NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = D.M.Brink Found 85 matches. 2021BO15 Eur.Phys.J. A 57, 171 (2021) Models of breakup: a final state interaction problem
doi: 10.1140/epja/s10050-021-00448-1
2018BO19 Eur.Phys.J. A 54, 152 (2018) On the eikonal approach to nuclear diffraction dissociation
doi: 10.1140/epja/i2018-12599-9
2018BR11 Phys.Rev. C 97, 064304 (2018) Skyrme density functional description of the double magic 78Ni nucleus NUCLEAR STRUCTURE 68,69,70,71,72,73,74,75,76,77,78Ni; calculated proton single-particle energy difference between the unoccupied 1f5/2 and occupied 1f7/2 levels, proton and neutron single particle energies around the Fermi sea with and without tensor force by Hartree-Fock calculations using the Skryme energy density functional; deduced contribution of tensor force to single-particle spectra gap, and doubly-magic character of 78Ni.
doi: 10.1103/PhysRevC.97.064304
2011AB09 Nucl.Phys. A864, 38 (2011) V.I.Abrosimov, D.M.Brink, A.Dellafiore, F.Matera Self-consistency and search for collective effects in semiclassical pairing theory
doi: 10.1016/j.nuclphysa.2011.06.020
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
2008AB04 Nucl.Phys. A800, 1 (2008) V.I.Abrosimov, D.M.Brink, A.Dellafiore, F.Matera Kinetic equation for finite systems of fermions with pairing NUCLEAR STRUCTURE A=208; calculated quadrupole and octupole strength functions with kinetic Vlasov equations and the effects of pairing correlations.
doi: 10.1016/j.nuclphysa.2007.11.009
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
2007BR12 Phys.Rev. C 75, 064311 (2007) Evolution of nuclear shells with the Skyrme density dependent interaction NUCLEAR STRUCTURE Z=20, Z=50, N=82; calculated proton and neutron single particle energies using Hartree-Fock method and density dependent Skyrme interaction.
doi: 10.1103/PhysRevC.75.064311
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
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
2004BR31 Nucl.Phys. A738, 195 (2004) Concluding remarks
doi: 10.1016/j.nuclphysa.2004.04.031
2004BR38 Prog.Theor.Phys.(Kyoto), Suppl. 154, 268 (2004) Fusion and Heavy Ion Reactions
doi: 10.1143/PTPS.154.268
2004KI18 Prog.Theor.Phys.(Kyoto), Suppl. 154, 317 (2004) S.Kimura, N.Takigawa, M.Abe, D.M.Brink, A.Bonasera Influence of Tunneling on Electron Screening in Low Energy Nuclear Reactions NUCLEAR REACTIONS 2H, 3He(d, X), E(cm) ≈ 1-1000 keV; calculated electron screening energy, tunneling effects.
doi: 10.1143/PTPS.154.317
2003KI01 Phys.Rev. C 67, 022801 (2003) S.Kimura, N.Takigawa, M.Abe, D.M.Brink Influence of tunneling on electron screening in low energy nuclear reactions in laboratories NUCLEAR REACTIONS 2H, 3He(d, X), E(cm)=1-500 keV; calculated electron screening potential, tunneling effects.
doi: 10.1103/PhysRevC.67.022801
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
2002BR02 Nucl.Phys. A697, 689 (2002) The Heavy-Ion Spin-Orbit Interaction NUCLEAR REACTIONS 58Ni(6Li, 6Li'), (7Li, 7Li'), E(cm)=12.7-20.7 MeV; calculated vector analyzing powers. Effective spin-orbit interaction.
doi: 10.1016/S0375-9474(01)01263-5
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
2001BA90 Phys.Rev.Lett. 87, 182501 (2001) V.Baran, D.M.Brink, M.Colonna, M.Di Toro Collective Dipole Bremsstrahlung in Fusion Reactions NUCLEAR REACTIONS 100Mo(40Ca, X), E=4 MeV/nucleon; 98Mo(16O, X), E=4, 8, 14, 20 MeV/nucleon; calculated dipole moment time evolution, γ spectra; deduced role of bremsstrahlung mechanism in pre-equilibrium and thermal emission.
