NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = N.Takigawa Found 73 matches. 2010MU02 Phys.Rev. C 81, 044609 (2010) Z.F.Muhammad, Z.M.M.Mahmoud, N.Takigawa, K.Hagino Structure of 72, 74Ge nuclei probed with a combined analysis of heavy-ion fusion reactions and Coulomb excitation NUCLEAR REACTIONS 74Ge(74Ge, X), 72Ge(72Ge, X), E=110-140 MeV; calculated fusion σ(E), fusion barrier distributions, effect of octupole and quadrupole phonon excitations on fusion excitation function and fusion barrier distributions using full order coupled-channels formalism with CCFULL computer code. Comparison with experimental data. NUCLEAR STRUCTURE 72,74Ge; analyzed shapes with combined analysis of heavy-ion fusion reactions and Coulomb excitation. Vibrational and rotational models.
doi: 10.1103/PhysRevC.81.044609
2007KA35 Phys.Rev. C 76, 014615 (2007) Effects of nonlinear screening and quantum motion of the target nucleus on low energy nuclear reactions in matter
doi: 10.1103/PhysRevC.76.014615
2007MI13 Phys.Rev. C 75, 045802 (2007) F.Minato, K.Hagino, N.Takigawa, A.B.Balantekin, Ph.Chomaz Effect of electronic environment on neutrino-nucleus reactions at r-process sites NUCLEAR REACTIONS 56Fe, 208Pb(ν, e), E not given; calculated σ(E), electron screening and Pauli blocking effects.
doi: 10.1103/PhysRevC.75.045802
2007TA20 Nucl.Phys. A787, 190c (2007) N.Takigawa, Z.M.M.Mahmoud, Z.F.Muhammad, N.W.Lwin, T.Takehi, K.Hagino Effects of Transitional Shape and Shape Admixture and of Anti-symmetrization on Sub-Barrier Fusion NUCLEAR REACTIONS 72Ge(72Ge, X), 74Ge(74Ge, X), E(cm)=105-155 MeV; calculated fusion σ, fusion barrier distribution. 72,74Ge deduced levels, coupling matrix elements, shape deformation and admixture. Vibrational and rotational models. 208Pb(16O, X), E(cm)=70-110 MeV; calculated fusion σ. Resonating group method. Anti-symmetrization effect.
doi: 10.1016/j.nuclphysa.2006.12.031
2006HA39 Phys.Rev. C 74, 037601 (2006) K.Hagino, T.Takehi, N.Takigawa No-recoil approximation to the knock-on exchange potential in the double folding model for heavy-ion collisions NUCLEAR REACTIONS 40Ca(6Li, 6Li), E=30, 50.6, 156 MeV; calculated σ(θ). No-recoil approximation, comparison with data.
doi: 10.1103/PhysRevC.74.037601
2005AY01 Phys.Rev. C 71, 054611 (2005) S.Ayik, B.Yilmaz, A.Gokalp, O.Yilmaz, N.Takigawa Quantum statistical effects on fusion dynamics of heavy ions
doi: 10.1103/PhysRevC.71.054611
2005HA22 Phys.Rev. C 71, 044612 (2005) K.Hagino, T.Takehi, A.B.Balantekin, N.Takigawa Surface diffuseness anomaly in heavy-ion potentials for large-angle quasielastic scattering NUCLEAR REACTIONS 154Sm(16O, X), E(cm) ≈ 35-70 MeV; calculated quasielastic scattering σ, dependence on surface diffuseness parameter. Comparison with data.
