NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = V.D.Efros Found 78 matches. 2019EF01 Phys.Rev. C 99, 034620 (2019) Calculating reactions with use of no-core shell-model states
doi: 10.1103/PhysRevC.99.034620
2017LE11 Few-Body Systems 58, 27 (2017) W.Leidemann, S.Deflorian, V.D.Efros Determination of S-Factors with the LIT Method NUCLEAR REACTIONS 3He(γ, pn), E not given;2H(p, γ), E not given; calculated σ, S-factor using LIT (Lorentz Integral Transform). Calculations just to indicate, whether this method is suitable to get high-precision S-factor.
doi: 10.1007/s00601-016-1193-y
2016EF01 Eur.Phys.J. A 52, 275 (2016) V.D.Efros, I.S.Timchenko, A.Yu.Buki Relation between (e, e') sum rules in 6, 7Li and 4He nuclei: Experiment and cluster model NUCLEAR STRUCTURE 4He, 6,7Li; calculated longitudinal sum rule; deduced, suggested expressing these sums in Li nuclei using α-particle values.
doi: 10.1140/epja/i2016-16275-x
2014BA40 Few-Body Systems 55, 1051 (2014) N.Barnea, V.Efros, W.Leidemann, G.Orlandini, E.Tomusiak Transverse (e, e') Response Functions for 4He NUCLEAR REACTIONS 4He(E, E'), E=500 MeV; calculated transverse response function parameters.
doi: 10.1007/s00601-014-0826-2
2014EF01 Phys.Rev. C 89, 027301 (2014) V.D.Efros, P.von Neumann-Cosel, A.Richter Properties of the first excited state of 9Be derived from (γ, n) and (e, e') reactions NUCLEAR REACTIONS 9Be(e, e'), E not given; 9Be(γ, n), E<2.21 MeV; deduced level energy and width of the first excited state in 9Be, B(E1) strength of decay of near-threshold 1/2+ resonance to ground state. R-matrix approach.
doi: 10.1103/PhysRevC.89.027301
2011EF01 Phys.Rev. C 83, 057001 (2011) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Frame dependence of 3He transverse (e, e') response functions at intermediate momentum transfers NUCLEAR REACTIONS 3H(e, e'), E at 500-700 MeV/c; analyzed frame dependence of transverse response function using two-fragment model. relativistic effects, realistic NN- and NNN-forces.
doi: 10.1103/PhysRevC.83.057001
2011LE02 Few-Body Systems 49, 71 (2011) W.Leidemann, Vi.D.Efros, G.Orlandini, E.L.Tomusiak Inclusive Electron Scattering Response Functions of 3He
doi: 10.1007/s00601-010-0114-8
2011YU02 Few-Body Systems 50, 375 (2011) L.Yuan, V.D.Efros, W.Leidemann, E.L.Tomusiak 3He Transverse Electron Scattering Response Function with Δ Degrees of Freedom
doi: 10.1007/s00601-010-0152-2
2010EF01 Phys.Rev. C 81, 034001 (2010) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Improved transverse (e, e') response function of 3He at intermediate momentum transfers NUCLEAR REACTIONS 3He(e, e'), E at 400-700 MeV/c; calculated transverse response functions using one-photon exchange approximation and AV18 NN potential and the UIX 3NF as the nuclear force in active nucleon Breit (ANB) frame. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.034001
2010YU08 Phys.Rev. C 82, 054003 (2010) L.Yuan, V.D.Efros, W.Leidemann, E.L.Tomusiak Transverse electron scattering response function of 3He with Δ-isobar degrees of freedom NUCLEAR REACTIONS 3He(e, e'), E at 850, 862, 927 MeV/c; calculated transverse inclusive response function using the Lorentz integral transform method. Comparisons with experimental data.
doi: 10.1103/PhysRevC.82.054003
2008DE15 Phys.Rev. C 77, 044007 (2008) S.Della Monaca, V.D.Efros, A.Khugaev, W.Leidemann, G.Orlandini, E.L.Tomusiak, L.P.Yuan Transverse electron scattering response function of 3He NUCLEAR REACTIONS 3He(e, e), E=250-500 MeV/c; calculated transverse response function, meson exchange currents.
