NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = D.Pereira Found 41 matches. 2013OL04 J.Phys.(London) G40, 105101 (2013) J.R.B.Oliveira, F.Cappuzzello, L.C.Chamon, D.Pereira, C.Agodi, M.Bondi, D.Carbone, M.Cavallaro, A.Cunsolo, M.De Napoli, A.Foti, L.R.Gasques, P.R.S.Gomes, R.Linares, J.Lubian, D.Nicolosi, S.Tropea Study of the rainbow-like pattern in the elastic scattering of 16O on 27Al at Elab. = 100 MeV NUCLEAR REACTIONS 27Al(16O, 16O), E=100 MeV; calculated σ, scattering parameters. Comparison with experimental data.
doi: 10.1088/0954-3899/40/10/105101
2011CA20 Nucl.Instrum.Methods Phys.Res. A648, 46 (2011) M.Cavallaro, F.Cappuzzello, D.Carbone, A.Cunsolo, A.Foti, R.Linares, D.Pereira, J.R.B.Oliveira, P.R.S.Gomes, J.Lubian, R.Chen Challenging measurement of the 16O+27Al elastic and inelastic angular distributions up to large angles NUCLEAR REACTIONS 27Al(16O, 16O), (16O, 16O'), E=100 MeV; measured reaction products; deduced σ(θ). MAGNEX quadrupole-dipole magnetic spectrometer.
doi: 10.1016/j.nima.2011.04.042
2010OL05 J.Phys.:Conf.Ser. 205, 012046 (2010) J.R.B.Oliveira, V.A.B.Zagatto, D.Pereira, J.Lubian, P.R.P.Allegro, L.C.Chamon, E.W.Cybulska, R.Linares, N.H.Medina, R.V.Ribas, E.S.Rossi, Jr, W.A.Seale, C.P.Silva, D.L.Toufen, M.A.G.Silveira, G.S.Zahn, F.A.Genezini, L.Gasques, J.M.B.Shorto Nuclear reaction studies with particle-gamma coincidences using the Saci-Perere spectrometer NUCLEAR REACTIONS 110Pd(18O, X), E=46-60 MeV; measured Eγ, Iγ, E(particle), I(particle, θ), (particle)γ-coin; deduced σ(θ) to 2+ states. Preliminary.
doi: 10.1088/1742-6596/205/1/012046
2010SO10 Nucl.Phys. A836, 1 (2010) D.P.Sousa, D.Pereira, J.Lubian, L.C.Chamon, J.R.B.Oliveira, E.S.Rossi, Jr., C.P.Silva, P.N.de Faria, V.Guimaraes, R.Lichtenthaler, M.A.G.Alvarez Probing the 6, 7Li nucleon densities through a new break-up process approach NUCLEAR REACTIONS 120Sn(6Li, X), E=19.5 MeV; 120Sn(7Li, X), E=19.5, 20.5, 25 MeV; measured elastic and quasi-elastic σ(θ) using silicon barrier detectors; deduced optical model parameters, sensitivity radius, nuclear densities and introduced new imaginery potential component.
doi: 10.1016/j.nuclphysa.2010.01.245
2009PE14 Nucl.Phys. A826, 211 (2009) D.Pereira, C.P.Silva, J.Lubian, E.S.Rossi, L.C.Chamon, G.P.A.Nobre, T.Correa Understanding fusion suppression and enhancement in the 18O + 58, 60, 64Ni systems NUCLEAR REACTIONS 58,60,64Ni(18O, 18O), (18O, 18O'), (18O, 16O), E=34.5-65 MeV; analyzed σ(θ), σ, fusion σ, B(E2) using coupled-channels analysis; deduced spectroscopic factors. Comparison with data.
doi: 10.1016/j.nuclphysa.2009.06.015
2008GA18 Nucl.Phys. A806, 146 (2008) A.R.Garcia, J.Lubian, P.R.S.Gomes, I.Padron, L.C.Chamon, D.Pereira Limitation of double folding potentials to simulate the polarization in reactions involving halo nuclei NUCLEAR REACTIONS 209Bi(6He, 6He), E(cm)=14.3, 15.8, 17.4, 18.6, 21.4 MeV; analyzed elastic σ(θ) and total σ using three different optical model potentials.
doi: 10.1016/j.nuclphysa.2008.03.004
2006PE02 Phys.Rev. C 73, 014601 (2006) D.Pereira, C.P.Silva, J.Lubian, E.S.Rossi, Jr., L.C.Chamon Reaction dynamics of the 18O + 58Ni system: A wide-ranging test NUCLEAR REACTIONS 58Ni(18O, 18O), (18O, 18O'), (18O, 16O), (18O, 17O), E ≈ 38-65 MeV; calculated σ(θ). 58Ni(18O, X), E(cm)=28-50 MeV; calculated fusion σ. Coupled channels approach, comparison with data.
