NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.S.Vaagen Found 97 matches. 2018GR02 Phys.Rev. C 97, 034605 (2018) L.V.Grigorenko, J.S.Vaagen, M.V.Zhukov Exploring the manifestation and nature of a dineutron in two-neutron emission using a dynamical dineutron model RADIOACTIVITY 26O, 5H(2n); calculated half-life of 26O g.s., neutron-neutron correlations in the decay of 26O g.s., n-n relative energy spectra for 5H g.s. using three models: two-body dineutron emission model, static three-body dineutron model (S2nM), and dynamic three-body dineutron model (D2nM), based on Migdal-Watson approximation for final state interactions (FSI).
doi: 10.1103/PhysRevC.97.034605
2018PA43 Phys.Rev. C 98, 034608 (2018) Yu.L.Parfenova, L.V.Grigorenko, I.A.Egorova, N.B.Shulgina, J.S.Vaagen, M.V.Zhukov From Coulomb excitation cross sections to nonresonant astrophysical rates in three-body systems: The 17Ne case NUCLEAR REACTIONS C, Si, Pb(17Ne, X), E=500 MeV/nucleon; calculated σ, and 17Ne E1 strength function extrapolated to astrophysical energies, eikonal model cross sections of the nuclear, E1 nuclear, and E1 Coulomb dissociation on Pb target, EMD cross sections. 15O(2p, γ)17Ne, T9=0.02-10; calculated astrophysical non-resonant radiative capture rate. Three-body hyperspherical harmonic (HH) method. Comparison with experimental data.
doi: 10.1103/PhysRevC.98.034608
2018SH22 Phys.Rev. C 97, 064307 (2018) N.B.Shulgina, S.N.Ershov, J.S.Vaagen, M.V.Zhukov Superhalo of 22C reexamined NUCLEAR STRUCTURE 22C; calculated two-neutron removal energy, matter radius, two neutron halo structure, B(E1), and correlation density by three-body model using hyperspherical harmonics method. Comparison with available theoretical and experimental results. NUCLEAR REACTIONS 12C, 208Pb(22C, 20C), E=240 MeV/nucleon; calculated fragmentation σ on C and Pb targets, and Coulomb dissociation σ on Pb target.
doi: 10.1103/PhysRevC.97.064307
2017GR04 Phys.Rev. C 95, 021601 (2017) L.V.Grigorenko, T.A.Golubkova, J.S.Vaagen, M.V.Zhukov Decay mechanism and lifetime of 67Kr RADIOACTIVITY 67Kr(2p); calculated half-life as function of p-wave ground-state resonance energy in 66Br, and from three-body model results for P3 and P5 potentials producing different configuration mixings, energy correlations between the 65Se core and one of the protons in 2p decay of 67Kr. Improved direct decay model (IDDM). Comparison with experimental value of T1/2.
doi: 10.1103/PhysRevC.95.021601
2014ER01 Phys.Atomic Nuclei 77, 374 (2014) S.N.Ershov, J.S.Vaagen, M.V.Zhukov New method for solution of coupled radial Schrodinger equations: application to the Borromean two-neutron halo nucleus 22C NUCLEAR STRUCTURE 22C; calculated radii, dipole strength function distributions. Prufer transformations. NUCLEAR REACTIONS 208Pb(22C, xn), E=40, 140, 240 MeV/nucleon; calculated E1 electromagnetic dissociation σ.
doi: 10.1134/S1063778814030077
2014ER03 Phys.Atomic Nuclei 77, 989 (2014) S.N.Ershov, J.S.Vaagen, M.V.Zhukov Cluster model with core excitations. The 11Be example NUCLEAR STRUCTURE 11Be; calculated energy levels, J, π. Two-body cluster model with core excitations.
doi: 10.1134/S1063778814070072
2012ER07 Phys.Rev. C 86, 034331 (2012) S.N.Ershov, J.S.Vaagen, M.V.Zhukov Binding energy constraint on matter radius and soft dipole excitations of 22C NUCLEAR STRUCTURE 22C; calculated electromagnetic dissociation σ, E1 strength function and other observables as function of S(2n) to explore effect of S(2n) on the spatial extension of an s-dominated Borromean halo nucleus. Cluster three-body hyperspherical harmonic (HH) model.
doi: 10.1103/PhysRevC.86.034331
2012VA10 J.Phys.:Conf.Ser. 381, 012049 (2012) J.S.Vaagen, S.N.Ershov, M.V.Zhukov Lessons from two paradigmatic developments; Rutherford's nuclear atom and halo nuclei
doi: 10.1088/1742-6596/381/1/012049
2011ER05 Phys.Rev. C 84, 064308 (2011) S.N.Ershov, J.S.Vaagen, M.V.Zhukov Modified variable phase method for the solution of coupled radial Schrodinger equations NUCLEAR STRUCTURE 6He; calculated S-matrix elements as a function of the hyper radius of continuum states. Modified variable phase method for the numerical solution of coupled radial Schrodinger equations.