doi: 10.1103/PhysRevC.77.044007
2008EF01 Phys.Atomic Nuclei 71, 1239 (2008); Yad.Fiz. 71, 1267 (2008) Electromagnetic processes in light nuclei: Results within a microscopic approach NUCLEAR REACTIONS 3H(e, e'X), 3He(e, e'X), 4He(e, e'X), E at 250-600 MeV/c; calculated longitudinal and transverse response function, σ; 3H(γ, X), 3He(γ, X), 4He(γ, X), 6He(γ, X), 6Li(γ, x), 7Li(γ, X), E not known; calculated σ(E); Dynamical non-relativistic calculation using realistic NN interaction.
doi: 10.1134/S106377880807017X
2007EF02 Bull.Rus.Acad.Sci.Phys. 71, 803 (2007); Izv.Akad.Nauk RAS, Ser.Fiz. 71, 831 (2007) Studies of the lightest nuclei in electromagnetic processes NUCLEAR REACTIONS 3H, 3He(γ, X), E≈ threshold; 4He(γ, n), E < 80 MeV; Analyzed cross sections and response functions.
doi: 10.3103/S106287380706010X
2006BA42 Few-Body Systems 39, 1 (2006) N.Barnea, W.Leidemann, G.Orlandini, V.D.Efros, E.L.Tomusiak On the Accuracy of Hyperspherical Harmonics Approaches to Photonuclear Reactions
doi: 10.1007/s00601-006-0152-4
2006EF01 Bull.Rus.Acad.Sci.Phys. 70, 308 (2006) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Allowance for relativistic effects in (e, e') response functions NUCLEAR REACTIONS 3He(e, e'), E ≈ 50-400 MeV; analyzed response functions, relativistic effects. Various approaches discussed.
2005EF02 Phys.Rev. C 72, 011002 (2005) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Improved (e, e') response functions at intermediate momentum transfers: The 3He case NUCLEAR REACTIONS 3He(e, e'), E ≈ 50-350 MeV; calculated response functions vs momentum transfer. Frame dependence, realistic NN and NNN forces. Comparison with data.
doi: 10.1103/PhysRevC.72.011002
2005QU04 Phys.Rev. C 72, 064002 (2005) S.Quaglioni, V.D.Efros, W.Leidemann, G.Orlandini 4He(e, e'p)3H reaction with full final-state interactions NUCLEAR REACTIONS 4He(e, e'p), E=high; calculated longitudinal response. Comparison with data.
doi: 10.1103/PhysRevC.72.064002
2004BB02 Few-Body Systems 35, 155 (2004) N.Barnea, V.D.Efros, W.Leidemann, G.Orlandini Incorporation of Three-Nucleon Force in the Effective-Interaction Hyperspherical-Harmonic Approach NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, radii. Three-nucleon force, comparison with previous results.
doi: 10.1007/s00601-004-0066-y
2004EF01 Phys.Rev. C 69, 044001 (2004) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Longitudinal electron scattering response functions of 3H and 3He NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, radii, electron scattering longitudinal response functions, three-nucleon force effects.
doi: 10.1103/PhysRevC.69.044001
2004QU02 Phys.Rev. C 69, 044002 (2004) S.Quaglioni, W.Leidemann, G.Orlandini, N.Barnea, V.D.Efros Two-body photodisintegration of 4He with full final state interaction NUCLEAR REACTIONS 4He(γ, p), (γ, n), E=20-120 MeV; calculated σ, final state interaction effects. Comparison with data.
doi: 10.1103/PhysRevC.69.044002
2003FO18 Nucl.Phys. A718, 434c (2003) C.Forssen, V.D.Efros, N.B.Shul'gina, M.V.Zhukov Analytical studies of 8B electromagnetic dissociation NUCLEAR REACTIONS Pb(8B, p7Be), E=936 MeV/nucleon; calculated σ, dependence on radius parameter. Analytical model.
