NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = B.V.Carlson Found 148 matches. Showing 1 to 100. [Next]2024TO02 Nucl.Phys. A1041, 122793 (2024) F.Torabi, E.F.Aguilera, B.V.Carlson Threshold anomalies in 9Be + 12C NUCLEAR REACTIONS 12C(9Be, 9Be), E(cm)=5-12 MeV; analyzed available data; deduced σ within the extended optical model (EOM) framework.
doi: 10.1016/j.nuclphysa.2023.122793
2023CA05 Phys.Rev. C 107, 035805 (2023) B.V.Carlson, M.Dutra, O.Lourenco, J.Margueron Low-energy nuclear physics and global neutron star properties NUCLEAR STRUCTURE 16O, 34Si, 40,48,52,54Ca, 48,56,78Ni, 90Zr, 100,132Sn, 208Pb; calculated binding energies, charge radii, isoscalar giant monopole resonance (ISGMR) centroid energy; deduced symmetry energy parameters, neutron star properties (mass, radius). Calculation testing 415 relativistic mean field and nonrelativistic Skyrme-type interactions.
doi: 10.1103/PhysRevC.107.035805
2023TO04 J.Phys.(London) G50, 045107 (2023) A systematic analysis of deuteron breakup NUCLEAR REACTIONS 181Ta(d, X), E=100 MeV; 27Al, 58Ni, 90Zr, 118Sn, 209Bi(d, p), E=56, 70, 80, 100 MeV; 27Al, Cu, 93Nb(d, X), E=102 MeV; calculated σ(θ, E), σ(θ) for proton spectra using the code EMPIRE. Comparison with experimental data.
doi: 10.1088/1361-6471/acb95f
2023TO08 Eur.Phys.J. A 59, 192 (2023) Elastic Coulomb breakup analysis via different approaches NUCLEAR REACTIONS 12C, 27Al, 58Ni, 90Zr, 93Nb, 181Ta, 208Pb(d, X), E<20 MeV; calculated integrated Coulomb breakup σ using the Coulomb excitation (CE) method. Comparison with the Continuum Discretized Coupled Channel (CDCC) model.
doi: 10.1140/epja/s10050-023-01106-4
2022BH05 Phys.Rev. C 106, 044602 (2022) M.Bhuyan, S.Rana, N.Jain, R.Kumar, S.K.Patra, B.V.Carlson Medium-dependent relativistic NN potential: Application to fusion dynamics NUCLEAR REACTIONS 40Ca(16O, X), E(cm)=20-40 MeV;58Ni(40Ca, X), E(cm)=65-100 MeV;90Zr(40Ca, X), E(cm)=65-120 MeV;144Sm(16O, X), E(cm)=55-80 MeV;208Pb(16O, X), E(cm)=70-90 MeV;208Pb(48Ca, X), E(cm)=170-220 MeV; calculated positions and heights of the fusion barriers, fusion σ(E). Calculations using R3Y NN potential described in terms of density-dependent nucleonmeson couplings within the framework of the relativistic-Hartree-Bogoliubov (RHB) approach. Comparison to the available experimental data and calculations using different forms of the NN potential (R3Y, DDR3Y, M3Y, and DDM3Y).
doi: 10.1103/PhysRevC.106.044602
2022JO04 Phys.Rev. C 106, L011603 (2022) J.E.Johnstone, V.Singh, R.Giri, S.Hudan, J.Vadas, R.T.deSouza, D.Ackermann, A.Chbihi, Q.Hourdille, A.Abbott, C.Balhoff, A.Hannaman, A.B.McIntosh, M.Sorensen, Z.Tobin, A.Wakhle, S.J.Yennello, M.A.Famiano, K.W.Brown, C.Santamaria, J.Lubian, H.O.Soler, B.V.Carlson Proton and neutron exchange as a prelude to fusion at near-barrier energies NUCLEAR REACTIONS 39,41,45,47K(28Si, X), 36,44Ar(28Si, X), E(cm)=34-46 MeV; measured reaction products, evaporation residues; deduced fusion excitation functions, fusion σ(E), potential energy surfaces for binary fragments. Comparison to Dirac-Hartree-Bogoliubov (DHB) calculations for the ground state densities used in Sao Paulo fusion model. Radioactive beams of K and Ar ions were produced by the coupled cyclotron facility at MSU-NSCL and thermalized in a linear gas stopper before being reaccelerated by the ReA3 linac.
doi: 10.1103/PhysRevC.106.L011603
2022TE05 Eur.Phys.J. A 58, 205 (2022) E.A.Teixeira, T.Aumann, C.A.Bertulani, B.V.Carlson Nuclear fragmentation reactions as a probe of neutron skins in nuclei NUCLEAR REACTIONS 208Pb(p, X), E<500 MeV; 12C(12C, X), E<1000 MeV/nucleon; analyzed available data; deduced σ, neutron skin thickness as a function of the isospin asymmetry parameter.
doi: 10.1140/epja/s10050-022-00849-w
2021BH10 J.Phys.(London) G48, 075105 (2021) M.Bhuyan, B.Maheshwari, H.A.Kassim, N.Yusof, S.K.Patra, B.V.Carlson, P.D.Stevenson The kinks in charge radii across N = 82 and 126 revisited NUCLEAR STRUCTURE 126,128,130,132,134,136,138Sn, 202,204,206,208,210,212,214Pb; analyzed available data; deduced isotopic shift over the isotopic chains, energy levels, J, π, yrast states within the relativistic mean-field (RMF) and relativistic-Hartree-Bogoliubov (RHB) approach.
doi: 10.1088/1361-6471/abf7d7
2021BH12 Phys.Rev. C 104, 045801 (2021) A.Bhattacharyya, U.Datta, A.Rahaman, S.Chakraborty, T.Aumann, S.Beceiro Novo, K.Boretzky, C.Caesar, B.V.Carlson, W.N.Catford, M.Chartier, D.Cortina-Gil, P.Das, G.D.Angelis, P.Diaz Fernandez, H.Emling, H.Geissel, D.Gonzalez-Diaz, M.Heine, H.Johansson, B.Jonson, N.Kalantar-Nayestanaki, T.Kroll, R.Krucken, J.Kurcewicz, C.Langer, T.Le Bleis, Y.Leifels, J.Marganiec, G.Munzenberg, T.Nilsson, C.Nociforo, V.Panin, S.Paschalis, R.Plag, R.Reifarth, M.V.Ricciardi, C.Rigollet, D.Rossi, C.Scheidenberger, H.Scheit, H.Simon, Y.Togano, S.Typel, Y.Utsuno, A.Wagner, F.Wamers, H.Weick, J.S.Winfield Neutron capture cross sections of light neutron-rich nuclei relevant for r-process nucleosynthesis NUCLEAR REACTIONS 208Pb, 12C(29Na, X), (30Na, X), (33Mg, X), (35Al, X), E=410-430 MeV/nucleon, [secondary 29,30Na, 33Mg, 35Al beams from fragmentation of 540 MeV/nucleon 40Ar beam, followed by separation of ions of interest using the FRS-ALADIN-LAND apparatus at GSI]; measured reaction products, Eγ, Iγ, invariant mass spectra in coincidence with the sum energy of γ rays in different energy ranges using an array of 162 NaI(Tl) detectors for γ rays emitted from the excited core of the projectiles after Coulomb dissociation; deduced number of E1 type virtual photons from Coulomb, invariant mass spectra of breakup of incident beams into 28Na, 29Na, 32Mg and 34Al and one neutron in each case, and analyzed using direct breakup model. 29Na, 30Na, 33Mg, (γ, n), E*=2-16 MeV; 35Al(γ, n), E*=5-20 MeV, virtual photons from Coulomb breakup of incident beams; deduced photoabsorption σ(E) as function of excitation energy. 28,29Na, 32Mg, 34Al(n, γ), E<13 MeV; deduced neutron capture σ(E) using the photoabsorption cross sections. 28,29Na, 32Mg, 34Al(n, γ), T9=0.01-100; deduced astrophysical total reaction rates at the onset and at the end of the r-process. 14C(n, γ), E(cm)=10-1000 keV; analyzed previous experimental cross section data, and compared with theoretical calculations. 29,30Na, 33Mg, 35Al; deduced spectroscopic factors for the occupied orbitals of valence neutron(s) in the ground states from Coulomb breakup cross sections, and compiled previous experimental spectroscopic factors. Relevance to neutrino-driven wind model of core-collapse supernovae, and r-process nucleosynthesis.
