NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = A.Bonaccorso Found 67 matches. 2023MO24 Phys.Rev. C 108, 044609 (2023) Optical potentials and nuclear reaction cross sections for n-12C and N-12C scattering
doi: 10.1103/PhysRevC.108.044609
2022GI04 Phys.Rev. C 105, 044321 (2022) S.A.Gillespie, K.W.Brown, R.J.Charity, L.G.Sobotka, A.K.Anthony, J.Barney, A.Bonaccorso, B.A.Brown, J.Crosby, D.Dell'Aquila, J.Elson, J.Estee, A.Gade, M.Ghazali, G.Jhang, Y.Jin, B.Longfellow, W.G.Lynch, J.Pereira, M.Spieker, S.Sweany, F.C.E.Teh, A.Thomas, M.B.Tsang, C.Y.Tsang, D.Weisshaar, H.Y.Wu, K.Zhu Proton decay spectroscopy of 28S and 30Cl NUCLEAR REACTIONS 9Be(29S, n), (31Ar, p), E=150 MeV/nucleon; measured reaction products, Ep, Ip, Eγ, Iγ, (particle)p-coin, pγ-coin; deduced invariant mass, momentum distribution. Setup consisting of S800 spectrograph, Si-CsI(Tl) DSSD array of 128 concentric rings and 128 annular sectors, CAESAR CsI(Na) photon detection array, BC-400-type scintillation fiber detector at A1900 fragment separator (NSCL). RADIOACTIVITY 28S(p), (2p) [from 9Be(29S, n), E=150 MeV/nucleon]; 30Cl(p), (2p) [from 9Be(29S, n), E=150 MeV/nucleon]; measured Ep, Ip, Eγ, Iγ, pγ-coin; deduced total decay kinetic energy, decay energy spectrum. 30Cl; deduced levels, J, π, S(p). 28S; deduced levels, J, π, spectroscopic factors. Comparison to previous experimental results and shell model calculations.
doi: 10.1103/PhysRevC.105.044321
2021AU02 Prog.Part.Nucl.Phys. 118, 103847 (2021) T.Aumann, C.Barbieri, D.Bazin, C.A.Bertulani, A.Bonaccorso, W.H.Dickhoff, A.Gade, M.Gomez-Ramos, B.P.Kay, A.M.Moro, T.Nakamura, A.Obertelli, K.Ogata, S.Paschalis, T.Uesaka Quenching of single-particle strength from direct reactions with stable and rare-isotope beams
doi: 10.1016/j.ppnp.2021.103847
2021BO15 Eur.Phys.J. A 57, 171 (2021) Models of breakup: a final state interaction problem
doi: 10.1140/epja/s10050-021-00448-1
2021MO03 Nucl.Phys. A1006, 122109 (2021) Localization of peripheral reactions and sensitivity to the imaginary potential NUCLEAR REACTIONS 9Be(5Li, X), (6Be, X), (8C, X), (9Be, X), (9C, X), (12N, X), (12O, X), (13O, X), (14C, X), (15C, X), (17Ne, X), (23Si, X), (27S, X), (31Ar, X), (31S, X), (32Cl, X), (33Ar, X), (33Si, X), (35Ca, X), (45Ar, X), (56Ni, X), E=40-100 MeV/nucleon; analyzed available data; deduced σ, potential parameters.
doi: 10.1016/j.nuclphysa.2020.122109
2019BO10 Phys.Rev. C 100, 024617 (2019) A.Bonaccorso, F.Cappuzzello, D.Carbone, M.Cavallaro, G.Hupin, P.Navratil, S.Quaglioni Application of an ab initio S matrix to data analysis of transfer reactions to the continuum populating 11Be NUCLEAR REACTIONS 9Be(18O, 16O)11Be, E=84 MeV; measured reaction products, 16O ejectiles; deduced differential cross section. Results compared to an ab initio no-core shell model calculation for continuum states. 11Be; deduced levels, wave functions of the n+10Be system. Experiment performed at the Tandem Van de Graaff facility of the Istituto Nazionale di Fisica Nucleare Laboratori Nazionali el Sud, Italy, using MAGNEX magnetic spectrometer to momentum analyze 16O particles.
doi: 10.1103/PhysRevC.100.024617
2018BO13 Prog.Part.Nucl.Phys. 101, 1 (2018) Direct reaction theories for exotic nuclei: An introduction via semi-classical methods
doi: 10.1016/j.ppnp.2018.01.005
2018BO19 Eur.Phys.J. A 54, 152 (2018) On the eikonal approach to nuclear diffraction dissociation
doi: 10.1140/epja/i2018-12599-9
2016BO13 Few-Body Systems 57, 331 (2016) A.Bonaccorso, F.Carstoiu, R.J.Charity, R.Kumar, G.Salvioni Differences Between a Single- and a Double-Folding Nucleus-9Be Optical Potential NUCLEAR REACTIONS 9Be(8B, X), (8Li, X), (8C, X), E=100 MeV; analyzed available data; deduced neutron-, and nucleus-9Be imaginary potentials, energy dependent strong absorption radii and total reaction σ. Comparison with experimental values.
