NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = R.M.Anjos Found 46 matches. 2007AN22 Nucl.Phys. A787, 642c (2007) R.M.Anjos, R.Veiga, C.Carvalho, K.D.Macario, P.R.S.Gomes Geological provenance of Quaternary deposits from the southeastern Brazilian coast
doi: 10.1016/j.nuclphysa.2006.12.075
2007GA39 Phys.Rev. C 76, 024612 (2007) L.R.Gasques, M.Evers, D.J.Hinde, M.Dasgupta, P.R.S.Gomes, R.M.Anjos, M.L.Brown, M.D.Rodriguez, R.G.Thomas, K.Hagino Systematic study of the nuclear potential through high precision back-angle quasi-elastic scattering measurements NUCLEAR REACTIONS 170Er, 186W, 197Au, 208Pb(32S, X), E=90-155 MeV; measured quasi-elastic scattering excitation functions. Compared results to single and coupled channel calculations.
doi: 10.1103/PhysRevC.76.024612
2006GO10 Phys.Lett. B 634, 356 (2006) P.R.S.Gomes, I.Padron, E.Crema, O.A.Capurro, J.O.Fernandez Niello, G.V.Marti, A.Arazi, M.Trotta, J.Lubian, M.E.Ortega, A.J.Pacheco, M.D.Rodriguez, J.E.Testoni, R.M.Anjos, L.C.Chamon, M.Dasgupta, D.J.Hinde, K.Hagino Disentangling the reaction mechanism of weakly bound nuclei NUCLEAR REACTIONS 9Be(144Sm, X), E=30-44 MeV; measured delayed Eγ, Iγ; deduced total-, complete-, incomplete-fusion and inelastic σ, total fusion suppression factor, reaction mechanism. Comparison with coupled-channels model calculations.
doi: 10.1016/j.physletb.2006.02.005
2006GO19 Phys.Rev. C 73, 064606 (2006) P.R.S.Gomes, I.Padron, E.Crema, O.A.Capurro, J.O.Fernandez Niello, A.Arazi, G.V.Marti, J.Lubian, M.Trotta, A.J.Pacheco, J.E.Testoni, M.D.Rodriguez, M.E.Ortega, L.C.Chamon, R.M.Anjos, R.Veiga, M.Dasgupta, D.J.Hinde, K.Hagino Comprehensive study of reaction mechanisms for the 9Be + 144Sm system at near- and sub-barrier energies NUCLEAR REACTIONS 144Sm(9Be, 9Be), E=33-41 MeV; measured elastic σ(θ). 144Sm(9Be, n), (9Be, 2n), (9Be, 3n), (9Be, 4n), (9Be, np), (9Be, 2np), E=30-44 MeV; 144Sm(9Be, X)147Gd, E=3-44 MeV; measured σ; deduced complete and incomplete fusion σ, reaction σ. Delayed x-ray detection technique, comparison with model predictions.
doi: 10.1103/PhysRevC.73.064606
2006PE26 Phys.Rev. C 74, 034608 (2006) D.Pereira, E.S.Rossi, Jr., G.P.A.Nobre, L.C.Chamon, C.P.Silva, L.R.Gasques, M.A.G.Alvarez, R.V.Ribas, J.R.B.Oliveira, N.H.Medina, M.N.Rao, E.W.Cybulska, W.A.Seale, N.Carlin, P.R.S.Gomes, J.Lubian, R.M.Anjos 18O+110Pd: Measurements and realistic coupled-channel analysis in a transitional region NUCLEAR REACTIONS 110Pd(18O, 18O'), (18O, 16O), (18O, 14C), E=40-58 MeV; measured Eγ, Iγ, (particle)γ-coin; deduced excitation functions. Coupled-channels analysis.
