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NSR database version of May 24, 2024.

Search: Author = J.S.Vaagen

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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2006HA14      Phys.Rev. C 73, 034321 (2006)

G.Hagen, J.S.Vaagen

Study of resonant structures in a deformed mean field by the contour deformation method in momentum space

doi: 10.1103/PhysRevC.73.034321
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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2000GR06      Phys.Rev. C61, 054304 (2000)

D.K.Gridnev, J.S.Vaagen

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
Citations: PlumX Metrics

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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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
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1986EN07      Phys.Scr. 34, 703 (1986)

T.Engeland, J.S.Vaagen

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1795.

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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetF0854.

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
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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
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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
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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
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1980BA38      Z.Phys. A297, 223 (1980)

J.M.Bang, J.S.Vaagen

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
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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
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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
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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
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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
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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
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1978TH05      Phys.Lett. 76B, 270 (1978)

T.F.Thorsteinsen, J.S.Vaagen

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
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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
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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
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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
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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
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1976VA10      Nucl.Phys. A260, 317 (1976)

J.S.Vaagen, R.J.Ascuitto

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
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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
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1975LI22      Nucl.Phys. A253, 165 (1975)

J.R.Lien, J.S.Vaagen, A.Graue

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
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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
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