doi: 10.1016/S0375-9474(03)00823-6
2002EF02 Few-Body Systems 32, 169 (2002) Elimination of Rotational Degrees of Freedom in Expansion Methods for Three Nucleons NUCLEAR STRUCTURE A=3; calculated Euler angle integrated matrix elements.
doi: 10.1007/s00601-002-0116-2
2002FO01 Nucl.Phys. A697, 639 (2002) C.Forssen, V.D.Efros, M.V.Zhukov Analytical E1 Strength Functions of Two-Neutron Halo Nuclei: The 6He example NUCLEAR REACTIONS Pb(6He, 2nα), E=37, 240 MeV/nucleon; calculated dissociation σ, excitation energy spectrum. Three-body model, comparisons with data. NUCLEAR STRUCTURE 6He; calculated wave functions, B(E1) distribution. Three-body model.
doi: 10.1016/S0375-9474(01)01260-X
2002FO06 Nucl.Phys. A706, 48 (2002) C.Forssen, V.D.Efros, M.V.Zhukov Analytical E1 Strength Functions of Two-Neutron Halo Nuclei: 11Li and 14Be NUCLEAR STRUCTURE 11Li, 14Be; calculated wave functions, E1 strength distributions, electromagnetic dissociation spectra. Analytical model.
doi: 10.1016/S0375-9474(02)00865-5
2002GO24 Nucl.Phys. A707, 365 (2002) J.Golak, R.Skibinski, W.Glockle, H.Kamada, A.Nogga, H.Witala, V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Benchmark Calculation of the Three-Nucleon Photodisintegration NUCLEAR REACTIONS 3H, 3He(γ, X), E < 140 MeV; calculated photoabsorption and photodisintegration σ. Fadeev equations and Lorentz integral transform method. Comparison with data.
doi: 10.1016/S0375-9474(02)00989-2
2001BA40 Phys.Rev. C63, 057002 (2001) N.Barnea, V.D.Efros, W.Leidemann, G.Orlandini Total 4He Photoabsorption Cross Section Reexamined: Correlated versus effective interaction hyperspherical harmonics NUCLEAR REACTIONS 4He(γ, X), E=20-35 MeV; calculated total photoabsorption σ. Comparison of hyperspherical harmonics expansions.
doi: 10.1103/PhysRevC.63.057002
2001EF01 Nucl.Phys. A684, 457c (2001) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Photodisintegration of Three-Body Nuclei with Realistic Interactions and Effects of 3N Forces NUCLEAR REACTIONS 3H, 3He(γ, X), E=0-30 MeV; calculated total photoabsorption σ; deduced 3N force contribution. Comparisons with data.
doi: 10.1016/S0375-9474(01)00503-6
2001EF02 Yad.Fiz. 64, No 3, 536 (2001); Phys.Atomic Nuclei 64, 482 (2001) V.D.Efros, W.Leidemann, G.Orlandini Electromagnetic Response Functions of Few-Nucleon Systems NUCLEAR REACTIONS 4He(e, e'), R ≈ 20-320 MeV; calculated longitudinal response functions. 3H, 3,4He(γ, X), E=20-140 MeV; calculated photoabsorption σ; deduced role of final state interactions, sensitivity to nuclear dynamics. Comparisons with data.
doi: 10.1134/1.1358473
2001EF03 Nucl.Phys. A689, 421c (2001) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Photodisintegration of Trinucleons with Realistic Interactions and Effects of NNN Forces NUCLEAR REACTIONS 3H, 3He(γ, X), E=5-140 MeV; calculated total photoabsorption σ, three-nucleon force effects.
doi: 10.1016/S0375-9474(01)00869-7
2000EF03 Phys.Lett. 484B, 223 (2000) V.D.Efros, W.Leidemann, G.Orlandini, E.L.Tomusiak Photodisintegration of Three-Body Nuclei with Realistic 2N and 3N Forces NUCLEAR REACTIONS 3H, 3He(γ, X), E=5-140 MeV; calculated total photoabsorption σ; deduced three-nucleon force contributions. Several models compared. Comparison with data.