doi: 10.1103/PhysRevC.74.034608
2005AL03 Nucl.Phys. A748, 59 (2005) J.J.S.Alves, P.R.S.Gomes, J.Lubian, L.C.Chamon, D.Pereira, R.M.Anjos, E.S.Rossi, Jr., C.P.Silva, M.A.G.Alvarez, G.P.A.Nobre, L.R.Gasques Consistent analysis of peripheral reaction channels and fusion for the 16, 18O + 58Ni systems NUCLEAR REACTIONS 58Ni(16O, 16O), (16O, 16O'), (16O, 12C), E=46 MeV; 58Ni(18O, 18O), (18O, 18O'), (18O, 17O), (18O, 16O), E=46 MeV; measured elastic, inelastic, and transfer σ(E, θ). Coupled-channels analysis, comparison with previous results.
doi: 10.1016/j.nuclphysa.2004.10.020
2005AL45 Braz.J.Phys. 35, 909 (2005) J.J.S.Alves, P.R.S.Gomes, J.Lubian, L.C.Chamon, R.M.Anjos, D.Pereira, E.S.Rossi, Jr., C.P.Silva, M.A.G.Alvarez, G.P.A.Nobre, L.R.Gasques Elastic, Inelastic Scatterings and Transfer Reactions for 16, 18O on 58Ni Described by the Sao Paulo Potential NUCLEAR REACTIONS 58Ni(16O, 16O), (16O, 16O'), (16O, X), (18O, 18O), (18O, 18O'), (18O, X), E=46 MeV; measured elastic, inelastic, and transfer σ(θ). Comparison with model predictions.
doi: 10.1590/S0103-97332005000500052
2005GO01 Phys.Rev. C 71, 017601 (2005) P.R.S.Gomes, J.Lubian, I.Padron, R.M.Anjos Uncertainties in the comparison of fusion and reaction cross sections of different systems involving weakly bound nuclei NUCLEAR REACTIONS 64Zn(α, X), (6He, X), (6Li, X), (7Li, X), (9Be, X), (16O, X), E(cm) ≈ 10-30 MeV; analyzed fusion σ.
doi: 10.1103/PhysRevC.71.017601
2005GO09 Phys.Rev. C 71, 034608 (2005) P.R.S.Gomes, M.D.Rodriguez, G.V.Marti, I.Padron, L.C.Chamon, J.O.Fernandez Niello, O.A.Capurro, A.J.Pacheco, J.E.Testoni, A.Arazi, M.Ramirez, R.M.Anjos, J.Lubian, R.Veiga, R.Liguori Neto, E.Crema, N.Added, C.Tenreiro, M.S.Hussein Effect of the breakup on the fusion and elastic scattering of weakly bound projectiles on 64Zn NUCLEAR REACTIONS 64Zn(6Li, X), (7Li, X), (9Be, X), (16O, X), E ≈ 16-69 MeV; measured fusion and reaction σ; deduced reaction mechanism features. 64Zn(9Be, 9Be), E=17-28 MeV; 64Zn(16O, 16O), E=40-64 MeV; measured elastic σ(θ). Coupled channels analysis.
doi: 10.1103/PhysRevC.71.034608
2005GO35 J.Phys.(London) G31, S1669 (2005) P.R.S.Gomes, I.Padron, J.O.Fernandez Niello, G.V.Marti, M.D.Rodriguez, O.A.Capurro, A.J.Pacheco, J.E.Testoni, A.Arazi, J.Lubian, R.M.Anjos, L.C.Chamon, E.Crema, M.S.Hussein Fusion, break-up and elastic scattering of weakly bound nuclei NUCLEAR REACTIONS 27Al, 64Zn(9Be, X), E(cm) ≈ 14-25 MeV; 64Zn(6Li, X), E(cm) ≈ 15-40 MeV; measured reaction, break-up, and fusion σ; deduced optical potential features.
doi: 10.1088/0954-3899/31/10/051
2005GO42 Braz.J.Phys. 35, 902 (2005) P.R.S.Gomes, I.Padron, O.A.Capurro, J.O.Fernandez Niello, G.V.Marti, R.M.Anjos, J.Lubian, R.Veiga, E.Crema, A.J.Pacheco, J.E.Testoni, A.Arazi, M.D.RodrIguez, ME.Ortega, M.Trotta Complete Fusion of Weakly Bound Nuclei Applying the Delayed X-Ray Technique: the 9Be + 144Sm System NUCLEAR REACTIONS 144Sm(9Be, X), E ≈ 30-45 MeV; measured delayed X-ray spectra; deduced fusion σ.
