NSR Query Results
Output year order : Descending NSR database version of April 26, 2024. Search: Author = V.I.Kukulin Found 124 matches. Showing 1 to 100. [Next]2021RU01 Phys.Rev. C 103, 014307 (2021) O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev In-medium T matrix in case of pairing instability
doi: 10.1103/PhysRevC.103.014307
2020KA56 Eur.Phys.J. A 56, 266 (2020) M.Kakenov, V.I.Kukulin, V.N.Pomerantsev, O.Bayakhmetov Properties of dibaryons in nuclear medium
doi: 10.1140/epja/s10050-020-00272-z
2020KU25 Eur.Phys.J. A 56, 229 (2020) V.I.Kukulin, O.A.Rubtsova, M.N.Platonova, V.N.Pomerantsev, H.Clement, T.Skorodko Nature of S-wave N N interaction and dibaryon production at nucleonic resonance thresholds
doi: 10.1140/epja/s10050-020-00236-3
2020PL01 Eur.Phys.J. A 56, 132 (2020) Theoretical study of spin observables in pd elastic scattering at energies Tp = 800-1000 MeV
doi: 10.1140/epja/s10050-020-00120-0
2018FR04 Phys.Lett. B 784, 277 (2018) C.Fritzsch, S.Barsov, I.Burmeister, S.Dymov, R.Gebel, M.Hartmann, A.Kacharava, A.Khoukaz, V.Komarov, V.I.Kukulin, P.Kulessa, A.Kulikov, A.Lehrach, B.Lorentz, D.Mchedlishvili, T.Mersmann, M.Mielke, S.Mikirtychiants, H.Ohm, M.Papenbrock, M.N.Platonova, D.Prasuhn, V.Serdyuk, H.Stroher, A.Taschner, Yu.Valdau, C.Wilkin Experimental and theoretical study of deuteron-proton elastic scattering for proton kinetic energies between T=882.2 MeV and T=918.3 MeV NUCLEAR REACTIONS 2H(p, p), E=882.2-918.3 MeV; 1H(d, d), E not given; measured reaction products; deduced σ(E). Comparison with available data.
doi: 10.1016/j.physletb.2018.07.045
2018KO31 Phys.Atomic Nuclei 81, 595 (2018); Yad.Fiz. 81, 555 (2018) E.S.Konobeevski, S.V.Zuyev, A.A.Kasparov, V.I.Kukulin, V.M.Lebedev, M.V.Mordovskoy, V.N.Pomerantsev, A.V.Spassky Low-Energy Parameters of Neutron-Neutron Interaction: Analysis of Data Obtained in nd and dd Breakup Reactions
doi: 10.1134/S1063778818050083
2018SA34 Eur.Phys.J. A 54, 126 (2018) D.A.Sailaubek, O.A.Rubtsova, V.I.Kukulin Charged particle scattering problem with a complex-range Gaussian basis NUCLEAR REACTIONS 4He(n, n), (p, p), E(cm)=0-20 MeV; calculated S-, P-, D-waves partial shifts found with real Gaussians and with CRGB (Complex-Range Gaussian basis).
doi: 10.1140/epja/i2018-12563-9
2017RU06 Phys.Rev. C 96, 034327 (2017) O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev, H.Muther In-medium bound states and pairing gap
doi: 10.1103/PhysRevC.96.034327
2016AB05 Eur.Phys.J. A 52, 259 (2016) Kh.U.Abraamyan, A.B.Anisimov, M.I.Baznat, K.K.Gudima, M.A.Kozhin, V.I.Kukulin, M.A.Nazarenko, S.G.Reznikov, A.S.Sorin Diphoton and dipion productions at the Nuclotron/NICA NUCLEAR REACTIONS C(d, 2γ), E at 2.75 GeV/c/nucleon; measured Eγ, Iγ(θ), γγ-coin using lead-glass calorimeter PHOTON-2; deduced photon pairs, 2π0 pairs invariant mass distribution resonance at 360 MeV.
doi: 10.1140/epja/i2016-16259-x
2016MU08 Phys.Rev. C 94, 024328 (2016) H.Muther, O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev Discrete wave-packet representation in nuclear matter calculations
doi: 10.1103/PhysRevC.94.024328
2016PL01 Nucl.Phys. A946, 117 (2016) Hidden dibaryons in one- and two-pion production in NN collisions
doi: 10.1016/j.nuclphysa.2015.11.009
2014KU21 Few-Body Systems 55, 633 (2014) Dibaryon Concept for Short-Range 2N and 3N Forces: Consequences for Hadronic and Nuclear Physics
doi: 10.1007/s00601-013-0775-1
2014PO04 Phys.Rev. C 89, 064008 (2014) V.N.Pomerantsev, V.I.Kukulin, O.A.Rubtsova New general approach in few-body scattering calculations: Solving discretized Faddeev equations on a graphics processing unit NUCLEAR REACTIONS 2H(n, n), E=13, 35 MeV; analyzed neutron analyzing power Ay(θ) data; calculated σ(θ) by wave packets (WPs) approach using standard Faddeev equations, and ultrafast graphic processing unit (GPU). Comparison of GPU and CPU realizations. New way of extensive many-body scattering calculations via continuum discretization procedure.