doi: 10.1103/PhysRevC.84.064308
2011JE02 Phys.Rev. C 83, 021305 (2011) O.Jensen, G.Hagen, M.Hjorth-Jensen, J.S.Vaagen Closed-shell properties of 24O with ab initio coupled-cluster theory NUCLEAR STRUCTURE 23O, 23Ne; calculated single-particle levels, J, π. 24O; calculated neutron- and proton-removal spectroscopic factors for hole states in 24O. Coupled-cluster method with chiral nucleon-nucleon N3L interaction including role of continuum states. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.021305
2010JE03 Phys.Rev. C 82, 014310 (2010) O.Jensen, G.Hagen, T.Papenbrock, D.J.Dean, J.S.Vaagen Computation of spectroscopic factors with the coupled-cluster method NUCLEAR STRUCTURE 15N, 15,16O; calculated ground-state energies, spectroscopic factors for removal of proton and neutron from 16O using coupled-cluster theory and equation of motion.
doi: 10.1103/PhysRevC.82.014310
2007DA30 Phys.Rev. C 76, 064612 (2007) B.V.Danilin, J.S.Vaagen, T.Rogde, S.N.Ershov, I.J.Thompson, M.V.Zhukov, and the RNBT Collaboration Three-body continuum energy correlations in Borromean halo nuclei. III. Short-range external fields NUCLEAR STRUCTURE 6He, 11Li; calculated energy correlations using three-body cluster model for halo nuclides.
doi: 10.1103/PhysRevC.76.064612
2007VA11 Int.J.Mod.Phys. E16, 1033 (2007) J.S.Vaagen, B.V.Danilin, S.N.Ershov Continuum spectroscopy of Halo nuclei NUCLEAR REACTIONS 208Pb(6He, X), E=240 MeV/nucleon; calculated cross sections, excitation functions and angular correlations. Compared results to available data.
doi: 10.1142/S0218301307006484
2006DA13 Phys.Rev. C 73, 054002 (2006) B.V.Danilin, J.S.Vaagen, T.Rogde, S.N.Ershov, I.J.Thompson, M.V.Zhukov, and the Russian-Nordic-British Theory (RNBT) Collaboration Three-body continuum energy correlations in Borromean halo nuclei. II NUCLEAR STRUCTURE 6He; calculated energy correlations in three-body continuum, resonance features.
doi: 10.1103/PhysRevC.73.054002
2006ER04 Phys.Rev. C 74, 014603 (2006) S.N.Ershov, B.V.Danilin, J.S.Vaagen Continuum spectroscopy of Borromean two-neutron halo nuclei NUCLEAR REACTIONS 208Pb(6He, 2nα), E=240 MeV/nucleon; calculated fragment energy and angular correlations. Microscopic four-body distorted wave approach, comparison with data.
doi: 10.1103/PhysRevC.74.014603
2006HA14 Phys.Rev. C 73, 034321 (2006) Study of resonant structures in a deformed mean field by the contour deformation method in momentum space
doi: 10.1103/PhysRevC.73.034321
2005DA21 Phys.Rev. C 71, 057301 (2005) B.V.Danilin, S.N.Ershov, J.S.Vaagen Charge and matter radii of Borromean halo nuclei: The 6He nucleus NUCLEAR STRUCTURE 4,6He; calculated charge form factors, matter density distributions.
doi: 10.1103/PhysRevC.71.057301
2005ER06 Phys.Rev. C 72, 044606 (2005) S.N.Ershov, B.V.Danilin, J.S.Vaagen Electron scattering on two-neutron halo nuclei with full inclusion of final state interactions NUCLEAR REACTIONS 6He(e, e'), (e, e'α), E=500 MeV; calculated σ(E, θ), final state interaction contributions.
doi: 10.1103/PhysRevC.72.044606
2005HA21 Phys.Rev. C 71, 044314 (2005) G.Hagen, M.Hjorth-Jensen, J.S.Vaagen Effective interaction techniques for the Gamow shell model NUCLEAR STRUCTURE 5,6,7He; calculated level energies, configurations. Gamow shell model, effective interactions compared.
doi: 10.1103/PhysRevC.71.044314
2005HA41 J.Phys.(London) G31, S1337 (2005) G.Hagen, M.Hjorth-Jensen, J.S.Vaagen State-dependent interactions for the Gamow shell model NUCLEAR STRUCTURE 5,6,7He; calculated resonance energies, configurations. Gamow shell model.
doi: 10.1088/0954-3899/31/8/012
2004DA07 Phys.Rev. C 69, 024609 (2004) B.V.Danilin, T.Rogde, J.S.Vaagen, I.J.Thompson, M.V.Zhukov, and the RNBT Collaboration Three-body continuum spatial correlations in Borromean halo nuclei NUCLEAR STRUCTURE 6He; calculated low-lying resonance features, spatial correlations in three-body continuum. Hyperspherical harmonics method.
