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NSR database version of April 11, 2024.

Search: Author = A.Szanto De Toledo

Found 99 matches.

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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 dataset31824. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0837.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1765. Data from this article have been entered in the XUNDL database. For more information, click here.


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1973.


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


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1973.


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
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.


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1639.


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


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
Citations: PlumX Metrics


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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetA0719.


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.


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
Citations: PlumX Metrics


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
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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
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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
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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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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
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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
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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
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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.


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
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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
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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
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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
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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
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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
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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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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
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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
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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
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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
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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
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1996BE14      Phys.Rev. C53, 1989 (1996)

C.Beck, A.Szanto de Toledo

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


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
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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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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
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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
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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
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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
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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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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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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
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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
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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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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
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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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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
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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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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
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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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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetC0219.


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
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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
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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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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
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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
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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
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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
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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
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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
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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
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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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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
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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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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
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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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