doi: 10.1016/S0370-2693(00)00656-0
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
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
1999EF05 Few-Body Systems 26, 251 (1999) V.D.Efros, W.Leidemann, G.Orlandini Electromagnetic Few-Body Response Functions with the Lorentz Integral Transform Method NUCLEAR REACTIONS 3H(γ, X), E < 130 MeV; calculated photoabsorption σ. 4He(e, e'X), E not given; calculated longitudinal response function. Lorentz integral transform method.
doi: 10.1007/s006010050118
1999EF08 Yad.Fiz. 62, No 11, 1975 (1999); Phys.Atomic Nuclei 62, 1833 (1999) Method of Integral Transforms for Few-Body Reactions NUCLEAR REACTIONS 2H(e, e'), E not given; calculated longitudinal response function. 4He(γ, X), E not given; calculated Lorentz transform of the photodisintegration response function.
1999GR21 Phys.Rev. C60, 044312 (1999) L.V.Grigorenko, B.V.Danilin, V.D.Efros, N.B.Shulgina, M.V.Zhukov Extended Three-Cluster Model with Two-Cluster Long-Range Correlations: Application to the 8Li, 8B Nuclei NUCLEAR STRUCTURE 8Li, 8B; calculated binding energies, radii, levels spectroscopic factors. Three-cluster model, comparison with data.
doi: 10.1103/PhysRevC.60.044312
1999LE41 Fizika(Zagreb) B8, 135 (1999) W.Leidemann, V.D.Efros, G.Orlandini, E.L.Tomusiak Electromagnetic Few-Body Response Functions with the Lorentz Integral Transform NUCLEAR REACTIONS 3He(γ, X), E<140 MeV; 4He(γ, X), E<35 MeV; calculated photoabsorption σ. 4He(e, e'), E not given; calculated longitudinal response function. Lorentz integral transform method. Comparison with data.
1999OR05 Nucl.Phys. A649, 21c (1999) G.Orlandini, V.D.Efros, W.Leidemann Fully Microscopic Calculations of Giant Resonance in Few-Body Systems NUCLEAR REACTIONS 3,4He(γ, X), E < 140 MeV; calculated total photodisintegration σ; deduced resonance features. Lorentz integral transform method. Comparisons with data.
doi: 10.1016/S0375-9474(99)00033-0
1998EF02 Nucl.Phys. A631, 658c (1998) V.D.Efros, W.Leidemann, G.Orlandini Method of Integral Transforms for Calculating Few-Body Reactions
doi: 10.1016/S0375-9474(98)00086-4
1998EF05 Eur.Phys.J. A 1, 447 (1998) V.D.Efros, H.Oberhummer, A.Pushkin, I.J.Thompson Low-Energy Photodisintegration of 9Be and α + α + n ← → 9Be + γ Reactions at Astrophysical Conditions NUCLEAR REACTIONS 9Be(γ, n), E=1.6-2.2 MeV; calculated photodisintegration σ; deduced astrophysical reaction rates. Comparison with data. NUCLEAR STRUCTURE 9Be; calculated ground state, continuum wavefunctions. Three-body model.
doi: 10.1007/s100500050079
1998EF07 Phys.Rev. C58, 582 (1998) V.D.Efros, W.Leidemann, G.Orlandini Exact 4He Spectral Function in a Semirealistic NN Potential Model NUCLEAR REACTIONS 4He(e, e'), E not given; calculated longitudinal response vs momentum transfer. Momentum distribution approximations in spectral function calculation.
doi: 10.1103/PhysRevC.58.582
1998GR07 Phys.Rev. C57, R2099 (1998) L.V.Grigorenko, B.V.Danilin, V.D.Efros, N.B.Shulgina, M.V.Zhukov Structure of the 8Li and 8B Nuclei in an Extended Three-Body Model and Astrophysical S17 Factor NUCLEAR STRUCTURE 8Li, 8B; calculated levels, radii, quadrupole moments, wavefunctions. Three-body model. Comparison with data. NUCLEAR REACTIONS 7Be(p, γ), E not given; calculated astrophysical S-factor. Three-body model, asymptotic normalization coefficients.