doi: 10.1103/PhysRevC.69.024609
2004ER07 Phys.Rev. C 70, 054608 (2004) S.N.Ershov, B.V.Danilin, J.S.Vaagen, A.A.Korsheninnikov, I.J.Thompson Structure of the 11Li continuum from breakup on proton target NUCLEAR REACTIONS 1H(11Li, 11Li'), E=68 MeV/nucleon; calculated σ(E, θ), energy and angular correlations. 11Li deduced continuum features. Microscopic four-body distorted-wave model, comparisons with data.
doi: 10.1103/PhysRevC.70.054608
2003HE02 Nucl.Phys. A713, 63 (2003) H.Heiberg-Andersen, R.S.Mackintosh, J.S.Vaagen A new phenomenological τ-α interaction NUCLEAR REACTIONS 4He(3He, 3He), E=20-30 MeV; calculated σ(θ), analyzing powers, parity dependence features, three-nucleon exchange process. 7Be deduced level energy. Phenomenological interaction, comparisons with data.
doi: 10.1016/S0375-9474(02)01291-5
2002AN28 Bull.Rus.Acad.Sci.Phys. 65, 1668 (2002) G.S.Anagnostatos, J.S.Vaagen, K.A.Gridnev, M.P.Kartamyshev, V.K.Lukyanov Role of Linear α-Cluster Configuration in Formation of Charge Form Factors of 12C Nucleus NUCLEAR STRUCTURE 12C; calculated electron scattering form factors; deduced role of linear α-cluster configuration.
2002GR26 Int.J.Mod.Phys. E11, 359 (2002) K.A.Gridnev, M.P.Kartamyshev, J.S.Vaagen, V.K.Lukyanov, G.S.Anagnostatos The Role of Linear Alpha-Cluster Configuration for 12C NUCLEAR STRUCTURE 12C; calculated electron scattering form factors; deduced role of linear α-cluster configuration.
doi: 10.1142/S0218301302000934
2002ZH14 Yad.Fiz. 65, 777 (2002); Phys.Atomic Nuclei 65, 746 (2002) M.V.Zhukov, Yu.L.Parfenova, J.S.Vaagen Reaction Mechanisms for Light Halo Nuclei
doi: 10.1134/1.1471285
2001DA17 Yad.Fiz. 64, No 7, 1290 (2001); Phys.Atomic Nuclei 64, 1215 (2001) B.D.Danilin, I.J.Thompson, M.V.Zhukov, J.S.Vaagen, and the RNBT (Russian-Nordic-British Theory) Collaboration Few-Body Cluster Models for Borromean Halo Nuclei NUCLEAR STRUCTURE 6H, 11Li; analyzed resonances, cluster correlations, halo features. Few-body cluster models.
doi: 10.1134/1.1389545
2001ER05 Yad.Fiz. 64, No 7, 1298 (2001); Phys.Atomic Nuclei 64, 1223 (2001) S.N.Ershov, B.V.Danilin, J.S.Vaagen Four-Body Distorted-Wave Theory for Halo Excitations in Peripheral Fragmentation Reactions NUCLEAR REACTIONS 12C, 208Pb(6He, 2nα), E=240 MeV; calculated σ, excitation spectra, fragments relative energy spectra. Four-body distorted-wave theory, comparison with data.
doi: 10.1134/1.1389546
2001ER08 Phys.Rev. C64, 064609 (2001) S.N.Ershov, B.V.Danilin, J.S.Vaagen Inelastic Excitations and Momentum Distributions in Kinematically Complete Breakup Reactions of Two-Neutron Halo Nuclei NUCLEAR REACTIONS 12C, 208Pb(6He, 2nα), E=240 MeV; calculated σ(E), σ(θ), fragment momentum distributions, multipole contributions, Coulomb and nuclear contributions; deduced role of inelastic excitations. Microscopic quantum-mechanical approach, comparisons with data.
doi: 10.1103/PhysRevC.64.064609
2001HE24 Nucl.Phys. A690, 306c (2001) H.Heiberg-Andersen, J.S.Vaagen, I.J.Thompson Comparative Coupled Channels Studies of 6Li(p, τ)α and p(6He, α)t at E/A = 25 MeV NUCLEAR REACTIONS 6Li(p, 3He), E=25 MeV; 1H(6He, α), (6He, 5He), E=151 MeV; calculated σ(θ); deduced reaction mechanism features. Comparisons with data.
doi: 10.1016/S0375-9474(01)01047-8
2001VA25 Nucl.Phys. A690, 302c (2001) J.S.Vaagen, B.V.Danilin, S.N.Ershov, I.J.Thompson, M.V.Zhukov, with the RNBT Collaboration Extracting Reliable Knowledge of Halo Characteristics
doi: 10.1016/S0375-9474(01)00964-2
2000ER09 Phys.Rev. C62, 041001 (2000) S.N.Ershov, B.V.Danilin, J.S.Vaagen Four-Body Distorted Wave Theory for Halo Excitations NUCLEAR REACTIONS 12C, 208Pb(6He, 2nα), E=240 MeV/nucleon; calculated σ(E), total σ for elastic and inelastic breakup. Four-body DWIA. Comparisons with data.