doi: 10.1103/PhysRevLett.87.182501
1999BR14 Nucl.Phys. A650, 418 (1999) The Heavy-Ion Spin-Orbit Interaction
doi: 10.1016/S0375-9474(99)00119-0
1999BR19 Nucl.Phys. A649, 218c (1999) Summary Talk: Giant resonances at finite temperature
doi: 10.1016/S0375-9474(99)00065-2
1999TA02 Phys.Rev. C59, R593 (1999); Erratum Phys.Rev. C60, 069901 (1999) N.Takigawa, Y.Nozawa, K.Hagino, A.Ono, D.M.Brink Bremsstrahlung in α Decay RADIOACTIVITY 210Po(α); analyzed bremsstrahlung spectra; deduced contributions.
doi: 10.1103/PhysRevC.59.R593
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
1998BR06 J.Phys.(London) G24, 867 (1998) Finite-Size Effects on QGP
doi: 10.1088/0954-3899/24/4/015
1998SU09 Phys.Lett. 421B, 25 (1998) Geometric Magnetism and the Heavy Ion Spin-Orbit Interaction
doi: 10.1016/S0370-2693(98)00003-3
1998UR05 Phys.Rev. C58, 3163 (1998) C.A.Ur, D.Bucurescu, S.M.Lenzi, G.Martinez-Pinedo, D.R.Napoli, D.Bazzacco, F.Brandolini, D.M.Brink, J.A.Cameron, E.Caurier, G.de Angelis, M.De Poli, A.Gadea, S.Lunardi, N.Marginean, M.A.Nagarajan, P.Pavan, C.Rossi Alvarez, C.E.Svensson Excited States in 52Fe and the Origin of the Yrast Trap at Iπ = 12+ NUCLEAR REACTIONS 28Si(28Si, α), E=115 MeV; measured Eγ, Iγ, γγ-coin, DSA. 52Fe deduced levels, J, π, T1/2, B(E2), isomer decay B(E4) upper limits. GASP spectrometer. NUCLEAR STRUCTURE 52Fe; calculated levels, J, π, quadrupole moments, isomer decay log ft, branching ratios. Comparison with 44Ti.
doi: 10.1103/PhysRevC.58.3163
1997LE15 Phys.Rev. C56, 1313 (1997) S.M.Lenzi, C.A.Ur, D.R.Napoli, M.A.Nagarajan, D.Bazzacco, D.M.Brink, M.A.Cardona, G.de Angelis, M.De Poli, A.Gadea, D.Hojman, S.Lunardi, N.H.Medina, C.Rossi Alvarez Band Termination and Second Backbending in 50Cr NUCLEAR REACTIONS 24Mg(32S, 2pα), E=130 MeV; measured Eγ, Iγ, γγ-, (charged-particle)γ-coin, γγ(θ), DCO ratios. 50Cr deduced high-spin levels, J, π, configurations, band structure. Cranked shell-model analysis.
doi: 10.1103/PhysRevC.56.1313
1995BO07 Nucl.Phys. A583, 101c (1995) P.F.Bortignon, M.Braguti, D.M.Brink, R.A.Broglia, C.Brusati, F.Camera, W.Cassing, M.Cavinato, N.Giovanardi, F.Gulminelli On the Giant Dipole Resonance Excitation in Very Hot Nuclei NUCLEAR REACTIONS 90Zr(36Ar, X), E at 27 MeV/nucleon; calculated dipole strength function; deduced model impact parameter choice critical role in GDR excitation. BNV model.
doi: 10.1016/0375-9474(94)00639-5
1995HA14 Phys.Rev. C51, 3190 (1995) K.Hagino, N.Takigawa, J.R.Bennett, D.M.Brink Effects of Finite Excitation Energy of Environment on Fast Quantum Tunneling NUCLEAR REACTIONS 194Pt, 148Sm(16O, X), E not given; calculated fusion σ(E); deduced environment excitation energy role on fast quantum tunneling.
doi: 10.1103/PhysRevC.51.3190
1995RO02 Nucl.Phys. A584, 362 (1995) E.J.Roberts, C.V.Sukumar, R.C.Johnson, D.M.Brink Semi-Classical Analysis of Scattering of Deformed Heavy-Ions Below the Coulomb Barrier NUCLEAR REACTIONS 58Ni(polarized 7Li, 7Li), E=10 MeV; calculated T20(θ), T21(θ), T22(θ). Semi-classical approach.