doi: 10.1103/PhysRevC.57.R2099
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
1997EF01 Phys.Rev.Lett. 78, 432 (1997) V.D.Efros, W.Leidemann, G.Orlandini Accurate Four-Body Response Function with Full Final State Interaction: Application to electron scattering off 4He NUCLEAR REACTIONS 4He(e, e'), E not given; calculated response function. Full final state interaction used.
doi: 10.1103/PhysRevLett.78.432
1997EF04 Phys.Rev.Lett. 78, 4015 (1997); Erratum Phys.Rev.Lett. 80, 1570 (1998) V.D.Efros, W.Leidemann, G.Orlandini Is There a Pronounced Giant Dipole Resonance in 4He ( Question ) NUCLEAR REACTIONS 4He(γ, X), E=20-35 MeV; calculated σ(E). 4He deduced pronounced GDR, (γ, np) channel role. Four nucleon calculation, final state interactions.
doi: 10.1103/PhysRevLett.78.4015
1997EF05 Phys.Lett. 408B, 1 (1997) V.D.Efros, W.Leidemann, G.Orlandini Photodistintegration of the Three-Nucleon Systems and Their Polarizabilities NUCLEAR REACTIONS 3H, 3He(γ, X), E=5-150 MeV; analyzed absorption σ(E); deduced sum rule. 3H, 3He deduced polarizability. Lorentz integral transform method, several potentials compared.
doi: 10.1016/S0370-2693(97)00772-7
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
1996EF02 Z.Phys. A355, 101 (1996) V.D.Efros, W.Balogh, H.Herndl, R.Hofinger, H.Oberhummer Reaction Rate for Two-Neutron Capture by 4He NUCLEAR REACTIONS 5He(n, γ), E ≤ 1 MeV; 6He(γ, n), E ≈ 2-8 MeV; calculated σ(E); 6He(γ, 2n), E not given; calculated photodisintegration reaction rate vs temperature; comparison with 6He(α, n) reaction rate. Two-step mechanism, 4He(2n, γ) reaction rate also evaluated.
doi: 10.1007/s002180050084
1996EF03 Phys.Rev. C54, 1485 (1996) Ground-State Energies and Widths of 5He and 5Li Nuclei NUCLEAR REACTIONS 3H, 3He(d, γ), E not given; analyzed data analyses. 5He, 5Li deduced level energy, Γ. Comparison with other work.
doi: 10.1103/PhysRevC.54.1485
1996NU02 Nucl.Phys. A609, 43 (1996) F.M.Nunes, J.A.Christley, I.J.Thompson, R.C.Johnson, V.D.Efros Core Excitation in Three-Body Systems: Application to 12Be NUCLEAR STRUCTURE 12Be; calculated ground state binding energy, rms matter radius, levels, 10Be momentum distribution, spectroscopic factors for 11Be+n. Three-body hyperspherical formulation. NUCLEAR REACTIONS 12Be(p, d), E=30 MeV; calculated σ(θ). Finite-range DWBA, three-body hyperspherical formulation.
doi: 10.1016/S0375-9474(96)00284-9
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
1995DO35 Yad.Fiz. 58, No 9, 1601 (1995); Phys.Atomic Nuclei 58, 1509 (1995) V.Yu.Dobretsov, V.D.Efros, B.Shao Study of 3He(e, e') Longitudinal Response Functions with the Integral-Transform Method NUCLEAR REACTIONS 3He(e, e'), E not given; calculated longitudinal response function. Integral transform method.