doi: 10.1103/PhysRevC.104.045801
2021CH31 Eur.Phys.J. A 57, 212 (2021) Nucleon-induced inelastic scattering with statistical strength functions and the ECIS direct reaction code NUCLEAR REACTIONS 90Zr(p, p), E=80 MeV; calculated σ, σ(θ, E) using DWBA reaction calculations using the ECIS code. Comparison with available data.
doi: 10.1140/epja/s10050-021-00497-6
2021CH69 Braz.J.Phys. 51, 323 (2021) E.V.Chimanski, L.A.Souza, B.V.Carlson The Sao Paulo Potential and the 3He Breakup Reaction at 130 MeV on 93Nb and 197Au NUCLEAR REACTIONS 93Nb, 197Au(3He, X), (3He, d), E=130 MeV; calculated σ(θ, E); deduced Sao Paulo potential parameters adjusted for the nuclear diffusivity.
doi: 10.1007/s13538-020-00819-x
2021GA14 Phys.Rev. C 103, 034616 (2021) L.R.Gasques, M.A.G.Alvarez, A.Arazi, B.V.Carlson, L.C.Chamon, J.P.Fernandez-Garcia, A.Lepine-Szily, J.Lubian, J.Rangel, M.Rodriguez-Gallardo, V.Scarduelli, V.A.B.Zagatto Understanding the mechanisms of nuclear collisions: A complete study of the 10B + 120Sn reaction NUCLEAR REACTIONS 120Sn(10Be, 10Be), (10B, X)4He/6He/6Li/7Li/9Be/10Be/10B/11B/11C/12C, E≈39.70 MeV; measured reaction products, particle spectra, σ(θ) for elastic and inelastic scattering using SATURN and STAR particle-detector arrays of semiconductor silicon surface barrier detectors and single sided silicon strip detector (SSSSD) at the 8 MV tandem accelerator of the University of Sao Paulo; deduced σ(θ) for the 1-neutron transfer channel, energy projection of 9Be nuclei, σ(θ) for 6,7Li, 9,10Be, 11B and 12C. Comparison with coupled reaction channels (CRC) calculations using the SPP as the bare interaction.
doi: 10.1103/PhysRevC.103.034616
2021KU12 Eur.Phys.J. A 57, 87 (2021) Y.Kucuk, V.Guimaraes, B.V.Carlson Towards a systematic optical model potential for A = 8 projectiles NUCLEAR STRUCTURE 8B, 8Li, 8He; analyzed available data; deduced potential set using a Woods-Saxon potential shape; calculated σ(θ).
doi: 10.1140/epja/s10050-021-00405-y
2021SI16 Phys.Rev. C 103, 054605 (2021) M.Sin, R.Capote, M.W.Herman, A.Trkov, B.V.Carlson Modeling photon-induced reactions on 233-238U actinide targets NUCLEAR REACTIONS 233,234,235,236,237,238U(γ, X), (γ, γ), (γ, F), (γ, n), (γ, 2n), (γ, 3n), E=3-30 MeV; calculated photoreaction total, photoabsorption, fission, elastic and (γ, xn) σ(E) using the EMPIRE-3.2 code and compared with the available experimental data in the EXFOR library, and with the evaluated data from JENDL/PD-2016 and IAEA-Photonuclear Data Library 1999 (IAEA-PD); deduced set of giant dipole resonances (GDR) parameters consistent with all the available experimental data. Discussed differences and the similarities between the models and parameters used in calculations of photon- and neutron-induced reactions on the same nuclei, with focus on fission process.
doi: 10.1103/PhysRevC.103.054605
2021SI29 Phys.Rev. C 104, L041601 (2021) V.Singh, J.E.Johnstone, R.Giri, S.Hudan, J.Vadas, R.T.deSouza, D.Ackermann, A.Chbihi, Q.Hourdille, A.Abbott, C.Balhoff, A.Hannaman, A.B.McIntosh, M.Sorensen, Z.Tobin, A.Wakhle, S.J.Yennello, M.A.Famiano, K.W.Brown, C.Santamaria, J.Lubian, H.O.Soler, B.V.Carlson Impact of shell structure on the fusion of neutron-rich mid-mass nuclei NUCLEAR REACTIONS 16O(39K, X), (41K, X), (45K, X), (47K, X), (36Ar, X), (44Ar, X), E(cm)=23-33 MeV, [secondary radioactive 45,47K, 44Ar beams from 9Be(48Ca, X), E=140 MeV/nucleon, followed by separation of ions using A1900 at NSCL-MSU facility]; measured reaction products, fusion σ(E); deduced reduced fusion excitation functions; investigated influence of shell effects on fusion of mid-mass nuclei. Comparison of experimental fusion cross sections with Sao Paulo model using Dirac-Hartree-Bogoliubov (DHB) densities, and densities from systematics; deduced over prediction of fusion experimental σ for closed-shell nuclei using DHB densities. 39,41,45,47K, 36,44Ar; predicted DHB density distributions of protons and neutrons. Relevance to importance of understanding shell effects at the saddle point for accurate description of fusion process.
doi: 10.1103/PhysRevC.104.L041601
2021SO26 Phys.Rev. C 104, 034623 (2021) L.A.Souza, E.V.Chimanski, B.V.Carlson Inclusive breakup cross sections in reactions induced by the nuclides 6He and 6, 7Li in the two-body cluster model NUCLEAR REACTIONS 64Zn, 209Bi(6He, α), E=9-25 MeV; 64Zn(6He, α), E=9.8, 13.5, 14.85, 17.9 MeV; 120Sn(6He, α), E=17.4, 18.05, 19.8, 20.5, 22.2 MeV; 208Pb(6Li, α), (6Li, d), E=19-40 MeV; 90Zr(6Li, α), E=14-31, 19, 21, 25, 30 MeV; 58Ni(6Li, α), E=14, 16, 18, 20 MeV; 118Sn(6Li, α), E=18, 19, 21, 24 MeV; 56Fe(7Li, α), E=68 MeV; 58Ni(7Li, α), E=14.22, 16.25, 18.28, 20.31 MeV; calculated inclusive σ(E) for α and deuteron emission, α angular distributions, and spectra; deduce zero-range overall large contribution from inclusive breakup emission of α particles. Zero-range post-form Ichimura, Austern, and Vincent (IAV)-distorted-wave Born approximation (DWBA) formalism for elastic and nonelastic breakup cross sections, with Wood-Saxon parametrization of Sao Paulo optical potential with a modified diffuseness, and with projectiles treated as two-body clusters, 6He as α+dineutron, 6Li as α+d and 7Li as α+triton. Comparison with experimental data.
doi: 10.1103/PhysRevC.104.034623
2020BH02 Phys.Rev. C 101, 044603 (2020); Errata Phys.Rev. C 104, 059901 (2021) M.Bhuyan, R.Kumar, S.Rana, D.Jain, S.K.Patra, B.V.Carlson Effect of density and nucleon-nucleon potential on the fusion cross section within the relativistic mean field formalism NUCLEAR STRUCTURE 26Mg, 31Al, 39,46K, 48Ca, 64Ni, 154Sm, 181Ta, 197Au, 238U, 248Cm; calculated total radial density distributions, neutron and proton equivalent diffusiveness parameters using relativistic mean field formalism with NL3* interaction. Comparison with experimental data. NUCLEAR REACTIONS 154Sm, 238U, 248Cm(48Ca, X), E(cm)=135-234 MeV; 238U(64Ni, X), E(cm)=245-305 MeV; 248Cm(26Mg, X), E(cm)=105-150 MeV; 181Ta(46K, X), (39K, X), E(cm)=140-176 MeV; 197Au(31Al, X), E(cm)=105-160 MeV; calculated σ(E), barrier heights, fusion barrier distributions. Comparison with experimental fusion cross section data. Relativistic mean field formalism using the double-folding procedure, and R3Y and M3Y interactions. Discussion of the role of nucleon-nucleon potential and nucleon densities in fusion cross sections.