2005MA09 Phys.Rev. C 71, 027602 (2005) G.V.Marti, P.R.S.Gomes, M.D.Rodriguez, J.O.Fernandez Niello, O.A.Capurro, A.J.Pacheco, J.E.Testoni, M.Ramirez, A.Arazi, I.Padron, R.M.Anjos, J.Lubian, E.Crema Fusion, reaction, and breakup cross sections of 9Be on a light mass target NUCLEAR REACTIONS 27Al(9Be, X), E=12-24 MeV; measured fusion σ; deduced reaction and breakup σ.
doi: 10.1103/PhysRevC.71.027602
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
2004GO21 Nucl.Phys. A734, 233 (2004) P.R.S.Gomes, J.Lubian, R.M.Anjos How does the break-up of weakly bound nuclei influence the fusion cross section? NUCLEAR REACTIONS 209Bi(6Li, X), E(cm)=25-50 MeV; 64Zn(6Li, X), (7Li, X), (9Be, X), (16O, X), E(cm)=10-40 MeV; analyzed fusion σ, break-up channel effects.
doi: 10.1016/j.nuclphysa.2004.01.042
2004GO43 Prog.Theor.Phys.(Kyoto), Suppl. 154, 92 (2004) P.R.S.Gomes, R.M.Anjos, J.Lubian The Fusion of Stable Weakly Bound Nuclei
2004GO47 Phys.Lett. B 601, 20 (2004) P.R.S.Gomes, I.Padron, M.D.Rodriguez, G.V.Marti, R.M.Anjos, J.Lubian, R.Veiga, R.Liguori Neto, E.Crema, N.Added, L.C.Chamon, J.O.Fernandez Niello, O.A.Capurro, A.J.Pacheco, J.E.Testoni, D.Abriola, A.Arazi, M.Ramirez, M.S.Hussein Fusion, reaction and break-up cross sections of weakly bound projectiles on 64Zn NUCLEAR REACTIONS 64Zn(16O, X), E(cm) ≈ 32-55 MeV; 64Zn(9Be, X), E(cm) ≈ 14-25 MeV; 64Zn(6Li, X), (7Li, X), E(cm) ≈ 14-40 MeV; 64Zn(6He, X), E(cm) ≈ 7-13 MeV; measured fusion, reaction, and breakup σ. Comparison with previous results.
doi: 10.1016/j.physletb.2004.09.029
2004GO49 Phys.Rev. C 70, 054605 (2004) P.R.S.Gomes, R.M.Anjos, C.Muri, J.Lubian, I.Padron, L.C.Chamon, R.Liguori Neto, N.Added, J.O.Fernandez Niello, G.V.Marti, O.A.Capurro, A.J.Pacheco, J.E.Testoni, D.Abriola Threshold anomaly with weakly bound projectiles: Elastic scattering of 9Be + 27Al NUCLEAR REACTIONS 27Al(9Be, 9Be), E=12-47.5 MeV; measured σ(θ); deduced model parameters, no threshold anomaly.
doi: 10.1103/PhysRevC.70.054605
2004GO60 Braz.J.Phys. 34, 737 (2004) P.R.S.Gomes, R.M.Anjos, J.Lubian Does the Break-up Process Influence the Fusion Cross Section? NUCLEAR REACTIONS 209Bi(6Li, X), (7Li, X), E(cm) ≈ 25-50 MeV; 208Pb(9Be, X), E(cm) ≈ 35-50 MeV; analyzed fusion σ, projectile break-up effects.
