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NSR database version of April 11, 2024.

Search: Author = K.Topolnicki

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2022GO15      Phys.Rev. C 106, 064003 (2022)

J.Golak, V.Urbanevych, R.Skibinski, H.Witala, K.Topolnicki, V.Baru, A.A.Filin, E.Epelbaum, H.Kamada, A.Nogga

Pion absorption from the lowest atomic orbital in 2H, 3H, and 3He

NUCLEAR REACTIONS 2H(π-, 2n), 3He(π-, nd), (π-, 2np), 3H(π-, 3n), E at rest; calculated single and double differential absorption rates, total absorption rates. Calculations using chiral LO single-nucleon and two-nucleon transition operators with consistent initial and final nuclear states obtained with the chiral nucleon-nucleon SMS potential up to N4LO+ augmented by the consistently regularized chiral N2LO three-nucleon potential. Comparison with previous theoretical predictions and experimental data.

doi: 10.1103/PhysRevC.106.064003
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2021MA32      Phys.Rev. C 103, 054001 (2021)

P.Maris, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, Ulf-G.Meissner, J.A.Melendez, A.Nogga, P.Reinert, R.Roth, R.Skibinski, V.Soloviov, K.Topolnicki, J.P.Vary, Yu.Volkotrub, H.Witala, T.Wolfgruber, for the LENPIC Collaboration

Light nuclei with semilocal momentum-space regularized chiral interactions up to third order

NUCLEAR STRUCTURE 3H, 3,4,6,8He, 6,7,8,9Li, 8,10Be, 10,11,12,13B, 12,13,14C, 14,15N, 16O; calculated energies of ground and excited states, S(2n) for 6He and 6Li, α+d breakup up for 6Li, and 3α breakup for 12C, energies, wave functions and radii for 3H, 3,4He. Semilocal momentum-space (SMS) regularized two- and three-nucleon forces up to third chiral order (N2LO), with the two low-energy constants entering the three-body force determined from the triton binding energy and the differential cross-section minimum in elastic nucleon-deuteron scattering. Comparison with experimental data.

NUCLEAR REACTIONS 1H(polarized d, d), E=70, 140, 200, 270 MeV; 2H(p, d), (polarized p, d), E=65 MeV; calculated analyzing powers Ay(θ) and differential cross sections for elastic scattering using semilocal momentum-space (SMS) regularized two- and three-nucleon forces up to third chiral order (N2LO) three-nucleon force (3NF). Comparison with experimental data.

doi: 10.1103/PhysRevC.103.054001
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2021TO07      Acta Phys.Pol. B52, 391 (2021)

K.Topolnicki

Three Nucleon Scattering Using a "Three-dimensional" Approach-Challenges

doi: 10.5506/aphyspolb.52.391
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2021UR01      Phys.Rev. C 103, 024003 (2021)

V.Urbanevych, R.Skibinski, H.Witala, J.Golak, K.Topolnicki, A.Grassi, E.Epelbaum, H.Krebs

Application of a momentum-space semi-locally regularized chiral potential to selected disintegration processes

NUCLEAR REACTIONS 2H(γ, np), E=30, 100 MeV; 3He(γ, n2p), E=120 MeV; 2H(ν, npν), (ν-bar, npν-bar), (ν-bar, e+2n), E<200 MeV; calculated semi-inclusive and exclusive differential σ(E, θp) and photon and proton analyzing powers in photodisintegration of 2H and 3He, total σ(E) for electron neutrino and anti-neutrino disintegration of 2H using the fifth-order newest semilocal chiral nucleon-nucleon potentials. Comparison with results from Argonne V18 potential and an older chiral force, and with available experimental data.

doi: 10.1103/PhysRevC.103.024003
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2021WI04      Phys.Rev. C 104, 014002 (2021)

H.Witala, J.Golak, R.Skibinski, K.Topolnicki, E.Epelbaum, H.Krebs, P.Reinert

Comprehensive investigation of the symmetric space-star configuration in the nucleon-deuteron breakup

NUCLEAR REACTIONS 2H(n, 2n)1H, E=10.5, 13, 16, 19, 25, 65 MeV; 2H(n, np)1n, E=13, 65 MeV; analyzed available experimental data for double-differential cross sections from Bochum, Erlangen, TUNL, CIAE, Cologne, Fukuoka and PSI facilities for symmetric space star (SST) configurations using three-nucleon (3N) Faddeev equations based on two- and three-nucleon semi-phenomenological and four different chiral NN potentials including the most precise SMS N4LO+; predicted stable SST cross sections with respect to the underlying dynamics for incoming nucleon energies; discussed possible origins of discrepancies between theory and data in low-energy nd and pd SST breakup measurements.

doi: 10.1103/PhysRevC.104.014002
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2020EP01      Eur.Phys.J. A 56, 92 (2020)

E.Epelbaum, J.Golak, K.Hebeler, H.Kamada, H.Krebs, U.-G.Meissner, A.Nogga, P.Reinert, R.Skibinski, K.Topolnicki, Yu.Volkotrub, H.Witala

Towards high-order calculations of three-nucleon scattering in chiral effective field theory

doi: 10.1140/epja/s10050-020-00102-2
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2020VO01      Acta Phys.Pol. B51, 273 (2020)