doi: 10.1103/PhysRevC.101.044603
2020CH14 Phys.Rev. C 101, 034603 (2020) L.C.Chamon, L.R.Gasques, B.V.Carlson Velocity-dependent model for the α-α interaction in the context of the double-folding potential NUCLEAR REACTIONS 4He(α, α), E<30 MeV; calculated elastic scattering phase shifts. 208Pb(α, α), E=23.6, 139 MeV; calculated σ(θ, E). Double-folding approach using Sao Paulo potential (SPP) and velocity dependence. Comparison with experimental data. 8Be; described s-wave resonance of the ground state.
doi: 10.1103/PhysRevC.101.034603
2019AL32 Phys.Rev. C 100, 064602 (2019) M.A.G.Alvarez, J.P.Fernandez-Garcia, J.L.Leon-Garcia, M.Rodriguez-Gallardo, L.R.Gasques, L.C.Chamon, V.A.B.Zagatto, A.Lepine-Szily, J.R.B.Oliveira, V.Scarduelli, B.V.Carlson, J.Casal, A.Arazi, D.A.Torres, F.Ramirez Systematic study of optical potential strengths in reactions on 120Sn involving strongly bound, weakly bound, and exotic nuclei NUCLEAR REACTIONS 120Sn(6Li, 6Li), E=19, 24, 27 MeV; measured scattered 6Li, σ(E, θ) using SATURN array of Si detectors at the tandem accelerator of LAFN, University of Sao Paulo. 120Sn(α, α), E(reduced)=5.1, 12.0, 15.6, 19.1 MeV; 120Sn(6He, 6He), E(reduced)=3.8, 4.4, 6.1, 6.7, 8.4 MeV; 120Sn(7Li, 7Li), E(reduced)=0.6, 1.3, 3.2, 5.1, 7.0, 8.9 MeV; 120Sn(9Be, 9Be), E(reduced)=0.3, 0.7, 1.6, 1.7, 3.1, 13.3, 20.7 MeV; 120Sn(10B, 10B), E(reduced)=0.2, 1.6, 2.1, 3.4 MeV; 120Sn(16O, 16O), E(reduced)=2.3, 3.1, 4.0 MeV; 120Sn(18O, 18O), E(reduced)=2.1 MeV; analyzed previous σ(E, θ) data as part of the E-125 experimental campaign, developed at the LAFN, with experiments carried out at Sao Paulo and TANDAR facility in Buenos Aires. Optical model analyses based on the double-folding Sao Paulo potential. NUCLEAR STRUCTURE 6Li, 6He, 9,10Be; calculated matter densities using Hartree-Bogoliubov (HB) theory with NL3 and DDME1 interactions, and from charge densities obtained in (e, e') experiments. 4,6He, 6,7Li, 9,10Be, 16,18O; calculated s-wave barrier parameters using double-folding Sao Paulo potential (SPP) for systems with projectiles focusing on 120Sn.
doi: 10.1103/PhysRevC.100.064602
2019BH08 Phys.Rev. C 100, 054312 (2019) M.Bhuyan, B.V.Carlson, S.K.Patra, RajK.Gupta Neck configuration of Cm and Cf nuclei in the fission state within the relativistic mean field formalism NUCLEAR STRUCTURE 242,244,246,248Cm, 248,250,252,254Cf; calculated potential energy surfaces, binding energies, rms charge radii, quadrupole deformation parameters β2, first and second barrier heights, static fission paths as a function of quadrupole deformation, total matter density distribution of the fission states, neutron and proton densities in the neck region, fission neck length parameters using relativistic mean field formalism with NL3 parameter set. Comparison with FRDM calculations and available experimental values; investigated the mechanism of fission decay and the shape of the fissioning nucleus by following the static fission path to the configuration before the breakup.
doi: 10.1103/PhysRevC.100.054312
2019CH01 Phys.Rev. C 99, 014305 (2019) E.V.Chimanski, B.V.Carlson, R.Capote, A.J.Koning Quasiparticle nature of excited states in random-phase approximation NUCLEAR STRUCTURE 56Ni; calculated level energy deviation, state strength function and width as function of excitation energy, contributions to the RPA transition matrix from collective, two-noncollective, and 3- states, response functions for low-energy 3-, and high energy particle-hole configurations of 3- states, single-particle contribution to the response function, width of the Breit-Wigner distribution for 3- and 4+ states, energy level spacing with local widths of particle-hole pair configurations. 16O, 56Ni, 90Zr, 120Sn; calculated spreading width of Breit Wigner distributions. Random phase approximation (RPA) on the basis of particle-hole configurations of excited states. Relevance to multistep direct (MSD) nuclear reactions.
doi: 10.1103/PhysRevC.99.014305
2019EN01 Nucl.Data Sheets 155, 56 (2019) J.W.Engle, A.V.Ignatyuk, R.Capote, B.V.Carlson, A.Hermanne, M.A.Kellett, T.Kibedi, G.Kim, F.G.Kondev, M.Hussain, O.Lebeda, A.Luca, Y.Nagai, H.Naik, A.L.Nichols, F.M.Nortier, S.V.Suryanarayana, S.Takacs, F.T.Tarkanyi, M.Verpelli Recommended Nuclear Data for the Production of Selected Therapeutic Radionuclides COMPILATION 131Cs, 131Ba, 225Ac, 225Ra, 227Th, 227Ac, 230U, 230Pa; analyzed σ data leading to formation of therapeutic radionuclides.
doi: 10.1016/j.nds.2019.01.003
2019QU02 Phys.Rev. C 99, 044314 (2019) A.Quddus, M.Bhuyan, S.Ahmad, B.V.Carlson, S.K.Patra Temperature-dependent symmetry energy of neutron-rich thermally fissile nuclei NUCLEAR STRUCTURE 234,236,250U, 240Pu; calculated nuclear densities, effective symmetry energy coefficients and curvatures, binding energies, charge radius, and β deformation parameter at finite temperature, neutron pressure and symmetry energy coefficients as function of neutron skin thickness using temperature-dependent relativistic mean field model (TRMF) with FSUGarnet, IOPB-I, and NL3 parameters. Comparison with available experimental data.
doi: 10.1103/PhysRevC.99.044314
2019SO12 Nucl.Phys. A989, 69 (2019) S.R.Souza, B.V.Carlson, R.Donangelo Post breakup dynamical evolution of fragments produced in nuclear multifragmentation NUCLEAR REACTIONS 112Sn(112Sn, x)168Re; calculated proton, deuteron, triton multiplicity evolutions (and also those for 3He, 9,11,12,13C), d-d correlation function, d-d pair total momentum at initial moment and at long (infinite) time using hybrid model based on Statistical Multifragmentation Model (SMM) and GEMINI++ code
doi: 10.1016/j.nuclphysa.2019.05.017
2019TA25 J.Radioanal.Nucl.Chem. 319, 533 (2019) F.T.Tarkanyi, A.V.Ignatyuk, A.Hermanne, R.Capote, B.V.Carlson, J.W.Engle, M.A.Kellett, T.Kibedi, G.Kim, F.G.Kondev, M.Hussain, O.Lebeda, A.Luca, Y.Nagai, H.Naik, A.L.Nichols, F.M.Nortier, S.V.Suryanarayana, S.Takacs, M.Verpelli Recommended nuclear data for medical radioisotope production: diagnostic positron emitters COMPILATION 44Sc, 52Mn, 55Co, 61,62Cu, 66,68Ga, 72As, 73Se, 76Br, 82Rb, 86Y, 89Zr, 90Nb, 94Tc, 110In, 118Sb, 120,122I, 128Cs, 140Pr; compiled, evaluated and recommended data on σ for the production of medical radionuclides.
doi: 10.1007/s10967-018-6380-5
2019TA26 J.Radioanal.Nucl.Chem. 319, 487(2019) F.T.Tarkanyi, A.V.Ignatyuk, A.Hermanne, R.Capote, B.V.Carlson, J.W.Engle, M.A.Kellett, T.Kibedi, G.Kim, F.G.Kondev, M.Hussain, O.Lebeda, A.Luca, Y.Nagai, H.Naik, A.L.Nichols, F.M.Nortier, S.V.Suryanarayana, S.Takacs, M.Verpelli Recommended nuclear data for medical radioisotope production: diagnostic gamma emitters COMPILATION 51Cr, 99Tc, 111In, 123I, 203Tl; anal yzed available data; deduced σ for production of diagnostic gamma-ray emitting radionuclides.
