Phys. 26, 446 (1961) The Magnetic Moment of the Second Excited State of F19 NUCLEAR STRUCTURE 19F; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(61)90102-X
1957FR20 Proc.Roy.Soc.(London) 242A, 455 (1957) R.Freeman, G.R.Murray, R.E.Richards
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