NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Szanto de Toledo Found 99 matches. 2019GU32 Eur.Phys.J. A 55, 211 (2019) G.L.Guardo, C.Spitaleri, L.Lamia, R.Spartá, N.Carlin, S.Cherubini, G.Gimenez Del Santo, I.Indelicato, M.La Cognata, D.Lattuada, S.Messina, M.Munhoz, S.S.Perrotta, R.G.Pizzone, G.G.Rapisarda, S.Romano, M.L.Sergi, F.A.Souza, A.Szanto de Toledo, S.Tudisco, A.Tumino The 10B(n, α)7Li cross sections at ultra-low energy through the Trojan Horse Method applied to the 2H(10B, α7Li)1H
doi: 10.1140/epja/i2019-12914-0
2017SP04 Phys.Rev. C 95, 035801 (2017) C.Spitaleri, S.M.R.Puglia, M.La Cognata, L.Lamia, S.Cherubini, A.Cvetinovic, G.D'Agata, M.Gulino, G.L.Guardo, I.Indelicato, R.G.Pizzone, G.G.Rapisarda, S.Romano, M.L.Sergi, R.Sparta, S.Tudisco, A.Tumino, M.Gimenez Del Santo, N.Carlin, M.G.Munhoz, F.A.Souza, A.Szanto de Toledo, A.Mukhamedzhanov, C.Broggini, A.Caciolli, R.Depalo, R.Menegazzo, V.Rigato, I.Lombardo, D.Dell'Aquila Measurement of the 10B(p, α0)7Be cross section from 5 keV to 1.5 MeV in a single experiment using the Trojan horse method NUCLEAR REACTIONS 2H(10B, α7Be), E=27 MeV; measured α and 7Be spectra using ΔE-E method at Pelletron-Linac laboratory of DFN-Sao Paulo; deduced Q-value spectrum, energy scatter plots, momentum distribution, astrophysical S(E) factors, Trojan horse method (THM) astrophysical factor, R-matrix fit of THM data 11C; deduced levels, resonances, center-of-mass energies, J, π, Γp, Γα0, Γα1.
doi: 10.1103/PhysRevC.95.035801
2014SP03 Phys.Rev. C 90, 035801 (2014) C.Spitaleri, L.Lamia, S.M.R.Puglia, S.Romano, M.La Cognata, V.Crucilla, R.G.Pizzone, G.G.Rapisarda, M.L.Sergi, M.Gimenez Del Santo, N.Carlin, M.G.Munhoz, F.A.Souza, A.Szanto de Toledo, A.Tumino, B.Irgaziev, A.Mukhamedzhanov, G.Tabacaru, V.Burjan, V.Kroha, Z.Hons, J.Mrazek, S.-H.Zhou, C.Li, Q.Wen, Y.Wakabayashi, H.Yamaguchi, E.Somorjai Measurement of the 10 keV resonance in the 10B(p, α0)7Be reaction via the Trojan Horse method NUCLEAR REACTIONS 2H(10B, α7Be), E=24.5 MeV; measured particle spectra by ΔE-E method using ionization chambers and position-sensitive detectors at LNS-Catania accelerator facility; analyzed data by Trojan Horse method (THM); deduced Eα-Be and Eα-n two-dimensional plots, experimental momentum distribution and its comparison with DWBA and PWIA calculations, THM bare nucleus astrophysical S(E) factors using R-matrix formalism for 5-100 keV resonances in 11C, dominated by 10-keV resonance corresponding to 8699-keV, 5/2+ level in 11C. 11C; deduced widths of three resonances.
doi: 10.1103/PhysRevC.90.035801
2012LA01 J.Phys.(London) G39, 015106 (2012) L.Lamia, C.Spitaleri, V.Burjan, N.Carlin, S.Cherubini, V.Crucilla, M.G.Munhoz, M.G.Del Santo, M.Gulino, Z.Hons, G.G.Kiss, V.Kroha, S.Kubono, M.La Cognata, C.Li, J.Mrazek, A.Mukhamedzhanov, R.G.Pizzone, S.M.R.Puglia, Q.Wen, G.G.Rapisarda, C.Rolfs, S.Romano, M.L.Sergi, E.Somorjai, F.A.Souza, A.Szanto de Toledo, G.Tabacaru, A.Tumino, Y.Wakabayashi, H.Yamaguchi, S.-H.Zhou New measurement of the 11B(p, α0)8Be bare-nucleus S(E) factor via the Trojan horse method NUCLEAR REACTIONS 2H(11B, α), E=27 MeV; measured reaction products, Eα, Iα. 8Be; deduced σ(θ), S-factors.
doi: 10.1088/0954-3899/39/1/015106
2011BE19 Int.J.Mod.Phys. E20, 943 (2011) C.Beck, N.Rowley, P.Papka, S.Courtin, M.Rousseau, F.A.Souza, N.Carlin, F.Liguori Neto, M.M.De Moura, M.G.Del Santo, A.A.I.Suade, M.G.Munhoz, E.M.Szanto, A.Szanto de Toledo, N.Keeley, A.Diaz-Torres, K.Hagino Cluster model for reactions induced by weakly bound and/or exotic halo nuclei with medium-mass targets
doi: 10.1142/S0218301311019027
2011OL01 Nucl.Phys. A856, 46 (2011) R.A.N.Oliveira, N.Carlin, R.Liguori Neto, M.M.de Moura, M.G.Munhoz, M.G.del Santo, F.A.Souza, E.M.Szanto, A.Szanto de Toledo, A.A.P.Suaide Study of 9Be+ 12C elastic scattering at energies near the Coulomb barrier NUCLEAR REACTIONS 12C(9Be, 9Be), (9Be, X), E=13.0, 14.5, 17.3, 19.0, 21.0 MeV; measured E(particle), I(particle, θ); deduced σ(θ), deformation parameters; calculated σ(θ), M(Eλ) using FRESCO optical model code with Sao Paulo parameters and including also cluster transfer.
doi: 10.1016/j.nuclphysa.2011.02.005
2010BE22 Nucl.Phys. A834, 440c (2010) C.Beck, N.Rowley, P.Papka, S.Courtin, M.Rousseau, F.A.Souza, N.Carlin, R.Liguori Neto, M.M.de Moura, M.G.Del Santo, A.A.P.Suaide, M.G.Munhoz, E.M.Szanto, A.Szanto de Toledo, N.Keeley, A.Diaz-Torres, K.Hagino Reaction mechanisms for weakly-bound, stable nuclei and unstable, halo nuclei on medium-mass targets NUCLEAR REACTIONS 59Co(6Li, X), E=10-40 MeV; calculated evaporation residue σ, σ(θ). 58Ni(7Be, 7Be), E=15.09, 17.13, 18.53, 19.93, 21.43 MeV; calculated σ(θ). Discussed interplay of different processes and systematics of reaction mechanism. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.01.059
2010LA11 Nucl.Phys. A834, 655c (2010) L.Lamia, S.M.R.Puglia, C.Spitaleri, S.Romano, M.G.Del Santo, N.Carlin, M.G.Munhoz, S.Cherubini, G.G.Kiss, V.Kroha, S.Kubono, M.La Cognata, C.-B.Li, R.G.Pizzone, Q.-G.Wen, M.L.Sergi, A.Szanto de Toledo, Y.Wakabayashi, H.Yamaguchi, S.-H.Zhou Indirect study of 11B(p, α0)8Be and 10B(p, α)7Be reactions at astrophysical energies by means of the Trojan Horse Method: recent results NUCLEAR REACTIONS 2H(11B, α8Be), E=27 MeV; 2H(10B, α7Be), E=24.4 MeV; measured Eα, Iα(θ), E(particle), I(particle). 11B(p, α), E(cm)=0-0.6 MeV; 10B(p, α), E(cm)=0-0.15 MeV; deduced S-factor using Trojan Horse Method.