doi: 10.1103/PhysRevC.89.064008
2013KA39 Bull.Rus.Acad.Sci.Phys. 77, 830 (2013); Izv.Akad.Nauk RAS, Ser.Fiz 77, 914 (2013) R.S.Kabatayeva, O.A.Rubtsova, V.I.Kukulin Dynamic polarization of 6, 7Li nuclei in the elastic scattering of α particles NUCLEAR REACTIONS 6,7Li(α, α), E(cm)=7.8 MeV; calculated σ(θ). Comparison with available data.
doi: 10.3103/S1062873813070125
2013KU20 Phys.Atomic Nuclei 76, 1465 (2013); Yad.Fiz. 76, 1549 (2013) Short-range components of nuclear forces: Experiment versus mythology NUCLEAR REACTIONS 2H(d, 2n), E<12 MeV; 3He(γ, 2p), (E, d), E<0.75 GeV; calculated σ, σ(θ). QCD-based calculations, comparison with available data.
doi: 10.1134/S1063778813120120
2013PL01 Phys.Rev. C 87, 025202 (2013) ABC effect as a signal of chiral symmetry restoration in hadronic collisions
doi: 10.1103/PhysRevC.87.025202
2012KU35 Phys.Atomic Nuclei 75, 1373 (2012); Yad.Fiz. 75, 1447 (2012) Modern approaches for the theoretical description of multiparticle scattering and nuclear reactions NUCLEAR REACTIONS 17O(p, d), E=35 MeV; 13C(p, d), E=25.4 MeV; 12C(p, d), E=30 MeV; analyzed available data; deduced σ, phase shift, new formulation of quantum scattering theory in a discrete Hilbert space.
doi: 10.1134/S1063778812110130
2012PL05 J.Phys.:Conf.Ser. 381, 012110 (2012) Quark degrees of freedom in the deuteron and their testing in nucleon-deuteron scattering NUCLEAR REACTIONS 2H(p, p), E=250, 1000 MeV; calculated σ(θ) using ONE (one-nucleon exchaNGE) with DBM (dressed bag model) and CD-Bonn forces and Glauber model plus ONE. Compared with data.
doi: 10.1088/1742-6596/381/1/012110
2012RU04 Phys.Rev. C 86, 034004 (2012) O.A.Rubtsova, V.N.Pomerantsev, V.I.Kukulin, A.Faessler Three-body breakup within the fully discretized Faddeev equations NUCLEAR REACTIONS 2H(n, 2np), E=42 MeV; calculated σ(θ), three-body breakup amplitudes with fully discretized and modified Faddeev equations.
doi: 10.1103/PhysRevC.86.034004
2011BL05 Bull.Rus.Acad.Sci.Phys. 75, 490 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 526 (2011) L.D.Blokhintsev, V.I.Kukulin, V.N.Pomerantsev, D.A.Savin Exchange mechanism of dα interaction and vertex constants of 6Li NUCLEAR STRUCTURE 6Li; calculated wave functions of dα interaction, orbital angular momenta.
doi: 10.3103/S1062873811040083
2011KO25 Bull.Rus.Acad.Sci.Phys. 75, 443 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 478 (2011) E.S.Konobeevsky, V.I.Kukulin, M.V.Mordovskoi, V.N.Pomerantsev, S.I.Potashev, O.A.Rubtsova, V.A.Sergeev, S.V.Zuev, I.M.Sharapov Determination of neutron-neutron scattering length from the nd-breakup reaction: Experimental and theoretical aspects
doi: 10.3103/S1062873811040265
2011KU09 Bull.Rus.Acad.Sci.Phys. 75, 515 (2011); Izv.Akad.Nauk RAS, Ser.Fiz 75, 551 (2011) Studying the possibility of recovering np and nn helicity amplitudes on the basis of p(pol) + d(pol) and n(pol) + d(pol) scattering data at intermediate energies NUCLEAR REACTIONS 2H(p, p), E=1 GeV; calculated σ(θ), helicity amplitudes.
doi: 10.3103/S1062873811040289
2011KU23 Phys.Atomic Nuclei 74, 1567 (2011); Yad.Fiz. 74, 1594 (2011) Di- and multibaryon clusters in nuclei: A nontraditional view on the nature of nuclear forces and on the structure of nuclei
doi: 10.1134/S1063778811110123
2011RU11 Phys.Rev. C 84, 044002 (2011) O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev Validity of the coupled-channel reduction in three-body scattering NUCLEAR REACTIONS 16O(d, d'), E(cm)=5-40 MeV; calculated inelasticity parameter, elastic cross section. Full wave-packet continuum discretization (WPCD) approach and Pseudostate-Continuum (PC) approximation.
doi: 10.1103/PhysRevC.84.044002
2010KU16 Phys.Atomic Nuclei 73, 1376 (2010); Yad.Fiz. 73, 1418 (2010) Pinch-based thermonuclear D3He fusion driven by a femtosecond laser
doi: 10.1134/S1063778810080107
2010PL01 Phys.Atomic Nuclei 73, 86 (2010); Yad.Fiz. 73, 90 (2010) Description of spin-dependent observables in elastic proton-deuteron scattering on the basis of a generalized diffraction model
doi: 10.1134/S1063778810010114
2010PL02 Phys.Rev. C 81, 014004 (2010); Erratum Phys.Rev. C 94, 069902 (2016) Refined Glauber model versus Faddeev calculations and experimental data for pd spin observables NUCLEAR REACTIONS 2H(p, p), E=250, 440, 1000 MeV; calculated σ(E), proton and deuteron vector and tensor analyzing powers using the refined Glauber model. Comparison with experimental data.
