NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = J.M.Bang Found 39 matches. 2000SH23 Phys.Rev. C62, 014312 (2000) N.B.Shulgina, B.V.Danilin, L.V.Grigorenko, M.V.Zhukov, J.M.Bang Nuclear Structure of 5H in a Three-Body 3H + n + n Model NUCLEAR STRUCTURE 5He; calculated levels energies, J, π, widths. Three-body model.
doi: 10.1103/PhysRevC.62.014312
2000TH01 Phys.Rev. C61, 024318 (2000) I.J.Thompson, B.V.Danilin, V.D.Efros, J.S.Vaagen, J.M.Bang, M.V.Zhukov Pauli Blocking in Three-Body Models of Halo Nuclei NUCLEAR STRUCTURE 6He, 6Be; calculated ground-state, continuum features; deduced effects of different approaches to Pauli blocking. Three-body models.
doi: 10.1103/PhysRevC.61.024318
2000VA19 Phys.Scr. T88, 209 (2000) J.S.Vaagen, D.K.Gridnev, H.Heiberg-Andersen, B.V.Danilin, S.N.Ershov, V.I.Zagrebaev, I.J.Thompson, M.V.Zhukov, J.M.Bang Borromean Halo Nuclei
doi: 10.1238/Physica.Topical.088a00209
1999EF01 Eur.Phys.J. A 4, 33 (1999) The First Excited States of 9Be and 9B NUCLEAR STRUCTURE 9Be, 9B; calculated first excited states energies, line shape for excitation. Three-body representation.
doi: 10.1007/s100500050201
1997LU08 Bull.Rus.Acad.Sci.Phys. 61, 69 (1997) Yu.A.Lurie, A.M.Shirokov, J.M.Bang Exactly Solvable Model for Multineutron Halo Nuclei NUCLEAR STRUCTURE 6He, 11Li; calculated reduced transition probabilities, breakup fragment transverse momenta distributions. Weakly bound 3-body systems, minimal approximation of hyperspherical expansion method, exactly solvable model.
1997SH19 Nucl.Phys. A619, 143 (1997) N.B.Shulgina, L.V.Grigorenko, M.V.Zhukov, J.M.Bang 8He β-Decay to the 6Li + n + n Channel RADIOACTIVITY 8He(β-); calculated 6Li, 2n-spectra, Gamow-Teller strength following β-decay; deduced implications for 8Li Gamow-Teller sum rule. Cluster-orbital shell-model approximation.
doi: 10.1016/S0375-9474(97)00151-6
1997VA06 Nucl.Phys. A616, 426c (1997) J.S.Vaagen, B.V.Danilin, S.N.Ershov, T.Rogde, D.Ridikas, H.Heiberg-Andersen, J.M.Bang, M.V.Zhukov, I.J.Thompson, and the Russian-Nordic-British Theory (RNBT) Collaboration Theortical Studies of Light Halo Nuclei; Bound states and continuum NUCLEAR REACTIONS 6Li(n, p), E=200 MeV; calculated σ(θ) vs residual nucleus matter radii. Monople COSMA model transition densities.
doi: 10.1016/S0375-9474(97)00114-0
1996BA02 Phys.Rev. C53, R18 (1996) J.M.Bang, L.S.Ferreira, E.Maglione, J.M.Hansteen Energy Dependence of Fusion Cross Sections NUCLEAR REACTIONS 3He(d, p), E=low; analyzed fusion σ enhancement; deduced beam energy underestimation effects role.
doi: 10.1103/PhysRevC.53.R18
1996BA60 Phys.Rep. 264, 27 (1996) J.M.Bang, B.V.Danilin, V.D.Efros, J.S.Vaagen, M.V.Zhukov, I.J.Thompson, and the Russian-Nordic-British Theory (RNBT) Collaboration Few-Body Aspects of Borromean Halo Nuclei NUCLEAR STRUCTURE 6He; calculated correlation, spatial density distributions. 6Be; calculated correlation distributions. 11Li; calculated spatial correlation density, electric dipole response.