doi: 10.1103/PhysRevC.73.014601
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
2005CH74 Braz.J.Phys. 35, 906 (2005) L.C.Chamon, G.P.A.Nobre, D.Pereira, C.P.Silva, E.S.Rossi, Jr., L.R.Gasques, B.V.Carlson Coulomb and Nuclear Potentials Between Deformed Nuclei Applied to the Fusion Process NUCLEAR REACTIONS 64Ni(64Ni, X), E(cm)=85-110 MeV; calculated fusion σ. Coulomb and nuclear interactions, barrier penetration model. Comparison with data.
doi: 10.1590/S0103-97332005000500051
2004CH36 Phys.Rev. C 70, 014604 (2004) L.C.Chamon, G.P.A.Nobre, D.Pereira, E.S.Rossi, Jr., C.P.Silva, L.R.Gasques, B.V.Carlson Coulomb and nuclear potentials between deformed nuclei NUCLEAR STRUCTURE Z=0-100; compiled, analyzed quadrupole and octupole deformation lengths. NUCLEAR REACTIONS 58Ni(58Ni, X), E not given; calculated Coulomb and nuclear potentials, deformation and orientation dependence.
doi: 10.1103/PhysRevC.70.014604
2004CH47 Prog.Theor.Phys.(Kyoto), Suppl. 154, 169 (2004) L.C.Chamon, L.R.Gasques, D.Pereira, B.V.Carlson A Consistent Description of the Heavy-Ion Fusion and Elastic Scattering Processes Using a Nonlocal Model NUCLEAR REACTIONS 12C, 16O(12C, X), E(cm)=1-18 MeV; 58,64Ni(58Ni, X), (64Ni, X), E(cm)=88-112 MeV; 154Sm(12C, X), E(cm)=40-60 MeV; 58Ni, 144,148,150,154Sm(16O, X), E(cm) ≈ 28-100 MeV; 208Pb(16O, X), (32S, X), E(cm) ≈ 70-180 MeV; 58,64Ni, 94,100Mo(28Si, X), E(cm) ≈ 45-100 MeV; 40Ca, 58Ni, 90,96Zr(40Ca, X), E(cm) ≈ 50-130 MeV; 110Pd, 100Mo(32S, X), (36S, X), E(cm) ≈ 70-120 MeV; 144,154Sm(40Ar, X), E(cm) ≈ 110-170 MeV; 74Ge(58Ni, X), (74Ge, X), E(cm) ≈ 90-160 MeV; 90,96Zr(90Zr, X), E(cm) ≈ 170-200 MeV; 70,76Ge, 92,100Mo, 102,104Ru(86Kr, X), E(cm) ≈ 120-220 MeV; calculated fusion σ. Nonlocal model, comparisons with data.
doi: 10.1143/PTPS.154.169
2004GA16 Phys.Rev. C 69, 034603 (2004) L.R.Gasques, L.C.Chamon, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, B.V.Carlson Global and consistent analysis of the heavy-ion elastic scattering and fusion processes NUCLEAR REACTIONS 144,148,150,154Sm, 208Pb(16O, X), E(cm)=50-100 MeV; 12C, 16O(12C, X), E(cm)=2-20 MeV; 64Ni(58Ni, X), E(cm)=80-120 MeV; 27Al, 32S(12C, X), E(cm)=20-150 MeV; calculated fusion σ.
doi: 10.1103/PhysRevC.69.034603
2003AL17 Nucl.Phys. A723, 93 (2003) M.A.G.Alvarez, L.C.Chamon, M.S.Hussein, D.Pereira, L.R.Gasques, E.S.Rossi, Jr., C.P.Silva A parameter-free optical potential for the heavy-ion elastic scattering process NUCLEAR REACTIONS 12C, 16O, 40Ca, 90Zr, 208Pb(12C, 12C), 208Pb(16O, 16O), (40Ar, 40Ar), E ≈ 16-2400 MeV; analyzed σ(θ); deduced optical potential features.