doi: 10.1007/s00601-016-1082-4
2016BO21 Phys.Rev. C 94, 034604 (2016) A.Bonaccorso, F.Carstoiu, R.J.Charity Imaginary part of the 9C-9Be single-folded optical potential NUCLEAR REACTIONS 9Be(9C, X), E=20, 38, 65, 83 MeV/nucleon; calculated nucleus-nucleus imaginary potentials for scattering of exotic light nuclei, the corresponding S matrices and total reaction σ(E) using a single-folding model where nucleus - 9Be target potential taken from a phenomenological fit to data over a large range of energies, and projectile densities from a series of microscopic calculations.
doi: 10.1103/PhysRevC.94.034604
2014BO02 Phys.Rev. C 89, 024619 (2014) Optical potential for the n-9Be reaction NUCLEAR REACTIONS 9Be(n, n), (n, X), E=0.1-200 MeV; analyzed elastic, and reaction σ(E), σ(E, θ), neutron knockout cross sections by two parameterization of the optical-model potential: phenomenological used in earlier studies, and dispersive optical model (DOM). Comparison of the two approaches with experimental data.
doi: 10.1103/PhysRevC.89.024619
2014BO10 Acta Phys.Pol. B45, 397 (2014) Direct Reaction Mechanisms for Exotic Nuclei NUCLEAR REACTIONS 9Be(14O, n), (14O, p), E=53 MeV/nucleon; calculated σ. Comparison with available data.
doi: 10.5506/APhysPolB.45.397
2014CA11 Acta Phys.Pol. B45, 431 (2014) D.Carbone, A.Bonaccorso, C.Agodi, M.Bondi, F.Cappuzzello, M.Cavallaro, A.Cunsolo, M.De Napoli, A.Foti, D.Nicolosi, S.Tropea The Continuum of 11Be Populated by the (18O, 16O) Two-neutron Transfer Reaction NUCLEAR REACTIONS 9Be(18O, 16O), E=84 MeV; measured reaction products; deduced σ(E).
doi: 10.5506/APhysPolB.45.431
2014CA25 Bull.Rus.Acad.Sci.Phys. 78, 607 (2014) D.Carbone, A.Bonaccorso, C.Agodi, M.Bondi, F.Cappuzzello, M.Cavallaro, A.Cunsolo, M.De Napoli, A.Foti, D.Nicolosi, S.Tropea Transfer to the continuum of 14C via (18O, 16O) reaction NUCLEAR REACTIONS 12C(18O, 16O), E=84 MeV; measured reaction products; deduced σ(E). Comparison with theoretical calculations.
doi: 10.3103/S1062873814070065
2014CA45 Phys.Rev. C 90, 064621 (2014) D.Carbone, M.Bondi, A.Bonaccorso, C.Agodi, F.Cappuzzello, M.Cavallaro, R.J.Charity, A.Cunsolo, M.De Napoli, A.Foti First application of the n- 9Be optical potential to the study of the 10Be continuum via the (18O, 17O) neutron-transfer reaction NUCLEAR REACTIONS 9Be(18O, 17O)10Be, E=84 MeV; measured E(17O) spectrum, angular distribution using MAGNEX spectrometer at tandem Van de Graaff facility of INFN-LNS. 10Be; deduced levels, J, π, resonances in the continuum. Breakup calculations describing the n-9Be interaction by means of an optical potential. Semi-classical approximation for the relative ion motion. Comparison between the measured cross section and the calculated using two parameterization of the optical potential.
doi: 10.1103/PhysRevC.90.064621
2014MA85 Phys.Rev.Lett. 113, 182501 (2014) T.Marchi, G.de Angelis, J.J.Valiente-Dobon, V.M.Bader, T.Baugher, D.Bazin, J.Berryman, A.Bonaccorso, R.Clark, L.Coraggio, H.L.Crawford, M.Doncel, E.Farnea, A.Gade, A.Gadea, A.Gargano, T.Glasmacher, A.Gottardo, F.Gramegna, N.Itaco, P.R.John, R.Kumar, S.M.Lenzi, S.Lunardi, S.McDaniel, C.Michelagnoli, D.Mengoni, V.Modamio, D.R.Napoli, B.Quintana, A.Ratkiewicz, F.Recchia, E.Sahin, R.Stroberg, D.Weisshaar, K.Wimmer, R.Winkler Quadrupole Transition Strength in the 74Ni Nucleus and Core Polarization Effects in the Neutron-Rich Ni Isotopes NUCLEAR REACTIONS 197Au(74Ni, 74Ni'), E=95.8 MeV/nucleon; measured reaction products, Eγ, Iγ. 74Ni; deduced energy levels, B(E2). Comparison with shell model calculations.
