NSR Query Results
Output year order : Descending NSR database version of May 3, 2024. Search: Author = C.Tenreiro Found 25 matches. 2014KH01 J.Radioanal.Nucl.Chem. 299, 303 (2014) A.Khorshidi, M.Sadeghi, A.Pazirandeh, C.Tenreiro, Y.Kadi Radioanalytical prediction of radiative capture in 99Mo production via transmutation adiabatic resonance crossing by cyclotron NUCLEAR REACTIONS 9Be, 181Ta, 184W(p, xn), E=30 MeV; 98Mo(n, γ), E<30 MeV; calculated En, In, radiative capture yield of 99Mo; Transmutation Adiabatic Resonance Crossing (TARC) method.
doi: 10.1007/s10967-013-2749-7
2013MA36 Ann.Nucl.Energy 57, 195 (2013) M.Mahmodi, M.Sadeghi, C.Tenreiro Prediction of palladium-103 production using the Monte Carlo code MCNPX NUCLEAR REACTIONS 103Rh(p, n), E<40 MeV; calculated σ, yield. MCNPX calculations, comparison with available data.
doi: 10.1016/j.anucene.2013.02.009
2013SA24 Appl.Radiat.Isot. 77, 14 (2013) M.Sadeghi, N.Jokar, T.Kakavand, H.Ghafoori-Fard, C.Tenreiro Prediction of 67Ga production using the Monte Carlo code MCNPX NUCLEAR REACTIONS 68Zn(p, 2n), Zn(p, xn)67Ga, 67Zn(p, n), E = 15-30 MeV; calculated production yield. MCNPX code, comparison with experimental results.
doi: 10.1016/j.apradiso.2013.02.001
2013SA53 Appl.Radiat.Isot. 82, 347 (2013) M.Sadeghi, N.Hashemi, H.Afarideh, C.Tenreiro Prediction of 94mTc production for positron emission tomography studies using the Monte Carlo code MCNPX-2.6 NUCLEAR REACTIONS 94Mo(p, xn)93Tc/94Tc, E=15 MeV; measured reaction products; deduced isomeric σ. calculated isomeric σ using MCNPX, TALYS nuclear model codes.
doi: 10.1016/j.apradiso.2013.09.010
2011SA54 J.Korean Phys.Soc. 59, 1111s (2011) Sang In Bak, R.Brun, Fe.Carminati, J.S.Chai, A.Gheata, M.Gheata, S.-W.Hong, Y.Kadi, V.Manchanda, T.-S.Park, C.Tenreiro A New Format for Handling Nuclear Data
doi: 10.3938/jkps.59.1111
2008SA20 Radiochim.Acta 96, 399 (2008) M.Sadeghi, M.Amiri, P.Roshanfarzad, M.Avila, C.Tenreiro Radiochemical studies relevant to the no-carrier-added production of 61, 64Cu at a cyclotron NUCLEAR REACTIONS Ni(p, n)64Cu, E=15, 16 MeV; measured Eγ, Iγ using chemical separation. 64Cu; deduced yield.
doi: 10.1524/ract.2008.1504
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
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
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
1995ES04 Phys.Rev. C52, 104 (1995) F.R.Espinoza-Quinones, E.W.Cybulska, L.G.R.Emediato, C.L.Lima, N.H.Medina, J.R.B.Oliveira, M.N.Rao, R.V.Ribas, M.A.Rizzutto, W.A.Seale, C.Tenreiro Band Structures in 108Ag NUCLEAR REACTIONS 100Mo(11B, 3n), E=39 MeV; measured Eγ, Iγ, Iγ(θ), γγ-coin, γγ(t), DCO, quadrupole transitions. 108Ag deduced levels, J, π, γ multipolarity, band structure, B(λ) ratios. Total Routhian surface calculations.
doi: 10.1103/PhysRevC.52.104
1995SM02 Nucl.Phys. A587, 150 (1995) A.G.Smith, R.Chapman, D.C.Clark, J.Copnell, S.J.Freeman, F.Khazaie, G.S.Li, J.C.Lisle, J.N.Mo, C.Tenreiro, D.M.Thompson, G.J.Yuan, J.Espino, G.B.Hagemann Electromagnetic Properties of 161Tm at High Spin NUCLEAR REACTIONS 128Te(37Cl, 4n), E=170 MeV; measured Eγ, γγ-coin, Iγ, DSA. 161Tm deduced high-spin levels, T1/2, B(M1), B(E2). Enriched targets, array of Compton-suppressed Ge detectors.