doi: 10.1016/S0375-9474(03)01158-8
2003CH85 Braz.J.Phys. 33, 238 (2003) L.C.Chamon, B.V.Carlson, L.R.Gasques, D.Pereira, C.De Conti, M.A.G.Alvarez, M.S.Hussein, M.A.Candido Ribeiro, E.S.Rossi, Jr., C.P.Silva Nonlocal Description of the Nuclear Interaction
doi: 10.1590/s0103-97332003000200012
2003GA04 Phys.Rev. C 67, 024602 (2003) L.R.Gasques, L.C.Chamon, D.Pereira, V.Guimaraes, A.Lepine-Szily, M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, B.V.Carlson, J.J.Kolata, L.Lamm, D.Peterson, P.Santi, S.Vincent, P.A.De Young, G.Peasley Experimental determination of the surface density for the 6He exotic nucleus NUCLEAR REACTIONS 58Ni(α, α), (6He, 6He), E=8.1, 9.0, 9.1, 9.6 MeV; measured σ(θ). 58Ni(α, α), E=82-288 MeV; analyzed σ(θ). 4,6He deduced ground-state nuclear densities. Unfolding method, comparison with model predictions.
doi: 10.1103/PhysRevC.67.024602
2003GA18 Phys.Rev. C 67, 067603 (2003) L.R.Gasques, L.C.Chamon, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., C.P.Silva, G.P.A.Nobre, B.V.Carlson Systematical study of the optical potential for systems like A+58Ni from sub-barrier data analyses NUCLEAR REACTIONS 58Ni(28Si, 28Si), E=74, 75.5, 77 MeV; measured σ(θ); deduced optical model parameters. 28Si deduced density distribution. NUCLEAR STRUCTURE 4,6He, 12C, 16,18O, 28Si; analyzed scattering data; deduced radii, density distributions.
doi: 10.1103/PhysRevC.67.067603
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
2002CH39 Phys.Rev. C66, 014610 (2002) L.C.Chamon, B.V.Carlson, L.R.Gasques, D.Pereira, C.De Conti, M.A.G.Alvarez, M.S.Hussein, M.A.Candido Ribeiro, E.S.Rossi, Jr., C.P.Silva Toward a Global Description of the Nucleus-Nucleus Interaction NUCLEAR STRUCTURE Z=1-82; analyzed charge distribution data, radii. 16O, 56Fe, 120Sn, 208Pb; calculated nucleon density distributions. NUCLEAR REACTIONS 58Ni(16O, X), E not given; 58Ni(α, X), E=139 MeV; calculated folding potential; deduced parameters. Other reaction data analyzed.
doi: 10.1103/PhysRevC.66.014610
2002GA16 Phys.Rev. C65, 044314 (2002) L.R.Gasques, L.C.Chamon, C.P.Silva, D.Pereira, M.A.G.Alvarez, E.S.Rossi, Jr., V.P.Likhachev, B.V.Carlson, C.De Conti Determination of the 12C Nuclear Density Through Heavy-Ion Elastic Scattering Experiments NUCLEAR REACTIONS 58Ni(12C, 12C), E=26-28.5 MeV; 208Pb(12C, 12C), E=54.5-57 MeV; measured σ(θ); deduced potential features. 12C deduced nucleon density distribution. Comparisons with other reactions and with model predictions.
doi: 10.1103/PhysRevC.65.044314
2002RO29 Nucl.Phys. A707, 325 (2002) E.S.Rossi, Jr., D.Pereira, L.C.Chamon, C.P.Silva, M.A.G.Alvarez, L.R.Gasques, J.Lubian, B.V.Carlson, C.De Conti Effect of the 18O Nuclear Density on the Nuclear Potentials of the 18O + 58, 60Ni Systems NUCLEAR REACTIONS 58,60Ni(18O, 18O'), (18O, 17O), (18O, 16O), E=34-38 MeV; measured quasielastic, inelastic, transfer σ, σ(θ); deduced nuclear potential features. 18O deduced neutron density distribution. Comparison with previous results, model predictions.
doi: 10.1016/S0375-9474(02)01009-6
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
1999AL23 Nucl.Phys. A656, 187 (1999) M.A.G.Alvarez, L.C.Chamon, D.Pereira, E.S.Rossi, Jr., C.P.Silva, L.R.Gasques, H.Dias, M.O.Roos Experimental Determination of the Ion-Ion Potential in the N = 50 Target Region: A tool to probe ground-state nuclear densities NUCLEAR REACTIONS 88Sr, 90,92Zr, 92Mo(16O, 16O), E=43-49 MeV; measured elastic, inelastic σ(θ); deduced optical potentials. Shell model and double-folding calculations.
doi: 10.1016/S0375-9474(99)00304-8
1998CH18 Phys.Rev. C58, 576 (1998) L.C.Chamon, D.Pereira, M.S.Hussein Parameterfree Account of Quasielastic Scattering of Stable and Radioactive Nuclei NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=1016, 1449, 2400 MeV; 12C(11Li, 11Li'), E=637 MeV; calculated σ(θ). Parameterfree model, nonlocal energy-independent potential. Comparison with data.