doi: 10.1103/PhysRevC.81.014004
2010RU05 Phys.Rev. C 81, 064003 (2010) O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev, A.Faessler New approach toward a direct evaluation of the multichannel multienergy S matrix without solving the scattering equations
doi: 10.1103/PhysRevC.81.064003
2010RU08 Physics of Part.and Nuclei 41, 1123 (2010) O.A.Rubtsova, V.I.Kukulin, V.N.Pomerantsev Quantum scattering theory on the momentum lattice
doi: 10.1134/S1063779610070324
2009KU20 Phys.Atomic Nuclei 72, 1786 (2009) Dibaryon concept for nuclear force and its experimental evidence
doi: 10.1134/S1063778809100226
2009PO03 Phys.Rev. C 79, 034001 (2009) V.N.Pomerantsev, V.I.Kukulin, O.A.Rubtsova Solving three-body scattering problems in the momentum lattice representation
doi: 10.1103/PhysRevC.79.034001
2009RU06 Phys.Rev. C 79, 064602 (2009) O.A.Rubtsova, V.N.Pomerantsev, V.I.Kukulin Quantum scattering theory on the momentum lattice NUCLEAR REACTIONS 56Fe(n, n'), E(cm)<120 MeV; calculated σ(θ), s-wave phase shifts, inelasticity parameters, matrix elements using the wave-packet continuum discretization method to solve quantum-mechanical scattering problems.
doi: 10.1103/PhysRevC.79.064602
2008KU07 Phys.Rev. C 77, 041001 (2008) V.I.Kukulin, I.T.Obukhovsky, V.N.Pomerantsev, A.Faessler, P.Grabmayr Photon-induced neutron polarization from the 2H(γ, n(pol))1H reaction within the NN-force model with an intermediate dibaryon NUCLEAR REACTIONS 2H(γ, n), E<30 MeV; calculated σ, angular distributions, photon induced neutron polarizations using di-baryon (DB) and Nijmegen potential for nucleon-nucleon force. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.041001
2008RU10 Phys.Rev. C 78, 034603 (2008) O.A.Rubtsova, V.I.Kukulin, A.M.Moro Continuum discretization methods in a composite particle scattering off a nucleus: Benchmark calculations NUCLEAR REACTIONS 58Ni(d, d), E=12, 21.6, 80 MeV; calculated σ, σ(θ). Continuum discretized coupled channels method, wave-packet continuum discretization method.
doi: 10.1103/PhysRevC.78.034603
2007KU02 Phys.Atomic Nuclei 70, 215 (2007) V.I.Kukulin, I.T.Obukhovsky, V.N.Pomerantsev, P.Grabmayr, A.Faessler New short-range electromagnetic current in the deuteron NUCLEAR STRUCTURE 2H; calculated μ. NUCLEAR REACTIONS 2H(e, e), E not given; calculated structure function. 1H(polarized n, γ), E not given; calculated photon polarization.
doi: 10.1134/S1063778807020020
2007KU26 Phys.Rev. C 76, 047601 (2007) Elastic scattering on a nucleus and the breakup of the composite projectile via wave-packet continuum discretization
doi: 10.1103/PhysRevC.76.047601
2006KU27 Phys.Rev.C 74, 064005 (2006) V.I.Kukulin, I.T.Obukhovsky, P.Grabmayr, A.Faessler Isoscalar short-range current in the deuteron induced by an intermediate dibaryon NUCLEAR STRUCTURE 2H; calculated energy, radius, quadrupole moment, μ, form factors. Short range interaction via intermediate dibaryon.
doi: 10.1103/PhysRevC.74.064005
2005BL17 Yad.Fiz. 68, 1165 (2005); Phys.Atomic Nuclei 68, 1120 (2005) L.D.Blokhintsev, V.I.Kukulin, V.N.Pomerantsev Puzzle of the 6Li Quadrupole Moment: Steps toward Solving It NUCLEAR MOMENTS 6Li; calculated quadrupole moment; deduced role of three-deuteron configuration and negative exchange contribution.
doi: 10.1134/1.1992566
2005FA14 Ann.Phys.(New York) 320, 71 (2005) A.Faessler, V.I.Kukulin, M.A.Shikhalev Description of intermediate- and short-range NN nuclear force within a covariant effective field theory
doi: 10.1016/j.aop.2005.05.008
2005KU08 Yad.Fiz. 68, 374 (2005); Phys.Atomic Nuclei 68, 348 (2005) V.I.Kukulin, V.T.Voronchev, B.M.Kuzhevsky On Neutron Generation in Beryllium Plasma under the Effect of a Fast-Electron Beam NUCLEAR REACTIONS 9Be(e, e'nα), E=2-10 MeV; calculated reaction probability, neutron yield from beryllium plasma. Application as neutron source discussed.
doi: 10.1134/1.1866390
2005PO19 Yad.Fiz. 68, 1511 (2005); Phys.Atomic Nuclei 68, 1453 (2005) V.N.Pomerantsev, V.I.Kukulin, V.T.Voronchev, A.Faessler Dibaryon Model for Nuclear Force and the Properties of the 3N System NUCLEAR STRUCTURE 2H; calculated binding energy, radius, quadrupole moment. 3H, 3He; calculated binding energies, radii, three-nucleon force effects, related features. Dibaryon model.
