NSR Query Results
Output year order : Descending NSR database version of May 1, 2024. Search: Author = C.Muri Found 13 matches. 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
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
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
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
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
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