doi: 10.1016/j.nuclphysa.2010.01.115
2010PI09 Nucl.Phys. A834, 673c (2010) R.G.Pizzone, C.Spitaleri, S.Cherubini, M.La Cognata, L.Lamia, S.Romano, M.L.Sergi, A.Tumino, C.Li, Q.Wen, S.Zhou, V.Burjan, V.Kroha, J.Mrazek, N.Carlin, M.G.del Santo, A.Szanto de Toledo, S.Kubono, T.Wakabayashi, H.Yamaguchi, C.Rolfs Trojan Horse Method: a useful tool for electron screening effect investigation NUCLEAR REACTIONS 2H(3He, p), 6Li(p, α), 6Li(d, α), 7Li(p, α), 9Be(p, α), E not given; calculated electron screening effect with Trojan Horse Method.
doi: 10.1016/j.nuclphysa.2010.01.121
2010SO14 Eur.Phys.J. A 44, 181 (2010) F.A.Souza, N.Carlin, C.Beck, N.Keeley, A.Diaz-Torres, R.Liguori Neto, C.Siqueira-Mello, M.M.de Moura, M.G.Munhoz, R.A.N.Oliveira, M.G.Del Santo, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo Projectile breakup dynamics for 6Li + 59Co: Kinematical analysis of α - d coincidences NUCLEAR REACTIONS 59Co(6Li, X), E=29.6 MeV; measured p-spectra, d-spectra, α-spectra, αd-coin; deduced σ, σ(θ), breakup reaction mechanism features. Comparison with CDCC model.
doi: 10.1140/epja/i2010-10940-0
2010SO16 Nucl.Phys. A834, 420c (2010) F.A.Souza, N.Carlin, C.Beck, N.Keeley, A.Diaz-Torres, R.Liguori Neto, C.Siqueira-Mello, M.M.de Moura, M.G.Munhoz, R.A.N.Oliveira, M.G.Del Santo, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo 6Li direct breakup lifetimes NUCLEAR REACTIONS 59Co(6Li, dα), E=29.6 MeV; measured Eα, Iα(θ), Ed, Id(θ), dα-coin; deduced σ(θ), direct breakup T1/2; calculated T1/2. Discussed breakup reaction mechanism features.
doi: 10.1016/j.nuclphysa.2010.01.054
2009SO04 Nucl.Phys. A821, 36 (2009) F.A.Souza, C.Beck, N.Carlin, N.Keeley, R.Liguori Neto, M.M.de Moura, M.G.Munhoz, M.G.Del Santo, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo Reaction mechanisms in the 6Li + 59Co system NUCLEAR REACTIONS 59Co(6Li, X), E=17.4, 21.5, 25.5, 29.6 MeV; measured p-spectra, d-spectra, α-spectra, αd-coin; deduced total α and deuteron production σ and reaction mechanism features using different reaction models.
doi: 10.1016/j.nuclphysa.2009.02.009
2008LA18 Nuovo Cim. B 31, 423 (2008) L.Lamia, C.Spitaleri, N.Carlin, S.Cherubini, M.G.Del Santo, M.Gulino, M.La Cognata, M.G.Munhoz, R.G.Pizzone, S.M.R.Puglia, G.G.Rapisarda, S.Romano, M.L.Sergi, A.Szanto de Toledo, S.Tudisco, A.Tumino Indirect study of (p, α) and (n, α) reactions induced on boron isotopes NUCLEAR REACTIONS 2H(11B, nα), (10B, pα), E=27 MeV; measured Eα, Iα, fragment spectra, cross sections. 11B(p, α), 10B(n, α); deduced S-factors.
doi: 10.1393/ncc/i2009-10303-2
2008RO05 J.Phys.(London) G35, 014008 (2008) S.Romano, C.Spitaleri, S.Cherubini, V.Crucilla, M.Gulino, M.La Cognata, L.Lamia, R.G.Pizzone, S.M.R.Puglia, G.G.Rapisarda, M.L.Sergi, S.Tudisco, A.Tumino, R.E.Tribble, V.Z.Goldberg, A.M.Mukhamedzhanov, G.Tabacaru, L.Trache, V.Kroha, V.Burjan, Z.Hons, J.Mrazek, E.Somorjai, Z.Elekes, Z.Fulop, G.Gyurky, G.Kiss, A.Szanto de Toledo, N.Carlin, M.M.De Moura, M.G.Del Santo, M.G.Munhoz, R.Liguori Neto, F.A.Souza, A.A.P.Suaide, E.Szanto The Trojan horse method in nuclear astrophysics: recent results NUCLEAR REACTIONS 7Li(p, α)α, E(cm)=0-7 MeV; 10B(p, α)7Be, E(cm)=0-400 keV; p(p, p)p, E ≈ 0-0.6 MeV; analyzed cross section, S-factors.Trojan Horse Method.
doi: 10.1088/0954-3899/35/1/014008
2007KN02 Phys.Rev. C 75, 064602 (2007) G.N.Knyazheva, E.M.Kozulin, R.N.Sagaidak, A.Yu.Chizhov, M.G.Itkis, N.A.Kondratiev, V.M.Voskressensky, A.M.Stefanini, B.R.Behera, L.Corradi, E.Fioretto, A.Gadea, A.Latina, S.Szilner, M.Trotta, S.Beghini, G.Montagnoli, F.Scarlassara, F.Haas, N.Rowley, P.R.S.Gomes, A.Szanto de Toledo Quasifission processes in 40, 48Ca+144, 154Sm reactions NUCLEAR REACTIONS 144Sm(40Ca, F), 140 MeV; 154Sm(40Ca, F), E=141 MeV; 154Sm(48Ca, F), E=137 MeV; 186W(16O, F), E=69.9 MeV; measured σ, mass, energy, and angular distribution of fission fragments. Deduced fission and quasifission cross sections.
doi: 10.1103/PhysRevC.75.064602
2007LA25 Nucl.Phys. A787, 309c (2007) L.Lamia, S.Romano, N.Carlin, S.Cherubini, V.Crucilla, M.M.De Moura, M.G.Del Santo, M.G.Munhoz, M.Gulino, R.Liguori Neto, M.La Cognata, F.Mudo, R.G.Pizzone, S.M.R.Puglia, M.L.Sergi, F.A.Souza, C.Spitaleri, A.A.P.Suaide, E.Szanto, A.Szanto de Toledo, S.Tudisco, A.Tumino Boron depletion: indirect measurement of the 10B(p, α)7Be S(E)-factor NUCLEAR REACTIONS 2H(10B, nα), E=27 MeV; measured Eα, Iα, σ; deduced astrophysical S-factor. Trojan horse method, three-body process.
doi: 10.1016/j.nuclphysa.2006.12.049
2007SO09 Phys.Rev. C 75, 044601 (2007), Erratum Phys.Rev. C 76, 029901 (2007) F.A.Souza, L.A.S.Leal, N.Carlin, M.G.Munhoz, R.Liguori Neto, M.M.de Moura, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, J.Takahashi Effect of breakup on elastic scattering for the 6, 7Li + 59Co systems NUCLEAR REACTIONS 59Co(6Li, 6Li), (7Li, 7Li), E=12-30 MeV; measured elastic σ(θ); deduced breakup threshold anomaly. NUCLEAR STRUCTURE 208Pb; calculated binding energy, neutron and proton radii, sensitivity to coupling corrections. Relativistic mean field theory.
doi: 10.1103/PhysRevC.75.044601
2007WE01 Nucl.Phys. A781, 342 (2007); Erratum Nucl.Phys. A794, 231 (2007) J.C.Werner, L.A.S.Leal, M.G.Munhoz, N.Carlin, L.C.Chamon, N.Added, J.A.P.Brage, R.Liguori Neto, M.M.Coimbra, M.M.de Moura, F.A.Souza, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, J.Takahashi Structure effects in the elastic scattering for the 16O + 46, 50Ti systems NUCLEAR REACTIONS 46,50Ti(16O, 16O), E=30-70 MeV; measured elastic σ(θ); deduced model parameters, threshold anomaly. Unexpected structure effects not observed.