doi: 10.1016/0375-9474(94)00810-A
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
1994TE01 Phys.Rev. C49, 1218 (1994) C.Tenreiro, P.R.S.Gomes, T.J.P.Penna, R.Liguori Neto, J.C.Acquadro, P.A.B.Freitas, E.Crema Elastic Scattering and Fusion of 16O + 59Co at Near Barrier Energies: A signature for long range fusion potentials NUCLEAR REACTIONS, ICPND 59Co(16O, 16O), E=37-62 MeV; measured σ(θ). 59Co(16O, X), E=35-50 MeV; analyzed fusion σ(E); deduced fusion features. Optical potential.
doi: 10.1103/PhysRevC.49.1218
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
1993PA22 Phys.Rev. C48, 1573 (1993) A.A.Pakou, J.Billowes, A.W.Mountford, C.Tenreiro, D.D.Warner f7/2 Proton Alignment in 49Cr NUCLEAR REACTIONS 12C(40Ca, n2p), E=140 MeV; measured Eγ, Iγ(θ), recoil in thick polarized Gd foil. 49Cr level deduced g, T1/2. Cranked shell model analysis.
doi: 10.1103/PhysRevC.48.1573
1992CO25 J.Phys.(London) G18, 1943 (1992) J.Copnell, K.Kumar, S.J.Robinson, C.Tenreiro An Application of the Dynamic Deformation Model to the N = 84 Isotones 138Xe-146Sm NUCLEAR STRUCTURE 138Xe, 146Sm, 140Ba, 142Ce, 144Nd; calculated levels, B(λ), δ. Dynamic deformation model.
doi: 10.1088/0954-3899/18/12/010
1991GO20 Nucl.Phys. A534, 429 (1991) P.R.S.Gomes, T.J.P.Penna, E.F.Chagas, R.Liguori Neto, J.C.Acquadro, P.R.Pascholati, E.Crema, C.Tenreiro, N.Carlin Filho, M.M.Coimbra Fusion of 59Co with Light Projectiles at Near Barrier Energies NUCLEAR REACTIONS, ICPND 59Co(14N, xnypzα), (16O, xnypzα), E=32-56 MeV; measured fusion σ(E), σ(elastic)/σ(Rutherford).
doi: 10.1016/0375-9474(91)90510-D
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
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. 1989GO15 Nucl.Instrum.Methods Phys.Res. A280, 395 (1989) P.R.S.Gomes, T.J.P.Penna, R.Liguori Neto, J.C.Acquadro, C.Tenreiro, P.A.B.Freitas, E.Crema, N.Carlin Filho, M.M.Coimbra Nuclear Fusion between Heavy Ions by the Gamma-Ray Spectroscopy Method NUCLEAR REACTIONS, ICPND 46Ti(16O, X), E(cm) ≈ 20-35 MeV; 50Ti(16O, X), E(cm) ≈ 20-50 MeV; 64,66Zn(16O, X), E=30-65 MeV; 59Co(16O, X), E(cm) ≈ 27.5-55 MeV; 59Co(14N, X), E ≈ 30-60 MeV; measured fusion σ(E). 59Co(14N, 2n2p), E=threshold-60 MeV; measured σ(E). 59Co(14N, xnypzα), E=32-56 MeV; measured σ(E).
doi: 10.1016/0168-9002(89)90940-6
1989PE03 Phys.Lett. 220B, 347 (1989) D.Pereira, G.Ramirez, O.Sala, L.C.Chamon, C.A.Rocha, J.C.Acquadro, C.Tenreiro Effect of the Threshold Anomaly on the Fusion Cross Sections for the Systems 16O + 63,65Cu NUCLEAR REACTIONS, ICPND 63,65Cu(16O, X), E=40-72 MeV; measured evaporation residue σ(E). 63,65Cu(16O, 16O), E=46 MeV; measured σ(θ); deduced optical model parameters, threshold anomaly role.
doi: 10.1016/0370-2693(89)90885-X
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