doi: 10.1103/PhysRevLett.113.182501
2013BO05 Phys.Scr. T152, 014019 (2013) Reaction mechanisms in the scattering of exotic nuclei
doi: 10.1088/0031-8949/2013/T152/014019
2012BO15 Phys.Scr. T150, 014008 (2012) Unbound nuclei studied by projectile fragmentation NUCLEAR STRUCTURE 12,13,14Be; calculated two-neutron separation energies, rms radii, density distributions, scattering lengths. NUCLEAR REACTIONS 12C(14Be, X)12Be, E=250 MeV/nucleon; analyzed experimental data. 13Be; deduced σ(E), level ordering. Time-dependent projectile fragmentation model, three-body model of Borromean nuclei, comparison with available data.
doi: 10.1088/0031-8949/2012/T150/014008
2012CA20 Phys.Lett. B 711, 347 (2012) F.Cappuzzello, C.Rea, A.Bonaccorso, M.Bondi, D.Carbone, M.Cavallaro, A.Cunsolo, A.Foti, S.E.A.Orrigo, M.R.D.Rodrigues, G.Taranto New structures in the continuum of 15C populated by two-neutron transfer NUCLEAR REACTIONS 13C(18O, 16O)15C, E=84 MeV; measured reaction products; deduced excitation energy spectra, several bound and resonance states, unknown structures in the continuum. Comparison with theoretical calculations.
doi: 10.1016/j.physletb.2012.04.012
2012FL02 Phys.Rev.Lett. 108, 252501 (2012) F.Flavigny, A.Obertelli, A.Bonaccorso, G.F.Grinyer, C.Louchart, L.Nalpas, A.Signoracci Nonsudden Limits of Heavy-Ion Induced Knockout Reactions NUCLEAR REACTIONS 9Be(16C, p), (16C, n), E=75 MeV/nucleon; 9Be(14O, p), (14O, n), E=53 MeV/nucleon; measured reaction products, Eγ, Iγ. 13N, 13O, 15B, 15C; deduced energy levels, J, π, σ, spectroscopic factors. Comparison with available data.
doi: 10.1103/PhysRevLett.108.252501
2012KU34 Phys.Rev. C 86, 061601 (2012) Interplay of nuclear and Coulomb effects in proton breakup from exotic nuclei NUCLEAR REACTIONS 12C, 208Pb(8B, X), (17F, X), E=40, 60, 80 MeV/nucleon; calculated proton-breakup σ and parallel momentum distributions for nuclear, and Coulomb breakup mechanisms. Interference between the two Coulomb effects and nuclear diffraction.
doi: 10.1103/PhysRevC.86.061601
2012SH21 Phys.Rev. C 85, 064612 (2012) R.Shane, R.J.Charity, L.G.Sobotka, D.Bazin, B.A.Brown, A.Gade, G.F.Grinyer, S.McDaniel, A.Ratkiewicz, D.Weisshaar, A.Bonaccorso, J.A.Tostevin Proton and neutron knockout from 36Ca NUCLEAR REACTIONS 9Be(36Ca, 35K), (36Ca, 35Ca), [36Ca secondary beam from 9Be(40Ca, X), E=140 MeV/nucleon primary reaction], E=70 MeV/nucleon; measured Eγ, particle spectra, time-of-flight, energy loss, cross sections, longitudinal-momentum distributions. 35K, 35Ca; deduced spectroscopic factors, orbital angular momenta of removed nucleons; calculated S matrices, bound-state wave-functions. Eikonal reaction theory, dispersive optical model (DOM) extrapolations. Shell-model spectroscopic factors from USD, USDA, and USDB interactions. 9Be(36Ca, X)33Ar, [33Ar from decay of unbound states in 35Ca], E=70 MeV/nucleon; measured σ; deduced missing spectroscopic strength.