doi: 10.1103/PhysRevC.62.041001
2000GR06 Phys.Rev. C61, 054304 (2000) Necessary Conditions for Binding in Few-Body Systems NUCLEAR STRUCTURE 6He; analyzed conditions for existence of bound state. Variational principle.
doi: 10.1103/PhysRevC.61.054304
2000PA53 Phys.Rev. C62, 044602 (2000) Yu.L.Parfenova, M.V.Zhukov, J.S.Vaagen Breakup of 11Be and 15C on Light Targets Including Core Excitations NUCLEAR REACTIONS 9Be(11Be, 10Be), E=63 MeV/nucleon; 9Be(15C, 14C), E=83 MeV/nucleon; calculated σ, core fragment longitudinal momentum distribution; deduced role of core excitations. 15C deduced halo features. Eikonal approximation, comparisons with data.
doi: 10.1103/PhysRevC.62.044602
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
1999ER01 Phys.Rev.Lett. 82, 908 (1999) S.N.Ershov, B.V.Danilin, T.Rogde, J.S.Vaagen New Insight into Halo Fragmentation NUCLEAR REACTIONS 1H(6He, 2nα), E=50, 200 MeV/nucleon; calculated transverse, longitudinal momentum distributions for alphas, neutrons; deduced role of low-lying continuum structure. Microscopic four-body distorted wave theory.
doi: 10.1103/PhysRevLett.82.908
1999OG06 Phys.Rev.Lett. 82, 4996 (1999) Yu.Ts.Oganessian, V.I.Zagrebaev, J.S.Vaagen ' Di-Neutron ' Configuration of 6He NUCLEAR REACTIONS 4He(6He, 6He), E=151 MeV; 1H(6He, α), E(cm)=21.6 MeV; 6Li(p, 3He), E(cm)=21.4 MeV; analyzed σ(θ); deduced parameters. 6He deduced di-neutron configuration. Realistic four-body model.
doi: 10.1103/PhysRevLett.82.4996
1999OG09 Phys.Rev. C60, 044605 (1999) Yu.Ts.Oganessian, V.I.Zagrebaev, J.S.Vaagen Dynamics of Two-Neutron Transfer Reactions with the Borromean Nucleus 6He NUCLEAR REACTIONS 6Li(α, α), E=166 MeV; 1H(6He, 6He), E=151 MeV; 6Li(p, 3He), E(cm)=21.4 MeV; analyzed σ(θ); deduced optical model parameters. 4He(6He, 6He), (6He, α), E=151 MeV; 1H(6He, α), E(cm)=21.4 MeV; calculated σ(θ); deduced two-neutron transfer features. 4He(8He, 8He), E=5-35 MeV/nucleon; calculated σ(θ). Four-body three-dimensional DWBA approach.
doi: 10.1103/PhysRevC.60.044605
1998DA08 Nucl.Phys. A632, 383 (1998) B.V.Danilin, I.J.Thompson, J.S.Vaagen, M.V.Zhukov Three-Body Continuum Structure and Response Functions of Halo Nuclei (I): 6He NUCLEAR STRUCTURE 6He; calculated ground-state properties, levels, continuum features, electric dipole strength distribution, resonances. Three-body model.
doi: 10.1016/S0375-9474(98)00002-5
1998RI02 Nucl.Phys. A628, 363 (1998) D.Ridikas, M.H.Smedberg, J.S.Vaagen, M.V.Zhukov Exploratory Coupled Channels Calculations for Loosely Bound Carbon Isotopes NUCLEAR STRUCTURE 17,19C; calculated matter radii, E1 strength functions, neutron stripping, Coulomb dissociation cross sections. Neutron-plus-core coupling model. NUCLEAR REACTIONS Be(19C, n18C), E=77 MeV/nucleon; Be(17C, n16C), E=83 MeV/nucleon; analyzed fragments transverse, longitudinal momentum distributions. Neutron-plus-core coupling model.
doi: 10.1016/S0375-9474(98)00657-5
1998TH04 J.Phys.(London) G24, 1505 (1998) I.J.Thompson, B.V.Danilin, V.D.Efros, M.V.Zhukov, J.S.Vaagen, and the Russian-Nordic-British Theory (RNBT) Collaboration Structure and Continuum Response of Halo Nuclei NUCLEAR STRUCTURE 6He, 11Li; calculated low-energy continuum states features; deduced neutron-neutron correlations role.
doi: 10.1088/0954-3899/24/8/026
1997DA01 Phys.Rev. C55, R577 (1997); Comment Phys.Rev. C59, 554 (1999) B.V.Danilin, T.Rogde, S.N.Ershov, H.Heiberg-Andersen, J.S.Vaagen, I.J.Thompson, M.V.Zhukov New Modes of Halo Excitation in the 6He Nucleus NUCLEAR REACTIONS 6He(p, p'), E=50 MeV; 6Li(n, p), E=50 MeV; calculated angle integrated σ. 6He deduced new modes of halo excitation. Three-body cluster model, DWIA.