doi: 10.1103/PhysRevC.58.576
1998GA23 Phys.Rev. C58, 1627 (1998) D.Galetti, S.S.Mizrahi, L.C.Chamon, D.Pereira, M.S.Hussein, M.A.Candido Ribeiro Nonlocal Effects in the 8Be Breakup NUCLEAR STRUCTURE 8Be; calculated collective potential, inertia function for spontaneous breakup; deduced nonlocal effects. Generator coordinate method.
doi: 10.1103/PhysRevC.58.1627
1997CH48 Phys.Rev.Lett. 79, 5218 (1997) L.C.Chamon, D.Pereira, M.S.Hussein, M.A.Candido Ribeiro, D.Galetti Nonlocal Description of the Nucleus-Nucleus Interaction NUCLEAR REACTIONS 12C(12C, 12C), E=16, 112, 300, 1016, 1449, 2400 MeV; 208Pb(12C, 12C), E=420, 1449, 2400 MeV; 12C, 58Ni(α, α), E=139 MeV; analyzed σ(θ). Non-local, parameter-free potential.
doi: 10.1103/PhysRevLett.79.5218
1997RI08 Phys.Rev.Lett. 78, 3270 (1997) M.A.C.Ribeiro, L.C.Chamon, D.Pereira, M.S.Hussein, D.Galetti Pauli Nonlocality in Heavy-Ion Rainbow Scattering: A further test of the folding model NUCLEAR REACTIONS 12C(12C, X), (16O, X), E=10-200 MeV/nucleon; calculated local equivalent potential energy dependence; deduced nonlocal exchange effects role in potential energy dependence.
doi: 10.1103/PhysRevLett.78.3270
1997RO16 J.Phys.(London) G23, 1473 (1997) E.S.Rossi, Jr., L.C.Chamon, D.Pereira, C.P.Silva, G.Ramirez The Ion-Ion Potential and Neutron Transfer Processes in the 18O + 58,60Ni Systems at Sub-Barrier Energies NUCLEAR REACTIONS 58Ni(18O, X), E=38.1, 37, 35 MeV; 60Ni(18O, X), E=37, 38.1 MeV; measured inelastic, 1n-, 2n-transfer σ; deduced ion-ion potential, 2n-transfer inhibition in 18O+58Ni system.
doi: 10.1088/0954-3899/23/10/038
1997SI13 Phys.Rev. C55, 3155 (1997) C.P.Silva, D.Pereira, L.C.Chamon, E.S.Rossi, Jr., G.Ramirez, A.M.Borges, C.E.Aguiar Fusion and Peripheral Processes in the 16,18O + 58,60,64Ni Systems NUCLEAR REACTIONS, ICPND 58,60,64Ni(16O, X), (18O, X), E=38-64 MeV; measured fusion σ(E). 58Ni(18O, 18O), E=35.1-55.1 MeV; measured fusion σ(E), σ(θ); deduced fusion barriers, standard radius deviation, reaction mechanism.
doi: 10.1103/PhysRevC.55.3155
1996CH03 Nucl.Phys. A597, 253 (1996) L.C.Chamon, D.Pereira, E.S.Rossi, Jr., C.P.Silva, H.Dias, L.Losano, C.A.P.Ceneviva Isotopic Dependence of the Ion-Ion Potential in the Systems 16O + 58,60,62,64Ni NUCLEAR REACTIONS 58,60,62,64Ni(16O, 16O), (16O, 16O'), E=34-37 MeV; measured σ(θ); deduced optical potential. 58,60,62,64Ni levels deduced B(E2), deformation lengths. Shell-model, double-folding calculations, coupled-channel analysis.
doi: 10.1016/0375-9474(95)00467-X
1995CH11 Nucl.Phys. A582, 305 (1995) L.C.Chamon, D.Pereira, E.S.Rossi, Jr., C.P.Silva, R.Lichtenthaler Filho, L.C.Gomes Experimental Investigation of the Ion-Ion Potential for the 16O + 60Ni System at Large Interaction Distances NUCLEAR REACTIONS 60Ni(16O, 16O), (16O, 16O'), E=35-37 MeV; measured σ(θ); deduced optical potential. Coupled-channels calculations.
doi: 10.1016/0375-9474(94)00491-5
1994LI31 Phys.Rev. C50, 3033 (1994) R.Lichtenthaler, D.Pereira, L.C.Chamon, L.C.Gomes, A.Ventura, L.Zuffi Second Order Effects in the Algebraic Potential for Heavy-Ion Systems Near the Coulomb Barrier NUCLEAR REACTIONS 63Cu(16O, 16O), E=39-64 MeV; measured σ(θ); deduced algebraic potential parameters, characteristics.