doi: 10.1016/j.nuclphysa.2006.11.034
2005SO14 Braz.J.Phys. 35, 888 (2005) F.A.Souza, R.Liguori Neto, M.M.de Moura, M.G.Munhoz, A.A.P.Suaide, E.M.Szanto, J.Takahashi, A.Szanto de Toledo, N.Carlin Direct Measurement of the Breakup Process NUCLEAR REACTIONS 12C(6Li, dα), E=26 MeV; 59Co(6Li, dα), E=30 MeV; measured particle spectra, σ(θ(α), θ(d)), three-body final state correlations; deduced reaction mechanism features.
doi: 10.1590/S0103-97332005000500046
2005TR14 Eur.Phys.J. A 25, Supplement 1, 615 (2005) M.Trotta, A.M.Stefanini, S.Beghini, B.R.Behera, A.Yu.Chizhov, L.Corradi, S.Courtin, E.Fioretto, A.Gadea, P.R.S.Gomes, F.Haas, I.M.Itkis, M.G.Itkis, G.N.Kniajeva, N.A.Kondratiev, E.M.Kozulin, A.Latina, G.Montagnoli, I.V.Pokrovsky, N.Rowley, R.N.Sagaidak, F.Scarlassara, A.Szanto de Toledo, S.Szilner, V.M.Voskressensky, Y.W.Wu Fusion hindrance and quasi-fission in 48Ca induced reactions: Implications for super-heavy element production NUCLEAR REACTIONS 154Sm(48Ca, X), E(cm) ≈ 120-200 MeV; 186W(16O, X), E(cm) ≈ 60-100 MeV; measured capture, evaporation, fission σ; deduced fusion hindrance features. 144,154Sm(48Ca, X), 154Sm(40Ca, X), E* ≈ 50 MeV; measured fission fragment kinetic energy and mass distributions; deduced mass-asymmetry and shell effects.
doi: 10.1140/epjad/i2005-06-084-2
2004DA23 Phys.Rev. C 70, 024606 (2004) M.Dasgupta, P.R.S.Gomes, D.J.Hinde, S.B.Moraes, R.M.Anjos, A.C.Berriman, R.D.Butt, N.Carlin, J.Lubian, C.R.Morton, J.O.Newton, A.Szanto de Toledo Effect of breakup on the fusion of 6Li, 7Li, and 9Be with heavy nuclei NUCLEAR REACTIONS 209Bi(6Li, X)213Rn/212Rn/211Rn/210Rn/213At/212At/211At/212Po/211Po/210Po, E=26-48 MeV; 209Bi(7Li, X)214Rn/213Rn/212Rn/211Rn/213At/212At/211At/212Po/211Po/210Po/211Bi, E=26-52 MeV; 208Pb(9Be, X)215Rn/214Rn/213Rn/212Rn/212Po/211Po/210Po, E=36-51 MeV; measured fission, complete and incomplete fusion σ; deduced barrier distributions, breakup effects, other reaction mechanism features.
doi: 10.1103/PhysRevC.70.024606
2004SO23 Prog.Theor.Phys.(Kyoto), Suppl. 154, 101 (2004) F.A.Souza, N.Carlin, P.Miranda, M.M.de Moura, M.G.Munhoz, A.A.P.Suaide, E.M.Szanto, J.Takahashi, A.Szanto de Toledo Study of the Influence of Projectile Breakup on the Fusion Cross Section of 6, 7Li + 12C, 59Co NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=12-30 MeV; measured fusion excitation functions; 12C(6Li, dα), (7Li, tα), E ≈ 30 MeV; measured particle spectra, angular correlations; deduced breakup contribution to fusion, related reaction mechanism features.
doi: 10.1143/PTPS.154.101
2004SO36 Braz.J.Phys. 34, 907 (2004) F.A.Souza, A.Szanto de Toledo, M.G.Munhoz, J.Takahashi, N.Carlin, A.A.P.Suaide, M.M.de Moura, e.M.Szanto Study of the Effect of the Breakup on the Fusion Cross Section of the Systems 6, 7Li+59Co NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=12-26 MeV; measured fusion σ; deduced breakup effects. 59Co(6Li, dα), E=26 MeV; measured Eα, Ed, dα-coin.
doi: 10.1590/S0103-97332004000500054
2004SU02 Phys.Lett. B 579, 271 (2004) A.A.P.Suaide, M.M.de Moura, N.Adde, N.N.Ajitanand, N.Carlin, M.G.Munhoz, F.A.Souza, E.M.Szanto, J.Takahashi, A.Szanto de Toledo Dynamics of light heavy-ion reactions in the framework of their time scales NUCLEAR REACTIONS 10B(16O, X), E(cm)=24 MeV; 12C(16O, X), E(cm)=27.4 MeV; measured particle spectra, correlations; deduced sequential particle emission time scale. 10B(16O, X), E(cm)=17-25 MeV; 12C(19F, X), E(cm)=22-24 MeV; measured excitation functions; deduced compound nucleus lifetime features.
doi: 10.1016/j.physletb.2003.11.012
2004SZ01 Nucl.Phys. A734, 311 (2004) A.Szanto de Toledo, F.A.Souza, C.Beck, S.J.Sanders, M.G.Munhoz, J.Takahashi, N.Carlin, A.A.P.Suaide, M.de Moura, E.M.Szanto Fusion and breakup in reactions involving weakly bound nuclei NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E(cm) ≈ 10-25 MeV; analyzed fusion σ. 59Co(6Li, X), E=26 MeV; analyzed deuteron and alpha spectra, correlations.
doi: 10.1016/j.nuclphysa.2004.01.055
2003BE34 Phys.Rev. C 67, 054602 (2003) C.Beck, F.A.Souza, N.Rowley, S.J.Sanders, N.Aissaoui, E.E.Alonso, P.Bednarczyk, N.Carlin, S.Courtin, A.Diaz-Torres, A.Dummer, F.Haas, A.Hachem, K.Hagino, F.Hoellinger, R.V.F.Janssens, N.Kintz, R.Liguori Neto, E.Martin, M.M.Moura, M.G.Munhoz, P.Papka, M.Rousseau, A.Sanchez i Zafra, O.Stezowski, A.A.Suaide, E.M.Szanto, A.Szanto de Toledo, S.Szilner, J.Takahashi Near-barrier fusion of weakly bound 6Li and 7Li nuclei with 59Co NUCLEAR REACTIONS 59Co(6Li, xnypzα), (7Li, xnypzα), E(cm) ≈ 10-25 MeV; measured fusion, evaporation residue σ; deduced reaction mechanism features.
doi: 10.1103/PhysRevC.67.054602
2003BE75 Acta Phys.Hung.N.S. 18, 297 (2003) C.Beck, M.Rousseau, P.Papka, A.Sanchez i Zafra, C.Bhattacharya, V.Rauch, P.Bednarczyk, S.Courtin, O.Dorvaux, F.Haas, A.Nourreddine, I.Piqueras, J.Robin, L.El Bakali, C.Enaux, E.Galmar, S.Szilner, O.Stezowski, A.Prevost, S.Thummerer, W.von Oertzen, A.Hachem, E.Martin, A.Fahli, A.Morsad, A.Szanto de Toledo, S.J.Sanders Search for Cluster Emission and Extremely Deformed Shapes Using Charged-Particle Spectroscopy NUCLEAR REACTIONS 12C, 28Si(28Si, X), E=180 MeV; 12C(27Al, X), E=150 MeV; 12C(31P, X), E=112 MeV; 12C(32S, X), E=140 MeV; measured Eα, Ep, angular correlations between light charged particles and evaporation residues; deduced highly deformed configurations, cluster emission features. Other reactions discussed.