doi: 10.1103/PhysRevC.55.R577
1997ER05 Phys.Rev. C56, 1483 (1997) S.N.Ershov, T.Rogde, B.V.Danilin, J.S.Vaagen, I.J.Thompson, F.A.Gareev Halo Excitation of 6He in Inelastic and Charge-Exchange Reactions NUCLEAR REACTIONS 6Li(n, p), E=118 MeV; analyzed σ(θ). 6He(p, p'), E=50 MeV; 6Li(n, p), E=50 MeV; calculated σ(θ) vs excitation energy, spin decomposition; deduced resonancelike structures, soft dipole excitation mode role. Four-body distorted wave theory.
doi: 10.1103/PhysRevC.56.1483
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
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
1995GA22 Yad.Fiz. 58, No 3, 422 (1995); Phys.Atomic Nuclei 58, 371 (1995) F.A.Gareev, S.N.Ershov, G.S.Kazacha, J.S.Vaagen Data-to-Data Relations between Elastic and Inelastic Scattering in the Nuclear Rainbow Region of Angles NUCLEAR REACTIONS 12C(12C, 12C), (12C, 12C'), E=240-1449 MeV; 12C(6Li, 6Li), (6Li, 6Li'), E=210, 318 MeV; 12C(3He, 3He), (3He, 3He'), E=72 MeV; 14C(3He, t), E=72 MeV; analyzed σ(θ); deduced model parameters. Data-to-data relations investigation, eikonal approximation, DWBA approaches.
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
1995ZH31 Phys.Rev. C52, 2461 (1995) M.V.Zhukov, B.V.Danilin, L.V.Grigorenko, J.S.Vaagen β Decay of 11Li to the Deuteron Channel and Halo Analog States in 11Be RADIOACTIVITY 11Li(β-); calculated β-decay probability vs E(d), total branching ratio for decay to deuteron channel. Microscopic hyperspherical harmonics method, halo analog states. NUCLEAR STRUCTURE 11Be; calculated wave functions, separation energies, halo analog state. 11Li; calculated wave functions, separation energies. Microscopic hyperspherical harmonics method.
doi: 10.1103/PhysRevC.52.2461
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
1994GA38 Yad.Fiz. 57, No 6, 1020 (1994); Phys.Atomic Nuclei 57, 959 (1994) F.A.Gareev, Yu.L.Ratis, P.P.Korovin, E.A.Strokovsky, J.S.Vaagen Analysis of Discrete Ambiguities for πNΔ aand ρNΔ Vertex Functions Using Inclusive Charge-Exchange Reactions NUCLEAR REACTIONS 1H(p, nX), (n, pX), E=1 GeV; calculated inclusive σ(θ, En), σ(θ, Ep); 1H(3He, t), E not given; analyzed data; deduced πNΔ, ρNΔ vertex function dependence. Feynman diagrams approach.
1994GA39 Yad.Fiz. 57, No 8, 1404 (1994); Phys.Atomic Nuclei 57, 1333 (1994) F.A.Gareev, Yu.L.Ratis, P.P.Korovin, E.A.Strokovsky, J.S.Vaagen Interference Effects in Inclusive Charge-Exchange p + p → n + X and n + p → n + X Reactions at Intermediate Energies NUCLEAR REACTIONS 1H(p, X), E=0.8-10 GeV; 1H(3He, tX), E=0.8-2.78 GeV/nucleon; 1H(n, X), E=1 GeV; analyzed inclusive σ(θp, Ep), σ(θn, En), invariant σ; deduced modes interference dependence on vertex parameters.
1994GA40 Yad.Fiz. 57, No 8, 1411 (1994); Phys.Atomic Nuclei 57, 1340 (1994) F.A.Gareev, Yu.L.Ratis, A.G.Semtchenkov, E.A.Strokovsky, J.S.Vaagen Inclusive (p, n) and (3He, t) Reactions on Nuclei in the Quasi-Elastic and Δ-Isobar Excitation Region NUCLEAR REACTIONS 1,2H, 7Li, 9Be, 10,11B, 12C, 16O, 19F, 24,25,26Mg, 40,44Ca, Cu, 116,124Sn, 181Ta, Pb(p, nX), E=0.8-2.78 GeV; 1H(3He, tX), E=0.8-2.78 GeV/nucleon; analyzed data; deduced reaction mechanism similarity. Quasi-elastic formation, Δ-isobar excitation.