doi: 10.1016/0375-9474(94)00458-Y
1995SU09 Nucl.Phys. A587, 413 (1995) A Path-Integral Approach to Inclusive Processes
doi: 10.1016/0375-9474(95)00034-X
1994BO10 Nucl.Phys. A569, 215c (1994) A.Bonasera, M.Di Toro, A.Smerzi, D.M.Brink Pre-Equilibrium and Temperature Effects on the Disappearing of Giant Dipole Resonances in Highly Excited Nuclei
doi: 10.1016/0375-9474(94)90112-0
1994BR20 Nucl.Phys. A574, 207c (1994) Collective Motion in Excited Nuclei NUCLEAR STRUCTURE A=108-112; compiled, reviewed GDR data, analyses. Collective motion.
doi: 10.1016/0375-9474(94)90046-9
1994SM01 Phys.Lett. 320B, 216 (1994) A.Smerzi, M.Di Toro, D.M.Brink Quenching of Photon Decay in Hot Giant Dipole Resonances NUCLEAR STRUCTURE Sn; analyzed GDR widths, neutron, proton emission yields in Sn isotopes vs excitation energy.
doi: 10.1016/0370-2693(94)90647-5
1993AI01 Nucl.Phys. A560, 765 (1993) Second RPA Calculations of the Charge-Exchange Quadrupole Response Functions in Closed-Shell Nuclei NUCLEAR STRUCTURE 40Ca, 60Ni, 90Zr, 120Sn, 208Pb; calculated charge exchange quadrupole states damping widths, response functions. Microscopic model, second RPA theory.
doi: 10.1016/0375-9474(93)90170-3
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
1991AI01 Phys.Lett. 255B, 163 (1991) S.Ait-Tahar, D.M.Brink, S.Adachi Damping Widths of the Charge Exchange IVQ States in 90Zr NUCLEAR STRUCTURE 90Zr; calculated isovector quadrupole strength distribution, spreading width. Self-consistent Hartree-Fock plus charge exchange RPA.
doi: 10.1016/0370-2693(91)90230-N
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
1988HA03 Nucl.Phys. A476, 107 (1988) Spin Dependence of Neutron Transfer in Heavy Ion Reactions NUCLEAR REACTIONS 208Pb(16O, 15O), (13C, 12C), (13C, 11C), (12C, 11C), E not given; calculated transfer probability; deduced spin dependence.
doi: 10.1016/0375-9474(88)90376-4
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
1987OH08 Phys.Rev. C36, 966 (1987) Internal and Barrier Wave Interpretation of the Oscillations of the Fusion Excitation Function NUCLEAR REACTIONS, ICPND 40Ca(α, α), E=5-20 MeV; calculated phase shifts vs E. 40Ca(α, X), E=5-20 MeV; calculated fusion σ(E). 44Ti deduced levels, J, π. Semi-classical model.
doi: 10.1103/PhysRevC.36.966
1987OH09 Phys.Rev. C36, 1375 (1987) Origin of the Oscillations in the 12C + 12C Fusion Excitation Function in Terms of Internal and Barrier Waves NUCLEAR REACTIONS 12C(12C, X), E ≈ 8-32 MeV; calculated fusion σ(E). 24Mg deduced levels, J, π. Semi-classical method.
doi: 10.1103/PhysRevC.36.1375
1986BR18 Nucl.Phys. A456, 205 (1986) D.M.Brink, A.Dellafiore, M.Di Toro Solution of the Vlasov Equation for Collective Modes in Nuclei NUCLEAR STRUCTURE A=40, 208; calculated isoscalar monopole, octupole strength distributions. Semi-classical theory, Vlasov equation.
doi: 10.1016/0375-9474(86)90390-8
1986DO02 Nucl.Phys. A448, 333 (1986) F.D.Dos Aidos, C.V.Sukumar, D.M.Brink Corrections to the Alder-Winther Theory of Coulomb Excitation NUCLEAR REACTIONS 152Sm(16O, 16O'), E=109.2 MeV; calculated Coulomb excitation probability corrections. Corrections to Alder-Winther theory.
doi: 10.1016/0375-9474(86)90096-5
1986FA11 J.Phys.(London) G12, L251 (1986) M.Fatemian, R.A.Baldock, D.M.Brink Coulomb Excitation of 7Li in the Cluster Model NUCLEAR REACTIONS 208Pb(7Li, 7Li'), E=20 MeV; 138Ba(7Li, 7Li'), E not given; calculated Coulomb excitation probability. Cluster model.
doi: 10.1088/0305-4616/12/11/002
1986SC08 Nucl.Phys. A452, 1 (1986) The Moment of Inertia in the Interacting Boson Model NUCLEAR STRUCTURE 160Yb; calculated levels, band structure. Interacting boson model, self-consistent cranking.