doi: 10.1103/PhysRevC.85.064612
2011BA27 Phys.Rev. C 84, 015803 (2011) A.Banu, L.Trache, F.Carstoiu, N.L.Achouri, A.Bonaccorso, W.N.Catford, M.Chartier, M.Dimmock, B.Fernandez-Dominguez, M.Freer, L.Gaudefroy, M.Horoi, M.Labiche, B.Laurent, R.C.Lemmon, F.Negoita, N.A.Orr, S.Paschalis, N.Patterson, E.S.Paul, M.Petri, B.Pietras, B.T.Roeder, F.Rotaru, P.Roussel-Chomaz, E.Simmons, J.S.Thomas, R.E.Tribble Structure of 23Al from the one-proton breakup reaction and astrophysical implications NUCLEAR REACTIONS 12C(23Al, 22Mg), [23Al secondary beam from C(32S, X)E=95 MeV/nucleon primary reaction], E=57 MeV/nucleon; measured fragment spectra, inclusive and exclusive longitudinal momentum distributions, and widths, Eγ, (fragment)γ-coin. 22Mg; deduced levels, J, π, σ, spectroscopic factors, asymptotic normalization coefficients. 23Al; deduced g.s. Jπ, configuration mixing. Comparison with Glauber and large-scale shell model calculations. 22Mg(p, γ)23Al, E<1 MeV; deduced stellar reaction rates; discussed astrophysical significance of 22Na nucleosynthesis in ONe novae.
doi: 10.1103/PhysRevC.84.015803
2011KU14 Phys.Rev. C 84, 014613 (2011) Dynamical effects in proton breakup from exotic nuclei NUCLEAR REACTIONS 208Pb(8B, X), (17F, X), E=72 MeV/nucleon; calculated proton and neutron Coulomb and nuclear breakup, parallel momentum distributions, σ(θ) after breakup. All-order formalism method based on the eikonal approximation, with a regularized first order Coulomb term.
doi: 10.1103/PhysRevC.84.014613
2010BL08 Phys.Rev. C 82, 034313 (2010) G.Blanchon, N.Vinh Mau, A.Bonaccorso, M.Dupuis, N.Pillet Particle-particle random-phase approximation applied to beryllium isotopes NUCLEAR STRUCTURE 8,10,12,14Be; calculated levels, J, π, pp-RPA amplitudes, E1 strength distribution, S(2n), rms radii. Comparison to experimental data. Particle-particle random-phase approximation (pp-RPA) method using Woods-Saxon potential for the neutron-core interaction and D1S Gogny force for the neutron-neutron interaction.
doi: 10.1103/PhysRevC.82.034313
2010BL12 J.Phys.:Conf.Ser. 205, 012003 (2010) G.Blanchon, A.Bonaccorso, D.M.Brink, N.Vinh Mau 10-11Li and 13-14Be studied by projectile fragmentation and pp-RPA NUCLEAR STRUCTURE 10Li, 13Be; calculated halo nuclei scattering lengths, resonance parameters, 2n separation energies. 12,14Be; calculated halo nuclei radii, 2n separation energies. Time-dependent projectile fragmentation model with core-vibration model of two-neutron halo nuclei. Compared with data. NUCLEAR REACTIONS 12C(11Li, n9Li), (14Be, n12Be), E=250 MeV/nucleon; calculated σ(E), n-9Li and n-12Be relative energy spectrum using time-dependent projectile fragmentation model with core-vibration model of two-neutron halo nuclei. Compared with data.
doi: 10.1088/1742-6596/205/1/012003
2010HA04 Phys.Rev. C 81, 021302 (2010) C.C.Hall, E.M.Lunderberg, P.A.DeYoung, T.Baumann, D.Bazin, G.Blanchon, A.Bonaccorso, B.A.Brown, J.Brown, G.Christian, D.H.Denby, J.Finck, N.Frank, A.Gade, J.Hinnefeld, C.R.Hoffman, B.Luther, S.Mosby, W.A.Peters, A.Spyrou, M.Thoennessen First observation of excited states in 12Li NUCLEAR REACTIONS Be(14B, 2p), E=53.4 MeV/nucleon; measured neutron and 11Li spectra from decay of 12Li, and (11Li)n-coin using Modular Neutron Array (MONA). 12Li; deduced levels, J, π. Comparisons with shell model calculations using WBP interaction.
doi: 10.1103/PhysRevC.81.021302
2010SP02 Phys.Lett. B 683, 129 (2010) A.Spyrou, T.Baumann, D.Bazin, G.Blanchon, A.Bonaccorso, E.Breitbach, J.Brown, G.Christian, A.DeLine, P.A.DeYoung, J.E.Finck, N.Frank, S.Mosby, W.A.Peters, A.Russel, A.Schiller, M.J.Strongman, M.Thoennessen First evidence for a virtual 18B ground state NUCLEAR REACTIONS Be(19C, pX)18B, E=62 MeV/nucleon; Be(17C, pX)16B, E=55 MeV/nucleon; measured decay energy spectra, (fragment)(neutron)-coin using time of flight technique with Modular Neutron Array (MoNA). 16B; deduced ground state energies. 17B; deduced level energies, J, π. 18B; calculated level energies, J, π. Comparison with shell model calculations using WBP interaction and other data. Secondary radioactive beam.