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
1993SA35 Europhys.Lett. 22, 511 (1993) S.B.Sakuta, A.A.Ogloblin, O.Ya.Osadchy, Yu.A.Glukhov, S.N.Ershov, F.A.Gareev, J.S.Vaagen Direct Experimental Evidence for a Soft-Dipole Response in 6He NUCLEAR REACTIONS 6Li(7Li, 7Be), E=78, 82 MeV; measured σ(θ), σ(E(7Be)). 6He deduced soft dipole response evidence.
doi: 10.1209/0295-5075/22/7/006
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
1992DE18 Nucl.Phys. A542, 208 (1992) A.S.Demyanova, E.F.Svinareva, S.A.Goncharov, S.N.Ershov, F.A.Gareev, G.S.Kazacha, A.A.Ogloblin, J.S.Vaagen Scattering of 3He on 12C and the Inelastic Form Factor NUCLEAR REACTIONS 12C(3He, 3He'), E=72 MeV; measured σ(θ); deduced strong absorption radius form factor role. DWBA.
doi: 10.1016/0375-9474(92)90213-4
1992GA27 Europhys.Lett. 20, 487 (1992) F.A.Gareev, S.N.Ershov, E.F.Svinareva, B.V.Danilin, S.A.Fayans, D.V.Fedorov, M.V.Zhukov, S.A.Goncharov, J.S.Vaagen Proton Elastic Scattering on Neutron Halo Nuclei NUCLEAR REACTIONS 6Li, 6He(p, p), E=100-270 MeV; calculated σ(θ); deduced size, halo effect roles. Folding model.
doi: 10.1209/0295-5075/20/6/003
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
1991ZH25 Phys.Lett. 265B, 19 (1991) M.V.Zhukov, B.V.Danilin, D.V.Fedorov, J.S.Vaagen, F.A.Gareev, J.Bang Calculation of 11Li in the Framework of a Three-Body Model with Simple Central Potentials NUCLEAR STRUCTURE 11Li; calculated binding energy, constituents rms distances, inclusive momentum distributions. Three-body model, central potentials.
doi: 10.1016/0370-2693(91)90006-C
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
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
1987RA16 Nucl.Phys. A470, 79 (1987) T.Ramsoy, A.Atac, T.Engeland, M.Guttormsen, J.Rekstad, G.Lovhoiden, T.F.Thorsteinsen, J.S.Vaagen Particle-Vibration Coupled States in 161Dy NUCLEAR REACTIONS 161Dy(3He, 3He'), E=32 MeV; measured σ(E), Eγ, Iγ, 3Heγ-coin. 161Dy deduced levels, J, π. Particle-core model calculations. Ge, Si counters, enriched target.
doi: 10.1016/0375-9474(87)90121-7
1987RO15 Nucl.Phys. A469, 407 (1987) T.Rodland, J.R.Lien, G.Lovhoiden, T.F.Thorsteinsen, J.S.Vaagen Nuclear Structure Studies with Pick-Up Reactions on Even Tellurium Nuclei: The 120Te (d, t)119Te and the 120Te (τ, α)119Te reactions NUCLEAR REACTIONS 120Te(d, t), E=17 MeV; 120Te(3He, α), E=24 MeV; measured σ(E(t), θ), σ(E(α), θ); deduced model parameters. 119Te deduced levels, J, π, L, S. DWBA, CCBA analyses.
doi: 10.1016/0375-9474(87)90029-7
1986EN07 Phys.Scr. 34, 703 (1986) Population of Non-Coherent Intrinsic States in Anomalous (t, p) Monopole Transfer on Odd-Mass Rare-Earth Isotopes NUCLEAR STRUCTURE 181Hf, 169Er, 163Dy; calculated levels, pair occupation amplitudes, pair gaps, (t, p) transfer strengths. Microscopic model.
doi: 10.1088/0031-8949/34/6A/027
1986VA32 Phys.Scr. 34, 508 (1986) G.M.Vagradov, S.A.Kulagin, S.V.Akulinichev, F.A.Gareev, G.S.Kazacha, J.S.Vaagen Discussion of the EMC-Effect in Terms of Information from Knock-Out Reactions NUCLEAR STRUCTURE 2H, 14N, 56Fe; calculated normalized structure function ratio. Nucleon off-shell effects.
doi: 10.1088/0031-8949/34/6A/006
1985RO19 Phys.Scr. 32, 201 (1985) T.Rodland, J.R.Lien, G.Lovhoiden, J.S.Vaagen, V.Oygaard, C.Ellegaard Nuclear Structure Studies with Pick-Up Reactions on Even Tellurium Nuclei: The 128Te(d, t)127Te and the 128Te(τ, α)127Te reactions NUCLEAR REACTIONS 128Te(d, t), E=17 MeV; 128Te(3He, α), E=24 MeV; measured σ(Et), σ(Eα), σ(θ); deduced optical model parameters. 127Te deduced levels, L, S. DWBA, CCBA analyses.
