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NSR database version of May 20, 2024.

Search: Author = R.M.Freeman

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1456.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1535.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1000.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO0999.


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
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0604.


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
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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
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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)

N.Cindro, R.M.Freeman, F.Haas

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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0409.


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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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)

R.M.Freeman, F.Haas

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1970FR10      Nucl.Phys. A156, 305 (1970)

R.M.Freeman, A.Gallmann

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
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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
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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
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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
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1965FR02      Proc.Phys.Soc.(London) 85, 267 (1965)

R.M.Freeman, G.S.Mani

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA1358.


1964FR03      Nucl.Phys. 51, 593 (1964)

R.M.Freeman, G.S.Mani

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO2290.


1962FR06      Nuclear Phys. 37, 215 (1962)

R.M.Freeman

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
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1961FR07      Nuclear Phys. 26, 446 (1961)

R.M.Freeman

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
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