doi: 10.1134/1.2053331
2005VO02 Nucl.Instrum.Methods Phys.Res. A539, 640 (2005) V.T.Voronchev, V.I.Kukulin, B.M.Kuzhevskij Electrodisintegration reaction in beryllium plasma as a source of neutrons NUCLEAR REACTIONS 9Be(e, e'nα), E < 10 MeV; calculated reaction probabilities in dense plasma.
doi: 10.1016/j.nima.2004.11.007
2004KU02 J.Phys.(London) G30, R1 (2004) The application of inversion to nuclear scattering
doi: 10.1088/0954-3899/30/R01
2004KU05 J.Phys.(London) G30, 287 (2004) V.I.Kukulin, V.N.Pomerantsev, M.Kaskulov, A.Faessler The properties of the three-nucleon system with the dressed-bag model for NN interaction: I. New scalar three-body force NUCLEAR STRUCTURE 3H, 3He; calculated bound-state energies, three-body force contributions. Dressed-bag model.
doi: 10.1088/0954-3899/30/3/005
2004KU06 J.Phys.(London) G30, 309 (2004) V.I.Kukulin, V.N.Pomerantsev, A.Faessler The properties of the three-nucleon system within the dressed bag model for 2N and 3N forces: II. Coulomb and CSB effects NUCLEAR STRUCTURE 3H, 3He; calculated Coulomb displacement energies, radii, three-body force contributions, charge-symmetry breaking effects. Dressed-bag model.
doi: 10.1088/0954-3899/30/3/006
2004KU17 Yad.Fiz. 67, 1558 (2004); Phys.Atomic Nuclei 67, 1536 (2004) Field-Theory Approach to the Dibaryon Model of Nuclear Forces
doi: 10.1134/1.1788045
2003KA56 Int.J.Mod.Phys. E12, 449 (2003) M.M.Kaskulov, P.Grabmayr, V.I.Kukulin A six-quark dressed-bag description of np → dγ radiative capture NUCLEAR REACTIONS 1H(n, γ), E=thermal; calculated capture σ. Six-quark dressed bag model.
doi: 10.1142/S0218301303001375
2003OB02 J.Phys.(London) G29, 2207 (2003) I.T.Obukhovsky, V.I.Kukulin, M.M.Kaskulov, P.Grabmayr, A.Faessler A dressed-bag model study of the short-range NΔ interaction in pion photoproduction processes off the deuteron NUCLEAR REACTIONS 1H(γ, π0), 1n(γ, π-), E ≈ 190-350 MeV; 2H(γ, pπ0), (γ, pπ-), E ≈ 100-500 MeV; calculated pion production σ, σ(θ); deduced role of short-range NΔ interaction. Dressed-bag model, comparison with data.
doi: 10.1088/0954-3899/29/9/315
2002KU14 Int.J.Mod.Phys. E11, 1 (2002) V.I.Kukulin, I.T.Obukhovsky, V.N.Pomerantsev, A.Faessler Two-Component Dressed-Bag Model for NN Interaction: Deuteron structure and phase shifts up to 1 GeV NUCLEAR STRUCTURE 2H; calculated energy, radius, μ, quadrupole moment, phase shifts. Two-component dressed-bag model.
doi: 10.1142/S0218301302000715
2001KU14 Nucl.Phys. A689, 327c (2001) V.I.Kukulin, I.T.Obukhovsky, T.Gutsche, V.E.Lyubovitsky, A.Faessler Dressed Six-Quark Bags at Short and Intermediate NN Ranges
doi: 10.1016/S0375-9474(01)00847-8
2001KU16 J.Phys.(London) G27, 1851 (2001) V.I.Kukulin, I.T.Obukhovsky, V.N.Pomerantsev, A.Faessler New Mechanism for Intermediate- and Short-Range Nucleon-Nucleon Interaction
doi: 10.1088/0954-3899/27/9/301
2001KU23 Yad.Fiz. 64, No 9, 1748 (2001); Phys.Atomic Nuclei 64, 1667 (2001) V.I.Kukulin, I.T.Obukhovsky, V.N.Pomerantsev, A.Faessler Arguments Against One-Boson-Exchange Models of Nuclear Forces and New Mechanism for Intermediate- and Short-Range Nucleon-Nucleon Interaction NUCLEAR REACTIONS 1H(p, X), E=0-1200 MeV; calculated partial waves, phase shifts. Symmetric six-quark bag.
doi: 10.1134/1.1409508
2001RU13 Yad.Fiz. 64, No 9, 1769 (2001); Phys.Atomic Nuclei 64, 1689 (2001) New Approach to Solving the Problem of Composite-Particle Scattering on Nuclei
doi: 10.1134/1.1409509
2001RU15 Yad.Fiz. 64, No 10, 1882 (2001); Phys.Atomic Nuclei 64, 1799 (2001) Green's Function and Scattering Matrix in a Discrete Oscillator Basis
doi: 10.1134/1.1414928
2001VO02 Phys.Rev. E 63, 026413 (2001) V.T.Voronchev, V.I.Kukulin, Y.Nakao Use of γ-Ray-Generating Nuclear Reactions for Temperature Diagnostics of DT Fusion Plasma NUCLEAR REACTIONS 6Li(t, d), (t, p), (d, p), (d, n); 2H(d, γ), E=0-1000 keV; calculated σ, reaction rates, monoenergetic γ yields.