doi: 10.1103/PhysRevC.50.3033
1992BO32 Phys.Rev. C46, 2360 (1992) A.M.Borges, C.P.da Silva, D.Pereira, L.C.Chamon, E.S.Rossi, Jr., C.E.Aguiar Pair Transfer and the Sub-Barrier Fusion of 18O + 58Ni NUCLEAR REACTIONS, ICPND 58Ni(18O, X), E=51.7 MeV; 60Ni(16O, X), E=64 MeV; measured evaporation residue σ(θ). 58Ni(18O, X), 60Ni(16O, X), E(cm)=31.6-56.8 MeV; measured fusion σ(E); deduced reaction mechanism.
doi: 10.1103/PhysRevC.46.2360
1992CH06 Phys.Lett. 275B, 29 (1992) L.C.Chamon, D.Pereira, E.S.Rossi, C.P.Silva, G.R.Razeto, A.M.Borges, L.C.Gomes, O.Sala Isotopic Dependence of the Fusion Cross Section in the Systems 16,18O + 63,65Cu NUCLEAR REACTIONS 63,65Cu(18O, X), E=40.1-64 MeV; measured fusion σ(E). 63,65Cu(16O, 16O), E=40.1-64 MeV; measured σ(θ). 63,65Cu(16O, X), E(cm)=30-50 MeV; analyzed fusion σ(E); deduced fusion σ isotopic dependence.
doi: 10.1016/0370-2693(92)90846-V
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
1984PE11 Ann.Acad.Brasil.Cienc. 56, 27 (1984) D.Pereira, J.C.Acquadro, O.Sala Fusion and Quasi-Elastic Processes in the 27Al + 16O System NUCLEAR REACTIONS 27Al(16O, X), (16O, 16O), (16O, 16O'), E=45.6 MeV; measured evaporation residue, elastic, inelastic σ(θ); deduced fusion σ, quasielastic σ ratio. Frahn-Rehm formalism.
1982MA30 Phys.Rev. C26, 500 (1982) W.Mayer, D.Pereira, K.E.Rehm, H.J.Scheerer, H.J.Korner, G.Korschinek, W.Mayer, P.Sperr, S.C.Pieper, R.D.Lawson Strong Population of Excited 0+ States in Even Zr Isotopes Observed with the (14C, 16O) Reaction NUCLEAR REACTIONS 92,100Mo(14C, 14C), (14C, 14C'), (14C, 16O), 94,96,98Mo(14C, 16O), E=71 MeV; measured σ(θ), σ(E(16O)); deduced optical model parameters. 90,92,94,96,98Zr levels deduced spectroscopic amplitudes. DWBA analysis.
doi: 10.1103/PhysRevC.26.500
1982PE13 Z.Phys. A308, 361 (1982) D.Pereira, H.-J.Korner, G.Korschinek, W.Mayer, H.-J.Scheerer Analogies between the (p, t) and the (14C, 16O) Reaction on Semi-Magic Nuclei NUCLEAR REACTIONS 140Ce, 142Nd, 144Sm(14C, 16O), E=71 MeV; measured σ(E(16O)), σ(θ). 138Ba, 140Ce, 142Nd level deduced collective characteristics, proton orbital coherence effect. Cluster transfer DWBA analysis.
doi: 10.1007/BF01415885
1982SC25 Z.Phys. A308, 183 (1982) H.J.Scheerer, D.Pereira, A.Chalupka, R.Gyufko, C.-A.Wiedner Mass Excess of 145Eu NUCLEAR REACTIONS 144Sm, 142Nd, 209Bi, 92Mo(3He, d), E=33 MeV; measured σ(Ed), relative Q. 145Eu deduced mass excess. Q3D magnetic spectrograph.
doi: 10.1007/BF01413010
1981KO30 Phys.Rev. C24, 2076 (1981) I.Koenig, H.Bohn, T.Faestermann, P.Kienle, H.J.Korner, W.A.Mayer, D.Pereira, K.E.Rehm, H.J.Scheerer Spectroscopy of Excited States in 102Mo and 106Ru NUCLEAR REACTIONS 100Mo(18O, 16O), E=84 MeV; 104Ru(18O, 16O), E=84, 100 MeV; measured 16Oγ-coin, Eγ. 102Mo, 106Ru deduced levels, J, π, yrast transitions. Enriched targets.
doi: 10.1103/PhysRevC.24.2076
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