doi: 10.1103/PhysRevC.71.044612
2004HU14 Prog.Theor.Phys.(Kyoto), Suppl. 154, 146 (2004) M.S.Hussein, A.J.Sargeant, M.P.Pato, N.Takigawa, M.Ueda Energy Averages over Regular and Chaotic States in the Decay Out of Superdeformed Bands
doi: 10.1143/PTPS.154.146
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
2004SA30 Phys.Rev. C 69, 067301 (2004) A.J.Sargeant, M.S.Hussein, M.P.Pato, N.Takigawa, M.Ueda Addendum: Attenuation of the intensity within a superdeformed band
doi: 10.1103/PhysRevC.69.067301
2004TA14 Phys.Rev. C 69, 054605 (2004) N.Takigawa, S.Ayik, K.Washiyama, S.Kimura Quantum effect in the diffusion along a potential barrier: Comments on the synthesis of superheavy elements
doi: 10.1103/PhysRevC.69.054605
2004TA29 Prog.Theor.Phys.(Kyoto), Suppl. 154, 192 (2004) N.Takigawa, T.Rumin, T.Masamoto, T.Takehi, K.Washiyama, S.Ayik Recent Theoretical Activities of Heavy-Ion Fusion Reactions in Sendai
doi: 10.1143/PTPS.154.192
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
2003TA20 J.Korean Phys.Soc. 43, S91 (2003) N.Takigawa, T.Masamoto, T.Takehi, T.Rumin Heavy Ion Fusion Reactions and Tunneling Nuclear Microscope NUCLEAR REACTIONS 112,122Sn, 144,148,154Sm(40Ar, X), E(cm) ≈ 80-150 MeV; 96Zr(64Ni, X), E(cm) ≈ 120-150 MeV; 144Sm, 186W(16O, X), E(cm) ≈ 60-78 MeV; analyzed fusion σ, barrier distributions, deformation dependence.
2002KI16 Phys.Rev. C66, 024603 (2002) Fusion from an excited state
doi: 10.1103/PhysRevC.66.024603
2002SA04 Phys.Rev. C65, 024302 (2002); Comment Phys.Rev. C 68, 069801 (2003) A.J.Sargeant, M.S.Hussein, M.P.Pato, N.Takigawa, M.Ueda Attenuation of the Intensity within a Superdeformed Band
doi: 10.1103/PhysRevC.65.024302
2001RU05 Phys.Rev. C63, 044603 (2001) Applicability of the Orientation Average Formula in Heavy-Ion Fusion Reactions of Deformed Nuclei NUCLEAR REACTIONS 154Sm(12C, X), (20Ne, X), (24Mg, X), (28Si, X), (32S, X), (36Ar, X), E ≈ threshold; 154Sm(16O, X), E(cm)=50-75 MeV; 154Sm(40Ar, X), E(cm)=105-145 MeV; calculated fusion σ, barrier distributions, target orientation effects; deduced accuracy of average orientation approximation.
doi: 10.1103/PhysRevC.63.044603
2000ME20 Phys.Rev. C61, 064319 (2000) Structure of Superheavy Elements Suggested in the Reaction of 86Kr with 208Pb NUCLEAR STRUCTURE 86Kr, 208Pb, 265Rf, 269Sg, 273Hs, 277Ds, 281Cn, 285Fl, 289Lv, 293,294Og; calculated binding energies, single-particle level energies, deformations, matter and charge radii, pairing gaps. 269Sg, 273Hs, 277Ds, 281Cn, 285Fl, 289Lv, 293Og; calculated Qα. Relativistic mean field, several forces compared.
doi: 10.1103/PhysRevC.61.064319
2000RU01 Phys.Rev. C61, 014605 (2000) Effects of β6 Deformation and Low-Lying Vibrational Bands on Heavy-Ion Fusion Reactions at Sub-Barrier Energies NUCLEAR REACTIONS 154Sm, 186W, 238U(16O, X), E(cm)=50-100 MeV; calculated fusion σ, barrier distribution; deduced deformation dependence features, rotational coupling effects.
doi: 10.1103/PhysRevC.61.014605
2000TA02 Phys.Rev. C61, 044607 (2000) Coulomb Interaction between Spherical and Deformed Nuclei NUCLEAR REACTIONS 238U(16O, X), E not given; calculated fusion barrier, form factors; deduced role of target deformation.
doi: 10.1103/PhysRevC.61.044607
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
1999UE02 Nucl.Phys. A648, 229 (1999) M.Ueda, M.P.Pato, M.S.Hussein, N.Takigawa Glory ' In the Shadow of the Rainbow ' NUCLEAR REACTIONS 90Zr(α, α), E=40-200 MeV; calculated σ(θ), forward scattering features; deduced rainbow scattering shadow effect. Semiclassical interpretation. Sum-of-differences approach.