doi: 10.1103/PhysRevE.63.026413
2000CO22 Nucl.Phys. A677, 187 (2000) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, V.N.Pomerantsev An Inversion Procedure for Coupled-Channel Scattering: Determining the deuteron-nucleus tensor interaction NUCLEAR REACTIONS 58Ni(d, d'), E=56 MeV; 4He(d, d'), E=8-13 MeV; 56Fe(d, d'), E=30 MeV; calculated scattering potential. 4He(d, d'), E=10 MeV; calculated σ(θ), analyzing powers. S-matrix to potential inversion procedure, coupled channels approach.
doi: 10.1016/S0375-9474(00)00309-2
2000VO08 J.Phys.(London) G26, L103 (2000) Rate Parameters of 6Li(d, pα)T and 6Li(d, nα)3He Nuclear Reactions at Thermonuclear Temperatures NUCLEAR REACTIONS 6Li(d, pα), (d, nα);E=0-300 keV; calculated penetrabilities, σ and reaction rates. Astrophysical interest discussed.
doi: 10.1088/0954-3899/26/6/105
2000VO22 J.Phys.(London) G26, L123 (2000) Cross Sections of 6Li(t, d1)7Li*[0.478] and 6Li(t, p1)8Li*[0.981] Nuclear Reactions in the 0-2 MeV Energy Range NUCLEAR REACTIONS 6Li(t, d), (t, p), E=0-2 MeV; calculated σ for first excited state production. Importance of these reactions in plasma research discussed. Comparison with previous calculations.
doi: 10.1088/0954-3899/26/12/101
2000VO24 Yad.Fiz. 63, No 12, 2147 (2000); Phys.Atomic Nuclei 63, 2051 (2000) Nuclear-Physics Aspects of Controlled Thermonuclear Fusion: Analysis of promising fuels and gamma-ray diagnostics of hot plasma
doi: 10.1134/1.1333874
1999CO11 Phys.Rev. C59, 2361 (1999) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, V.N.Pomerantsev Spin 1 Inversion: A Majorana tensor force for deuteron alpha scattering NUCLEAR REACTIONS 4He(polarized d, d'), E ≈ 10 MeV; analyzed σ(θ), tensor analyzing powers; deduced tensor interaction. S-matrix to potential inversion.
doi: 10.1103/PhysRevC.59.2361
1999KU12 Phys.Rev. C59, 3021 (1999) V.I.Kukulin, V.N.Pomerantsev, A.Faessler Generalized Orthogonality-Condition Model for the NN Interaction
doi: 10.1103/PhysRevC.59.3021
1999KU21 Yad.Fiz. 62, No 7, 1187 (1999); Phys.Atomic Nuclei 62, 1114 (1999) V.I.Kukulin, V.N.Pomerantsev, S.G.Cooper, R.S.Mackintosh Majorana Tensor FOrce for Deuteron-Nucleus Interactions NUCLEAR REACTIONS 4He(d, d), E not given; analyzed data; deduced parity-dependent tensor component in internucleus interaction. Coupled-channel inversion technique.
1999MA02 Nucl.Phys. A645, 399 (1999) R.S.Mackintosh, S.G.Cooper, V.I.Kukulin Determination of 6Li-4He Interaction from Multi-Energy Scattering Data NUCLEAR REACTIONS 4He(polarized 6Li, 6Li), E=19.6, 27.7, 37.5 MeV; analyzed σ(θ), vector analyzing power vs theta; deduced interaction potential. Energy dependent components, Majorana terms.
doi: 10.1016/S0375-9474(98)00623-X
1998CO17 Phys.Rev. C58, R31 (1998) S.G.Cooper, V.I.Kukulin, R.S.Mackintosh, E.V.Kuznetsova New Technique for Phase Shift Analysis: Multienergy Solution of Inverse Scattering Problem NUCLEAR REACTIONS 4He(polarized d, d), E=3-12 MeV; analyzed σ(θ), iT11(θ); deduced phase shifts. Direct inversion from multienergy data to potentials.
doi: 10.1103/PhysRevC.58.R31
1998KU03 Phys.Rev. C57, 535 (1998) V.I.Kukulin, V.N.Pomerantsev, A.Faessler, A.J.Buchmann, E.M.Tursunov Moscow-Type NN Potentials and Three-Nucleon Bound States NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, Coulomb displacement energies, charge radii. Moscow potentials. Comparison with experiment.
doi: 10.1103/PhysRevC.57.535
1998KU10 Nucl.Phys. A631, 456c (1998) New Version of Moscow NN Model
doi: 10.1016/S0375-9474(98)00047-5
1998KU12 Phys.Rev. C57, 2462 (1998) V.I.Kukulin, V.N.Pomerantsev, S.G.Cooper, S.B.Dubovichenko Improved d + 4He Potentials by Inversion: The tensor force and validity of the double folding model NUCLEAR REACTIONS 4He(d, X), E not given; calculated interaction potentials; deduced double folding model validity.
doi: 10.1103/PhysRevC.57.2462
1997KU14 Yad.Fiz. 60, No 4, 608 (1997); Phys.Atomic Nuclei 60, 528 (1997) Reconstruction of the Analytic S Matrix from Experimental Data and Energy-Dependent Phase-Shift Analysis for d4He Scattering NUCLEAR REACTIONS 4He(d, d), E ≤ 10 MeV; analyzed phase shift data. 6Li deduced T=0 resonance Γ. Energy-dependent analysis, analytic S-matrix from data.