doi: 10.1007/s10967-018-6142-4
2018BH01 Phys.Rev. C 97, 024322 (2018) M.Bhuyan, B.V.Carlson, S.K.Patra, S.-G.Zhou Surface properties of neutron-rich exotic nuclei within relativistic mean field formalisms NUCLEAR STRUCTURE 70,72,74,76,78,80,82,84,86Fe, 72,74,76,78,80,82,84,86,88Ni, 74,76,78,80,82,84,86,88,90Zn, 76,78,80,82,84,86,88,90,92Ge, 78,80,82,84,86,88,90,92,94Se, 80,82,84,86,88,90,92,94,96Kr; calculated binding energies, charge radii, and quadrupole deformation parameter β2 for ground states, S(2n), total density distribution, symmetry energy and neutron pressure as function of neutron skin thickness. Calculations based on axially deformed self-consistent relativistic mean field for the nonlinear NL3* and density-dependent DD-ME1 interactions. Comparison with available experimental data.
doi: 10.1103/PhysRevC.97.024322
2018GA09 Phys.Rev. C 97, 034629 (2018) L.R.Gasques, A.S.Freitas, L.C.Chamon, J.R.B.Oliveira, N.H.Medina, V.Scarduelli, E.S.Rossi, M.A.G.Alvarez, V.A.B.Zagatto, J.Lubian, G.P.A.Nobre, I.Padron, B.V.Carlson Elastic, inelastic, and 1n transfer cross sections for the 10B+ 120Sn reaction NUCLEAR REACTIONS 120Sn(10B, 10B), (10B, 10B'), (10B, 11B), E=37.5 MeV; measured reaction products, particle spectra, σ(θ) for elastic and inelastic scattering using the Silicon Array and Telescopes of Usp for Reactions and Nuclear applications (SATURN) system at the Pelletron accelerator of University of Sao Paulo; analyzed data for σ(θ) using the coupled reaction channel (CRC) and one-step DWBA formalisms. 120Sn; deduced excitation of first 2+ and 3- levels, B(E2), B(E3), and deformation lengths. 10B; deduced excitation of 1+ level, B(E2), deformation length. 119Sn; deduced levels, σ, spectroscopic factors, CRC and DWBA analysis.
doi: 10.1103/PhysRevC.97.034629
2018HE06 Nucl.Data Sheets 148, 214 (2018) M.Herman, A.Trkov, R.Capote, G.P.A.Nobre, D.A.Brown, R.Arcilla, Y.Danon, A.Plompen, S.F.Mughabghab, Q.Jing, G.Zhigang, L.Tingjin, L.Hanlin, R.Xichao, L.Leal, B.V.Carlson, T.Kawano, M.Sin, S.P.Simakov, K.Guber Evaluation of Neutron Reactions on Iron Isotopes for CIELO and ENDF/B-VIII.0 NUCLEAR REACTIONS 56Fe(n, X), E<20 MeV; analyzed available data; calculated σ, σ(θ), σ(θ, E).
doi: 10.1016/j.nds.2018.02.004
2018HE07 Nucl.Data Sheets 148, 338 (2018) A.Hermanne, A.V.Ignatyuk, R.Capote, B.V.Carlson, J.W.Engle, M.A.Kellett, T.Kibedi, G.Kim, F.G.Kondev, M.Hussain, O.Lebeda, A.Luca, Y.Nagai, H.Naik, A.L.Nichols, F.M.Nortier, S.V.Suryanarayana, S.Takacs, F.T.Tarkanyi, M.Verpelli Reference Cross Sections for Charged-particle Monitor Reactions NUCLEAR REACTIONS 27Al(p, X)22Na/24Na, Ti(p, x)48V/46Sc, Ni(p, x)57Ni, Cu(p, X)62Zn/63Zn/65Zn/56Co/58Co, Mo(p, X)96Tc, 27Al(d, X)22Na/24Na, Ti(d, X)48V/46Sc, Cu(d, X)62Zn/63Zn/65Zn, Fe(d, X)56Co, Ni(d, X)61Cu/56Co/58Co, 27Al(3He, X)22Na/24Na, Ti(3He, X)48V, Cu(3He, X)66Ga/63Zn/65Zn, 27Al(α, X)22Na/24Na, Ti(α, X)51Cr, Cu(α, X)66Ga/67Ga/65Zn, E<1000 MeV; analyzed available data; deduced σ.
doi: 10.1016/j.nds.2018.02.009
2018LI67 Eur.Phys.J. A 54, 221 (2018) V.Liccardo, M.Malheiro, M.S.Hussein, B.V.Carlson, T.Frederico Nuclear processes in astrophysics: Recent progress
doi: 10.1140/epja/i2018-12648-5
2017CH36 Phys.Rev. C 96, 034301 (2017) S.Chakraborty, U.Datta, T.Aumann, S.Beceiro Novo, K.Boretzky, C.Caesar, B.V.Carlson, W.N.Catford, M.Chartier, D.Cortina-Gil, G.De Angelis, P.Diaz Fernandez, H.Emling, O.Ershova, L.M.Fraile, H.Geissel, D.Gonzalez-Diaz, H.Johansson, B.Jonson, N.Kalantar-Nayestanaki, T.Kroll, R.Krucken, C.Langer, T.Le Bleis, Y.Leifels, J.Marganiec, G.Munzenberg, M.A.Najafi, T.Nilsson, C.Nociforo, V.Panin, R.Plag, A.Rahaman, R.Reifarth, M.V.Ricciardi, C.Rigollet, D.Rossi, C.Scheidenberger, H.Scheit, H.Simon, J.T.Taylor, Y.Togano, S.Typel, Y.Utsuno, A.Wagner, F.Wamers, H.Weick, J.S.Winfield Ground-state configuration of neutron-rich 35Al via Coulomb breakup NUCLEAR REACTIONS C, Pb(35Al, 34Al), E=403 MeV/nucleon, [secondary 35Al beam from fragmentation of 531 MeV/nucleon 40Ar primary beam followed by separation of reaction products using FRS separator at GSI]; measured four-momenta of the projectile, fragments, and other decay products such as fragments, neutrons, and γ rays after secondary reaction using Large Area Neutron Detector for neutrons and Crystal Ball array of NaI(Tl) detectors for γ detection at GSI; deduced inclusive differential Coulomb dissociation (CD) cross section of 35Al breaking up into a neutron and 34Al fragment in its ground state and isomer. 34Al; deduced levels, Coulomb dissociation σ, spectroscopic factors. 35Al; deduced J, π, configurations, spectroscopic factor for the ground state.
doi: 10.1103/PhysRevC.96.034301
2017LI39 Phys.Rev. C 96, 054306 (2017) R.Lisboa, P.Alberto, B.V.Carlson, M.Malheiro Temperature effects on nuclear pseudospin symmetry in the Dirac-Hartree-Bogoliubov formalism NUCLEAR STRUCTURE 100,110,120,130,140,150,160,170Sn; calculated nuclear potentials as a function of the radial distance and temperature of 0-8 MeV, Woods-Saxon potential parameters. 100,150Sn; calculated Coulomb potentials, pseudospin energy splittings of the pseudospin partners for neutrons and protons as a function of temperature. Finite-temperature Dirac-Hartree-Bogoliubov (FTDHB) formalism.
doi: 10.1103/PhysRevC.96.054306
2017MO25 J.Phys.(London) G44, 105102 (2017) D.F.Morales Botero, L.C.Chamon, B.V.Carlson Transition densities in the context of the generalized rotation-vibration model NUCLEAR REACTIONS 28Si, 152Sm, 166Er, 192Os(E, E'), E=42, 81, 140, 500 MeV; calculated form factors, transition densities. NUCLEAR STRUCTURE 12C, 16O, 24Mg, 28Si, 32S, 40,48Ca, 52Cr, 58Ni, 64Zn, 70,76Ge, 88Sr, 90Zr, 92Mo, 108,110Pd, 110Cd, 120Sn, 142,150Nd, 152Sm, 154Gd, 166Er, 192Os, 194,196Pt, 208Pb; calculated B(E2), B(E3). Comparison with evaluated data. Collective model for the description of heavy-ion nuclear structure, called the generalized rotation-vibration model (GRVM).