doi: 10.1016/0370-1573(95)00024-0
1996DA31 Bull.Rus.Acad.Sci.Phys. 60, 21 (1996) B.V.Danilin, M.V.Zhukov, N.B.Shulgina, I.J.Thompson, J.M.Bang, F.A.Gareev, J.S.Vaagen Nuclei with Two-Particle Neutron Halo: Theory and modern experiment RADIOACTIVITY 6Li(β+); calculated Gamow-Teller transition strengths vs fragment energy. Hyperspherical harmonics method. NUCLEAR STRUCTURE 6He, 11Li; calculated three-particle strength function vs fragment energy. Hyperspherical harmonics method. NUCLEAR REACTIONS 6Li(p, n), (n, p), (p, p'), E not given; calculated σ(θ) vs momentum transfer. Hyperspherical harmonics methods.
1996RI14 Nucl.Phys. A609, 21 (1996) D.Ridikas, J.S.Vaagen, J.M.Bang Phase Equivalent Potentials for One-Neutron Halo Systems NUCLEAR STRUCTURE 11Be; calculated valence neutron rms radii with respect to 10Be core, 10Be fragment parallel momentum distribution, halo neutron excitation associated B(λ). Phase equivalent potentials, supersymmetric quantum mechanics.
doi: 10.1016/S0375-9474(96)00316-8
1996SH02 Nucl.Phys. A597, 197 (1996) N.B.Shulgina, B.V.Danilin, V.D.Efros, J.M.Bang, J.S.Vaagen, M.V.Zhukov, and the Russian-Nordic-British Theory (RNBT) Collaboration Three-Body Structure of 8Li and the 7Li(n, γ)8Li Reaction NUCLEAR REACTIONS 7Li(n, γ), E=25 keV; calculated σ. 3H(α, α), E=3-8 MeV; calculated phase shifts vs E. Three-body cluster model. NUCLEAR STRUCTURE 8Li; calculated matter density, cluster component separation rms radii. Three-body cluster model.
doi: 10.1016/0375-9474(95)00444-0
1995TH04 Nucl.Phys. A588, 59c (1995) I.J.Thompson, J.S.Al-Khalili, J.M.Bang, B.V.Danilin, V.D.Efros, F.M.Nunes, J.S.Vaagen, M.V.Zhukov, and the Russian-Nordic-British Theory (RNBT) Collaboration Structure and Reactions of the Li and Be Halo Nuclei NUCLEAR REACTIONS 12C(14Be, 14Be), (12Be, 12Be), E=57 MeV/nucleon; analyzed data; deduced rms matter radius role. Glauber, optical models. NUCLEAR STRUCTURE 11Li, 11,12,14Be; analyzed halo characteristics; deduced intruder state role. 14Be; calculated binding energies, rms radii, selected channels weights, Serber widths.
doi: 10.1016/0375-9474(95)00099-M
1994BA36 J.Phys.(London) G20, 741 (1994) New Aspects of Coulomb Dissociation
doi: 10.1088/0954-3899/20/5/008
1994DA27 Phys.Lett. 333B, 299 (1994) B.V.Danilin, I.J.Thompson, M.V.Zhukov, J.S.Vaagen, J.M.Bang, and the Russian-Nordic-British Theory (RNBT) Collaboration Electromagnetic Dipole Response of 11Li in a Solvable Three-Body Model NUCLEAR STRUCTURE 11Li; calculated electric dipole response; deduced no narrow resonance evidence. Hyperspherical three-body formulation.
doi: 10.1016/0370-2693(94)90145-7
1994EF04 Yad.Fiz. 57, No 7, 1341 (1994); Phys.Atomic Nuclei 57, 1271 (1994) How to Construct Subsets of Substantial Hyperspherical Harmonics
1994VA30 Z.Phys. A349, 285 (1994) J.S.Vaagen, I.J.Thompson, J.M.Bang, M.V.Zhukov, B.V.Danilin, D.V.Fedorov Clustering Aspects of Light Exotic Nuclei NUCLEAR STRUCTURE 6He, 11Li; compiled, reviewed halo structure studies.