doi: 10.1556/APH.18.2003.2-4.30
2003SO19 Nucl.Phys. A718, 544c (2003) F.A.Souza, A.Szanto de Toledo, N.Carlin, R.Liguori Neto, A.A.Suaide, M.M.Moura, E.M.Szanto, M.G.Munhoz, J.Takahashi, C.Beck, S.J.Sanders Fusion of weakly bound light nuclei NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=11-26 MeV; measured fusion σ.
doi: 10.1016/S0375-9474(03)00838-8
2003SZ04 Nucl.Phys. A722, 248c (2003) A.Szanto de Toledo, E.E.Alonso, N.Carlin, R.Liguori Neto, M.M.Moura, M.G.Munhoz, A.A.Suaide, F.A.Souza, E.M.Szanto, J.Takahashi, C.Beck, M.Rousseau, P.Bednarczyk, S.Courtin, F.Hass, O.Stezowski, S.Szilner, S.J.Sanders Fusion of light weakly bound nuclei NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E=11-26 MeV; measured fusion σ; deduced reaction mechanism features.
doi: 10.1016/S0375-9474(03)01373-3
2003SZ14 Braz.J.Phys. 33, 320 (2003) A.Szanto de Toledo, M.G.Munhoz, J.Takahashi, F.A.Souza, E.E.Alonso, N.Carlin, R.Liguori Neto, M.M.Moura, A.A.Suaide, E.M.Szanto Is the Inhibition/Enhancement of Fusion Due to Breakup Still a Puzzle? NUCLEAR REACTIONS 59Co(6Li, X), (7Li, X), E(cm) ≈ 10-26 MeV; analyzed fusion σ, breakup channel contributions.
doi: 10.1590/s0103-97332003000200031
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
2002DA23 Phys.Rev. C66, 041602 (2002) M.Dasgupta, D.J.Hinde, K.Hagino, S.B.Moraes, P.R.S.Gomes, R.M.Anjos, R.D.Butt, A.C.Berriman, N.Carlin, C.R.Morton, J.O.Newton, A.Szanto de Toledo Fusion and breakup in the reactions of 6Li and 7Li nuclei with 209Bi NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E(cm)=25-50 MeV; measured fusion, incomplete fusion, and fission excitation functions; deduced reaction mechanism features. Classical trajectory model.
doi: 10.1103/PhysRevC.66.041602
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
2002SU17 Phys.Rev. C66, 014607 (2002) A.A.P.Suaide, N.Added, N.Aissaoui, E.E.Alonso, W.H.Z.Cardenas, R.J.Fujii, M.M.de Moura, M.G.Munhoz, F.A.Souza, E.M.Szanto, A.Szanto de Toledo, N.Carlin, M.Papa Time Scales for Binary Processes from Light Heavy-Ion Reactions NUCLEAR REACTIONS 10B(16O, 16O), E=44-65 MeV; measured σ(θ). 10B(16O, 12C), E=44-65 MeV; 12C(19F, 12C), (19F, 15N), E=57-64 MeV; measured binary decay excitation functions, widths, σ(θ); deduced time scales, other reaction mechanism features.
doi: 10.1103/PhysRevC.66.014607
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. 2001DE50 Nucl.Phys. A696, 64 (2001) M.M.de Moura, A.A.P.Suaide, N.Added, E.E.Alonso, W.H.Z.Cardenas, R.J.Fujii, M.G.Munhoz, F.A.Souza, E.M.Szanto, A.Szanto de Toledo, J.Takahashi, N.Carlin, N.N.Ajitanand Light Heavy-Ion Reactions: Time scales and emission order of light products NUCLEAR REACTIONS 10B(16O, X), E=62.5 MeV; 12C(16O, X), E=64.0 MeV; measured fragments charge distributions, angular correlations, emission time scales, velocities. Comparison with three-body trajectory Monte Carlo simulation.
doi: 10.1016/S0375-9474(01)01126-5
2000SZ06 Nucl.Phys. A679, 175 (2000) A.Szanto de Toledo, N.Added, W.H.Z.Cardenas, N.Carlin, M.M.de Moura, M.G.Munhoz, A.A.P.Suaide, E.M.Szanto, J.Takahashi Fusion Hindrance in Light Nuclear Systems: Binding energy and/or surface diffuseness effect ? NUCLEAR STRUCTURE Z=3-13; analyzed fusion barrier features; deduced fusion inhibition factor for light systems.
doi: 10.1016/S0375-9474(00)00346-8
1999AI02 Phys.Rev. C60, 034614 (1999) N.Aissaoui, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, M.M.de Moura, D.Hirata, D.J.Morrissey, S.J.Sanders, J.Stasko, M.Steiner, A.A.P.Suaide, E.M.Szanto, A.Szanto de Toledo, M.Thoennessen, J.A.Winger Strong Absorption Radii from Reaction Cross Section Measurements for Neutron-Rich Nuclei NUCLEAR REACTIONS Si(30Al, X), (31Al, X), (32Al, X), (33Al, X), (32Si, X), (33Si, X), (34Si, X), (35Si, X), (36Si, X), (34P, X), (35P, X), (36P, X), (37P, X), (38P, X), (39P, X), (36S, X), (37S, X), (38S, X), (39S, X), (40S, X), (41S, X), (39Cl, X), (40Cl, X), (41Cl, X), (42Cl, X), (43Cl, X), (44Cl, X), (41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Ti, X), (54Ti, X), E ≈ 38-80 MeV/nucleon; measured mean energy-integrated reaction σ. 30,31,32,33Al, 32,33,34,35,36Si, 34,35,36,37,38,39P, 36,37,38,39,40,41S, 39,40,41,42,43,44Cl, 41,42,43,44,45,46Ar, 44,45,46,47,48K, 46,47,48,49,50Ca, 49,50,51,52Sc, 53,54Ti deduced strong absorption radii. Secondary beams from 55Mn fragmentation.
doi: 10.1103/PhysRevC.60.034614
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
1999CA50 Phys.Rev. C60, 067602 (1999) R.Cabezas, E.M.Szanto, N.Carlin, N.Added, A.A.P.Suaide, M.M.de Moura, M.Munhoz, R.Liguori Neto, J.Takahashi, R.M.dos Anjos, W.H.Z.Cardenas, A.Szanto de Toledo ' Elastic Fission ' of Very Light Nuclear Systems NUCLEAR REACTIONS 10,11B(9Be, X), (16O, X), (17O, X), (18O, X), 11B(10B, X), 12C(11B, X), (19F, X), E(cm) ≈ 19-56 MeV; measured elastic fission yields; deduced geometrical effects, other reaction mechanism features. Other data analyzed.
doi: 10.1103/PhysRevC.60.067602
1999DA07 Phys.Rev.Lett. 82, 1395 (1999) M.Dasgupta, D.J.Hinde, R.D.Butt, R.M.Anjos, A.C.Berriman, N.Carlin, P.R.S.Gomes, C.R.Morton, J.O.Newton, A.Szanto de Toledo, K.Hagino Fusion Versus Breakup: Observation of large fusion suppression for 9Be + 208Pb NUCLEAR REACTIONS 208Pb(9Be, X), E=35-51 MeV; measured complete, incomplete fusion σ; deduced projectile breakup effects.
doi: 10.1103/PhysRevLett.82.1395
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
1999SA45 Phys.Rep. 311, 487 (1999) S.J.Sanders, A.Szanto de Toledo, C.Beck Binary Decay of Light Nuclear Systems
doi: 10.1016/S0370-1573(98)00092-1
1999SZ03 Pramana 53, 483 (1999) A.Szanto de Toledo, N.Carlin, N.Added, E.M.Szanto, M.G.Munhoz, J.Takahashi, A.Suaide, M.M.de Moura Fusion-Fission of Light Nuclear Systems
1997DE15 Phys.Rev. C55, 3174 (1997) P.M.C.de Oliveira, J.S.Sa Martins, A.Szanto de Toledo Stochastic Behavior of Cooling Processes in Hot Nuclei NUCLEAR REACTIONS 10B(10B, X), E=48, 65, 80, 100, 110 MeV; 9Be(10B, X), E=100 MeV; analyzed fragment, mass distribution; deduced structure effects role in cluster evaporation. Dynamic lattice model.