doi: 10.1016/S0375-9474(99)00021-4
1998BA10 Rev.Mod.Phys. 70, 77 (1998) Quantum Tunneling in Nuclear Fusion
doi: 10.1103/RevModPhys.70.77
1998HA10 Phys.Rev. C57, 1349 (1998) K.Hagino, S.Kuyucak, N.Takigawa Excitation of Nuclear Anharmonic Vibrations in Heavy-Ion Fusion Reactions NUCLEAR REACTIONS 148Sm(16O, X), E(cm)=53-70 MeV; analyzed fusion σ, barrier distributions; deduced anharmonic phonon excitation effects.
doi: 10.1103/PhysRevC.57.1349
1998HA56 Phys.Rev. C58, 2872 (1998) Effects of Finite Width of Excited States on Heavy-Ion Sub-Barrier Fusion Reactions
doi: 10.1103/PhysRevC.58.2872
1998YO10 Phys.Rev. C58, 2796 (1998) S.Yoshida, H.Sagawa, N.Takigawa Incompressibility and Density Distributions in Asymmetric Nuclear Systems NUCLEAR STRUCTURE 100,104,108,112,116,120,124,128,132,136,140,150,160Sn; calculated neutron, charge, matter radii, density distributions; deduced correlation between surface diffuseness, incompressibility.
doi: 10.1103/PhysRevC.58.2796
1997DA22 J.Phys.(London) G23, 1491 (1997) M.Dasgupta, K.Hagino, C.R.Morton, D.J.Hinde, J.R.Leigh, N.Takigawa, H.Timmers, J.O.Newton Evidence of Double Phonon Excitations in the Fusion of 16O + 208Pb NUCLEAR REACTIONS, ICPND 208Pb(16O, X), E(cm)=68-83 MeV; measured fusion σ, barrier distribution; deduced coupling to double-phonon surface vibrations role in fusion dynamics.
doi: 10.1088/0954-3899/23/10/041
1997HA02 Phys.Rev. C55, 276 (1997) K.Hagino, N.Takigawa, M.Dasgupta, D.J.Hinde, J.R.Leigh Validity of the Linear Coupling Approximation in Heavy-Ion Fusion Reactions at Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 92,96Zr(64Ni, X), E(cm)=120-150 MeV; 112Cd(16O, F), E(cm)=40-65 MeV; 144Sm(16O, F), E=55-75 MeV; calculated fusion σ(E).
doi: 10.1103/PhysRevC.55.276
1997HA41 Phys.Rev. C56, 2104 (1997) K.Hagino, N.Takigawa, A.B.Balantekin Fusion Barrier Distributions in Systems with Finite Excitation Energy
doi: 10.1103/PhysRevC.56.2104
1997HA46 Phys.Rev.Lett. 79, 2014 (1997) K.Hagino, N.Takigawa, M.Dasgupta, D.J.Hinde, J.R.Leigh Adiabatic Quantum Tunneling in Heavy-Ion Sub-Barrier Fusion NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E(cm)=50-80 MeV; 194Pt(40Ca, X), E(cm)=160-200 MeV; 192Os(40Ca, X), E(cm)=150-190 MeV; calculated fusion σ with, without projectile excitation; deduced reaction mechanism, fusion barrier features. Comparison with data. Coupled-channels calculations.
doi: 10.1103/PhysRevLett.79.2014
1997HA47 Phys.Rev.Lett. 79, 2943 (1997) K.Hagino, N.Takigawa, S.Kuyucak Role of Anharmonicities of Nuclear Vibrations in Fusion Reactions at Sub-Barrier Energies NUCLEAR REACTIONS, ICPND 144Sm(16O, X), E(cm)=55-70 MeV; analyzed fusion σ; deduced fusion barrier, 144Sm anharmonic vibration role. sdf-interacting boson model.
doi: 10.1103/PhysRevLett.79.2943
1997HA50 J.Phys.(London) G23, 1413 (1997) K.Hagino, N.Takigawa, M.Dasgupta, D.J.Hinde, J.R.Leigh Importance of Nonlinear Couplings in Fusion-Barrier Distributions and Mean Angular Momenta NUCLEAR REACTIONS, ICPND 96Zr(64Ni, X), E(cm)=120-150 MeV; analyzed fusion σ, compound nucleus average angular momentum; 144Sm(16O, X), E(cm)=55-75 MeV; analyzed fusion σ, barrier distribution; deduced surface vibration coupling, projectile excitation effects. Coupled-channels calculations.