doi: 10.1088/0031-8949/32/3/006
1985TH02 Nucl.Phys. A435, 125 (1985) T.F.Thorsteinsen, J.S.Vaagen, G.Lovhoiden, N.Blasi, M.N.Harakeh, S.Y.Van Der Werf Distributions of i13/2 Transfer Strength in (τ, α)-Induced Population of Odd-A Platinum Isotopes NUCLEAR REACTIONS 192,194,196,198Pt(3He, α), E=50 MeV; measured σ(Eα), σ(θ). 191,193,195,197Pt deduced levels, L, J, π, spectroscopic factors, neutron number dependence. Quasiparticle-core coupling models.
doi: 10.1016/0375-9474(85)90308-2
1984RO14 Phys.Scr. 29, 529 (1984) T.Rodland, J.R.Lien, J.S.Vaagen, G.Lovhoiden, C.Ellegaard Nuclear Structure Studies with Pick-Up Reactions on Even Tellurium Nuclei: The 126Te(d, t)125Te and the 126Te(3He, α)125Te reactions NUCLEAR REACTIONS 126Te(d, t), E=17 MeV; 126Te(3He, α), E=24 MeV; measured σ(θ), σ(Et), σ(Eα). 125Te deduced levels, L, spectroscopic factors, J, π. DWBA, CCBA analyses.
doi: 10.1088/0031-8949/29/6/006
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
1982VA03 Phys.Scr. 25, 443 (1982) A.Vaagnes, J.S.Vaagen, K.Kumar Quasiparticle-Core-Coupling in 191Pt using Dynamic Deformation Theory Core Wave Functions NUCLEAR STRUCTURE 191Pt; calculated levels, S. Quasiparticle-core coupling, dynamic deformation.
doi: 10.1088/0031-8949/25/3/002
1981TH05 Nucl.Phys. A363, 205 (1981) T.F.Thorsteinsen, G.Lovhoiden, J.S.Vaagen, A.Bjornberg, D.G.Burke High-Spin Positive-Parity States in 179Hf Studied by the 180Hf(τ, α) Reaction at 32 MeV NUCLEAR REACTIONS 180Hf(3He, α), E=32 MeV; measured σ(θ, Eα). 179Hf deduced levels, J, π, L. Quasiparticle-rotor model, CCBA calculation, deformed Woods-Saxon orbitals, nonadiabatic Coriolis mixing effects.
doi: 10.1016/0375-9474(81)90462-0
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
1980RO06 Nucl.Phys. A338, 13 (1980) T.Rodland, J.S.Vaagen, J.R.Lien On the Role of Multistep Processes in (d, t) and (3He, α) Induced Population of Low-Lying Negative-Parity States in 125Te NUCLEAR REACTIONS 126Te(d, t), E=17 MeV; 126Te(3He, α), E=24 MeV; measured σ(Et, θ), σ(Eα, θ). CCBA analysis, 3-quasiparticle theory.
doi: 10.1016/0375-9474(80)90118-9
1980TH04 Phys.Lett. 93B, 223 (1980) T.F.Thorsteinsen, J.S.Vaagen, G.Lovhoiden, D.G.Burke, E.R.Flynn Examination of Anomalous (t, α) Angular Distributions for the 5/2- (532) Band in 153Pm. A Case Study of Multistep Population of h11/2 Dominated Bands NUCLEAR REACTIONS 154Sm(t, α), E=17 MeV; analyzed σ(θ). 153Pm levels deduced band structure. CCBA, rotational model form factors, multistep processes.
doi: 10.1016/0370-2693(80)90499-2
1980VA06 Phys.Lett. 91B, 361 (1980) J.S.Vaagen, D.L.Hillis, P.D.Bond, C.E.Thorn, M.J.LeVine, J.J.Kolata, C.Flaum, J.-C.Sens Striking Sensitivity of the Angular Distribution of 12C + 184W (4+) to the Nuclear Hexadecapole Parameter NUCLEAR REACTIONS 184W(12C, 12C'), E=70 MeV; measured σ(θ). 184W level deduced hexadecapole deformation length. Rotor model, coupled-channels calculation.
doi: 10.1016/0370-2693(80)90996-X
1979VA06 Nucl.Phys. A319, 143 (1979) J.S.Vaagen, B.S.Nilsson, J.Bang, R.M.Ibarra One- and Two-Nucleon Overlaps Generated by a Sturmian Method NUCLEAR STRUCTURE 18O, 42Ca; calculated ground-state wave functions. Improved Sturmian expansion technique for two interacting nucleons in field of spherical core.
doi: 10.1016/0375-9474(79)90176-3
1978MA03 Phys.Rev.Lett. 40, 358 (1978) C.F.Maguire, D.L.Hendrie, U.Jahnke, J.Mahoney, D.K.Scott, J.S.Vaagen, R.J.Ascuitto, K.Kumar Observation of Striking Shape Differences between 21+ Angular Distributions for Heavy-Ion-Induced Two-Neutron Stripping and Pickup Reactions in Transitional Samarium Nuclei NUCLEAR REACTIONS 148Sm(18O, 16O), E=98.4 MeV; 148Sm(16O, 18O), E=104 MeV; 150Sm(12C, 14C), E=78 MeV; measured σ(θ).