doi: 10.1007/BF01288976
1994ZH05 J.Phys.(London) G20, 201 (1994) M.V.Zhukov, L.V.Chulkov, D.V.Fedorov, B.V.Danilin, J.M.Bang, J.S.Vaagen, I.J.Thompson Fingerprints of a Possible Low-Lying Resonance in 11Li NUCLEAR REACTIONS C(6He, α), E=400 MeV/nucleon; analyzed α-particle transverse momentum distribution. C(11Li, 9Li), E=800 MeV/nucleon; analyzed 9Li transverse momentum distribution. 9Be(11Li, X), E=29 MeV/nucleon; analyzed σ(θn) following 11Li fragmentation. 9Be(11Li, 9Li), E=70 MeV/nucleon; analyzed 9Li relative longitudinal momentum distribution; deduced reaction mechanisms energy dependence, possible resonance in 11Li. Phenomenological approach.
doi: 10.1088/0954-3899/20/1/020
1993DA01 Phys.Lett. 302B, 129 (1993) B.V.Danilin, M.V.Zhukov, J.S.Vaagen, J.M.Bang Strength Functions for 6He Excitations NUCLEAR STRUCTURE 6He; calculated electric dipole, monopole response; deduced no narrow resonances. Three-body model.
doi: 10.1016/0370-2693(93)90371-N
1993FE04 Phys.Lett. 316B, 23 (1993) L.S.Ferreira, E.Maglione, J.M.Bang, I.J.Thompson, B.V.Danilin, M.V.Zhukov, J.S.Vaagen Cross Sections for Coulomb Break-Up of the Halo Nucleus 6He NUCLEAR REACTIONS Pb, Cu, C(6He, X), E ≥ 30 MeV/nucleon; calculated E1 dissociation σ. Three-body model.
doi: 10.1016/0370-2693(93)90651-W
1993TH01 Phys.Rev. C47, R1364 (1993) I.J.Thompson, J.S.Al-Khalili, J.A.Tostevin, J.M.Bang Quasielastic Scattering of 11Li using Realistic Three-Body Wave Functions NUCLEAR REACTIONS 12C(11Li, 11Li), (11Li, X), E=60 MeV/nucleon; calculated elastic, quasielastic σ(θ). Realistic three-body wave functions, four-body Glauber approximation.
doi: 10.1103/PhysRevC.47.R1364
1993ZH03 Nucl.Phys. A552, 353 (1993) M.V.Zhukov, D.V.Fedorov, B.V.Danilin, J.S.Vaagen, J.M.Bang, I.J.Thompson One-Particle Densities of 11Li in Different Three-Body Approaches NUCLEAR STRUCTURE 11Li; calculated one-particle density vs radius. Different three-body approaches.
doi: 10.1016/0375-9474(93)90498-M
1992BA18 Phys.Lett. 279B, 201 (1992) Three Body Calculations for 11Li NUCLEAR STRUCTURE 11Li; calculated binding energy, total matter density vs radius. Inert 9Li core + interacting 2n system, different potentials, Faddeev equations.
doi: 10.1016/0370-2693(92)90379-I
1992BA20 Europhys.Lett. 18, 679 (1992) J.M.Bang, L.S.Ferreira, E.Maglione 11Li Dipole Moments NUCLEAR STRUCTURE 11Li; calculated soft dipole mode energy. Three-body wave functions.
doi: 10.1209/0295-5075/18/8/003
1992ZH05 Nucl.Phys. A539, 177 (1992) M.V.Zhukov, D.V.Fedorov, B.V.Danilin, J.S.Vaagen, J.M.Bang Neutron Halo Structure, 9Li-Neutron and Neutron-Neutron Momentum Correlations in 11Li NUCLEAR STRUCTURE 11Li; calculated (9Li+n)-, nn- correlated momentum distributions, spatial densities; deduced neutron halo structure. Cluster orbital shell model, approximate three-body approach.
doi: 10.1016/0375-9474(92)90241-B
1991DA08 Phys.Rev. C43, 2835 (1991) B.V.Danilin, M.V.Zhukov, S.N.Ershov, F.A.Gareev, R.S.Kurmanov, J.S.Vaagen, J.M.Bang Dynamical Multicluster Model for Electroweak and Charge-Exchange Reactions NUCLEAR REACTIONS 6Li(p, p'), (n, p), (p, n), E=280 MeV; 6Li(p, n), E=160, 200 MeV; calculated σ(θ). Dynamical cluster model, hyperspherical harmonics method, DWIA. NUCLEAR STRUCTURE 6Li, 6He, 6Be; calculated transition densities. 6Li; calculated transverse M1 transition form factor. Dynamical cluster model, hyperspherical harmonics method.