1995EF05 Few-Body Systems 19, 167 (1995) Hyperspherical/Oscillator Brackets and Symmetrized States: A simple algorithm for A > 3 few-body calculations
doi: 10.1007/s006010050024
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
1994EF03 Phys.Lett. 338B, 130 (1994) V.D.Efros, W.Leidemann, G.Orlandini Response Functions from Integral Transforms with a Lorentz Kernel
doi: 10.1016/0370-2693(94)91355-2
1994EF04 Yad.Fiz. 57, No 7, 1341 (1994); Phys.Atomic Nuclei 57, 1271 (1994) How to Construct Subsets of Substantial Hyperspherical Harmonics
1992EF03 Yad.Fiz. 55, 2348 (1992); Sov.J.Nucl.Phys. 55, 1303 (1992) Electronuclear Sum Rules for the Lightest Nuclei NUCLEAR STRUCTURE 3,4He; calculated electronuclear longitudinal, transverse sum rule; deduced accuracy features.
1991DE21 Z.Phys. A339, 255 (1991) Electronuclear Sum Rules. Improved Realization and Statement. Experiment and Theory for 4He NUCLEAR REACTIONS 4He(e, e'), E ≈ 500-1180 MeV; calculated σ(θ(e'), E(e')). Electronuclear sum rule.
1989CH28 Europhys.Lett. 8, 245 (1989) L.V.Chulkov, B.V.Danilin, V.D.Efros, A.A.Korsheninnikov, M.V.Zhukov Nuclear-Reaction Cross-Sections at High Energies and Radii of Radioactive Nuclei. Radius of the 6He Nucleus NUCLEAR REACTIONS 9Be, 12C, 27Al(6He, X), E=790 MeV/nucleon; calculated reaction σ. Microscopic α+two-nucleon model.
doi: 10.1209/0295-5075/8/3/007
1989DA05 Yad.Fiz. 49, 351 (1989) B.V.Danilin, M.V.Zhukov, A.A.Korsheninnikov, L.V.Chulkov, V.D.Efros Calculation of 0+ T = 1 States of 6He, 6Li, and 6Be in Three-Particle α + 2N Model with Local Potentials NUCLEAR STRUCTURE 6He, 6Be, 6Li; calculated levels, Coulomb energy difference. Local potentials, hyperspherical harmonics method.
1989DA06 Yad.Fiz. 49, 360 (1989) B.V.Danilin, M.V.Zhukov, A.A.Korsheninnikov, L.V.Chulkov, V.D.Efros State Structure Study of the Isobaric Triplet of A = 6 Nuclei with J(π) = 0+ NUCLEAR STRUCTURE A=6; calculated correlation density. 6Be; calculated resonance three-particle decay. Hyperspherical harmonic method, α+2N model.
1989US02 Yad.Fiz. 49, 1297 (1989) Algebraic Cluster Approach to Low-Energy Reaction Calculations. n4He Scattering with Realistic NN Interactions. Inapplicability of Non-Polarization Approximation NUCLEAR REACTIONS 4He(n, n), E(cm)=1-7 MeV; calculated phase shifts; deduced nucleon-nucleon interaction dependence.
1988DA22 Yad.Fiz. 48, 1208 (1988); Sov.J.Nucl.Phys. 48, 766 (1988) B.V.Danilin, M.V.Zhukov, A.A.Korsheninnikov, V.D.Efros, L.V.Chulkov Pauli Focusing of Particles and Structure of the Ground State of the Nucleus 6He in the α + 2N Model NUCLEAR STRUCTURE 6He; calculated ground state density function profile.
1987DA31 Yad.Fiz. 46, 427 (1987) B.V.Danilin, M.V.Zhukov, A.A.Korsheninnikov, L.V.Chulkov, V.D.Efros Three-Particle Decays of Nuclei 6Be and 6He and Energy Spectra of α Particles and Nucleons NUCLEAR STRUCTURE 6He, 6Be; calculated α-spectra in three-particle decay mode.
1986EF01 Yad.Fiz. 43, 1439 (1986) Inelastic Scattering of Electrons by 3He and Traditional Low-Energy Scheme NUCLEAR REACTIONS 3He(e, e'), E ≈ 50-250 MeV; analyzed longitudinal response function. Traditional low energy scheme sum rule techniques.
1985BA39 Yad.Fiz. 41, 1460 (1985) A.M.Badalyan, T.I.Belova, N.B.Konyukhova, V.D.Efros Resonances in the 4H System NUCLEAR STRUCTURE 4H; calculated resonances. Central nucleon-nucleon potentials, microscopic model.