doi: 10.1016/0375-9474(86)90505-1
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
1985LO10 J.Phys.(London) G11, 935 (1985) Perturbation Approach to Nucleon Transfer in Heavy-Ion Reactions NUCLEAR REACTIONS 208Pb(16O, 15O), E=139, 312.6 MeV; 26Mg(11B, 10B), E=114 MeV; calculated σ(θ). Heavy ion nucleon transfer reactions, perturbation approach.
doi: 10.1088/0305-4616/11/8/010
1985ST25 Phys.Rev. C32, 1937 (1985) Effect of Shell Structure on the Nucleon Transfer Contribution to the Imaginary Part of the Heavy Ion Optical Potential NUCLEAR REACTIONS 40Ca(16O, 16O), E=40-214.1 MeV; 60Ni(16O, 16O), E=142 MeV; 208Pb(16O, 16O), E=129.5-312.6 MeV; 32S(32S, 32S), E=90.9 MeV; 40Ca(40Ca, 40Ca), E=143.6-240 MeV; calculated heavy ion optical potential imaginary term near strong absorption radius.
doi: 10.1103/PhysRevC.32.1937
1984SC26 Phys.Lett. 143B, 269 (1984) Calculations away from SU(3) Symmetry by Cranking the Interacting Boson Model NUCLEAR STRUCTURE 168Er; calculated levels, band characteristics. Self-consistent cranking calculation.
doi: 10.1016/0370-2693(84)91463-1
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
1982ST08 Phys.Rev. C25, 2450 (1982) Nucleon Transfer Contribution to the Absorptive Potential in Heavy-Ion Scattering NUCLEAR REACTIONS 40Ca(16O, 16O), E=55.6, 103.6, 214.1 MeV; 58Ni(16O, 16O), E=45, 60, 81 MeV; 60Ni(16O, 16O), E=142 MeV; 208Pb(16O, 16O), E=129.5, 192, 312.6 MeV; 40Ca(20Ne, 20Ne), E=151 MeV; 32S(32S, X), E=90.9 MeV; 40Ca(40Ca, 40Ca), E=143.6, 186, 240 MeV; 209Bi(136Xe, 136Xe), E=940, 1130 MeV; calculated nucleon transfer contribution to absorption potential. Proximity method, Pauli blocking, barrier penetration effects.
doi: 10.1103/PhysRevC.25.2450
1981BO21 Phys.Lett. 102B, 109 (1981) A.Bouyssy, N.Vinh Mau, D.M.Brink A Critical Analysis of the Eikonal Approximation in the Derivation of the Alpha-Nucleus Potential NUCLEAR REACTIONS 40Ca(α, α), E=75 MeV; calculated absorptive alpha-nucleus potential term. Exact Greens function, eikonal approximation.
doi: 10.1016/0370-2693(81)91041-8
1981BR01 J.Phys.(London) G7, 43 (1981) The Role of the Attractive Nuclear Potential in Determining Reaction Cross Sections NUCLEAR REACTIONS 40Ca(α, X), E=0.03-1.37 GeV; 12C(12C, X), E=0.07-10.44 GeV; calculated σ(reaction, E), transmission coefficients; deduced role of attractive nuclear potential. Woods-Saxon, Woods-Saxon squared potentials.
doi: 10.1088/0305-4616/7/1/009
1981BR11 Phys.Rev. C24, 144 (1981) Time-Dependent Hartree-Fock and the One-Body Dissipation for Head-On Collisions NUCLEAR REACTIONS 139La(86Kr, X), E=360-1000 MeV; 209Bi(84Kr, X), E=500-1000 MeV; calculated interaction potential vs separation distance, classical trajectories. Head-on collisions, window formula for friction, one-body dissipation.
doi: 10.1103/PhysRevC.24.144
1980TU03 Phys.Lett. B95, 35 (1980) G.Tungate, R.Bottger, P.Egelhof, K.-H.Mobius, Z.Moroz, E.Steffens, W.Dreves, D.Fick, D.M.Brink, T.F.Hill Investigation of the 58Ni(7Li, 6Li)59Ni Reaction with Vector Polarized 7Li NUCLEAR REACTIONS 58Ni(polarized 7Li, 6Li), E=20.3 MeV; measured σ(θ), vector analyzing power vs θ; deduced transferred neutron polarization effects.
doi: 10.1016/0370-2693(80)90393-7
1979HA25 J.Phys.(London) G5, 771 (1979) The Transfer Amplitude and Angular Distributions in Heavy-Ion Reactions NUCLEAR REACTIONS 26Mg(11B, 10B), E=114 MeV; calculated σ(θ). Analytic expressions, transfer amplitude dependent on distance of closest approach.