doi: 10.1016/j.physletb.2009.12.016
2009LI55 Phys.Rev. C 80, 064607 (2009) L.L.Li, Z.H.Li, E.G.Zhao, S.G.Zhou, W.Zuo, A.Bonaccorso, U.Lombardo Isospin splitting of the nucleon-nucleus optical potential NUCLEAR REACTIONS 28Si, 90Zr, 208Pb(n, n)(p, p), (n, γ), (p, γ), E<100 MeV; calculated volume term of the optical model potential and isospin splitting using the Brueckner-Hartree-Fock approach with three-body force.
doi: 10.1103/PhysRevC.80.064607
2007BL02 Nucl.Phys. A784, 49 (2007) G.Blanchon, A.Bonaccorso, D.M.Brink, A.Garcia-Camacho, N.Vinh Mau Unbound exotic nuclei studied by projectile fragmentation NUCLEAR REACTIONS 12C(11Be, n10Be), E=67 MeV/nucleon; calculated relative energy spectrum. NUCLEAR STRUCTURE 13,14Be; calculated resonance features in unbound neutron states.
doi: 10.1016/j.nuclphysa.2006.11.033
2007BL19 Nucl.Phys. A791, 303 (2007) G.Blanchon, A.Bonaccorso, D.M.Brink, N.Vinh Mau 10Li spectrum from 11Li fragmentation NUCLEAR REACTIONS 12C(11Li, n)9Li, E=264 MeV/nucleon; calculated σ as function of neutron-9Li relative energy using a projectile fragmentation model.
doi: 10.1016/j.nuclphysa.2007.04.014
2007BO26 Nucl.Phys. A787, 433c (2007) Status of art of reaction models for projectiles far from stability NUCLEAR REACTIONS Pb(34Si, X), E=70 MeV/nucleon; calculated σ. Pb(8B, p)7Be, E=936 MeV/nucleon; calculated residual momentum distribution. 12C(11Be, nX), E=69 MeV/nucleon; 12C(14Be, nX), E=250 MeV/nucleon; calculated σ(E). Various models reviewed. Reaction mechanism features and final state interactions discussed. Comparison with data.
doi: 10.1016/j.nuclphysa.2006.12.065
2007GA33 Phys.Rev. C 76, 014607 (2007) A.Garcia-Camacho, G.Blanchon, A.Bonaccorso, D.M.Brink All orders proton breakup from exotic nuclei NUCLEAR REACTIONS C, Pb(8B, p), E=936 MeV/nucleon; calculated single particle cross sections and particle momentum distributions.
doi: 10.1103/PhysRevC.76.014607
2006GA29 Nucl.Phys. A776, 118 (2006) A.Garcia-Camacho, A.Bonaccorso, D.M.Brink All orders breakup of heavy exotic nuclei in a semiclassical model NUCLEAR REACTIONS 208Pb(11Be, n10Be), E=70 MeV/nucleon; calculated Coulomb breakup σ(E), relative energy spectra. 208Pb(28Si, X), E=70 MeV/nucleon; calculated breakup σ. 208Pb(46Ar, 45ArX), E=70 MeV/nucleon; calculated parallel momentum distributions. 208Pb(n, X), (n, n), (n, n'), E=0-130 MeV; calculated total, elastic, and inelastic σ. Semiclassical model, full Coulomb potential.
doi: 10.1016/j.nuclphysa.2006.07.033
2005BO50 Eur.Phys.J. A 25, Supplement 1, 293 (2005) Unbound exotic nuclei studied via projectile fragmentation reactions NUCLEAR REACTIONS 12C(14Be, 12BeX), (14B, 12BeX), E=70 MeV/nucleon; calculated neutron-nucleus relative energy spectrum, role of neutron transfer to unbound states.
doi: 10.1140/epjad/i2005-06-002-8
2005BO51 Eur.Phys.J. A 25, Supplement 1, 753 (2005) Exotic nuclei within the INFN-PI32 network
doi: 10.1140/epjad/i2005-06-101-6
2005IB01 Nucl.Phys. A748, 414 (2005) Coulomb breakup effects on the optical potentials of weakly bound nuclei NUCLEAR REACTIONS 208Pb(10Be, 10Be), (11Be, 11Be), E=20, 40, 80 MeV/nucleon; calculated σ(θ), Coulomb breakup effects. Optical model.
doi: 10.1016/j.nuclphysa.2004.12.036
2004BL11 Nucl.Phys. A739, 259 (2004) G.Blanchon, A.Bonaccorso, N.Vinh Mau Unbound exotic nuclei studied by transfer to the continuum reactions NUCLEAR REACTIONS 9Li(d, p), (9Be, 8Be), (13C, 12C), E=2 MeV/nucleon; calculated transition probabilities for neutron transfer to unbound states, final state interaction features.