doi: 10.1590/s0103-97332004000500008
2004RO49 Braz.J.Phys. 34, 869 (2004) M.D.Rodriguez, I.Padron, G.V.Marti, R.M.Anjos, P.R.S.Gomes, J.Lubian, R.S.L.Veiga, A.J.Pacheco, O.A.Capurro, J.O.Fernandez Niello, J.E.Testoni, A.Arazi, M.Ramirez Fusion Cross Section Measurements for Systems 6Li + 27Al, 64Zn at Near-Barrier Energies NUCLEAR REACTIONS 27Al, 64Zn(6Li, X), E=14-24 MeV; 64Zn(9Be, X), E=20-24 MeV; measured fusion σ. Comparison with previous results.
2003LU18 Braz.J.Phys. 33, 323 (2003) J.Lubian, P.R.S.Gomes, R.M.Anjos, I.Padron, C.Muri, S.B.Moraes, J.J.S.Alves, A.M.M.Maciel, R.Liguori Neto, N.Added, G.V.Marti, M.Ramirez, A.J.Pacheco, O.A.Capurro, J.O.Fernandez Niello, J.E.Testoni, D.Abriola, M.R.Spinella Influence of the Break-up on the Fusion and Scattering Processes NUCLEAR REACTIONS 27Al(6Li, X), (7Li, X), (9Be, X), (11B, X), (16O, X), E(cm) ≈ 10-40 MeV; 64Zn(6Li, X), (7Li, X), (9Be, X), (16O, X), E(cm) ≈ 15-40 MeV; analyzed fusion σ, role of break-up process.
doi: 10.1590/s0103-97332003000200032
2002AL01 Phys.Rev. C65, 014602 (2002) M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, L.R.Gasques, L.C.Chamon, D.Pereira, M.N.Rao, B.V.Carlson, C.De Conti, R.M.Anjos, P.R.S.Gomes, J.Lubian, S.Kailas, A.Chatterjee, P.Singh Precise Nuclear Matter Densities from Heavy-Ion Collisions NUCLEAR REACTIONS 16O(16O, 16O), E=1120 MeV; 92Mo(16O, 16O), E=49 MeV; 58,60,62,64Ni, 88Sr, 90,92Zr, 120Sn, 138Ba, 208Pb(16O, 16O), E not given; 58,60Ni(18O, 18O), E not given; analyzed σ. 16,18O deduced matter density distributions, related features. 16O, 58Ni(e, e), E not given; calculated σ vs momentum transfer.
doi: 10.1103/PhysRevC.65.014602
2002AN11 Phys.Lett. 534B, 45 (2002) R.M.Anjos, C.Muri, J.Lubian, P.R.S.Gomes, I.Padron, J.J.S.Alves, G.V.Marti, J.O.Fernandez Niello, A.J.Pacheco, O.A.Capurro, D.Abriola, J.E.Testoni, M.Ramirez, R.Liguori Neto, N.Added No Evidence of Break-Up Effects on the Fusion of 9Be with Medium-Light Nuclei NUCLEAR REACTIONS 27Al(9Be, X), E=33-55 MeV; 27Al(9Be, 9Be), E=12-35 MeV; 9Be, 12C(19F, X), (19F, 19F), E=48-72 MeV; measured fusion and elastic scattering σ, angular distributions; deduced no fusion hindrance due to break-up contribution. One-dimensional barrier penetration model. Other data compared.
doi: 10.1016/S0370-2693(02)01554-X
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
2002PA46 Phys.Rev. C66, 044608 (2002) I.Padron, P.R.S.Gomes, R.M.Anjos, J.Lubian, C.Muri, J.J.S.Alves, G.V.Marti, M.Ramirez, A.J.Pacheco, O.A.Capurro, J.O.Fernandez Niello, J.E.Testoni, D.Abriola, M.R.Spinella Fusion of stable weakly bound nuclei with 27Al and 64Zn NUCLEAR REACTIONS 27Al, 64Zn(6Li, X), (7Li, X), E=24-43 MeV; measured fusion σ; deduced no fusion hindrance from projectile breakup. Other reactions analyzed.