doi: 10.1103/PhysRevC.55.3174
1997LI15 Phys.Rev. C56, 250 (1997) I.Licot, N.Added, N.Carlin, G.M.Crawley, S.Danczyk, J.Finck, D.Hirata, H.Laurent, D.J.Morrissey, M.M.de Moura, H.R.Schelin, J.Stasko, M.Steiner, A.A.P.Suaide, A.Szanto de Toledo, E.M.Szanto, M.Thoennessen, J.A.Winger Reaction Cross Sections and Radii for f-p Shell Exotic Neutron-Rich Nuclei NUCLEAR REACTIONS, ICPND Si(41Ar, X), (42Ar, X), (43Ar, X), (44Ar, X), (45Ar, X), (46Ar, X), (44K, X), (45K, X), (46K, X), (47K, X), (48K, X), (49K, X), (46Ca, X), (47Ca, X), (48Ca, X), (49Ca, X), (50Ca, X), (51Ca, X), (49Sc, X), (50Sc, X), (51Sc, X), (52Sc, X), (53Sc, X), E=52-69 MeV/nucleon; measured reaction σ. 41,42,43,44,45,46Ar, 44,45,46,47,48,49K, 46,47,48,49,50,51Ca, 49,50,51,52,53Sc deduced strong absorption radii, neutron separation energies. Comparison to Glauber model, RMF theory.
doi: 10.1103/PhysRevC.56.250
1997SZ02 Phys.Rev. C56, 558 (1997) A.Szanto de Toledo, S.J.Sanders, C.Beck Statistical Description of Strongly Damped Binary Yields from the 28Si + 16O Reaction NUCLEAR REACTIONS 28Si(14N, X), 28Si(12C, X), 24Mg(12C, X), 24Mg(16O, X), 28Si, (16O, X), E not given; calculated number of reaction channels vs grazing angular momentum. 28Si(16O, X), E(cm)=39.1, 50.1 MeV; analyzed σ(E), fragment charge distributions; deduced energy-dependent orbiting component. Statistical model.
doi: 10.1103/PhysRevC.56.558
1997TA01 Phys.Rev.Lett. 78, 30 (1997) J.Takahashi, M.Munhoz, E.M.Szanto, N.Carlin, N.Added, A.A.P.Suaide, M.M.de Moura, R.Liguori Neto, A.Szanto de Toledo, L.F.Canto Is Fusion Inhibited for Weakly Bound Nuclei ( Question ) NUCLEAR REACTIONS 12C, 9Be(6Li, X), (7Li, X), E=6-33 MeV; measured evaporation residue spectra; deduced fusion probability vs E, effective separation energy.
doi: 10.1103/PhysRevLett.78.30
1996BE14 Phys.Rev. C53, 1989 (1996) Macroscopic Features of Light Heavy-Ion Fission Reactions NUCLEAR STRUCTURE 19F, 20,21Ne, 40Ca, 68Se, 56Ni, 80Zr; calculated light-heavy ion fission-fusion formation associated limiting angular momenta vs mass number. Standard, finite-range liquid drop models.
doi: 10.1103/PhysRevC.53.1989
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
1996SZ06 Phys.Rev. C54, 3290 (1996) A.Szanto de Toledo, B.V.Carlson, C.Beck, M.Thoennessen Entrance-Channel Mass-Asymmetry Dependence of Compound Nucleus Formation Time in Light Heavy-Ion Reactions NUCLEAR REACTIONS 29Si(9Be, X), 27Al(11B, X), 26Mg(12C, X), 19F(19F, X), E not given; calculated compound nucleus formation shape evolution, time; deduced entrance channel mass-asymmetry depednence related features.
doi: 10.1103/PhysRevC.54.3290
1995MU04 Nucl.Phys. A587, 367 (1995) J.T.Murgatroyd, S.J.Bennett, N.M.Clarke, B.R.Fulton, G.J.Gyapong, C.D.Jones, D.L.Watson, T.M.Cormier, H.Dejbakhsh, A.Szanto de Toledo, N.Carlin Termination of the 12C-12C Cluster States Revealed in the 12C)(20Ne, 12C12C)8Be Breakup Reaction NUCLEAR REACTIONS 12C(20Ne, 212C), E=300 MeV; measued (12C)(12C)-coin. 24Mg deduced energies of breakup states.
doi: 10.1016/0375-9474(95)00003-J
1994AN05 Phys.Rev. C49, 2018 (1994) R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, E.M.Szanto, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Competing Reaction Mechanisms for the 16,17,18O + 10,11B and 19F + 9Be Systems NUCLEAR REACTIONS 10,11B(16O, 16O), (17O, 17O), (18O, 18O), E=42-63 MeV; measured σ(θ); deduced optical model parameters. 10,11B(16O, X), (17O, X), (18O, X), E=22-64 MeV; 9Be(19F, X), E=56 MeV; measured fusion, quasielastic, strong damped reaction yields; deduced reaction systematics.
doi: 10.1103/PhysRevC.49.2018
1994HA03 Phys.Rev. C49, 1031 (1994) A.T.Hasan, S.J.Sanders, K.A.Farrar, F.W.Prosser, B.B.Back, R.R.Betts, M.Freer, D.J.Henderson, R.V.F.Janssens, A.H.Wuosmaa, A.Szanto de Toledo Heavy-Ion Resonance and Statistical Fission Competition in the 24Mg + 24Mg System at E(c.m.) = 44.4 MeV NUCLEAR REACTIONS 24Mg(24Mg, F), (24Mg, X), E(cm)=44.4 MeV; measured fission fragment, evaporation residue σ(θ). 48Cr deduced fission characteristics.
doi: 10.1103/PhysRevC.49.1031
1994SZ07 Phys.Rev. C50, 3151 (1994) A.Szanto de Toledo, E.M.Szanto, R.M.Anjos, W.Bohne, H.Morgenstern Saturation Effects in the 10B + 11B Reaction at E/A = 11 MeV NUCLEAR REACTIONS 11B(10B, X), E=110 MeV; measured fragment mass distributions, σ(evaporation residue); deduced saturation effects related features.
doi: 10.1103/PhysRevC.50.3151
1993AN08 Nucl.Phys. A555, 621 (1993) R.M.Anjos, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Fusion-Fission Rather Than Orbiting in 18O + 10,11B Reactions NUCLEAR REACTIONS 10,11B(18O, X), E=47 MeV; measured σ(θ), σ(fragment Z) for fusion, strongly damped binary processes.
doi: 10.1016/0375-9474(93)90491-F
1993AN15 Phys.Rev. C48, R2154 (1993) R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, H.R.Schelin, E.M.Szanto, C.Tenreiro, A.Szanto de Toledo, S.J.Sanders Fission Decay of Very Light Nuclear Systems NUCLEAR REACTIONS 10,11B(16O, X), (17O, X), (18O, X), 9Be(19F, X), E < 5 MeV/nucleon; measured σ(fragment θ); deduced fusion followed by fission evidence.
doi: 10.1103/PhysRevC.48.R2154
1993FA05 Nucl.Phys. A552, 82 (1993) L.Fante, Jr., N.Added, R.M.Anjos, N.Carlin, M.M.Coimbra, M.C.S.Figueira, R.Matheus, E.M.Szanto, A.Szanto de Toledo Fusion and Peripheral Processes in the 9Be + 10,11B Reactions NUCLEAR REACTIONS 10,11B(9Be, X), E=10-40 MeV; measured σ(fragment θ, E), σ(fragment A, Z) for fusion, quasi-elastic, elastic scattering; deduced critical grazing angular momentum, binary processes role. Statistical model calculations.