doi: 10.1103/PhysRevLett.40.358
1978TH05 Phys.Lett. 76B, 270 (1978) Anomalous l = 5 One-Nucleon Transfer Data Discussed in Terms of a Two-Step Process NUCLEAR REACTIONS 168Er(d, t), E=17 MeV; calculated σ(θ).
doi: 10.1016/0370-2693(78)90784-0
1977HA28 Phys.Rev. C16, 902 (1977) D.L.Hanson, K.A.Erb, J.S.Vaagen, R.J.Ascuitto, D.A.Bromley, J.J.Kolata Quadrupole Transfer Strength Studied Through Heavy-Ion Induced Two-Neutron Transfer between the Shape Transitional Nuclei 190,192Os NUCLEAR REACTIONS 192Os(12C, 12C), (12C, 14C), E=70 MeV; measured σ(θ); deduced effect of shape transitions on quadrupole transfer strength. CCBA analysis.
doi: 10.1103/PhysRevC.16.902
1977KU13 Phys.Rev. C16, 1235 (1977) K.Kumar, B.Remaud, P.Aguer, J.S.Vaagen, A.C.Rester, R.Foucher, J.H.Hamilton Deformed-Quasiparticle Basis for Calculating Potential Energy Surfaces And Nuclear Spectra NUCLEAR STRUCTURE 148,150,152,154Sm, 186,188,190,192,194Os, 184,186,188,190Hg; calculated deformation energy curves. 24Mg, 102Zr, 168Er; calculated deformation energy curves, collective spectra.
doi: 10.1103/PhysRevC.16.1235
1976AS06 Nucl.Phys. A273, 230 (1976) R.J.Ascuitto, J.S.Vaagen, D.J.Pisano, C.E.Thorn, J.R.Lien, G.Lovhoiden Study of Neutron Transfer Through Inelastic Excitation in the Reaction 124Te(12C, 14C)122Te NUCLEAR REACTIONS 122,124Te(12C, 12C), (12C, 12C'), E=70 MeV; measured σ(θ); deduced optical model parameters. 124Te(12C, 14C), E=70 MeV; measured σ(E(14C), θ); deduced reaction mechanism. CCBA analysis, enriched 124Te target.
doi: 10.1016/0375-9474(76)90310-9
1976HA46 Nucl.Phys. A269, 520 (1976) D.L.Hanson, R.J.Ascuitto, J.S.Vaagen, K.A.Erb, D.A.Bromley, J.J.Kolata, D.J.Pisano Quadrupole Transfer Strength for Deformed Rare-Earth Nuclei as Studied With Heavy-Ion Induced Two-Nucleon Transfer Reactions NUCLEAR REACTIONS 154Sm(12C, 14C), E=65 MeV; 182W(12C, 14C), E=70 MeV; measured σ(E(14C), θ); deduced σ(θ) dependence on quadrupole transfer strength in presence of multistep processes. Enriched targets.
doi: 10.1016/0375-9474(76)90697-7
1976VA10 Nucl.Phys. A260, 317 (1976) Rotational Nuclei: Overlap Functions and Heavy-Ion Transfer Form Factors NUCLEAR REACTIONS 154Sm, 186W(12C, 14C), E ≈ 70 MeV; calculated form factors.
doi: 10.1016/0375-9474(76)90033-6
1975AS01 Phys.Lett. 55B, 289 (1975) R.J.Ascuitto, J.S.Vaagen, K.A.Erb, D.L.Hanson, D.A.Bromley, J.J.Kolata Inelastic Nuclear-Coulomb Interference and Direct-Two-Step Interference in Heavy-Ion Induced Two-Nucleon Transfer Reactions on Rare-Earth Nuclei NUCLEAR REACTIONS 186W(12C, 10Be), E=70 MeV; measured σ(E(10Be), θ).
doi: 10.1016/0370-2693(75)90602-4
1975LI22 Nucl.Phys. A253, 165 (1975) Study of (d, p) Reactions on Even Tellurium Nuclei: The 122Te(d, p)123Te Reaction NUCLEAR REACTIONS 122Te(d, p), E=7.5 MeV; measured σ(Ep, θ); deduced Q. 123Te deduced levels, neutron separation energy, L, J, π, S. Enriched target.
doi: 10.1016/0375-9474(75)90126-8
1974ER03 Phys.Rev.Lett. 33, 1102 (1974) K.A.Erb, D.L.Hanson, R.J.Ascuitto, B.Sorensen, J.S.Vaagen, J.J.Kolata Observation of Multistep Inelastic Processes in Heavy-Ion-Induced Two-Neutron Transfer Reactions on Rare-Earth Nuclei NUCLEAR REACTIONS 186W(12C, 14C), E=70 MeV; measured σ(E(14C), θ). 184W levels deduced form factors.
doi: 10.1103/PhysRevLett.33.1102
Back to query form |