doi: 10.1103/PhysRevC.66.044608
2001LU08 Phys.Rev. C64, 027601 (2001) J.Lubian, I.Padron, P.R.S.Gomes, A.M.M.Maciel, R.M.Anjos, S.B.Moraes, J.J.S.Alves, C.Muri, R.Liguori Neto, N.Added Low-Lying Inelastic Channel Couplings versus Breakup Effects on the Fusion Cross Section NUCLEAR REACTIONS 138Ba(6Li, 6Li'), (7Li, 7Li'), 64Zn(9Be, 9Be'), E ≈ 20-30 MeV; analyzed data; deduced reaction mechanism features. Coupled channels analysis.
doi: 10.1103/PhysRevC.64.027601
2001SI02 Nucl.Phys. A679, 287 (2001) C.P.Silva, M.A.G.Alvarez, L.C.Chamon, D.Pereira, M.N.Rao, E.S.Rossi, Jr., L.R.Gasques, M.A.E.Santo, R.M.Anjos, J.Lubian, P.R.S.Gomes, C.Muri, B.V.Carlson, S.Kailas, A.Chatterjee, P.Singh, A.Shrivastava, K.Mahata, S.Santra The Heavy-Ion Nuclear Potential: Determination of a systematic behavior at the region of surface interaction distances NUCLEAR REACTIONS 120Sn(16O, 16O), E=53-55 MeV; 138Ba(16O, 16O), E=54-57 MeV; 208Pb(16O, 16O), E=74-78 MeV; measured σ(θ); deduced optical potentials. Double-folding calculations with microscopic densities.
doi: 10.1016/S0375-9474(00)00347-X
2000GO50 Acta Phys.Hung.N.S. 11, 361 (2000) P.R.S.Gomes, S.B.Moraes, J.J.S.Alves, A.M.M.Maciel, R.M.Anjos, J.Lubian, C.Muri, M.M.Sant'Anna, I.Padron, R.Cabezas, R.Liguori Neto, N.Added Investigation of the Role of the Breakup Process on the Fusion and Scattering of Weakly Bound Projectile Induced Reactions NUCLEAR REACTIONS 138Ba(6Li, 6Li), (7Li, 7Li), E=21-32 MeV; 64Zn(9Be, 9Be), E=17-28 MeV; measured σ(θ), optical model dispersion relation following coupled channel calculations. 64Zn(9Be, X), E=21-29 MeV; measured Eγ, fusion σ. Comparison with other targets, projectile breakup effects discussed.
2000MO15 Phys.Rev. C61, 064608 (2000) S.B.Moraes, P.R.S.Gomes, J.Lubian, J.J.S.Alves, R.M.Anjos, M.M.Sant'Anna, I.Padron, C.Muri, R.Liguori Neto, N.Added Fusion and Elastic Scattering of 9Be + 64Zn: A search of the breakup influence on these processes NUCLEAR REACTIONS 64Zn(9Be, xnypzα), E=21, 23, 26, 29 MeV; measured Eγ, Iγ, fusion σ; 64Zn(9Be, 9Be), E=17-28 MeV; measured σ(θ); deduced role of projectile breakup.
doi: 10.1103/PhysRevC.61.064608
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
1999MA16 Phys.Rev. C59, 2103 (1999) A.M.M.Maciel, P.R.S.Gomes, J.Lubian, R.M.Anjos, R.Cabezas, G.M.Santos, C.Muri, S.B.Moraes, R.Liguori Neto, N.Added, N.Carlin Filho, C.Tenreiro Influence of the 6, 7Li Breakup Process on the Near Barrier Elastic Scattering by Heavy Nuclei NUCLEAR REACTIONS 138Ba(6Li, 6Li), (7Li, 7Li), E=21-32 MeV; measured σ(θ); deduced optical model parameters, breakup channel role, other reaction mechanism features.
