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Search: Author = D.M.Brink

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2021BO15      Eur.Phys.J. A 57, 171 (2021)

A.Bonaccorso, D.M.Brink

Models of breakup: a final state interaction problem

doi: 10.1140/epja/s10050-021-00448-1
Citations: PlumX Metrics

2018BO19      Eur.Phys.J. A 54, 152 (2018)

A.Bonaccorso, D.M.Brink

On the eikonal approach to nuclear diffraction dissociation

doi: 10.1140/epja/i2018-12599-9
Citations: PlumX Metrics

2018BR11      Phys.Rev. C 97, 064304 (2018)

D.M.Brink, Fl.Stancu

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
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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
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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
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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
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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
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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
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2007BR12      Phys.Rev. C 75, 064311 (2007)

D.M.Brink, Fl.Stancu

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
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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
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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
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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
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2004BR31      Nucl.Phys. A738, 195 (2004)


Concluding remarks

doi: 10.1016/j.nuclphysa.2004.04.031
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2004BR38      Prog.Theor.Phys.(Kyoto), Suppl. 154, 268 (2004)


Fusion and Heavy Ion Reactions

doi: 10.1143/PTPS.154.268
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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
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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
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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
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2002BR02      Nucl.Phys. A697, 689 (2002)

D.M.Brink, C.V.Sukumar

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
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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
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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
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1999BR14      Nucl.Phys. A650, 418 (1999)

D.M.Brink, C.V.Sukumar

The Heavy-Ion Spin-Orbit Interaction

doi: 10.1016/S0375-9474(99)00119-0
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1999BR19      Nucl.Phys. A649, 218c (1999)


Summary Talk: Giant resonances at finite temperature

doi: 10.1016/S0375-9474(99)00065-2
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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
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1998BO01      Phys.Rev. C57, R22 (1998)

A.Bonaccorso, D.M.Brink

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
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1998BO28      Phys.Rev. C58, 2864 (1998)

A.Bonaccorso, D.M.Brink

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
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1998BR06      J.Phys.(London) G24, 867 (1998)

D.M.Brink, L.Lo Monaco

Finite-Size Effects on QGP

doi: 10.1088/0954-3899/24/4/015
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1998SU09      Phys.Lett. 421B, 25 (1998)

C.V.Sukumar, D.M.Brink

Geometric Magnetism and the Heavy Ion Spin-Orbit Interaction

doi: 10.1016/S0370-2693(98)00003-3
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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
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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
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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
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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
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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
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1995SU09      Nucl.Phys. A587, 413 (1995)

C.V.Sukumar, D.M.Brink

A Path-Integral Approach to Inclusive Processes

doi: 10.1016/0375-9474(95)00034-X
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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
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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
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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
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1993AI01      Nucl.Phys. A560, 765 (1993)

S.Ait-Tahar, D.M.Brink

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
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1992BO24      Phys.Rev. C46, 700 (1992)

A.Bonaccorso, D.M.Brink

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
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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
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1991BO01      Phys.Rev. C43, 299 (1991)

A.Bonaccorso, D.M.Brink

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
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1991BO24      Phys.Rev. C44, 1559 (1991)

A.Bonaccorso, D.M.Brink

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
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1988BO26      Phys.Rev. C38, 1776 (1988)

A.Bonaccorso, D.M.Brink

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
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1988HA03      Nucl.Phys. A476, 107 (1988)

H.Hashim, D.M.Brink

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
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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
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1987OH08      Phys.Rev. C36, 966 (1987)

S.Ohkubo, D.M.Brink

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
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1987OH09      Phys.Rev. C36, 1375 (1987)

S.Ohkubo, D.M.Brink

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
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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
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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
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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
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1986SC08      Nucl.Phys. A452, 1 (1986)

H.Schaaser, D.M.Brink

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
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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
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1985LO10      J.Phys.(London) G11, 935 (1985)

L.Lo Monaco, D.M.Brink

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
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1985ST25      Phys.Rev. C32, 1937 (1985)

Fl.Stancu, D.M.Brink

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
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1984SC26      Phys.Lett. 143B, 269 (1984)

H.Schaaser, D.M.Brink

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
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1982BO23      Nucl.Phys. A384, 161 (1982)

A.Bonaccorso, D.M.Brink

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
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1982ST08      Phys.Rev. C25, 2450 (1982)

Fl.Stancu, D.M.Brink

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
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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
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1981BR01      J.Phys.(London) G7, 43 (1981)

D.M.Brink, G.R.Satchler

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
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1981BR11      Phys.Rev. C24, 144 (1981)

D.M.Brink, Fl.Stancu

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
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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
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1979HA25      J.Phys.(London) G5, 771 (1979)

H.Hasan, D.M.Brink

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
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1978HA45      J.Phys.(London) G4, 1573 (1978)

H.Hasan, D.M.Brink

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
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1977BR06      Nucl.Phys. A279, 159 (1977)

D.M.Brink, N.Takigawa

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
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1977CA06      Nucl.Phys. A279, 85 (1977)

L.F.Canto, D.M.Brink

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
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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
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1976BR05      Nucl.Phys. A258, 285 (1976)

D.M.Brink, R.Leonardi

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
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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
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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
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1976ST15      Nucl.Phys. A270, 236 (1976)

F.Stancu, D.M.Brink

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
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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
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1975BR13      Nucl.Phys. A243, 175 (1975)

D.M.Brink, F.Stancu

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
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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
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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
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1974BR07      Nucl.Phys. A219, 79 (1974)

D.M.Brink, N.Rowley

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
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1972BR21      Phys.Lett. 40B, 37 (1972)


Kinematical Effects in Heavy-Ion Reactions

doi: 10.1016/0370-2693(72)90274-2
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1972VA09      Phys.Rev. C5, 626 (1972)

D.Vautherin, D.M.Brink

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
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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
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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
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1970BR37      Nucl.Phys. A154, 449 (1970)

D.M.Brink, J.P.Svenne

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
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1970VA16      Phys.Lett. 32B, 149 (1970)

D.Vautherin, D.M.Brink

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
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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
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1967BR16      Nucl.Phys. A98, 460 (1967)

D.M.Brink, C.H.Taylor

An Approximate Calculation of Multiple Coulomb Excitation

doi: 10.1016/0375-9474(67)90092-9
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1967RO21      Rev.Mod.Phys. 39, 306 (1967)

H.J.Rose, D.M.Brink

Angular Distributions of Gamma Rays in Terms of Phase-Defined Reduced Matrix Elements

doi: 10.1103/RevModPhys.39.306
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1963BR07      Nucl.Phys. 40, 608 (1963)

D.M.Brink, G.F.Nash

Excited States in Oxygen 16

NUCLEAR STRUCTURE 16O; measured not abstracted; deduced nuclear properties.

doi: 10.1016/0029-5582(63)90306-7
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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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