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NSR database version of April 11, 2024.

Search: Author = E.M.Szanto

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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0648.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0618.

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0564.

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0442.

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0427.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0520.

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0407.

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
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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
Citations: PlumX Metrics
Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0407.

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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0410.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0415.

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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