doi: 10.1088/1361-6471/aa846e
2017PO13 Eur.Phys.J. A 53, 178 (2017) G.Potel, G.Perdikakis, B.V.Carlson, M.C.Atkinson, W.H.Dickhoff, J.E.Escher, M.S.Hussein, J.Lei, W.Li, A.O.Macchiavelli, A.M.Moro, F.M.Nunes, S.D.Pain, J.Rotureau Toward a complete theory for predicting inclusive deuteron breakup away from stability NUCLEAR REACTIONS 93Nb(d, pn), E=10, 25.5 MeV; calculated σ(ln), σ(θn) assuming both elastic and nonelastic breakup. Compared with published calculations. 40,48,60Ca(d, pn), E=20, 40 MeV; calculated σ(Ep) vs En and vs ln using both elastic and nonelastic breakup and using Hussein-McVoy theory.
doi: 10.1140/epja/i2017-12371-9
2017RA03 J.Phys.(London) G44, 045101 (2017) A.Rahaman, U.Datta, T.Aumann, S.Beceiro Novo, K.Boretzky, C.Caesar, B.V.Carlson, W.N.Catford, S.Chakraborty, M.Chartier, D.Cortina-Gil, G.De Angelis, P.Diaz Fernandez, H.Emling, O.Ershova, L.M.Fraile, H.Geissel, D.Gonzalez-Diaz, H.Johansson, B.Jonson, N.Kalantar-Nayestanaki, T.Kroll, R.Krucken, J.Kurcewicz, C.Langer, T.Le Bleis, Y.Leifels, J.Marganiec, G.Munzenberg, M.A.Najafi, T.Nilsson, C.Nociforo, V.Panin, S.Paschalis, R.Plag, R.Reifarth, M.V.Ricciardi, C.Rigollet, D.Rossi, C.Scheidenberger, H.Scheit, H.Simon, J.T.Taylor, Y.Togano, S.Typel, V.Volkov, A.Wagner, F.Wamers, H.Weick, M.Weigand, J.S.Winfield, D.Yakorev, M.Zoric Coulomb breakup of neutron-rich 29, 30Na isotopes near the island of inversion NUCLEAR REACTIONS 208Pb(29Na, n), (30Na, n), E=400-430 MeV/nucleon; measured reaction products, Eγ, Iγ. 28,29Na; deduced σ, J, π, spectroscopic factors. Comparison with available data.
doi: 10.1088/1361-6471/aa594d
2016CA20 Few-Body Systems 57, 307 (2016) Inclusive Proton Emission Spectra from Deuteron Breakup Reactions NUCLEAR REACTIONS 12C, 25Mg, 27Al, 48Ti, 51V, 54Fe, 58,62Ni, 89Y, 90Zr, 93Nb, 118,119Sn, 159Tb, 181Ta, 197Au, 209Bi(d, p), E=56 MeV; calculated σ(θ, E), Ep, Ip using the post-form DWBA approximation.
doi: 10.1007/s00601-016-1054-8
2016DA06 Phys.Rev. C 94, 034304 (2016) U.Datta, A.Rahaman, T.Aumann, S.Beceiro Novo, K.Boretzky, C.Caesar, B.V.Carlson, W.N.Catford, S.Chakraborty, M.Chartier, D.Cortina-Gil, G.de Angelis, P.Diaz Fernandez, H.Emling, O.Ershova, L.M.Fraile, H.Geissel, D.Gonzalez-Diaz, B.Jonson, H.Johansson, N.Kalantar-Nayestanaki, T.Kroll, R.Krucken, J.Kurcewicz, C.Langer, T.Le Bleis, Y.Leifels, J.Marganiec, G.Munzenberg, M.A.Najafi, T.Nilsson, C.Nociforo, V.Panin, S.Paschalis, R.Plag, R.Reifarth, V.Ricciardi, D.Rossi, H.Scheit, C.Scheidenberger, H.Simon, J.T.Taylor, Y.Togano, S.Typel, V.Volkov, A.Wagner, F.Wamers, H.Weick, M.Weigand, J.S.Winfield, D.Yakorev, M.Zoric Direct experimental evidence for a multiparticle-hole ground state configuration of deformed 33Mg NUCLEAR REACTIONS 12C, 208Pb(33Mg, 32Mg), E=400 MeV/nucleon, [33Mg secondary beam produced in fragmentation of 540 MeV/nucleon 40Ar beam]; measured reaction products, Eγ, Iγ, (33Mg)γ-coin, partial and total inclusive Coulomb dissociation (CD) cross sections for breakup of 33Mg into n+32Mg using FRS-ALADIN-LAND arrangement at GSI facility 32Mg; deduced levels, spectroscopic factors. 33Mg; deduced multiparticle-hole ground state configuration, and occupancy by valence neutrons by s and p orbitals.
doi: 10.1103/PhysRevC.94.034304
2016LI08 Phys.Rev. C 93, 024321 (2016) R.Lisboa, M.Malheiro, B.V.Carlson Dirac-Hartree-Bogoliubov calculation for spherical and deformed hot nuclei: Temperature dependence of the pairing energy and gaps, nuclear deformation, nuclear radii, excitation energy, and entropy NUCLEAR STRUCTURE 40Ca, 90Zr, 124Sn, 140Ce, 150Sm, 168Er, 208Pb; calculated binding energies, p-p and n-n pairing gaps, neutron and proton energy levels, nuclear densities, deformation, radii, entropy, and caloric curves as function of temperature for spherical and deformed nuclei. Shape transition for deformed nuclei at higher temperatures. Dirac-Hartree-Bogoliubov (DHB) and relativistic mean field (RMF) theory for hot nuclei. Solution of Dirac-Gorkov and Klein-Gordon equations. Comparison with available experimental data.
doi: 10.1103/PhysRevC.93.024321
2015SO18 Phys.Rev. C 92, 024612 (2015) S.R.Souza, B.V.Carlson, R.Donangelo, W.G.Lynch, M.B.Tsang Internal and kinetic temperatures of fragments in the framework of a nuclear statistical multifragmentation model NUCLEAR STRUCTURE 40Ca, 80Zr, 120Nd; calculated breakup temperature as function of excitation energy (E*/A), internal temperature for selected fragments of 4He, 5Li, 10B, 12C, 16O, average excitation energy per nucleon of fragments as function of mass number A. Density of states of fragments from their internal temperatures and excitation energies. Statistical multifragmentation model.
doi: 10.1103/PhysRevC.92.024612
2014CA18 Nucl.Data Sheets 118, 276 (2014) B.V.Carlson, L.Brito, D.F.Mega, R.Capote, M.Herman, M.E.Rego Exclusive Multiple Emission Cross Sections in the Hybrid Monte Carlo Pre-equilibrium Model and in EMPIRE-3.1 NUCLEAR REACTIONS 59Co(p, 2n), (p, 3n), E=50, 100, 200 MeV; calculated exclusive neutron σ(En) using hybrid Monte Carlo simulation model; discussed implementation to EMPIRE-3.1.
doi: 10.1016/j.nds.2014.04.057
2014CA42 Phys.Rev. C 90, 054616 (2014) N.L.Calleya, S.R.Souza, B.V.Carlson, R.Donangelo, W.G.Lynch, M.B.Tsang, J.R.Winkelbauer Influence of the density of states on the odd-even staggering in the charge distribution of the emitted fragments in nuclear heavy-ion collisions NUCLEAR STRUCTURE 40Ca, 80Zr; calculated effect of density of states on odd-even staggering in charge distribution of fragments emitted in the breakup of 40Ca and 80Zr nuclei at E=1.5-4 MeV/nucleon excitation energies. Statistical Multifragmentation Model (SMM) considering pairing gaps for state densities.