1997KU17 Yad.Fiz. 60, No 7, 1228 (1997); Phys.Atomic Nuclei 60, 1103 (1997) Solving a Realistic Inverse Scattering Problem for d4He Scattering and Some General Properties of the Interaction of Composite Particles NUCLEAR REACTIONS 4He(d, d), E ≤ 43 MeV; analyzed phase shift vs E. Realistic solution of inverse problem.
1996KU14 Yad.Fiz. 59, No 3, 428 (1996); Phys.Atomic Nuclei 59, 403 (1996) V.I.Kukulin, V.N.Pomerantsev, S.V.Zuev Rapidly Convergent Method for Reconstructing Complex Interaction Potentials from Phase Shifts and Scattering Cross Sections NUCLEAR REACTIONS 9Be(p, p), (polarized p, p), E=30.3-100 MeV; analyzed σ(θ), vector analyzing power vs θ. 4He(d, d), E ≤ 16 MeV; analyzed phase shifts vs E. Rapidly convergent method for constructing complex potentials.
1996KU16 Yad.Fiz. 59, No 5, 795 (1996); Phys.Atomic Nuclei 59, 757 (1996) V.I.Kukulin, V.N.Pomerantsev, E.M.Tursunov New Class of Nonlocal Models for Describing Interactions of Composite Particles and Testing of These Models in the Three-Body Problem NUCLEAR STRUCTURE 3H; calculated charge form factor. New nonlocal model.
1995KU08 Nucl.Phys. A586, 151 (1995) V.I.Kukulin, V.N.Pomerantsev, Kh.D.Razikov, V.T.Voronchev, G.G.Ryzhikh Detailed Study of the Cluster Structure of Light Nuclei in a Three-Body Model (IV). Large Space Calculation for A = 6 Nuclei with Realistic Nuclear Forces NUCLEAR STRUCTURE 6Li; calculated charge, mass rms radii, quadrupole moment, levels, Γγ. 6Be, 6He; calculated levels, mass rms radii. Three-body α+2N model. NUCLEAR REACTIONS 6Li(e, e), (e, e'), E not given; calculated longitudinal form factors. Three-body α+2N model.
doi: 10.1016/0375-9474(94)00494-8
1994TU05 Yad.Fiz. 57, No 12, 2155 (1994); Phys.Atomic Nuclei 57, 2075 (1994) E.M.Tursunov, Kh.D.Razikov, V.I.Kukulin, V.T.Voronchev, V.N.Pomerantsev High-Accuracy Variational Method for Few-Body Calculations: Application to 3N System NUCLEAR STRUCTURE 3H; calculated binding energy, rms radius, S-, D-, P-state probabilities. New variational technique, high accuracy.
1994VO21 Yad.Fiz. 57, No 11, 1964 (1994); Phys.Atomic Nuclei 57, 1890 (1994) V.T.Voronchev, V.I.Kukulin, V.N.Pomerantsev, Kh.D.Razikov, G.G.Ryzhikh Analysis of the Structure and Properties of Nuclei with A = 9 (9Be-9Be) in the Dynamic Multicluster 2α + N Model NUCLEAR STRUCTURE 9B; calculated levels. 9Be; calculated levels, μ, quadrupole moment, charge, magnetic form factors, clustering probabilities. Dynamic multi-cluster 2α+N model.
1994ZH28 Yad.Fiz. 57, No 11, 2013 (1994); Phys.Atomic Nuclei 57, 1937 (1994) M.A.Zhusupov, E.T.Ibraeva, V.I.Kukulin, V.V.Peresypkin Elastic and Inelastic Scattering of Protons and Antiprotons by the 6Li Nucleus at Intermediate Energies NUCLEAR REACTIONS 6Li(p, p), (p-bar, p-bar), (p, p'), (p-bar, p-bar'), E=0.185-1.04 GeV; calculated σ(θ). Glauber-Sitenko diffraction theory, α+n+p model for target wave functions.
1993BL09 Phys.Rev. C48, 2390 (1993) L.D.Blokhintsev, V.I.Kukulin, A.A.Sakharuk, D.A.Savin, E.V.Kuznetsova Determination of the 6Li → α + d Vertex Constant (Asymptotic Coefficient) from the 4He + d Phase-Shift Analysis NUCLEAR STRUCTURE 6Li; analyzed reaction data; deduced nuclear vertex constant for α+d channel.
doi: 10.1103/PhysRevC.48.2390
1993KU21 Bull.Rus.Acad.Sci.Phys. 57, 921 (1993) V.I.Kukulin, V.T.Voronchev, Kh.D.Razikov, V.N.Pomerantsev Spectra of 9Be and 9B Nuclei in Three-Particle Multicluster Model NUCLEAR STRUCTURE 9Be; calculated levels. Dynamic 2α+nucleon model α(nucleon)-, (αα)-scattering phase shifts fits input.
1993KU27 Bull.Rus.Acad.Sci.Phys. 57, 1696 (1993) V.I.Kukulin, G.G.Ryzhikh, Yu.M.Chuvilsky, R.A.Eramzhyan Prohibition and Suppression of Multicluster States by Pauli Principle in the Dynamical Approach NUCLEAR STRUCTURE 6Li; calculated reduced transition probability, rms charge radius, quadrupole moment. Multi-cluster dynamical model. NUCLEAR REACTIONS 6Li(e, e), E not given; calculated transverse form factor. Multi-cluster dynamical model. RADIOACTIVITY 6He(β-); calculated β-decay ft. Multi-cluster dynamical model.
