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NSR database version of May 24, 2024.

Search: Author = V.N.Pomerantsev

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2024PO02      Phys.Rev. C 109, 014002 (2024)

V.N.Pomerantsev, O.A.Rubtsova, V.A.Kulikov

Union of the discretized spectra for multichannel resonances

doi: 10.1103/PhysRevC.109.014002
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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2017PO01      Phys.Rev. A 95, 022506 (2017)

V.P.Popov, V.N.Pomerantsev

Isotopic effects in scattering and kinetics of the atomic cascade of excited μ-p and μ-d atoms

NUCLEAR REACTIONS 1,2H(μ-, X), E<100 eV; calculated σ. Comparison with available data.

doi: 10.1103/PhysRevA.95.022506
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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
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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
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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
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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
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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
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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
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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
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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
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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
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2009KU20      Phys.Atomic Nuclei 72, 1786 (2009)

V.I.Kukulin, V.N.Pomerantsev

Dibaryon concept for nuclear force and its experimental evidence

doi: 10.1134/S1063778809100226
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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
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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
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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
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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
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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
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2005KO26      Pisma Zh.Eksp.Teor.Fiz. 81, 675 (2005); JETP Lett. 81, 543 (2005)

G.Ya.Korenman, V.N.Pomerantsev, V.P.Popov

Coulomb Deexcitation of Muonic Hydrogen within the Quantum Close-Coupling Method

ATOMIC PHYSICS 1,2H; calculated Coulomb deexcitation σ for muonic atoms.

doi: 10.1134/1.2029940
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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
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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
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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
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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
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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
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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
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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
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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
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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
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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.

1998KO17      Yad.Fiz. 61, No 4, 641 (1998); Phys.Atomic Nuclei 61, 569 (1998)

I.V.Kopytin, A.A.Khuskivadze, V.N.Pomerantsev

Photodisintegration of the 7Li Nucleus and Structure of the αt Potential

NUCLEAR REACTIONS 7Li(γ, t), (polarized γ, t), E < 90 MeV; calculated σ(θ), asymmetry; deduced tα interaction sensitivity. Comparison with data.

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
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1998KU10      Nucl.Phys. A631, 456c (1998)

V.I.Kukulin, V.N.Pomerantsev

New Version of Moscow NN Model

doi: 10.1016/S0375-9474(98)00047-5
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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
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1997KU17      Yad.Fiz. 60, No 7, 1228 (1997); Phys.Atomic Nuclei 60, 1103 (1997)

V.I.Kukulin, V.N.Pomerantsev

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
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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.

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.

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
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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
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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
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1990KU06      Yad.Fiz. 51, 376 (1990); Sov.J.Nucl.Phys. 51, 240 (1990)

V.I.Kukulin, V.N.Pomerantsev

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.

1990NE14      Yad.Fiz. 52, 738 (1990); Sov.J.Nucl. 52, 473 (1990)

V.G.Neudachin, V.N.Pomerantsev, A.A.Sakharuk

Potential Description of the Photonuclear Reactions 3Heγ → dp and 3Hed → 5Liγ

NUCLEAR REACTIONS 3He(γ, p), E=6-24 MeV; 1H(d, γ), E=15.3 MeV; 3He(d, γ), E not given; analyzed σ(θ); deduced cluster scattering role.

1989KU18      Yad.Fiz. 50, 27 (1989)

V.I.Kukulin, V.N.Pomerantsev

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.

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.

1986EM02      Izv.Akad.Nauk SSSR, Ser.Fiz. 50, 902 (1986); Bull.Acad.Sci.USSR, Phys.Ser. 50, No.5, 70 (1986)

V.G.Emelyanov, V.I.Klimov, V.N.Pomerantsev

Calculating the Energy and Width of the 2+-State of a 6He Nucleus

NUCLEAR STRUCTURE 6He; calculated 2+ state energy, width. Nonspin α-n-n model.

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.

1985EM01      Phys.Lett. 157B, 105 (1985)

V.G.Emelyanov, V.I.Klimov, V.N.Pomerantsev

The Calculation of the Three-Body Resonance Energy and Width above the Threshold for the Three-Body Break-Up

NUCLEAR STRUCTURE 6He; calculated 2+ level energy, Γ, three-body resonance characteristics. Orthogonal projection technique.

doi: 10.1016/0370-2693(85)91526-6
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1985KR22      Phys.Lett. 165B, 7 (1985)

V.M.Krasnopolsky, V.I.Kukulin, V.N.Pomerantsev, P.B.Sazonov

The Deuteron Structure and NN-Phase Shifts for Realistic Local Superdeep NN-Potential with an Extra State

NUCLEAR STRUCTURE 2H; calculated μ, rms radius, quadrupole moment, form factors. Realistic local, superdeep, nucleon-nucleon potential.

doi: 10.1016/0370-2693(85)90680-X
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1984KU01      Phys.Lett. 135B, 20 (1984)

V.I.Kukulin, V.N.Pomerantsev, V.M.Krasnopolsky, P.B.Sazonov

The NN-Potential with Forbidden State Suggested from a Six-Quark Model with One-Pion Exchange

NUCLEAR REACTIONS 1H(n, n), E=100, 200, 300 400 MeV; calculated 1S0, 3S1, 3D1 phase shifts vs mixing parameter. Six quark model, one pion exchange based realistic interaction.

NUCLEAR STRUCTURE 2H; calculated wave function, μ, quadrupole moment, rms charge radius. Six quark model, one pion exchange based realistic interaction.

doi: 10.1016/0370-2693(84)90445-3
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1983KU06      Yad.Fiz. 37, 862 (1983)

V.I.Kukulin, V.N.Pomerantsev, V.G.Emelyanov, V.I.Klimov

Theory of Resonance States in Nuclei using the Orthogonal Projection Method

NUCLEAR STRUCTURE 5He; calculated single particle resonances. Orthogonal projection method, generalized Wigner-Brillouin perturbation theory.

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