doi: 10.1103/PhysRevC.43.2835
1991ZH11 Phys.Rev. C44, R12 (1991) M.V.Zhukov, D.V.Fedorov, B.V.Danilin, J.S.Vaagen, J.M.Bang 9Li and Neutron Momentum Distributions in 11Li in a Simplified Three-Body Model NUCLEAR STRUCTURE 11Li; calculated rms matter radius, neutron momentum distribution. Three-body model. NUCLEAR REACTIONS C(11Li, 9Li), E=790 MeV/nucleon; calculated ejectile transverse momentum distribution. Three-body model.
doi: 10.1103/PhysRevC.44.R12
1991ZH13 Nucl.Phys. A529, 53 (1991) M.V.Zhukov, D.V.Fedorov, B.V.Danilin, J.S.Vaagen, J.M.Bang A Simplified Three-Body Model for 11Li and Associated 9Li and Neutron Momentum Distributions NUCLEAR STRUCTURE 11Li; calculated rms matter radius, geometric parameters. Three-body osillator cluster shell model. NUCLEAR REACTIONS C(11Li, 9Li), E=790 MeV/nucleon; calculated neutron, ejectile transverse momenta. Three-body oscillator cluster shell model wave functions.
doi: 10.1016/0375-9474(91)90785-5
1990BA06 Phys.Scr. 41, 202 (1990) J.M.Bang, F.A.Gareev, G.S.Kazacha, A.M.Kalinin Neutron-Rich Light Nuclei NUCLEAR STRUCTURE 6,8He, 6,7,8,9,11Li, 7,9,10Be; calculated interaction, rms radii. 9,7,5He, 10,5Li, 11N, 9B; calculated resonance energies, widths. Simple potential model.
doi: 10.1088/0031-8949/41/2/003
1990DE31 Phys.Scr. T32, 89 (1990) A.S.Demyanova, A.A.Ogloblin, S.N.Ershov, F.A.Gareev, R.S.Kurmanov, E.F.Svinareva, S.A.Goncharov, V.V.Adodin, N.Burtebaev, J.M.Bang, J.S.Vaagen Rainbows in Nuclear Reactions and the Optical Potential NUCLEAR REACTIONS 12,13,14C(3He, 3He), E=39.6, 12 MeV; 14N(3He, 3He), E=72 MeV; 14C(3He, 3He), E=22.06 MeV; 14N, 14C(3He, t), E=72 MeV; 14,13C(3He, t), E=39.6 MeV; analyzed σ(θ); deduced model parameters, rainbow characteristics.
doi: 10.1088/0031-8949/1990/T32/015
1989DE34 Nucl.Phys. A501, 336 (1989) A.S.Demyanova, J.M.Bang, F.A.Gareev, S.A.Goncharov, S.N.Ershov, A.A.Ogloblin, P.P.Korovin Investigation of the Nucleus-Nucleus Interaction at Small Distances in Elastic Scattering of 6Li and the Reaction (6Li, 6He) on Carbon Isotopes NUCLEAR REACTIONS 12,13,14C(6Li, 6Li), E=90-93 MeV; 13,14C(6Li, 6He), E=93 MeV; measured σ(θ); deduced potential parameters, reaction components. Microscopic DWBA.
doi: 10.1016/0375-9474(89)90297-2
1989ER05 Phys.Lett. 227B, 315 (1989) S.N.Ershov, F.A.Gareev, R.S.Kurmanov, E.F.Svinareva, G.S.Kazacha, A.S.Demyanova, A.A.Ogloblin, S.A.Goncharov, J.S.Vaagen, J.M.Bang Do Rainbows Observed in Light Ion Scattering Really Pin Down the Optical Potential ( Question ) NUCLEAR REACTIONS 14C(3He, 3He), 14C(3He, t), E=72 MeV; calculated σ(θ); deduced potential ambiguities, real, imaginary part correlations.