doi: 10.1088/0954-3899/23/10/031
1997TA24 J.Phys.(London) G23, 1367 (1997) N.Takigawa, K.Hagino, S.Kuyucak Probing Anharmonic Properties of Nuclear Surface Vibration by Heavy-Ion Fusion Reactions NUCLEAR REACTIONS, ICPND 154Dy(16O, X), E(cm)=60-80 MeV; 144Sm(16O, X), E(cm)=55-70; calculated fusion σ, fusion barrier distribution; deduced surface vibrations effects. Interacting boson model. Comparisons with data.
doi: 10.1088/0954-3899/23/10/026
1997YO04 Phys.Rev. C55, 1255 (1997) Shape Dependence of Pairing Gap Energies and the Structure of Hg and Pb Isotopes NUCLEAR STRUCTURE 194Hg; calculated energy surface, neutron, proton gap parameters, proton single particle levels. 180,182,184,186,188Hg; calculated charge radius isotope dependence, oblate, prolate states intrinsic energies. 190,192,194,196,198Hg; calculated charge radius isotope dependence. 190,192,194,196,198,200,202,204,206,208,210,212,214Pb; calculated scaled isotope shifts. Deformed relativistic mean field theory with pairing interactions in BCS theory.
doi: 10.1103/PhysRevC.55.1255
1996HA11 Phys.Rev. C53, 1840 (1996) Thermal Fission Rate Around Superfluid-Normal Phase Transition
doi: 10.1103/PhysRevC.53.1840
1996TA01 Phys.Rev. C53, 1038 (1996) N.Takigawa, S.Yoshida, K.Hagino, S.K.Patra, C.R.Praharaj Reply to ' Comment on ' Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model ' and ' Structure of Neutron-Deficient Pt, Hg, and Pb Isotopes ' ' NUCLEAR STRUCTURE 176,178,180,182,184,186,188,190,192,194,196,198,200Hg; analyzed predicted binding energy per particle, rms charge radii. 170,172,174Hg, 192,194,196,198,200,202,204,206,208Pb; analyzed predicted rms charge radii; deduced sensitivity to model parameters. Relativistic mean field theory.
doi: 10.1103/PhysRevC.53.1038
1996TA27 Prog.Theor.Phys.(Kyoto), Suppl. 124, 101 (1996) Heavy-Ion Fusion Reactions as Macroscopic Quantum Tunneling
doi: 10.1143/PTPS.124.101
1996UE01 Nucl.Phys. A598, 273 (1996) Forward Nuclear Glory Scattering of a Halo Nucleus NUCLEAR REACTIONS 12C(11Li, 11Li), (11C, 11C), E ≈ 60 MeV/nucleon; 28Si(7Li, 7Li), E=178 MeV; 28Si(11Li, 11Li), E=319 MeV; calculated sum-of-differences σ vs θ, forward angle scattering amplitude, deflection function. Forward nuclear glory.
doi: 10.1016/0375-9474(95)00481-5
1996UE07 Prog.Theor.Phys.(Kyoto), Suppl. 124, 135 (1996) Forward Nuclear Glory Scattering of a Halo Nucleus NUCLEAR REACTIONS 12C(11Li, 11Li), (11C, 11C), E not given; calculated forward-angle scatering amplitudes; deduced neutron halo role.
doi: 10.1143/PTPS.124.135
1996YO11 Prog.Theor.Phys.(Kyoto), Suppl. 124, 131 (1996) S.Yoshida, S.K.Patra, N.Takigawa Multi-Neutron and Proton Transfer Reactions in Deep Inelastic Heavy-Ion Collisions NUCLEAR REACTIONS 165Ho(56Fe, X), E=465 MeV; calculated projectile-like-fragment mass to charge ratio vs energy loss, multinucleon transfer related features. Comparison with data. Fokker-Planck equation.