doi: 10.1103/PhysRevC.59.2103
1998MU04 Eur.Phys.J. A 1, 143 (1998) C.Muri, R.M.Anjos, R.Cabezas, P.R.S.Gomes, S.B.Moraes, A.M.M.Maciel, G.M.Santos, J.Lubian, M.M.Sant'Anna, C.Tenreiro, R.Liguori Neto, J.C.Acquadro, P.A.B.Freitas Elastic, Inelastic Scattering and Fusion of the 14N + 59Co System at Energies Close to the Coulomb Barrier NUCLEAR REACTIONS 59Co(14N, 14N), (14N, 14N'), E=30-55 MeV; measured elastic, inelastic σ(θ); deduced optical model parameters. 59Co(14N, X), E(cm) ≈ 25-45 MeV; analyzed fusion σ. Coupled channels calculations.
doi: 10.1007/s100500050044
1998ZE06 Phys.Rev. C58, 3445 (1998) A.Zerwekh, R.Liguori Neto, N.Added, J.C.Acquadro, N.Carlin, M.Frizzarini, F.Malandrino, J.Lubian, R.Cabezas, P.R.S.Gomes, R.M.Anjos, G.M.Santos, A.M.M.Maciel, C.Muri, S.B.Moraes, G.Ramirez, C.Tenreiro Elastic Scattering of 27Al + 27Al at Near Barrier Energies NUCLEAR REACTIONS 27Al(27Al, 27Al), (27Al, 27Al'), E=50-70 MeV; measured σ(θ), integrated σ; deduced optical model parameters.
doi: 10.1103/PhysRevC.58.3445
1997AN17 J.Phys.(London) G23, 1423 (1997) R.M.Anjos, C.Muri, S.B.Moraes, R.Cabezas, P.R.S.Gomes, C.Tenreiro, R.Liguori Neto, A.M.M.Maciel, G.M.Santos Can Fusion, Elastic and Inelastic Scattering of Heavy Ions be Understood, Without a Simultaneous Analysis of Them ( Question ) NUCLEAR REACTIONS, ICPND 59Co(14N, 14N), E=30-55 MeV; analyzed σ(θ); 59Co(14N, 14N'), E=30-34 MeV; analyzed σ(θ) for excitation of target first excited state; 59Co(14N, X), E(cm)=25-45 MeV; analyzed fusion σ; deduced importance of simultaneous analysis. Optical, coupled-channels models.
doi: 10.1088/0954-3899/23/10/032
1997GO22 J.Phys.(London) G23, 1315 (1997) P.R.S.Gomes, A.M.M.Maciel, R.M.Anjos, S.B.Moraes, R.Liguori Neto, R.Cabezas, C.Muri, G.M.Santos, J.F.Liang Transfer Reactions as a Doorway to Fusion NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E=66 MeV; analyzed one-alpha, two-proton transfer σ(θ); 100Mo(32S, X), E=116 MeV; analyzed one-, two-nucleon transfer σ(θ); 100Mo(32S, X), E(cm)=72-92 MeV; analyzed fusion σ; deduced transfer channels fusion role.
doi: 10.1088/0954-3899/23/10/020
1996TE02 Phys.Rev. C53, 2870 (1996) C.Tenreiro, J.C.Acquadro, P.A.B.Freitas, R.Liguori Neto, G.Ramirez, N.Cuevas, P.R.S.Gomes, R.Cabezas, R.M.Anjos, J.Copnell Elastic amd Inelastic Scattering of 16O + 64Zn at Near-Barrier Energies NUCLEAR REACTIONS 64Zn(16O, 16O), (16O, 16O'), E(cm)=41.6-51.2 MeV; measured σ(θ); deduced model parameters. Optical, coupled-channels models.
doi: 10.1103/PhysRevC.53.2870
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
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
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
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
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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