doi: 10.1016/0370-2693(89)90936-2
1988DE34 Phys.Rev. C38, 1975 (1988) A.S.Demiyanova, A.A.Ogloblin, Yu.V.Lyashko, V.V.Adodin, N.Burtebaev, S.N.Ershov, F.A.Gareev, P.P.Korovin, J.M.Bang, S.A.Goncharov, J.S.Vaagen Observation of a Nuclear Rainbowlike Phenomenon in the (3He, t) Charge-Exchange Reaction NUCLEAR REACTIONS 14C(3He, t), (3He, 3He), E=72 MeV; measured σ(θ); deduced model parameters, nuclear rainbow. DWBA analysis.
doi: 10.1103/PhysRevC.38.1975
1988DE47 Nucl.Phys. A482, 383 (1988) A.S.Demyanova, A.A.Ogloblin, S.N.Ershov, F.A.Gareev, P.P.Korovin, S.A .Goncharov, U.V.Lyashko, V.V.Adonin, N.Burtebaev, J.M.Bang Rainbow effects in charge exchange reactions NUCLEAR REACTIONS 12C(6Li, 6Li'), 14C(3He, 3He), 14C(3He, t), 14C(6Li, 6He), 14C(6Li, 6Li), E=72-93 MeV; measured products, 14C, 14N, 6He, 3H, 12C; deduced σ(θ). Data were imported from EXFOR entry F0853.
doi: 10.1016/0375-9474(88)90598-2
1987DE02 Phys.Lett. 184B, 129 (1987) A.C.Demiyanova, V.N.Bragin, A.A.Ogloblin, A.L.Lebedev, J.M.Bang, S.A.Goncharov, S.N.Ershov, F.A.Gareev, P.P.Korovin Angular Distributions of Elastic, Inelastic and Charge Exchange Reactions of 6Li + 14C at E(6Li) = 93 MeV NUCLEAR REACTIONS 14C(6Li, 6Li), (6Li, 6Li'), (6Li, 6He), E=93 MeV; 12C(6Li, 6Li'), E=90 MeV; measured σ(θ). Enriched 14C target. Optical model, DWBA calculations.
doi: 10.1016/0370-2693(87)90555-7
1984CE04 Phys.Scr. 29, 526 (1984) J.Cejpek, J.Dobes, J.M.Bang, B.S.Nilsson On the Absolute Values of Simultaneous Two-Nucleon Transfer Cross Sections in Heavy Ion Reactions NUCLEAR REACTIONS 42Ca(16O, 18O), E=56 MeV; calculated absolute σ(θ). Sturmian expansion technique.
1982KU04 Phys.Lett. 112B, 5 (1982) P.D.Kunz, J.S.Vaagen, J.M.Bang, B.S.Nilsson Comments on Unhappiness Factors in Simultaneous Transfer DWBA Description of (t, p) and (p, t) Reactions NUCLEAR REACTIONS 18O(p, t), E=20 MeV; 40Ca(t, p), E=10.1 MeV; 42Ca(p, t), E=39.8 MeV; 48Ca(t, p), E=12.08 MeV; calculated σ(θ). Finite-range, one-step DWBA, simultaneous transfer.
doi: 10.1016/0370-2693(82)90893-0
1980BA38 Z.Phys. A297, 223 (1980) The Sturmian Expansion: A Well-Depth-Method for Orbitals in a Deformed Potential NUCLEAR STRUCTURE 167Er, 163Ho, 186W, 159Gd; calculated radial multipole amplitudes; deduced convergence properties. Deformed potentials, Sturmian expansion.
doi: 10.1007/BF01892802
1970AN04 Nucl.Phys. A147, 33 (1970) B.L.Andersen, B.B.Back, J.M.Bang One-Particle Transfer Reactions to Highly Excited States in Deformed Nuclei NUCLEAR REACTIONS 239Pu(d, p), E=13 MeV; 160Gd(d, t), E not given; calculated σ(Ep, θ), σ(Et).
doi: 10.1016/0375-9474(70)90507-5
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