doi: 10.1143/PTPS.124.131
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
1995HA15 Phys.Rev. C52, 286 (1995) K.Hagino, N.Takigawa, A.B.Balantekin, J.R.Bennett Path Integral Approach to No-Coriolis Approximation in Heavy-Ion Collisions
doi: 10.1103/PhysRevC.52.286
1995PA06 Phys.Rev. C51, 2248 (1995) S.K.Patra, S.Yoshida, N.Takigawa, C.R.Praharaj, A.K.Rath Hexadecapole Shape Change in Ytterbium Isotopes NUCLEAR STRUCTURE 160,162,164,166,168,170,172,174,176,178,180,182,184,186,188,190Yb; calculated binding energy, quadrupole deformation parameter, hexadecapole moments. Relativistic mean field model. 158,160,162,164,166,168,170,172,174,176,178,180,182,184Yb; calculated Hartree-Fock energy, quadrupole, hexadecapole moments. Hartree-Fock calculations, nonrelativistic, relativistic models.
doi: 10.1103/PhysRevC.51.2248
1995SA32 Z.Phys. A351, 385 (1995) H.Sagawa, N.Van Giai, N.Takigawa, M.Ishihara, K.Yazaki Life Time of Soft Multipole Excitations NUCLEAR STRUCTURE 11Be; calculated dipole strength distribution, soft dipole peak T1/2.
doi: 10.1007/BF01291143
1995TA01 Phys.Rev. C51, 187 (1995) Dynamical Norm Method for Nonadiabatic Macroscopic Quantum Tunneling RADIOACTIVITY 234U(SF); calculated potential energy surface, escape path, environment effects. Dynamical norm method, macroscopic quantum tunneling.
doi: 10.1103/PhysRevC.51.187
1995TA03 Nucl.Phys. A583, 291c (1995) Potential Resonance Affected by Non-Adibatic Transition in Nuclear Heavy-Ion Collisions
doi: 10.1016/0375-9474(94)00675-D
1995TA15 Nucl.Phys. A588, 91c (1995) N.Takigawa, S.Yoshida, K.Hagino, S.K.Patra Multi-Nucleon Transfer Reactions and Fusion with Unstable Nuclei NUCLEAR REACTIONS 58Ni(118Cs, X), (133Cs, X), (148Cs, X), E not given; calculated transferred nucleon number vs energy loss due to relative motion. 11Li(9Li, X), E(cm)=0.5-2.5 MeV; calculated fusion σ(E). Transport theory plus friction model. NUCLEAR STRUCTURE 113,133,148,181Cs, 53,58,63,68Ni; calculated neutron, proton separation energies. Mass formula.
doi: 10.1016/0375-9474(95)00105-A
1995YO01 Phys.Rev. C52, 157 (1995) S.Yoshida, S.K.Patra, N.Takigawa, C.R.Praharaj Surface Properties of Cs Isotopes NUCLEAR STRUCTURE 133,148,181Cs; calculated neutron, proton density distributions. Other aspects, other isotopes studies. 40,48Ca, 58,64Ni, 90Zr, 116Sn, 140Ce, 208Pb; calculated neutron, proton distributions rms radii. Deformed relativistic mean field, spherical nonrelativistic Hartree-Fock theories.
doi: 10.1103/PhysRevC.52.157
1994PA29 Phys.Rev. C50, 1924 (1994) S.K.Patra, S.Yoshida, N.Takigawa, C.R.Praharaj Shape and Superdeformed Structure in Hg Isotopes in Relativistic Mean Field Model NUCLEAR STRUCTURE 170,172,174,176,178,180,182,184,186,188,190,192,194,196,198,200Hg; calculated binding energy, quadrupole deformation parameter, hexadecupole moment, charge, rms radii. Relativistic mean field theory.
doi: 10.1103/PhysRevC.50.1924
1994SA30 Phys.Rev. C50, 985 (1994) Projectile Fragmentation of Halo Nuclei in a Peripheral Direct Reaction Model NUCLEAR REACTIONS 208Pb, 12C(11Be, X), 9Be, 181Ta(11Li, X), E not given; calculated transverse, longitudinal fragment momentum distribution, projectile fragmentation. Peripheral direct reaction model.