doi: 10.1103/PhysRevC.90.054616
2014DU14 Phys.Rev. C 90, 055203 (2014) M.Dutra, O.Lourenco, S.S.Avancini, B.V.Carlson, A.Delfino, D.P.Menezes, C.Providencia, S.Typel, J.R.Stone Relativistic mean-field hadronic models under nuclear matter constraints
doi: 10.1103/PhysRevC.90.055203
2014MO05 J.Phys.(London) G41, 055114 (2014) D.F.Morale Botero, L.C.Chamon, B.V.Carlson Calculation of deformed double-folding potentials in the context of the generalized rotation-vibration model NUCLEAR STRUCTURE 28Si, 154Sm; calculated matter density, Coulomb and nuclear potentials.
doi: 10.1088/0954-3899/41/5/055114
2013AV04 Eur.Phys.J. A 49, 75 (2013) S.S.Avancini, B.V.Carlson, J.R.Marinelli Nuclear monopole charge form factor calculation for relativistic models including center-of-mass corrections NUCLEAR STRUCTURE 4He, 12C; calculated charge formfactor, charge radius using Peierls-Yoccoz projection method for relativistic approaches with reparameterization of the coupling constants. Compared with available data.
doi: 10.1140/epja/i2013-13075-x
2013RA14 Eur.Phys.J. A 49, 57 (2013) J.Rangel, J.Lubian, P.R.S.Gomes, B.V.Carlson, L.C.Chamon, A.Gomez Camacho On the near-barrier fusion of the proton-halo 8B + 58Ni system NUCLEAR REACTIONS 58Ni(8B, X), E(cm)=16-32 MeV;208Pb(17F, X), E not given; calculated halo nuclei reactions σ, proton σ(θ) from 8B breakup using CDCC with double-folding potential. Compared with data.
doi: 10.1140/epja/i2013-13057-0
2013SO18 Phys.Rev. C 88, 014607 (2013) S.R.Souza, B.V.Carlson, R.Donangelo, W.G.Lynch, M.B.Tsang Statistical multifragmentation model with discretized energy and the generalized Fermi breakup: Formulation of the model NUCLEAR REACTIONS 20Ne(20Ne, X)40Ca* at 2-7 MeV/nucleon; calculated yields distributions of Z=1-20 primary fragments from 40Ca breakup, total multiplicity as function of excitation energy. Generalized Fermi breakup model (GFBM). Comparison with GEMINI++ sequential decay code and Weisskopf-Ewing evaporation model. statistical multifragmentation model (SMM).
doi: 10.1103/PhysRevC.88.014607
2012CA04 Nucl.Phys. A876, 77 (2012) B.V.Carlson, R.Donangelo, S.R.Souza, W.G.Lynch, A.W.Steiner, M.B.Tsang Fermi breakup and the statistical multifragmentation model NUCLEAR REACTIONS 16O(p, X), E=62 MeV fragmentation; calculated charge, mass yields using Fermi breakup model and microcanonical statistical multifragmentation model.
doi: 10.1016/j.nuclphysa.2011.12.009
2011CA02 Few-Body Systems 49, 85 (2011) Static and Covariant Meson-Exchange Interactions in Nuclear Matter
doi: 10.1007/s00601-010-0189-2
2011CA34 J.Phys.:Conf.Ser. 312, 082017 (2011) B.V.Carlson, R.Donangelo, S.R.Souza, W.G.Lynch, A.W.Steiner, M.B.Tsang Fermi breakup and the Statistical Multifragmentation Model NUCLEAR REACTIONS 16O(γ, X), E=50 MeV; calculated breakup Z=4-7 isotopes yields, σ using Fermi breakup model and statistical multifragmentation.
doi: 10.1088/1742-6596/312/4/082017
2011CH13 Phys.Rev. C 83, 034617 (2011) L.C.Chamon, B.V.Carlson, L.R.Gasques α + α scattering reexamined in the context of the Sao Paulo potential NUCLEAR REACTIONS 4He(α, α), E=0.6-29.5 MeV; analyzed σ, phase shift, charge distributions using the velocity-dependent Sao Paulo potential (SPP).
doi: 10.1103/PhysRevC.83.034617
2011CH44 Phys.Rev. C 84, 044607 (2011) L.C.Chamon, L.R.Gasques, B.V.Carlson Approximate treatment of relativistic effects in the low-energy α+α scattering
doi: 10.1103/PhysRevC.84.044607
2010CH59 Nucl.Phys. A846, 1 (2010) Systematics of nuclear densities, deformations and excitation energies within the context of the generalized rotation-vibration model NUCLEAR STRUCTURE A=4-252; calculated nuclear densities, deformation, level energies, B(E2), B(E3), associated quantities using a generalized rotation-vibration model. Comparison with data.
doi: 10.1016/j.nuclphysa.2010.06.003
2009CH01 J.Phys.(London) G36, 025102 (2009) L.C.Chamon, G.P.A.Nobre, B.V.Carlson Effect on the heavy-ion fusion and elastic scattering cross sections of common approximations assumed in coupled-channel calculations
doi: 10.1088/0954-3899/36/2/025102
2009SO07 Phys.Rev. C 79, 054602 (2009) S.R.Souza, B.V.Carlson, R.Donangelo, W.G.Lynch, A.W.Steiner, M.B.Tsang Statistical multifragmentation model with Skyrme effective interactions NUCLEAR STRUCTURE 150Nd; calculated temperature and charge distributions for breakup of the nucleus, average multiplicity and yields of light particles Li, Be, B, C, N and O. 10Be, 20Ne, 31P, 40Ca; calculated internal free energy as a function of temperature. Statistical multifragmentation and Thomas-Fermi (SMM-TF) model with Skyrme interaction.
doi: 10.1103/PhysRevC.79.054602
2009SO15 Phys.Rev. C 80, 041602 (2009) S.R.Souza, M.B.Tsang, B.V.Carlson, R.Donangelo, W.G.Lynch, A.W.Steiner Isospin effects and the density dependence of the nuclear symmetry energy NUCLEAR REACTIONS 58Ni(40Ar, X), (40Ca, X), E not given; calculated isoscaling parameters as a function of the excitation energy of the source, and Isotopic distribution of primary fragments Li, Be, B, C, N and O using improved statistical multifragmentation model (ISMM), SLy4 and Gs Skyrme effective interactions.
doi: 10.1103/PhysRevC.80.041602
2009SO16 Phys.Rev. C 80, 044606 (2009) S.R.Souza, M.B.Tsang, B.V.Carlson, R.Donangelo, W.G.Lynch, A.W.Steiner Temperature effects in nuclear isoscaling
doi: 10.1103/PhysRevC.80.044606
2007FU11 Nucl.Phys. A790, 588c (2007) B.Funke Haas, B.V.Carlson, T.Frederico Quasideuteron pairing in asymmetric nuclear matter
doi: 10.1016/j.nuclphysa.2007.03.131
2007FU13 Nucl.Phys. A788, 316c (2007) B.Funke Haas, B.V.Carlson, T.Frederico Standard and quasideuteron pairing in asymmetric nuclear matter
doi: 10.1016/j.nuclphysa.2007.01.088
2007HE31 Nucl.Data Sheets 108, 2655 (2007) M.Herman, R.Capote, B.V.Carlson, P.Oblozinsky, M.Sin, A.Trkov, H.Wienke, V.Zerkin EMPIRE: Nuclear Reaction Model Code System for Data Evaluation
doi: 10.1016/j.nds.2007.11.003
2007NO06 Nucl.Phys. A786, 90 (2007) G.P.A.Nobre, L.C.Chamon, B.V.Carlson, I.J.Thompson, L.R.Gasques Tunneling through a parabolic barrier coupled to an oscillatory degree of freedom: Application to heavy-ion fusion at sub-barrier energies NUCLEAR REACTIONS 58,64Ni(58Ni, X), (64Ni, X), E(cm)=85-115 MeV; calculated fusion excitation functions.