doi: 10.1016/0375-9474(93)90332-R
1993FI07 Nucl.Phys. A561, 453 (1993) M.C.S.Figueira, E.M.Szanto, R.M.Anjos, N.Added, N.Carlin, L.Fante, Jr., R.Matheus, A.Szanto de Toledo Complete Fusion of 9Be + 29Si NUCLEAR REACTIONS 29Si(9Be, X), (9Be, 9Be), E=17-40 MeV; measured σ(θ, E) for fusion, elastic scattering; deduced critical, grazing angular momentum. Statistical model calculations.
doi: 10.1016/0375-9474(93)90021-O
1993SZ02 Phys.Rev.Lett. 70, 2070 (1993) A.Szanto de Toledo, E.M.Szanto, M.Wotfe, B.V.Carlson, R.Donangelo, W.Bohne, K.Grabisch, H.Morgenstern, S.Proschitzki Are Hot Light Nuclei Liquid Droplets ( Question ) NUCLEAR REACTIONS 9Be, 10B(10B, X), E ≈ 11 MeV/nucleon; measured σ(evaporation residue, A); deduced no shell effects, composite nuclei liquid droplet behavior.
doi: 10.1103/PhysRevLett.70.2070
1992AD02 Nucl.Phys. A540, 328 (1992) N.Added, R.M.Dos Anjos, N.Carlin, L.Fante, Jr., M.C.S.Figueira, R.Matheus, E.M.Szanto, A.Szanto de Toledo, M.S.Hussein, C.A.Bertulani, L.F.Canto Direct Versus Statistical Break-Up Processes in the 16,18O + 27Al, 28Si Reactions at E/A ≤ 4 MeV NUCLEAR REACTIONS 27Al(18O, αX), 27Al, 28Si(16O, αX), E=48-64 MeV; measured Eα, σ(fragment θ, θα) for X=12,14C; deduced breakup, incomplete fusion yields. Direct, statistical models.
doi: 10.1016/0375-9474(92)90207-Z
1992FI04 Phys.Rev. C46, 1139 (1992) M.C.S.Figueira, E.M.Szanto, A.Szanto de Toledo, M.P.Pato, M.S.Hussein, L.F.Canto Role of the Breakup Process in the Hindrance of Light-Heavy-Ion Fusion Reactions NUCLEAR REACTIONS, ICPND 29Si(9Be, X), E(cm) ≈ 10-30 MeV; calculated fusion σ(E). 29Si(9Be, X), 19F(19F, X), 26Mg(12C, X), 27Al(11B, X), E(cm)=25 MeV; 10,11B, 12C, 28Si(9Be, X), E not given; calculated σ(fusion)/σ(reaction) vs cluster separation energy. One dimensional barrier penetration model, modified transmission coefficient.
doi: 10.1103/PhysRevC.46.1139
1991CO18 Nucl.Phys. A535, 161 (1991) M.M.Coimbra, R.M.Anjos, N.Added, N.Carlin Filho, L.Fante, Jr., M.C.S.Figueira, G.Ramirez, E.M.Szanto, A.Szanto de Toledo Study of the 10,11B + 10,11B Reactions up to E/A ≈ 5 MeV NUCLEAR REACTIONS 10,11B(10B, X), (11B, X), E=15-50 MeV; measured σ(θ, E), σ(A, Z) for fusion, quasi-elastic, elastic scattering; deduced critical, grazing angular momentum. Statistical model calculations.
doi: 10.1016/0375-9474(91)90521-7
1990AN14 Phys.Rev. C42, 354 (1990) R.M.Anjos, V.Guimaraes, N.Added, N.Carlin Filho, M.M.Coimbra, L.Fante, Jr., M.C.S.Figueira, E.M.Szanto, C.F.Tenreiro, A.Szanto de Toledo Effect of the Entrance Channel Mass Asymmetry on the Limitation of Light Heavy-Ion Fusion Cross Sections NUCLEAR REACTIONS, ICPND 27Al(11B, X), E=15-50 MeV; 19F(19F, X), E=32-72 MeV; measured evaporation residue σ(θ); deduced fusion barrier parameters, σ(E).
doi: 10.1103/PhysRevC.42.354
1990ET01 Nucl.Phys. A518, 572 (1990) M.C.Etchegoyen, A.Etchegoyen, A.O.Macchiavelli, G.Crawley, C.Djalali, M.Renteria, A.Szanto de Toledo, G.Westfall 18O + 58Ni Reaction at 35 MeV/Nucleon NUCLEAR REACTIONS, ICPND 58Ni(18O, X), E=630 MeV; measured fragment σ(θ), σ(Z, A) vs fragment momentum, integrated σ, fragments momentum width; deduced distribution reduced width.
doi: 10.1016/0375-9474(90)90147-E
1990LI16 Nucl.Phys. A512, 333 (1990) R.Liguori Neto, J.C.Acquadro, P.R.S.Gomes, A.Szanto de Toledo, C.F.Tenreiro, E.Crema, N.Carlin Filho, M.M.Coimbra Fusion of 16O + 46,50Ti Near and Below the Coulomb Barrier NUCLEAR REACTIONS, ICPND 46,50Ti(16O, X), E(cm) ≈ 21-49 MeV; measured evaporation residue, fusion σ(E); deduced barrier parameters. Hyperpure Ge detectors, in-beam, off-beam γ-rays. Wong model. Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0351. 1990SZ05 Phys.Rev. C41, 2164 (1990) E.M.Szanto, R.Liguori Neto, M.C.S.Figueira, A.Szanto de Toledo, M.G.Herman, N.G.Nicolis, P.M.Stwertka, T.M.Cormier Search for Valence Proton Effects in Sub-Barrier Fusion Reactions NUCLEAR REACTIONS, ICPND 50Ti, 51V, 52,54Cr, 54Fe(35Cl, X), E(cm) ≈ 50-80 MeV; measured fusion, residual production σ(E); deduced valence proton effects role.
doi: 10.1103/PhysRevC.41.2164
1990SZ06 Phys.Rev. C42, R815 (1990) A.Szanto de Toledo, L.Fante, Jr., R.M.Anjos, N.Added, M.M.Coimbra, M.C.S.Figueira, N.Carlin Filho, E.M.Szanto, M.S.Hussein, B.V.Carlson Dissipative Processes in Light-Heavy-Ion-Induced Reactions and Their Time Scales NUCLEAR REACTIONS 10,11B(9Be, X), E=10-40 MeV; 10,11B(10B, X), (11B, X), E=15-50 MeV; 10,11B(18O, X), E=20-72 MeV; measured σ(θ); deduced damped exit channel time scales.
doi: 10.1103/PhysRevC.42.R815
1989CA14 Phys.Rev. C40, 91 (1989) N.Carlin-Filho, M.M.Coimbra, N.Added, R.M.Anjos, L.Fante, Jr., M.C.S.Figueira, V.Guimaraes, E.M.Szanto, A.Szanto de Toledo, O.Civitarese Identification of Projectile Sequential Decay and Incomplete Fusion in the 16O + 28Si, 16O + 27Al, and 10B + 27Al Systems at 4-5 MeV/Nucleon NUCLEAR REACTIONS 27Al, 28Si(16O, α12C), E=64 MeV; 27Al(10B, α6Li), E=48 MeV; measured α(12C)(θ), α(6Li)(θ), σ(θ1, θ2); deduced reaction mechanism.
doi: 10.1103/PhysRevC.40.91
1989PR05 Phys.Rev. C40, 2600 (1989) F.W.Prosser, S.V.Reinert, D.G.Kovar, G.Rosner, G.S.F.Stephans, J.J.Kolata, C.F.Maguire, A.Szanto de Toledo, E.Szanto Fusion-Evaporation Cross Sections for 24Mg + 24Mg at 5 < E(lab) < 9 MeV/Nucleon NUCLEAR REACTIONS 24Mg(24Mg, 24Mg), (24Mg, X), E=111, 160, 206 MeV; measured evaporation residue σ(E, mass, θ), elastic σ(θ); deduced Galilean-invariant velocity distributions, limits on incomplete fusion. Model comparisons.