doi: 10.1016/j.nuclphysa.2004.04.106
2004BO04 Phys.Rev. C 69, 024615 (2004) A.Bonaccorso, D.M.Brink, C.A.Bertulani Proton vs neutron halo breakup NUCLEAR REACTIONS 58Ni, 208Pb(8B, X), (17F, X), E not given; calculated Coulomb and nuclear potentials. 208Pb(11Be, n10Be), (17F, p16O)=40 MeV/nucleon; calculated breakup σ. Differences between proton and neutron halo structures discussed.
doi: 10.1103/PhysRevC.69.024615
2004CA45 Phys.Rev. C 70, 054602 (2004) F.Carstoiu, E.Sauvan, N.A.Orr, A.Bonaccorso Extended sudden approximation modeling of high-energy nucleon-removal reactions NUCLEAR REACTIONS C(12B, 11BX), (13B, 12BX), (14B, 13BX), (15B, 14BX), (14C, 13CX), (15C, 14CX), (16C, 15CX), (17C, 16CX), (18C, 17CX), (17N, 16NX), (18N, 17NX), (19N, 18NX), (20N, 19NX), (21N, 20NX), (19O, 18OX), (20O, 19OX), (21O, 20OX), (22O, 21OX), (23O, 22OX), (22F, 21FX), (23F, 22FX), (24F, 23FX), (25F, 24FX), E ≈ 43-68 MeV/nucleon; calculated one-neutron removal σ, core-fragment longitudinal momentum distribution.
doi: 10.1103/PhysRevC.70.054602
2003BO51 Acta Phys.Hung.N.S. 18, 193 (2003) Reaction Mechanisms with Exotic Nuclei
doi: 10.1556/APH.18.2003.2-4.12
2003MA20 Nucl.Phys. A720, 337 (2003); Erratum Nucl.Phys. A741, 381 (2004) J.Margueron, A.Bonaccorso, D.M.Brink A non-perturbative approach to halo breakup NUCLEAR REACTIONS 208Pb(11Be, n10Be), E=72 MeV/nucleon; 208Pb(19C, n18C), E=67 MeV/nucleon; calculated neutron spectra relative to core fragment. 197Au(11Be, n10Be), E=41 MeV/nucleon; calculated neutron σ(θ). Coulomb and nuclear contributions, high-order effects discussed. Comparison with data.
doi: 10.1016/S0375-9474(03)01092-3
2002BO25 Nucl.Phys. A706, 322 (2002) Optical Potentials of Halo and Weakly Bound Nuclei NUCLEAR REACTIONS 7Be(11Be, X), E=57, 550 MeV; calculated optical potential parameters. 12C(11Be, 11Be), E=542 MeV; calculated σ(θ). Surface component of potential for weakly bound nuclei discussed.
doi: 10.1016/S0375-9474(02)00755-8
2002EN02 Phys.Rev. C65, 034318 (2002) J.Enders, A.Bauer, D.Bazin, A.Bonaccorso, B.A.Brown, T.Glasmacher, P.G.Hansen, V.Maddalena, K.L.Miller, A.Navin, B.M.Sherrill, J.A.Tostevin Single-Neutron Knockout from 34, 35Si and 37S NUCLEAR REACTIONS 9Be(34Si, 33SiX), (35Si, 34SiX), E ≈ 73 MeV; 9Be(37S, 36SX), E ≈ 69 MeV; measured particle spectra, γ-spectra, one-neutron removal σ; deduced spectroscopic factors. 33,34Si deduced transition probabilities. Comparisons with model predictions.
doi: 10.1103/PhysRevC.65.034318
2002MA26 Nucl.Phys. A703, 105 (2002) J.Margueron, A.Bonaccorso, D.M.Brink Coulomb-Nuclear Coupling and Interference Effects in the Breakup of Halo Nuclei NUCLEAR REACTIONS 9Be, 48Ti, 197Au(11Be, n10Be), E=30, 41, 120 MeV/nucleon; 208Pb(11Be, n10Be), E=72 MeV/nucleon; calculated neutron spectra, σ(E, θ), integrated breakup σ; deduced role of Coulomb-nuclear coupling and interference effects.
doi: 10.1016/S0375-9474(01)01336-7
2001BO10 Phys.Rev. C63, 044604 (2001) Comparison of Transfer-to-Continuum and Eikonal Models of Projectile Fragmentation Reactions NUCLEAR REACTIONS 9Be(n, n), E=20-180 MeV; calculated σ. 9Be(12Be, X), E=20-100 MeV; calculated breakup σ. Comparison of eikonal and transfer-to-continuum models. Comparison with data.