doi: 10.1016/j.nuclphysa.2007.02.005
2007NO08 Phys.Rev. C 75, 044606 (2007) G.P.A.Nobre, L.C.Chamon, L.R.Gasques, B.V.Carlson, I.J.Thompson Consistent analysis of fusion data without adjustable parameters for a wide variety of heavy-ion systems NUCLEAR REACTIONS 12C, 92Zr, 208Pb(12C, X), 16O, 144,148,152,154Sm, 182,186W, 208Pb, 238U(16O, X), 208Pb(18O, X), 68Zn, 92Zr, 100Mo, 144Sm, 208Pb(28Si, X), 92,94,98,100Mo, 104Ru, 108,110Pd, 182W, 208Pb(32S, X), 90,98Zr, 92,100Mo, 104Ru, 108,110Pd(36S, X), 112,122Sn, 144,148,154Sm(40Ar, X), 40,48Ca, 48Ti, 90,98Zr, 192Os, 194Pt(40Ca, X), 90,98Zr(48Ca, X), 58,64Ni, 74Ge, 112,124Sn(58Ni, X), 64Ni, 74Ge, 100Mo(64Ni, X), 70,76Ge, 92Mo, 104Ru(86Kr, X), 90,96Zr(90Zr, X), E ≈ barrier; calculated fusion σ. Sao Paolo potential, comparison with data.
doi: 10.1103/PhysRevC.75.044606
2007NO12 Phys.Rev. C 76, 024605 (2007) G.P.A.Nobre, C.P.Silva, L.C.Chamon, B.V.Carlson Consistent analysis of fusion data without adjustable parameters for systems involving odd nuclei NUCLEAR STRUCTURE Li, Be, B, N, O, F, Al, s, Cl, Sc, Ti, V, Co, Ni, Cu, Ge, Y, Zr, Nb, Ru, Rh, Pd, Sn, Sm, Tb, Ho, Pb, Bi, Th; calculated deformation parameters. NUCLEAR REACTIONS 14N, 159Tb, 232Th(11B, X), E not given; 159Tb(10B, X), E not given; 59Co, 209Bi(16O, X), E not given; 144Sm(17O, X), E not given; 65Cu(18O, X), E not given; 70,73,74,76Ge(27Al, X), E not given; 59Co(14N, X), E not given; 209Bi(15N, X), E not given; 208Pb, 232Th(19F, X), E not given; 93Nb, 101Ru, 103Rh, 105Pd(32S, X), (36S, X), E not given; 27Al, 58,60,62,64Ni, 59Co, 92Zr, 112Sn(35Cl, X), E not given; 58,60,62,64Ni(37Cl, X), E not given; calculated fusion cross sections.
doi: 10.1103/PhysRevC.76.024605
2007PO10 Nucl.Phys. A787, 211c (2007) Configuration mixing in nucleon-induced pre-equilibrium reactions
doi: 10.1016/j.nuclphysa.2006.12.034
2006BA02 Nucl.Phys. A765, 75 (2006) E.F.Batista, B.V.Carlson, T.Frederico Polarization effects in relativistic pairing in nuclear matter
doi: 10.1016/j.nuclphysa.2005.11.003
2006BA23 J.Phys.(London) G32, 655 (2006) E.Baldini-Neto, B.V.Carlson, D.Hirata Self-consistent Dirac quasi-particle blocking approximation applied to the α-decay scheme of the superheavy element 287115 NUCLEAR STRUCTURE 63,64,65,66,67,68Ga, 65,66,67,68,69,70Ge, 67,68,69,70,71,72As, 69,70,71,72,73Se, 72,73,74,75Br; calculated binding energies, radii, β2. 287,288Mc, 283,284Nh, 279,280Rg, 275,276Mt, 271,272Bh, 268Db; calculated binding energies, β2, level energies and configurations.Dirac-Hartree-Bogoliubov formalism. RADIOACTIVITY 287Mc, 283Nh, 279Rg, 275Mt(α); calculated Qα, T1/2. Dirac-Hartree-Bogoliubov formalism.
doi: 10.1088/0954-3899/32/5/005
2006FE14 Braz.J.Phys. 36, 1379 (2006) Trajectory Effects in Coulomb Excitation NUCLEAR REACTIONS 208Pb(208Pb, 208Pb'), E=500 MeV/nucleon; calculated cross sections, trajectory effects for Coulomb excitation of multiple giant dipole resonances.
doi: 10.1590/S0103-97332006000800010
2006PO16 Phys.Rev. C 74, 054609 (2006) Configuration mixing in pre-equilibrium reactions
doi: 10.1103/PhysRevC.74.054609
2005CA45 Phys.Rev. C 72, 041603 (2005) B.V.Carlson, L.F.Canto, M.S.Hussein Semiclassical Coulomb interaction
doi: 10.1103/PhysRevC.72.041603
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
2005NO01 Phys.Lett. B 605, 79 (2005) C.Nociforo, K.L.Jones, L.H.Khiem, P.Adrich, T.Aumann, B.V.Carlson, D.Cortina-Gil, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstrom, J.V.Kratz, R.Kulessa, T.Lange, Y.Leifels, H.Lenske, E.Lubkiewicz, G.Munzenberg, R.Palit, H.Scheit, H.Simon, K.Summerer, S.Typel, E.Wajda, W.Walus, H.Weick, and the LAND-FRS Collaboration Coulomb breakup of 23O NUCLEAR REACTIONS Pb(23O, n22O), E=422 MeV/nucleon; measured En, Eγ, Iγ, (fragment)γ-, nγ-coin, σ(E); deduced final-state interaction effects. 23O deduced ground state J, π, configuration, spectroscopic factor.
doi: 10.1016/j.physletb.2004.11.014
2005RE26 Braz.J.Phys. 35, 919 (2005) Comparison Between Models of the Decay of Light Compound Nuclei
doi: 10.1590/S0103-97332005000500055
2004BA18 Braz.J.Phys. 34, 773 (2004) E.Baldini-Neto, B.V.Carlson, R.A.Rego, M.S.Hussein p+6, 8He Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 6,8He(p, p), E ≈ 0.7 GeV; calculated σ(θ), analyzing power. Relativistic optical potential. NUCLEAR STRUCTURE 4,6,8He; calculated radii.
doi: 10.1590/s0103-97332004000500017
2004BA21 Braz.J.Phys. 34, 855 (2004) E.Baldini-Neto, B.V.Carlson, D.Hirata Dirac-Hartree-Bogoliubov Approximation for Finite Nuclei with Blocking NUCLEAR STRUCTURE O, Ni, Ca, Sn; calculated mass defects. Dirac-Hartree-Bogoliubov approximation with blocking, comparison with data. RADIOACTIVITY 277Cn, 273Ds, 269Hs, 265Sg, 261Rf, 257No, 253Fm, 249Cf(α); calculated Qα. Dirac-Hartree-Bogoliubov approximation with blocking, comparison with data.
doi: 10.1590/s0103-97332004000500039
2004BA22 Braz.J.Phys. 34, 889 (2004) E.F.Batista, B.V.Carlson, T.Frederico Vacuum Polarization Effects in Relativistic Nuclear Pairing
doi: 10.1590/s0103-97332004000500049
2004BB18 Braz.J.Phys. 34, 773 (2004) E.Baldini-Neto, B.V.Carlson, R.A.Rego, M.S.Hussein p+6, 8He Elastic Scattering at Intermediate Energies NUCLEAR REACTIONS 6,8He(p, p), E ≈ 0.7 GeV; calculated σ(θ), analyzing power. Relativistic optical potential. NUCLEAR STRUCTURE 4,6,8He; calculated radii.
doi: 10.1590/S0103-97332004000500017
2004BB21 Braz.J.Phys. 34, 855 (2004) E.Baldini-Neto, B.V.Carlson, D.Hirata Dirac-Hartree-Bogoliubov Approximation for Finite Nuclei with Blocking NUCLEAR STRUCTURE O, Ni, Ca, Sn; calculated mass defects. Dirac-Hartree-Bogoliubov approximation with blocking, comparison with data. RADIOACTIVITY 277Cn, 273Ds, 269Hs, 265Sg, 261Rf, 257No, 253Fm, 249Cf(α); calculated Qα. Dirac-Hartree-Bogoliubov approximation with blocking, comparison with data.
doi: 10.1590/S0103-97332004000500039
2004BB22 Braz.J.Phys. 34, 889 (2004) E.F.Batista, B.V.Carlson, T.Frederico Vacuum Polarization Effects in Relativistic Nuclear Pairing
doi: 10.1590/S0103-97332004000500049
2004CA16 Ann.Nucl.Energy 31, 1069 (2004) Computer codes for spectrum average cross section calculations
doi: 10.1016/j.anucene.2003.12.004
2004CA47 Phys.Rev. C 70, 057602 (2004) B.V.Carlson, L.C.Chamon, L.R.Gasques Accurate approximation for the Coulomb potential between deformed nuclei NUCLEAR REACTIONS 58Ni(58Ni, X), E not given; calculated Coulomb potential.