1993RY01 Nucl.Phys. A563, 247 (1993) G.G.Ryzhikh, R.A.Eramzhyan, V.I.Kukulin, Yu.M.Tchuvilsky Properties of a Six-Nucleon System in a Multicluster Dynamic Model with Antisymmetrization NUCLEAR STRUCTURE 6Li; calculated levels, Γ. Multi-cluster dynamic model, Pauli projection. RADIOACTIVITY 6He(β-); calculated β-decay matrix element. Multi-cluster dynamic model, Pauli projection. NUCLEAR REACTIONS 6Li(e, e), (e, e'), E not given; calculated longitudinal, transverse form factors. Multi-cluster dynamic model, Pauli projection.
doi: 10.1016/0375-9474(93)90604-V
1992GL01 Phys.Rev. C45, R17 (1992) L.Ya.Glozman, V.I.Kukulin, V.N.Pomerantsev Deep Attractive NN Potential as a Potential for the N(1440)-N System NUCLEAR STRUCTURE 2H; calculated N(1440)-N component momentum distribution. Deep attractive NN-potential.
doi: 10.1103/PhysRevC.45.R17
1992KA06 J.Phys.(London) G18, 379 (1992) M.Kamal, V.T.Voronchev, V.I.Kukulin, V.M.Krasnopolsky, Y.Nakao, K.Kudo Self-Consistent Calculation of the Interactions of Lightest Nuclei with 6Li NUCLEAR REACTIONS 6Li(n, n), E=12 MeV; 6Li(p, p), E=22 MeV; 6Li(3He, 3He), E=18 MeV; calculated σ(θ); deduced model parameters. Multi-cluster dynamic model.
doi: 10.1088/0954-3899/18/2/018
1992NE03 Phys.Rev. C45, 1512 (1992) V.G.Neudatchin, V.I.Kukulin, V.N.Pomerantsev, A.A.Sakharuk Generalized Potential-Model Description of Mutual Scattering of the Lightest p + d, d + 3He Nuclei and the Corresponding Photonuclear Reactions NUCLEAR REACTIONS 2H(p, p), E=10.83-13.28 MeV; calculated σ(θ). 3He(d, d), E=8.64-13.84 MeV; calculated σ(θ). 3He(d, γ), E not given; calculated σ(θ). Generalized potential model.
doi: 10.1103/PhysRevC.45.1512
1991BL04 Yad.Fiz. 53, 693 (1991); Sov.J.Nucl.Phys. 53, 433 (1991) L.D.Blokhintsev, V.I.Kukulin, D.A.Savin, A.A.Sakharuk Manifestation of Pauli-Forbidden States in Low-Energy d 4He Scattering NUCLEAR REACTIONS 4He(d, d), E < 12 MeV; calculated phase shift vs E; deduced Pauli-forbidden states role, nucleon-α interaction dependence.
1991KR02 Phys.Rev. C43, 822 (1991) V.M.Krasnopolsky, V.I.Kukulin, E.V.Kuznetsova, J.Horacek, N.M.Queen Energy-Dependent Phase-Shift Analysis of 2H + 4He Scattering in the Energy Range 0.87 < E(d) < 5.24 MeV NUCLEAR REACTIONS 4He(polarized d, d), E=0.87-5.24 MeV; analyzed phase shifts, σ(θ), analyzing power vs θ. Statistical Pade approximation, analytic S-matrix.
doi: 10.1103/PhysRevC.43.822
1991KU27 Izv.Akad.Nauk SSSR, Ser.Fiz. 55, 81 (1991); Bull.Acad.Sci.USSR, Phys.Ser. 55, No.1, 76 (1991) V.I.Kukulin, V.N.Pomerantsev, D.A.Savin, A.A.Sakharuk Recovering the α + d Potential from Faddeev and Measured Phase Shifts NUCLEAR REACTIONS 4He(d, d), E ≤ 20 MeV; calculated phase shifts. Effective linearized method for inverse treatment.
1991NE01 Phys.Lett. 255B, 482 (1991) V.G.Neudatchin, V.I.Kukulin, V.N.Pomerantsev, A.A.Sakharuk The Generalized Potential-Model Description of p + d and d + 3He Scattering NUCLEAR REACTIONS 2H(p, p), E=11.4, 15 MeV; 3He(d, d), E=10, 13.8 MeV; calculated σ(θ). Generalized potential model.
doi: 10.1016/0370-2693(91)90253-M
1990BL13 Yad.Fiz. 51, 1289 (1990); Sov.J.Nucl.Phys. 51, 819 (1990) L.D.Blokhintsev, V.I.Kukulin, D.A.Savin Analysis of Higher Partial Waves of Elastic D + 4He Scattering within the Framework of the Three-Body Problem NUCLEAR REACTIONS 4He(d, d), E ≤ 16 MeV; calculated phase shift, inelasticity coefficients vs E. Faddeev formalism.
1990KU06 Yad.Fiz. 51, 376 (1990); Sov.J.Nucl.Phys. 51, 240 (1990) Effective Linearized Method of Reconstruction of the Interaction Potential on the Basis of Scattering Data NUCLEAR REACTIONS 4He(d, d), E ≤ 5 MeV; calculated phase shifts; deduced model parameters. Effective linearized method to get interaction potential.