doi: 10.1103/PhysRevC.40.2600
1989SZ01 Phys.Rev.Lett. 62, 1255 (1989) A.Szanto de Toledo, M.M.Coimbra, N.Added, R.M.Anjos, N.Carlin Filho, L.Fante, Jr., M.C.S.Figueira, V.Guimaraes, E.M.Szanto Fissionlike Decay of 20Ne: Eccentric behavior in the B + B fusion processes NUCLEAR REACTIONS, ICPND 10,11B(10B, X), (11B, X), E=1.5-5 MeV/nucleon; measured σ(fragment θ, E), fusion σ(E).
doi: 10.1103/PhysRevLett.62.1255
1986BR26 J.Phys.(London) G12, 391 (1986) M.E.Brandan, A.Menchaca-Rocha, A.Szanto de Toledo, N.Carlin Filho, E.M.Szanto, M.M.Coimbra Detection of 8Be Nuclei from the Reaction 16O + 27Al at 65 MeV NUCLEAR REACTIONS 27Al(16O, 8Be), E=65 MeV; measured σ(E(8Be)), ejectile production σ. ΔE-E telescope. Two-body kinematic calculations.
doi: 10.1088/0305-4616/12/5/006
1986CA11 Ann.Phys.(New York) 169, 167 (1986) B.V.Carlson, O.Civitarese, M.S.Hussein, A.Szanto de Toledo Multi-Step Compound Model of Heavy-Ion Fusion NUCLEAR REACTIONS, ICPND 16,18O, 19F(12C, X), E ≈ 8-333.3 MeV; 27Al(12C, X), 24Mg(16O, X), 27Al(16O, X), E ≈ 13-150 MeV; 40Ca(16O, X), 32S(24Mg, X), E ≈ 25-200 MeV; 40Ca(40Ca, X), E ≈ 50-500 MeV; calculated fusion σ(E). Multi-step compound model.
doi: 10.1016/0003-4916(86)90163-6
1985CA01 Phys.Rev. C31, 152 (1985) N.Carlin Filho, M.M.Coimbra, J.C.Acquadro, R.Liguori Neto, E.M.Szanto, E.Farrelly-Pessoa, A.Szanto de Toledo Particle Emission in the Light Heavy-Ion Fusion Reactions: 14N, 16,18O + 12C NUCLEAR REACTIONS 12C(16O, X), (14N, X), (18O, X), E=30-60 MeV; measured σ(fragment θ, E) for X=d, t, 3He, α; deduced optical model parameters. 22Na, 23,24,25,26Mg, 25,26,27,28,29Al deduced level density parameters.
doi: 10.1103/PhysRevC.31.152
1985HU04 Phys.Rev.Lett. 54, 2659 (1985) M.S.Hussein, B.V.Carlson, O.Civitarese, A.Szanto De Toledo Dinucleus: A doorway to heavy-ion fusion NUCLEAR REACTIONS, ICPND 16O(12C, X), E ≈ 7-25 MeV; 27Al(12C, X), E ≈ 13-40 MeV; 12,13C, 15N, 16,18O, 19F, 20Ne(12C, X), 16O(10B, X), 17O(13C, X), 14,15N, 16O, 24,26Mg, 27Al, 28,29,30Si, 40Ca(16O, X), 23Na(19F, X), 24Mg, 27Al, 28Si(18O, X), 27Al(20Ne, X), 24Mg(32S, X), 40Ca(40Ca, X), E not given; calculated fusion σ(E). Two-step compound model, dinucleus channel coupling.
doi: 10.1103/PhysRevLett.54.2659
1985ST20 Phys.Lett. 161B, 60 (1985) G.S.F.Stephans, D.G.Kovar, R.V.F.Janssens, G.Rosner, H.Ikezoe, B.Wilkins, D.Henderson, K.T.Lesko, J.J.Kolata, C.K.Gelbke, B.V.Jacak, Z.M.Koenig, G.D.Westfall, A.Szanto De Toledo, E.M.Szanto, P.L.Gonthier Influence of Nucleon Fermi Motion on Incomplete Fusion NUCLEAR REACTIONS 24Mg, 27Al, 28Si, 40Ca, 48Ti(14N, X), E=5-35 MeV/nucleon; measured evaporation residue velocity spectra; deduced Fermi motion role in inelastic fusion. Other data input.
doi: 10.1016/0370-2693(85)90609-4
1984BO14 Phys.Lett. 138B, 357 (1984) R.Bonetti, B.V.Carlson, M.S.Hussein, A.Szanto de Toledo The Average Angular Distribution of Emitted Particles in Multi-Step Compound Processes NUCLEAR REACTIONS 12C(16O, α), E not given; calculated σ(θ); deduced precompound heavy ion configuration characteristics. Statistical window model, deviations from Hauser-Fesbach formalism.
doi: 10.1016/0370-2693(84)91916-6
1984CO27 Phys.Rev. C30, 2092 (1984) M.M.Coimbra, N.Carlin Filho, A.Szanto de Toledo, P.M.Stwertka, M.G.Herman, N.G.Nicolis, T.M.Cormier Use of Energy-Averaged Cross Sections for Nuclear Spectroscopy: 26Mg states in the continuum NUCLEAR REACTIONS 12C(18O, α), E=46-50 MeV: measured σ(Eα), σ(θ); deduced energy averaged σ. 26Mg deduced continuum states.
doi: 10.1103/PhysRevC.30.2092
1984SZ05 Phys.Rev. C30, 1706 (1984) A.Szanto de Toledo, T.M.Cormier, M.M.Coimbra, N.Carlin Filho, P.M.Stwertka, N.G.Nicolis 24Mg Yrast Sequence up to 30 MeV Excitation NUCLEAR REACTIONS 12C(16O, α), E=94, 97 MeV; measured σ(θ), σ(Eα). 24Mg deduced yrast sequence, effective moment of inertia.
doi: 10.1103/PhysRevC.30.1706
1983CI08 Phys.Lett. 125B, 22 (1983) O.Civitarese, B.V.Carlson, M.S.Hussein, A.Szanto de Toledo Multistep Nature of Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 12,13C, 14,15N, 16,18O, 19F, 20Ne(12C, X), 10B, 14,15N, 16O, 24,26Mg, 27Al, 28,29,30Si, 40Ca(16O, X), 23Na(19F, X), 24Mg, 27Al, 28Si(18O, X), 27Al(20Ne, X), 32S(24Mg, X), 40Ca(40Ca, X), E not given; analyzed σ(fusion) data; deduced reaction mechanism. Statistical yrast line model, multi-step processes.
doi: 10.1016/0370-2693(83)91226-1
1983SZ03 Nucl.Phys. A404, 142 (1983) E.M.Szanto, A.Szanto De Toledo, H.V.Klapdor, G.Rosner, M.Schrader Yrast and High-Spin States in 22Ne NUCLEAR REACTIONS 11B(13C, d), 13C(11B, d), E(cm)=19 MeV; measured σ(θ). 22Ne deduced high-spin states. 24Na deduced critical angular momentum. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(83)90419-0
1982CO25 Phys.Lett. 118B, 303 (1982) T.M.Cormier, A.Szanto De Toledo, M.M.Coimbra, N.Carlin Filho, P.Stwertka, M.Herman, N.Nicolis The Validity of the Compound Nucleus Mechanism in the 12C(16O, α) Reaction at High Energies NUCLEAR REACTIONS 12C(16O, α), E=40-150 MeV; measured σ(θ) vs E; deduced reaction mechanism. Compound nucleus model, Hauser-Feshbach analysis.