doi: 10.1088/0305-4616/5/6/005
1978HA45 J.Phys.(London) G4, 1573 (1978) A Study of Semiclassical Approximations for Heavy-Ion Transfer Reactions NUCLEAR REACTIONS 26Mg(11B, 10B), (11B, 10Be), E=114 MeV; calculated σ(θ). Semi-classical approximation for HI transfer reactions.
doi: 10.1088/0305-4616/4/10/008
1977BR06 Nucl.Phys. A279, 159 (1977) Barrier Penetration Effects in the Semi-Classical Theory of Elastic Scattering between Complex Nuclei NUCLEAR REACTIONS 40Ca(α, α), E=29 MeV; 16O(α, α), E=104 MeV; 16O(16O, 16O), E=50 MeV; Cu(p, p), E=17 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(77)90427-4
1977CA06 Nucl.Phys. A279, 85 (1977) Microscopic Description of the Collisions between Nuclei NUCLEAR REACTIONS 4He(α, α), E(cm) ≤ 20 MeV; calculated phase shifts.
doi: 10.1016/0375-9474(77)90422-5
1977ST13 Phys.Lett. 68B, 108 (1977) F.Stancu, D.M.Brink, H.Flocard The Tensor Part of Skyrme's Interaction NUCLEAR STRUCTURE 48Ca, 56Ni; calculated p, n levels.
doi: 10.1016/0370-2693(77)90178-2
1976BR05 Nucl.Phys. A258, 285 (1976) Multipole Sum Rules and Giant Resonances with Skyrme's Interaction NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated mean positions of giant resonances. Skyrme interaction.
doi: 10.1016/0375-9474(76)90007-5
1976GI11 Phys.Lett. 65B, 305 (1976) M.J.Giannoni, F.Moreau, P.Quentin, D.Vautherin, M.Veneroni, D.M.Brink A Method for Calculating Adiabatic Mass Parameters: Application to Isoscalar Quadrupole Modes in Light Nuclei NUCLEAR STRUCTURE 12C; calculated quadrupole mass.
doi: 10.1016/0370-2693(76)90227-6
1976ST13 Nucl.Phys. A269, 87 (1976) S.Stringari, R.Leonardi, D.M.Brink Spin Stability and Magnetic Polarizability with Skyrme's Interaction NUCLEAR STRUCTURE 12C, 28Si, 56Ni; calculated spin polarizability. Skyrme effective interaction.
doi: 10.1016/0375-9474(76)90398-5
1976ST15 Nucl.Phys. A270, 236 (1976) The Real Part of the Nucleus-Nucleus Interaction NUCLEAR REACTIONS 48Ca(16O, 16O), E=40, 60 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(76)90137-8
1975BE16 Nucl.Phys. A244, 58 (1975) R.Beck, J.Borysowicz, D.M.Brink, M.V.Mihailovic On Calculating Scattering Phase Shifts by the Generator Coordinate Method NUCLEAR REACTIONS 4He(α, α), E < 35 MeV; calculated scattering phase shifts.
doi: 10.1016/0375-9474(75)90006-8
1975BR13 Nucl.Phys. A243, 175 (1975) Interaction Potential between Two 16O Nuclei Derived from the Skyrme Interaction NUCLEAR REACTIONS 16O(16O, 16O); calculated potential.
doi: 10.1016/0375-9474(75)90027-5
1975EN01 Nucl.Phys. A249, 215 (1975) Y.M.Engel, D.M.Brink, K.Goeke, S.J.Krieger, D.Vautherin Time-Dependent Hartree-Fock Theory with Skyrme's Interaction NUCLEAR STRUCTURE 16O, 40Ca; calculated monopole vibrations.
doi: 10.1016/0375-9474(75)90184-0
1974AN36 Phys.Rep. 12, 201 (1974) N.Anyas-Weiss, J.C.Cornell, P.S.Fisher, P.N.Hudson, A.Menchaca-Rocha, D.J.Millener, A.D.Panagiotou, D.K.Scott, D.Strottman, D.M.Brink, B.Buck, P.J.Ellis, T.Engeland Nuclear structure of light nuclei using the selectivity of high energy transfer reactions with heavy ions NUCLEAR REACTIONS 12C, 16O, 40Ca(12C, 11B), (12C, 11C), (12C, 10B), (12C, 10Be), (12C, 10C), (12C, 9Be), E=114 MeV; 12,13C(11B, 9Li), E=114 MeV; 13C(11B, 10B), E=114 MeV; measured particle spectra, σ(E, θ). 13,14C, 13,14,15N, 14,15O deduced levels, J, π, spectroscopic amplitudes.