1990KU12 Nucl.Phys. A517, 221 (1990) V.I.Kukulin, V.T.Voronchev, T.D.Kaipov, R.A.Eramzhyan Detailed Study of the Cluster Structure of Light Nuclei in a Three-Body Model (III). Electromagnetic structure of 6Li NUCLEAR STRUCTURE 6Li; calculated form factor, transitions, radiative widths. Multi-cluster dynamic model, Pauli projection.
doi: 10.1016/0375-9474(90)90033-I
1990KU14 Yad.Fiz. 52, 402 (1990); Sov.J.Nucl.Phys. 52, 258 (1990) V.I.Kukulin, V.G.Neudachin, V.I.Pomerantsev, A.A.Sakharuk Generalized Potential Description of Scattering of the Lightest Cluster by One Another for the Example of the d + p and d + h Systems NUCLEAR REACTIONS 1H(d, d), E(cm)=10.83-13.28 MeV; 3He(d, d), E(cm)=8.64, 13.84 MeV; calculated σ(θ). Generalized potential.
1990KU16 Czech.J.Phys. B40, 945 (1990) V.I.Kukulin, V.M.Krasnopolsky, E.V.Kuznetsova, J.Horacek Pade-Approximant Techniques for Processing Scattering Data. II. Energy-Dependent Phase-Shift Analysis of Low-Energy 4He + 2H Scattering NUCLEAR REACTIONS 4He(d, d), E ≈ 8 MeV; calculated phase shifts vs E. Pade-approximant techniques.
doi: 10.1007/BF01607284
1989ER07 Phys.Lett. 228B, 1 (1989) R.A.Eramzhyan, G.G.Ryzhikh, V.I.Kukulin, Yu.M.Tchuvilsky Exchange and Correlation Effects in the Electromagnetic Structure of Light Nuclei NUCLEAR STRUCTURE 6Li; calculated transverse, longitudinal form factors. Multi-cluster dynamic model, microscopic version.
doi: 10.1016/0370-2693(89)90514-5
1989KR08 Czech.J.Phys. B39, 593 (1989) V.M.Krasnopolsky, V.I.Kukulin, J.Horacek Pade Approximant Technique for Processing Scattering Data I. Theory, Models and Parametrization of the Scattering Data NUCLEAR REACTIONS 4He(polarized d, d), E=6.24 MeV; calculated T20(θ). Pade approximant technique.
doi: 10.1007/BF01597902
1989KU18 Yad.Fiz. 50, 27 (1989) Break-Up and Elastic Scattering of a Composite Particle in the Field of a Nucleus in the Three-Body Realistic Problem NUCLEAR REACTIONS 58Ni(d, np), E=80 MeV; calculated breakup S-matrix convergence.
1989KU21 Izv.Akad.Nauk SSSR, Ser.Fiz. 53, 121 (1989); Bull.Acad.Sci.USSR, Phys.Ser. 53, No.1, 118 (1989) V.I.Kukulin, G.G.Ryzhikh, Yu.M.Chuvilsky, R.A.Eramzhyan Correlational and Exchange Effects in the Electromagnetic Form Factors of Light Nuclei within the Framework of the Multicluster Dynamic Model NUCLEAR STRUCTURE 6Li, 4He; calculated electromagnetic form factors. Shell, multi-cluster dynamic models.
1988GL01 Phys.Lett. 200B, 406 (1988) L.Ya.Glozman, N.A.Burkova, E.I.Kuchina, V.I.Kukulin Nucleonic, Mesonic and Quark Degrees of Freedom in the Description of Electromagnetic Processes in the Two-Nucleon System NUCLEAR REACTIONS 2H(e, e'p), E=300-700 MeV; calculated double differential σ. Consistent semi-microscopic model.
doi: 10.1016/0370-2693(88)90143-8
1988KU30 Izv.Akad.Nauk SSSR, Ser.Fiz. 52, 2088 (1988); Bull.Acad.Sci.USSR, Phys.Ser. 52, No.11, 7 (1988) Promising Nuclear Reactions for Controllable Thermonuclear Fusion
1987KR14 Izv.Akad.Nauk SSSR, Ser.Fiz. 51, 898 (1987); Bull.Acad.Sci.USSR, Phys.Ser. 51, No.5, 59 (1987) V.M.Krasnopolsky, V.I.Kukulin, V.N.Pomerantsev Realistic Nucleon-Nucleon Potential taking into Account Quark Degrees of Freedom NUCLEAR STRUCTURE 2H; calculated binding energy, rms radius. Six-quark model.
1986HO07 Phys.Lett. 172B, 1 (1986) J.Horacek, J.Bok, V.M.Krasnopolskij, V.I.Kukulin Determination of the Deuteron Asymptotic D- to S-State Ratio by a Pade-Approximant Technique NUCLEAR STRUCTURE 2H; calculated D- to S-state asymptotic wave function ratio. Pole Extrapolation method.
doi: 10.1016/0370-2693(86)90205-4
1986KU07 Yad.Fiz. 43, 559 (1986) V.I.Kukulin, V.M.Krasnopolsky, V.N.Pomerantsev, P.B.Sazonov Realistic NN Potential without Repulsive Core NUCLEAR STRUCTURE 2H; calculated rms radius, quadrupole moment, form factor, D- to S-state mixing asymptotic constants.
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