doi: 10.1016/0370-2693(82)90189-7
1982ST11 Phys.Rev.Lett. 49, 640 (1982) P.M.Stwertka, T.M.Cormier, M.Herman, N.Nicolis, A.Szanto de Toledo, M.M.Coimbra, N.Carlin Filho Kinematics of the Gross Structures in the α Spectrum of the 16O + 12C Reaction NUCLEAR REACTIONS 12C(16O, α), E=94-150 MeV; measured σ(Eα) vs E; deduced reaction mechanism. 24Mg deduced narrow, closely spaced levels. Kinematic analysis, inclusive reactions.
doi: 10.1103/PhysRevLett.49.640
1981HU10 Phys.Lett. 107B, 173 (1981) M.S.Hussein, A.Szanto De Toledo Statistical Windows in Angular Momentum Space: The basis of the heavy-ion compound cross section NUCLEAR REACTIONS 12C(16O, α), E(cm)=20 MeV; calculated σ(θ) vs final state spin; deduced statistical window effects.
doi: 10.1016/0370-2693(81)90806-6
1981SZ03 Phys.Rev.Lett. 46, 985 (1981) A.Szanto de Toledo, M.S.Hussein Low-Angular-Momentum Cutoff in Statistical Heavy-Ion Processes NUCLEAR REACTIONS 12C(16O, α), E(cm)=30 MeV; calculated σ(θ), cross correlation function vs θ; deduced fusion L mininum. Statistical theory.
doi: 10.1103/PhysRevLett.46.985
1981SZ05 Phys.Rev.Lett. 47, 632 (1981) A.Szanto de Toledo, M.M.Coimbra, N.Carlin Filho, T.M.Cormier, P.M.Stwertka Interpretation of Gross Structures in the Energy Spectra of the Reaction 12C(16O, α)24Mg NUCLEAR REACTIONS 12C(16O, α), E=48.8, 54.2, 58.6, 55, 60, 65 MeV; measured σ(Eα, θ). 24Mg deduced yrast sequence. Si surface barrier detector telescopes.
doi: 10.1103/PhysRevLett.47.632
1981SZ06 Phys.Rev.Lett. 47, 1881 (1981) A.Szanto de Toledo, T.M.Cormier, M.Herman, B.Lin, P.M.Stwertka, M.M.Coimbra, N.C.Filho Limiting Angular Momenta for Light Heavy-Ion Fusion at High Energy NUCLEAR REACTIONS 12C(16O, α), E=28.5-100 MeV; measured σ(θ); deduced no low-L cut off. Legendre polynomial analysis.
doi: 10.1103/PhysRevLett.47.1881
1981SZ07 Fizika(Zagreb) 13, Suppl.No.1, 29 (1981) A.Szanto de Toledo, M.M.Coimbra, N.C.Filho, T.M.Cormier, P.M.Stwertka An Interpretation of Gross Structures in the Energy Spectra of the 12C(16O, α)24Mg Reactions NUCLEAR REACTIONS 12C(16O, α), E=48.8, 54.2, 58.6, 55, 65 MeV; measured σ(θ), σ(Eα); deduced broad structures, angular momentum matching. 24Mg deduced selective yrast cluster population.
1979SC03 Z.Phys. A289, 193 (1979) M.Schrader, A.Szanto de Toledo, H.V.Klapdor A New Possibility of Identifying High-Spin States at High Excitation Energies NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; calculated probability of identifying high-spin states. Spin-dependent anisotropy of σ(θ) predicted by statistical model.
doi: 10.1007/BF01435937
1979SZ01 Phys.Rev.Lett. 42, 622 (1979) E.M.Szanto, A.Szanto de Toledo, H.V.Klapdor, M.Diebel, J.Fleckner, U.Mosel Backbending in 22Ne NUCLEAR REACTIONS 11B(13C, d), 13C(11B, d), E(cm)=19 MeV; measured σ(θ). 22Ne deduced levels, J, π, backbending. Strutinsky interpretation of rotational motion.
doi: 10.1103/PhysRevLett.42.622
1979SZ03 Phys.Rev. C19, 555 (1979) A.Szanto de Toledo, M.Schrader, E.M.Szanto, H.V.Klapdor Effect of the Critical Angular Momentum on the High Spin Selectivity of Heavy-Ion Compound Reactions NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; calculated σ(θ), σ(J); deduced σ(90°) is favored, useful for high spin spectroscopy. Statistical model.
doi: 10.1103/PhysRevC.19.555
1979SZ04 Nucl.Phys. A315, 500 (1979) A.Szanto de Toledo, M.Schrader, E.M.Szanto, G.Rosner, H.V.Klapdor High-Spin States in 24Mg and Upper Limits for Particle Spectroscopy of High Spins by Heavy-Ion Compound Reactions NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; measured σ(θ). 24Mg deduced high-spin states, critical angular momentum. Hauser-Feshbach analysis.
doi: 10.1016/0375-9474(79)90626-2
1979SZ05 Nucl.Phys. A320, 309 (1979) A.Szanto de Toledo, H.Hafner, H.V.Klapdor A Comparative Study of Proton States in 121,123,125,127,129,131I Excited by (α, t) and (3He, d) Reactions NUCLEAR REACTIONS 120,122,124,126,128,130Te(3He, d), 124,126,128,130Te(α, t), E=36 MeV; measured σ(Ed, θ), σ(Et, θ). 121,123,125,127,129,131I levels deduced L, J, π, relative S. DWBA analysis. Three-particle-cluster-phonon coupling model calculations for 121I.
doi: 10.1016/0375-9474(79)90192-1
1978SZ04 Phys.Rev. C17, 2253 (1978) A.Szanto de Toledo, H.V.Klapdor, H.Hafner, W.Saathoff, E.M.Szanto, M.Schrader Masses of 121,123,125I and Energy Levels of the Highly Neutron-Deficient 121I NUCLEAR REACTIONS 120,122,124Te(3He, d), E=36 MeV; measured σ(Ed, θ); deduced Q. 120,122,124,126,128,130Te(α, t), 126,128,130Te(3He, d), E=36 MeV; measured σ. 121I deduced mass excess, levels. 123,125I deduced mass excess.
doi: 10.1103/PhysRevC.17.2253
1978SZ09 J.Phys.(London) G4, L187 (1978) A.Szanto de Toledo, H.V.Klapdor, H.Hafner, W.Saathoff, E.M.Szanto, M.Schrader, H.Dias Structure of the Neutron-Deficient Nuclide 121I NUCLEAR REACTIONS 120Te(3He, d), E=36 MeV; measured σ(Ed, θ); deduced Q. 121I deduced mass excess, levels, L, J, π, S. DWBA analysis.
doi: 10.1088/0305-4616/4/7/007
1978SZ10 Phys.Lett. 78B, 58 (1978) A.Szanto de Toledo, M.Schrader, G.Rosner, E.M.Szanto, H.V.Klapdor Yrast States in 24Mg up to 24 MeV Excitation Energy NUCLEAR REACTIONS 10B(16O, d), E=60 MeV; measured σ(Ed, θ). 24Mg deduced levels, J, π.
doi: 10.1016/0370-2693(78)90347-7
1977SZ01 Phys.Rev. C15, 238 (1977) A.Szanto de Toledo, M.N.Rao, N.Ueta, O.Sala Levels in 123I and 125I from (3He, d) Reactions NUCLEAR REACTIONS 124Te(3He, d), E=19.5 MeV; measured σ(Ed, θ). 122Te(3He, d), E=19 MeV; measured σ(Ed, θ); deduced Q. 123I deduced mass excess. 123,125I deduced levels, L, J, π, S. DWBA analysis, enriched targets.
doi: 10.1103/PhysRevC.15.238
1977SZ04 Phys.Rev. C16, 438 (1977) A.Szanto de Toledo, M.N.Rao, O.Sala Semimicroscopic Description of the Odd Iodine Nuclei in the Mass Region 123 ≤ A ≤ 133 NUCLEAR STRUCTURE 123,125,127,129,131,133I; calculated levels, J, π, B(E2), B(M1), quadrupole moment, μ, S. Alaga model. Pairing, surface delta interaction.
doi: 10.1103/PhysRevC.16.438
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