doi: 10.1016/0370-1573(74)90045-3
1974BR07 Nucl.Phys. A219, 79 (1974) An Interaction Potential for Heavy-Ion Scattering NUCLEAR REACTIONS 54Fe(16O, 16O'), 107Ag(14N, 14N'), 116Sn(16O, 16O'), 208Pb(84Kr, 84Kr'), 232Th(84Kr, 84Kr'); measured nothing, calculated σ.
doi: 10.1016/0375-9474(74)90083-9
1972BR21 Phys.Lett. 40B, 37 (1972) Kinematical Effects in Heavy-Ion Reactions
doi: 10.1016/0370-2693(72)90274-2
1972VA09 Phys.Rev. C5, 626 (1972) Hartree-Fock Calculations with Skyrme's Interaction. I. Spherical Nuclei NUCLEAR STRUCTURE 16O, 40,48Ca, 90Zr, 208Pb; Z=114; calculated rms radii, binding energies, single-particle energies. Hartree-Fock method; Skyrme interaction. NUCLEAR REACTIONS 40Ca(e, e), E=249 MeV; 208Pb(e, e), E=248, 502 MeV; calculated σ(θ). Hartree-Fock method, Skyrme interaction.
doi: 10.1103/PhysRevC.5.626
1971NG01 Phys.Lett. 35B, 135 (1971) Nguyen Van Giai, D.Vautherin, M.Veneroni, D.M.Brink Coulomb Energy Differences in Mirror Nuclei in the Hartree-Fock Approximation NUCLEAR STRUCTURE 40Ca; calculated single-particle energies. 12C, 16O, 28Si, 32S, 40,48Ca, 90Zr, 208Pb; calculated binding energy. 13N, 13C, 17F, 17O, 29P, 29Si, 33Cl, 33S, 41Sc, 41Ca; calculated Coulomb displacement energy.
doi: 10.1016/0370-2693(71)90238-3
1970BR35 Phys.Lett. 33B, 143 (1970) D.M.Brink, H.Friedrich, A.Weiguny, C.W.Wong Investigation of the Alpha-Particle Model for Light Nuclei NUCLEAR STRUCTURE 12C, 16O, 20Ne, 24Mg, 28Si; calculated binding energies, quadrupole moment, rms radii. α-particle model.
doi: 10.1016/0370-2693(70)90284-4
1970BR37 Nucl.Phys. A154, 449 (1970) Isospin Mixing of Hartree-Fock Solutions NUCLEAR STRUCTURE 40,48Ca; calculated ground-state energy, proton, mass radii. Constrained Hartree-Fock method, isospin mixing.
doi: 10.1016/0375-9474(70)90117-X
1970VA16 Phys.Lett. 32B, 149 (1970) Hartree-Fock Calculations with Skyrme's Interaction NUCLEAR STRUCTURE 16O, 40Ca, 48Ca, 90Zr, 208Pb; calculated levels, binding energy, rms radii. Hartree-Fock theory.
doi: 10.1016/0370-2693(70)90458-2
1970VA30 Phys.Lett. 33B, 381 (1970) D.Vautherin, M.Veneroni, D.M.Brink A Hartree-Fock Calculation for the Stability of Super-Heavy Nuclei NUCLEAR STRUCTURE 206,207,208,209,210Pb; calculated binding energies, Qα, neutron separation energies. Element-106, Element-114, Element-120, Element-136; calculated Qα, single-particle states.
doi: 10.1016/0370-2693(70)90609-X
1967BR16 Nucl.Phys. A98, 460 (1967) An Approximate Calculation of Multiple Coulomb Excitation
doi: 10.1016/0375-9474(67)90092-9
1967RO21 Rev.Mod.Phys. 39, 306 (1967) Angular Distributions of Gamma Rays in Terms of Phase-Defined Reduced Matrix Elements
doi: 10.1103/RevModPhys.39.306
1963BR07 Nucl.Phys. 40, 608 (1963) Excited States in Oxygen 16 NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.
doi: 10.1016/0029-5582(63)90306-7
1957BR98 Nucl.Phys. 4, 215 (1957) Individual particle and collective aspects of the nuclear photoeffect
doi: 10.1016/0029-5582(87)90021-6
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