doi: 10.1103/PhysRevC.63.044604
2000BO04 Phys.Rev. C61, 034605 (2000) Final State Interaction Effects in Breakup Reactions of Halo Nuclei NUCLEAR REACTIONS 9Be, 28Si(11Be, n10Be), E=10-120 MeV/nucleon; calculated absorptive and diffractive breakup σ, ejectile energy spectrum; deduced final state interaction effects. Optical potential for neutron-target interactions. Comparisons with data.
doi: 10.1103/PhysRevC.61.034605
1999BO20 Nucl.Phys. A649, 315c (1999) Neutron Transfer to the Continuum Reactions NUCLEAR REACTIONS 208Pb(40Ar, 39Ar), E=41 MeV/nucleon; 9Be(17C, X), (19C, X), E not given; analyzed data; deduced neutron transfer features, application to structure studies.
doi: 10.1016/S0375-9474(99)00077-9
1999BO37 Acta Phys.Pol. B30, 1421 (1999) Transfer Reactions Near the Coulomb Barrier
1999BO49 Phys.Rev. C60, 054604 (1999) Initial State Dependence of the Breakup of Weakly Bound Carbon Isotopes NUCLEAR REACTIONS 9Be, 12C, 208Pb(19C, n18C), E=88 MeV/nucleon; 9Be(17C, n16C), E=84 MeV/nucleon; calculated breakup σ; deduced initial state dependence, energy sharing effects. Theory of transfer to the continuum.
doi: 10.1103/PhysRevC.60.054604
1998BO01 Phys.Rev. C57, R22 (1998) Neutron Angular Distribution from Halo Breakup NUCLEAR REACTIONS 9Be(11Be, n10Be), E=41 MeV/nucleon; calculated neutron σ(θ, φ), momentum distributions. Diffractional model.
doi: 10.1103/PhysRevC.57.R22
1998BO28 Phys.Rev. C58, 2864 (1998) Dynamical Effects on the Parallel Momentum Distributions of Neutrons from Halo Breakup NUCLEAR REACTIONS 9Be, 208Pb(11Be, n10Be), E=10, 41, 72 MeV/nucleon; calculated neutron spectra, parallel momentum distributions. 9Be, 28Si, 208Pb(11Be, n10Be), E=5-55 MeV/nucleon; calculated total, elastic, inelastic breakup σ. Theory of transfer to the continuum.
doi: 10.1103/PhysRevC.58.2864
1997BO08 Nucl.Phys. A615, 245 (1997) Low Energy Dipole Modes in 14C, 12Be and 11Li. Coulomb Dissociation of 11Li NUCLEAR STRUCTURE 14C, 12Be, 11Li; calculated levels, low energydipoles modes, B(λ). Two-neutron pairing model. NUCLEAR REACTIONS 208Pb, 63Cu, 27Al, 12C(11Li, X), E=0.03-0.8 Gev/nucleon; calculated two-neutron Coulomb dissociation σ. Two-neutron pairing model.
doi: 10.1016/S0375-9474(97)00013-4
1997BO21 Z.Phys. A358, 329 (1997) A.Bonaccorso, Z.Zelazny, E.Piasecki Separation of Coulomb Fission from Nuclear Fission at Medium Energies NUCLEAR REACTIONS 197Au(238U, 239U), E=8.1-50 MeV/nucleon; calculated electromagnetic field induced fission σ vs E; deduced Coulomb, nuclear fission separation related features.
doi: 10.1007/s002180050336
1996BO04 Phys.Rev. C53, 849 (1996) Neutron Elastic and Inelastic Breakup in Reactions Induced by 20Ne NUCLEAR REACTIONS 48Ca(20Ne, 19Ne), E=48 MeV/nucleon; analyzed σ(θ), reaction σ. Elastic, inelastic breakup.
doi: 10.1103/PhysRevC.53.849
1995BO02 Phys.Rev. C51, 822 (1995) High Energy Single Particle States in the Continuum NUCLEAR STRUCTURE 208Pb, 91Zr; calculated escape, spreading widths. NUCLEAR REACTIONS 120Sn, 64Ni, 90Zr, 208Pb(α, 3HeX), E=30 MeV/nucleon; 48Ca, 207Pb(20Ne, 19NeX), E=48 MeV/nucleon; 90Zr(20Ne, 19NeX), E=40 MeV/nucleon; calculated inclusive spectra. Semi-classical S-matrix, Bonaccorso-Brink reaction model.
doi: 10.1103/PhysRevC.51.822
1995BO08 Nucl.Phys. A583, 433c (1995) Single Particle States in the Continuum NUCLEAR REACTIONS 207Pb(20Ne, 19Ne), E=48 MeV/nucleon; 48Ca(20Ne, 19Ne), E=48 MeV/nucleon; analyzed data; deduced angular momentum terms overlap reaction dependence.