1981FO01 Phys.Lett. 98B, 389 (1981) Local Realistic NN Interactions in the Four-Nucleon Problem NUCLEAR STRUCTURE 4He; calculated binding energy, charge radius. Local realistic nucleon-nucleon interactions.
doi: 10.1016/0370-2693(81)90437-8
1981FO11 Yad.Fiz. 34, 868 (1981) Tensor Forces in the Four-Nucleon System NUCLEAR STRUCTURE 4He; calculated binding energy, rms charge radius. Hyperspherical harmonics method, tensor forces.
1980FO14 Yad.Fiz. 31, 1441 (1980); Sov.J.Nucl.Phys. 31, 748 (1980) Four-Nucleon Bound State with Realistic NN Interactions NUCLEAR STRUCTURE 4He; calculated binding energy. Realistic nucleon-nucleon interactions, hyperspherical harmonics.
1977BU09 Yad.Fiz. 25, 457 (1977); Sov.J.Nucl.Phys. 25, 246 (1977) A.Yu.Buki, N.G.Shevchenko, V.D.Efros, I.I.Chkalov Experimental Determination of the Coulomb Energy of the 6Li Nucleus NUCLEAR REACTIONS 6Li(e, e'), E=82-292 MeV; measured σ(E;θ); deduced form factor. 6Li deduced Coulomb energy.
1973DE19 Phys.Lett. 44B, 227 (1973) V.F.Demin, Y.E.Pokrovsky, V.D.Efros Bound-State Properties of Three and Four Nucleons with Realistic Forces NUCLEAR STRUCTURE 3H, 3He, 4He calculated binding energies.
doi: 10.1016/0370-2693(73)90210-4
1973EF01 Nucl.Phys. A202, 180 (1973) Some Properties of the Moshinsky Coefficients
doi: 10.1016/0375-9474(73)90250-9
1972DE61 Pisma Zh.Eksp.Teor.Fiz. 16, 504 (1972); JETP Lett.(USSR) 16, 360 (1972) Solution of the Nuclear Three-Body Problem with Relativistic Potentials NUCLEAR STRUCTURE 3H; calculated binding energy, rms radius.
1972EF01 Yad.Fiz. 15, 226 (1972); Sov.J.Nucl.Phys. 15, 128 (1972) K-Harmonics Method in the Few-Nucleon Problem
1972FE13 Yad.Fiz. 15, 887 (1972); Sov.J.Nucl.Phys. 15, 497 (1972) Correlated Basis in the Problem of Several Nucleons
1971DZ01 Yad.Fiz. 13, 22 (1971); Sov.J.Nucl.Phys. 13, 12 (1971) B.M.Dzyuba, V.V.Pustovalov, V.F.Rybachenko, A.A.Sadovoi, V.D.Efros Wave Function and Binding Energy of H3(He3) Nuclei with Allowance for the Tensor Interaction of the Nucleons NUCLEAR STRUCTURE 3H, 3He; calculated binding energy, wave function. K-harmonic method.
1971EF01 Phys.Lett. 37B, 18 (1971) Elastic n-4He Scattering as Five Body Problem NUCLEAR REACTIONS 4He(n, n), E=0-8 MeV; calculated σ(E). Five-body problem.
doi: 10.1016/0370-2693(71)90558-2
1971PE13 Yad.Fiz. 14, 567 (1971); Sov.J.Nucl.Phys. 14, 317 (1972) V.P.Permyakov, V.V.Pustovalov, Y.I.Fenin, V.D.Efros System of Four Nucleons, Neutron Scattering by Tritium NUCLEAR REACTIONS 3H(n, n), E < 7 MeV; calculated σ(E).
1971ZH05 Yad.Fiz. 14, 577 (1971); Sov.J.Nucl.Phys. 14, 322 (1972) Reactions in a System of Several Nucleons NUCLEAR REACTIONS 4He(n, n), E=0-8 MeV; calculated phase shifts. Variational principle.
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