doi: 10.1103/PhysRevC.70.057602
2004CA51 Braz.J.Phys. 34, 859 (2004) B.V.Carlson, L.F.Canto, M.S.Hussein Semiclassical Coulomb Excitation Matrix Elements
doi: 10.1590/s0103-97332004000500040
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
2004FR16 Nucl.Phys. A737, 260 (2004) T.Frederico, J.H.O.Sales, B.V.Carlson, P.U.Sauer Light-front time picture of few-body systems
doi: 10.1016/j.nuclphysa.2004.03.087
2004FU35 Braz.J.Phys. 34, 894 (2004) B.Funke Haas, B.V.Carlson, T.Frederico A Dirac Description of 1S0 + 3S1 - 3D1 Pairing in Nuclear Matter
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
2004HU05 Nucl.Phys. A731, 163 (2004) M.S.Hussein, B.V.Carlson, L.F.Canto Multiple giant resonances in nuclei: their excitation and decay NUCLEAR STRUCTURE 40Ca, 120Sn, 132Xe, 165Ho, 208Pb, 238U; calculated double and triple GDR excitation and decay features.
doi: 10.1016/j.nuclphysa.2003.11.029
2004HU12 Nucl.Phys. A738, 367 (2004) M.S.Hussein, B.V.Carlson, T.Frederico, T.Tarutina Three-body model for the complete fusion of a two-cluster composite projectile with a heavy target
doi: 10.1016/j.nuclphysa.2004.04.063
2004LI29 Nucl.Phys. A735, 303 (2004) G.F.Lima, A.Lepine-Szily, A.C.C.Villari, W.Mittig, R.Lichtenthaler, M.Chartier, N.A.Orr, J.C.Angelique, G.Audi, E.Baldini-Neto, B.V.Carlson, J.M.Casandjian, A.Cunsolo, C.Donzaud, A.Foti, A.Gillibert, D.Hirata, M.Lewitowicz, S.Lukyanov, M.MacCormick, D.J.Morrissey, A.N.Ostrowski, B.M.Sherrill, C.Stephan, T.Suomijarvi, L.Tassan-Got, D.J.Vieira, J.M.Wouters Reaction cross section and matter radius measurements of proton-rich Ga, Ge, As, Se and Br nuclides NUCLEAR REACTIONS Si(63Ga, X), (64Ga, X), (65Ga, X), (66Ga, X), (67Ga, X), (68Ga, X), (65Ge, X), (66Ge, X), (67Ge, X), (68Ge, X), (69Ge, X), (70Ge, X), (67As, X), (68As, X), (69As, X), (70As, X), (71As, X), (72As, X), (69Se, X), (70Se, X), (71Se, X), (72Se, X), (73Se, X), (72Br, X), (73Br, X), (74Br, X), (75Br, X), E ≈ 50-60 MeV/nucleon; measured reaction σ. 63,64,65,66,67,68Ga, 65,66,67,68,69,70Ge, 67,68,69,70,71,72As, 69,70,71,72,73Se, 72,73,74,75Br; deduced matter radii. Glauber model analysis.
doi: 10.1016/j.nuclphysa.2004.01.125
2003BA20 Braz.J.Phys. 33, 297 (2003) E.F.Batista, B.V.Carlson, C.De Conti, T.Frederico Polarization Effects in Relativistic Nuclear Pairing
doi: 10.1590/s0103-97332003000200026
2003BA65 Nucl.Phys. A724, 345 (2003) E.Baldini-Neto, B.V.Carlson, R.A.Rego, M.S.Hussein p + 4, 6, 8He elastic scattering at intermediate energies NUCLEAR REACTIONS 4He(p, p), E=0.561, 0.8, 1.029 GeV; 6He(p, p), E=0.717 GeV; 8He(p, p), E=0.671 GeV; calculated σ(θ), analyzing power. Relativistic optical model, comparison with data and other models.
doi: 10.1016/S0375-9474(03)01540-9
2003BB20 Braz.J.Phys. 33, 297 (2003) E.F.Batista, B.V.Carlson, C.De Conti, T.Frederico Polarization Effects in Relativistic Nuclear Pairing
doi: 10.1590/S0103-97332003000200026
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
2003FU14 Nucl.Phys. A728, 379 (2003) B.Funke Haas, T.Frederico, B.V.Carlson, F.B.Guimaraes A relativistic separable potential to describe pairing in nuclear matter
doi: 10.1016/j.nuclphysa.2003.08.027
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
2003LE36 Braz.J.Phys. 33, 328 (2003) A.Leistenschneider, T.Aumann, K.Boretzky, L.F.Canto, B.V.Carlson, D.Cortina, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, A.Grunschloss, K.Helariutta, M.Hellstrom, M.S.Hussein, S.Ilievski, K.Jones, J.V.Kratz, R.Kulessa, H.K.Le, E.Lubkiewicz, G.Munzenberg, R.Palit, P.Reiter, C.Scheidenberger, K.-H.Schmidt, H.Simon, K.Summerer, E.Wajda, W.Walus Fragmentation of Exotic Oxygen Isotopes NUCLEAR STRUCTURE C, Pb(17O, X), (18O, X), (19O, X), (20O, X), (21O, X), E ≈ 600, 1700 MeV/nucleon; analyzed fragment yields. Abrasion-ablation models.
doi: 10.1590/s0103-97332003000200033
2003LI01 Nucl.Phys. A713, 24 (2003) V.P.Likhachev, J.Mesa, J.D.T.Arruda-Neto, B.V.Carlson, W.R.Carvalho, Jr., L.C.Chamon, A.Deppman, H.Dias, M.S.Hussein Quasi-free 238U(e, e'f) cross section in macroscopic-microscopic approach NUCLEAR REACTIONS 238U(e, e'X), E=720 MeV; calculated quasifree electrofission σ(E, θ). Comparison with data. NUCLEAR STRUCTURE 238U; calculated single-particle level energies. 237,238U, 237Pa; calculated fissility vs excitation energy.
doi: 10.1016/S0375-9474(02)01302-7
2003PA31 Phys.Rev. C 68, 034318 (2003) R.Palit, P.Adrich, T.Aumann, K.Boretzky, B.V.Carlson, D.Cortina, U.Datta Pramanik, Th.W.Elze, H.Emling, H.Geissel, M.Hellstrom, K.L.Jones, J.V.Kratz, R.Kulessa, Y.Leifels, A.Leistenschneider, G.Munzenberg, C.Nociforo, P.Reiter, H.Simon, K.Summerer, W.Walus, and the LAND/FRS Collaboration Exclusive measurement of breakup reactions with the one-neutron halo nucleus 11Be NUCLEAR REACTIONS C, Pb(11Be, n10Be), E=520 MeV/nucleon; measured Eγ, Iγ, En, (fragment)n-, nγ-coin; deduced partial σ for Coulomb and nuclear processes. 11Be deduced dipole strength, spectroscopic factor, radius.
doi: 10.1103/PhysRevC.68.034318
2003PR01 Phys.Lett. 551B, 63 (2003) U.D.Pramanik, T.Aumann, K.Boretzky, B.V.Carlson, D.Cortina, Th.W.Elze, H.Emling, H.Geissel, A.Grunschloss, M.Hellstrom, S.Ilievski, J.V.Kratz, R.Kulessa, Y.Leifels, A.Leistenschneider, E.Lubkiewicz, G.Munzenberg, P.Reiter, H.Simon, K.Summerer, E.Wajda, W.Walus Coulomb breakup of the neutron-rich isotopes 15C and 17C NUCLEAR REACTIONS Pb(15C, n14C), (17C, n16C), E ≈ 500-600 MeV/nucleon; measured Eγ, (fragment)γ-coin, Coulomb dissociation σ(E); deduced breakup mechanism features. 15,17C deduced ground-state configurations.
doi: 10.1016/S0370-2693(02)03016-2
Back to query form [Next] |