doi: 10.1016/0375-9474(94)00699-N
1994BO02 Phys.Rev. C49, 329 (1994) A.Bonaccorso, I.Lhenry, T.Suomijarvi Inclusive Spectra of Stripping Reactions Induced by Heavy Ions NUCLEAR REACTIONS 207Pb, 209Bi(20Ne, 19Ne), E=48 MeV/nucleon; 208Pb(20Ne, 19Ne), E=40 MeV/nucleon; 207Pb, 209Bi(36Ar, 35Ar), E=42 MeV/nucleon; 208Pb(40Ar, 39Ar), E=41 MeV/nucleon; calculated spectra; deduced unbound high spin states role in structure. Bonaccorso-Brink single-particle transfer model.
doi: 10.1103/PhysRevC.49.329
1992BO24 Phys.Rev. C46, 700 (1992) Inelastic Breakup in Heavy-Ion Reactions NUCLEAR REACTIONS 208Pb(20Ne, 19Ne), E=40, 30 MeV/nucleon; 208Pb(14N, 13N), E=60 MeV/nucleon; calculated spectra; deduced various processes energy evolution. Inelastic breakup.
doi: 10.1103/PhysRevC.46.700
1991BO01 Phys.Rev. C43, 299 (1991) Absorption Versus Breakup in Heavy-Ion Reactions NUCLEAR REACTIONS 90Zr(20Ne, 19Ne), E=500 MeV; calculated breakup, absorption spectra. Green's function techniques.
doi: 10.1103/PhysRevC.43.299
1991BO24 Phys.Rev. C44, 1559 (1991) Stripping to the Continuum of 208Pb NUCLEAR REACTIONS 208Pb(20Ne, 19Ne), E=20-40 MeV/nucleon; 208Pb(14N, 13C), E=60 MeV/nucleon; calculated total reaction spectra.
doi: 10.1103/PhysRevC.44.1559
1988BO26 Phys.Rev. C38, 1776 (1988) Nucleon Transfer to Continuum States NUCLEAR REACTIONS 208Pb(16O, 15O), E=500, 800 MeV; 48Ti(40Ar, 39Ar), E=1760 MeV; 197Au(20Ne, 19F), E=341 MeV; calculated angle-integrated spectra. Semi-classical model, continuum nuclear transfer.
doi: 10.1103/PhysRevC.38.1776
1987BO48 J.Phys.(London) G13, 1407 (1987) A.Bonaccorso, D.M.Brink, L.Lo Monaco Nucleon Transfer in Heavy-Ion Reactions: Energy dependence of the cross section NUCLEAR REACTIONS, MECPD 208Pb(16O, 15O), E ≈ 20-100 MeV/nucleon; 12C(13C, 12C), E ≈ 20-80 MeV/nucleon; calculated transfer σ(E); deduced energy dependence. Analytical approach.
doi: 10.1088/0305-4616/13/11/013
1985BO30 Nucl.Phys. A441, 555 (1985) A.Bonaccorso, G.Piccolo, D.M.Brink Nucleon Transfer to Nuclear Matter and the Absorptive Heavy-Ion Scattering Potential NUCLEAR REACTIONS 40Ca(16O, X), E=55.6, 103.6, 214.1 MeV; 58Ni(16O, X), E=45, 60, 81 MeV; 208Pb(16O, X), E=129.5, 192, 312.6 MeV; 28Si(16O, X), E=36, 55, 81 MeV; 88Sr(16O, X), E=56, 59 MeV; 40Ca(40Ca, X), E=143.6, 186, 240 MeV; calculated nucleon transfer probability per unit time. First-order perturbation transfer mechanism treatment.
doi: 10.1016/0375-9474(85)90162-9
1982BO23 Nucl.Phys. A384, 161 (1982) The Imaginary Part of the α - 40Ca Optical Potential NUCLEAR REACTIONS 40Ca(α, α), E=29, 56, 104, 166 MeV; calculated phase shift imaginary part vs impact parameter; deduced optical potential imaginary term. Phenomenological α-nucleon interaction, harmonic oscillator wave functions.
doi: 10.1016/0375-9474(82)90311-6
1979BO17 Nucl.Phys. A324, 115 (1979) A.Bonaccorso, M.Di Toro, J.Lomnitz-Adler Exponential Convergence and Acceleration of Hartree-Fock Calculations NUCLEAR STRUCTURE 20Ne, 28Si; calculated shape, quadrupole moment. Hartree-Fock formalism, Skyrme interaction, exponential convergence during iteration procedure.
doi: 10.1016/0375-9474(79)90082-4
1977BO33 Phys.Lett. 72B, 27 (1977) A.Bonaccorso, M.Di Toro, G.Russo A Direct Determination of the Density Matrix in a Nuclear System NUCLEAR STRUCTURE 20Ne; calculated one-body density matrix.
doi: 10.1016/0370-2693(77)90054-5
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