doi: 10.1103/PhysRevC.50.985
1994TA07 Phys.Rev. C49, 2630 (1994) N.Takigawa, K.Hagino, M.Abe, A.B.Balentekin Role of Mass Renormalization in Adiabatic Quantum Tunneling
doi: 10.1103/PhysRevC.49.2630
1994YO05 Phys.Rev. C50, 1398 (1994) S.Yoshida, S.K.Patra, N.Takigawa, C.R.Praharaj Structure of Neutron-Deficient Pt, Hg, and Pb Isotopes NUCLEAR STRUCTURE 176,178,180Pt, 180,182,184Hg, 178,180,182,184,186,188,190,192,194,196,198,200,202,204,206,208Pb; calculated binding energy, quadrupole deformation parameter, hexadecapole moment, single particle spectra in some cases. Relativistic mean field formalism.
doi: 10.1103/PhysRevC.50.1398
1993TA04 Phys.Rev. C47, R2470 (1993) N.Takigawa, M.Kuratani, H.Sagawa Effect of Breakup Reactions on the Fusion of a Halo Nucleus NUCLEAR REACTIONS, ICPND 208Pb(11Li, X), E(cm)=20-35 MeV; calculated fusion σ(E); deduced breakup reactions role. Semi-classical method.
doi: 10.1103/PhysRevC.47.R2470
1992SA10 Nucl.Phys. A543, 575 (1992) H.Sagawa, N.Takigawa, Nguyen van Giai Sum Rule Study of New Vibrational Modes of Excitation in Halo Nuclei NUCLEAR STRUCTURE 11Li; calculated soft, giant dipole states transition densities. 10He; calculated RPA transition density. Sum rule approach.
doi: 10.1016/0375-9474(92)90280-W
1992TA16 Phys.Lett. 288B, 244 (1992) N.Takigawa, M.Ueda, M.Kuratani, H.Sagawa Elastic Scattering of a Halo Nucleus at Medium Energies NUCLEAR REACTIONS 12C(11Li, 11Li), E=360 MeV; calculated σ(θ), with, without neutron halo; deduced breakup reaction role for halo nuclei scattering, Glauber theory optical limit approximation validity features.
doi: 10.1016/0370-2693(92)91098-T
1991BA27 Phys.Rev. C44, 145 (1991) A.B.Balantekin, J.R.Bennett, N.Takigawa Description of Nuclear Structure Effects in Sub-Barrier Fusion by the Interacting Boson Model NUCLEAR REACTIONS, ICPND 154Sm(16O, X), E ≈ 54-69 MeV; 166Er(16O, X), E=58-83 MeV; calculated fusion σ(E). Interacting boson model.
doi: 10.1103/PhysRevC.44.145
1991TA12 Phys.Rev. C44, 477 (1991) N.Takigawa, F.Michel, A.B.Balantekin, G.Reidemeister Dynamic Polarization Potential Induced by the Coulomb Excitation of Deformed Heavy Ions: Geometric scattering approach NUCLEAR REACTIONS 184W(18O, 18O), E=90 MeV; calculated σ(θ). Geometric scattering theory, WKB approximation.
doi: 10.1103/PhysRevC.44.477
1991TA20 Phys.Lett. 262B, 199 (1991) N.Takigawa, F.Michel, A.B.Balantekin, G.Reidemeister A Geometric Approach to Strong Coupling Effects in Heavy-Ion Collisions. Deviation from the Fresnel Diffraction Pattern NUCLEAR REACTIONS 189W(18O, 18O), E=90 MeV; calculated σ(θ); deduced Coriolis coupling role. Geometric approach.
doi: 10.1016/0370-2693(91)91554-9
1991TA21 Phys.Lett. 265B, 23 (1991) Interaction Potential and Fusion of a Halo Nucleus NUCLEAR REACTIONS 208Pb(11Li, 11Li), E=low; calculated s-wave scattering potential surface separation energy dependence. 208Pb(11Li, 11Li), E(cm) ≈ 20-30 MeV; calculated fusion σ(E). Double folding procedure, neutron halo nucleus.
doi: 10.1016/0370-2693(91)90007-D
1989IW01 Phys.Lett. 219B, 176 (1989) Anomalous Enchancement of the Subbarrier Fusion Cross Section by Cooperative Shell and Deformation Effects NUCLEAR REACTIONS 74Ge(74Ge, X), E(cm)=110-135 MeV; calculated fusion σ(E).
doi: 10.1016/0370-2693(89)90372-9
1988AB06 Phys.Lett. 209B, 149 (1988) Dynamical Decay of a Hot Nucleus NUCLEAR REACTIONS 188Pt(16O, 16O), (16O, α), (16O, 40Ca), E=70-80 MeV; calculated particle spectra, transmission coefficient ratio. Hot nucleus, dymanical decay.
doi: 10.1016/0370-2693(88)90922-7
1986NI04 Z.Phys. A324, 139 (1986) Role of Nuclear Surface Vibrations in Low Energy Heavy Ion Collisions NUCLEAR REACTIONS 208Pb(84Sr, X), E=0.718, 1.5, 3 GeV; calculated energy, angular dissipation, retarded friction. Nuclear surface vibrations as transport phenomena.
1983NI02 Nucl.Phys. A397, 141 (1983) Quasi-Linear Response Theory of Statistical Heavy-Ion Collisions (II). Analysis of the friction tensor and the energy transport NUCLEAR REACTIONS 232Th(40Ar, X), E=388 MeV; 209Bi(136Xe, X), E=1130 MeV; calculated light fragment mean trajectories, σ(fragment θ, E). Quasilinear response theory, deep inelastic collisions.
doi: 10.1016/0375-9474(83)90082-9
1982TA24 Phys.Lett. 119B, 289 (1982) Charge Equilibration in Dissipative Heavy Ion Collisions as a Semi-Quantal Process NUCLEAR REACTIONS 92Mo(86Kr, X), E=430 MeV; calculated average fragment charge, dispersion vs total kinetic energy loss; deduced charge equilibration mechanism. Dynamical transport theory.
doi: 10.1016/0370-2693(82)90672-4
1979TA11 Phys.Lett. 84B, 371 (1979) Critical Energies in Elastic α-Nucleus Scattering NUCLEAR REACTIONS 90Zr(α, α), E=40, 99.5, 220 MeV; calculated σ(θ), classical deflection functions, energy surfaces for certain L-values; deduced critical energies. Semiclassical theory.
doi: 10.1016/0370-2693(79)91218-8
1978LE16 Nucl.Phys. A308, 161 (1978) A Semiclassical Study of Optical Potentials: Potential Resonances NUCLEAR REACTIONS 16O(16O, 16O), E=56 MeV; 40Ca(α, α), E ≤ 50 MeV; calculated σ.
doi: 10.1016/0375-9474(78)90448-7
1978LE17 Nucl.Phys. A308, 189 (1978) A Wave Propagation Matrix Method in Semiclassical Theory NUCLEAR REACTIONS 16O(16O, 16O), E=40 MeV; calculated reaction parameters.
doi: 10.1016/0375-9474(78)90449-9
1978TA16 Phys.Lett. 76B, 187 (1978) Long Life Potential Resonances in 16O-12C Scattering from an l-Dependent Absorptive Potential NUCLEAR REACTIONS 12C(16O, 16O), E=43 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(78)90271-X
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
1977TA14 Nucl.Phys. A292, 173 (1977) Nuclear Glory Effect and α-40Ca Scattering NUCLEAR REACTIONS 40Ca(α, α), E=45.6 MeV; calculated σ(θ).
doi: 10.1016/0375-9474(77)90365-7
1974LA13 Phys.Lett. 50B, 414 (1974) A Note on Diffraction Phenomena in the Inelastic Scattering of Complex Nuclei NUCLEAR REACTIONS 58Ni(16O, 16O'), E=60 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(74)90248-2
1972AB19 Progr.Theor.Phys.Suppl. 52, 228 (1972) Alpha-Like Four-Body Correlations and Molecular Aspects in Nuclei. Chapter V. Stability and Persistency of Alpha-Cluster Structures NUCLEAR STRUCTURE 9,8Be, 12C; calculated α-cluster structures.
doi: 10.1143/PTPS.52.228
1971TA13 Nucl.Phys. A168, 593 (1971) Structure of 12C NUCLEAR STRUCTURE 12C; calculated levels, B(EL), α-width, (E, E) form factors. Heitler-London approximation.
doi: 10.1016/0375-9474(71)90549-5
Back to query form |