Y.Volkotrub, J.Golak, R.Skibinski, K.Topolnicki, H.Witala

Correlations among observables in two- and three-nucleon systems

doi: 10.5506/APhysPolB.51.273
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2020WI02      Phys.Rev. C 101, 024003 (2020)

H.Witala, J.Golak, R.Skibinski, K.Topolnicki, V.Urbanevych

Investigation of the interaction of circularly and linearly polarized photon beams with a polarized 3He target

NUCLEAR REACTIONS 3He(polarized γ, p)d, (polarized γ, p)np, (polarized γ, 2p)n, E=15, 30 MeV; calculated σ(E), analyzing powers, spin correlation coefficients for the two-body and the three-body photodisintegration of polarized 3He target using three-nucleon Faddeev equations, and semi-phenomenological AV18 nucleon-nucleon potential combined with the Urbana IX three-nucleon force. Discussed several kinematically complete configurations, symmetric space-star (SST) and final-state interactions (FSI). Relevance to new generation of precise experiments on 3He photodisintegration.

doi: 10.1103/PhysRevC.101.024003
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2020WI04      Phys.Rev. C 101, 054002 (2020)

H.Witala, J.Golak, R.Skibinski, V.Soloviov, K.Topolnicki

Three-nucleon force effects in inclusive spectra of the neutron-deuteron breakup reaction

NUCLEAR REACTIONS 2H(n, n)np, E=14, 70, 135, 200 MeV; calculated differential σ(E, θ), threefold differential σ(E) for the outgoing nucleon in deuteron breakup reaction using three-nucleon Faddeev equation with the CD Bonn nucleon-nucleon potential; deduced magnitudes and the distributions of 3NF effects in incomplete neutron-deuteron breakup. Comparison with experimental data.

doi: 10.1103/PhysRevC.101.054002
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2019EP01      Phys.Rev. C 99, 024313 (2019)

E.Epelbaum, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, P.Maris, Ulf-G.Meissner, A.Nogga, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, K.Vobig, H.Witala, for the LENPIC Collaboration

Few- and many-nucleon systems with semilocal coordinate-space regularized chiral two- and three-body forces

NUCLEAR REACTIONS 2H(n, n), E=14.1, 70, 108, 135, 250 MeV; analyzed differential σ(θ); deduced low energy coefficients; calculated differential σ(θ), neutron analyzing powers Ay(θ), and deuteron vector and tensor analyzing powers using chiral effective field theory with semilocal coordinate-space regularized two- and three-nucleon forces. Comparison with experimental data.

NUCLEAR STRUCTURE 4,6,8He, 6,7,8,9Li, 8,9,10Be, 10,11,12B, 12C, 16O; calculated ground state binding energies, and excitation energies using chiral N2LO interactions.

doi: 10.1103/PhysRevC.99.024313
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2019GO32      Phys.Rev. C 100, 064003 (2019)

J.Golak, R.Skibinski, K.Topolnicki, H.Witala, A.Grassi, H.Kamada, L.E.Marcucci

From response functions to cross sections in neutrino scattering off the deuteron and trinucleons

NUCLEAR REACTIONS 2H(ν-bar, e+)2n, (ν, e-)2p, (ν-bar, ν-bar), (ν, ν), 3H, 3He(ν-bar, e+), (ν-bar, ν-bar), (ν, ν), E<160 MeV; calculated response functions, charged and neutral current differential σ(E, θ, Ω), total σ(E) for electron neutrino scattering using the AV18 nucleon-nucleon potential and a single-nucleon weak current operator.

doi: 10.1103/PhysRevC.100.064003
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2019TO05      Phys.Rev. C 99, 044004 (2019)

K.Topolnicki

3H and 3He calculations without angular momentum decomposition

NUCLEAR STRUCTURE 3H, 3He; calculated scalar functions of bound states, bound state energy, expectation value of the kinetic energy, expectation value of the two-nucleon and three-nucleon-potentials, expectation value of the screened Coulomb potential using three-dimensional formalism. Comparison with predictions from other models.

RADIOACTIVITY 3H(β-); calculated matrix elements of the Fermi current and Gamow-Teller current using three-dimensional formalism.

doi: 10.1103/PhysRevC.99.044004
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2019TO12      Acta Phys.Pol. B50, 371 (2019)

K.Topolnicki, J.Golak, R.Skibinski, H.Witala, Y.Volkotrub

Few-nucleon Systems Without Partial Wave Decomposition

NUCLEAR STRUCTURE 3H, 3He; calculated scalar functions of bound states using three dimensional formalism.

doi: 10.5506/aphyspolb.50.371
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2019VO15      Acta Phys.Pol. B50, 367 (2019)

Y.Volkotrub, R.Skibinski, J.Golak, K.Topolnicki, H.Witala

Theoretical Uncertainties in the Description of the Nucleon-Deuteron Elastic Scattering at E=135 MeV

NUCLEAR REACTIONS 2H(p, p), E=135 MeV; calculated elastic scattering spin correlation coefficient, nucleon to nucleon spin transfer coefficient. Calculations with One-Pion-Exchange (OPE) Gaussian and chiral N4LO potentials.

doi: 10.5506/aphyspolb.50.367
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2018BI08      Phys.Rev. C 98, 014002 (2018)

S.Binder, A.Calci, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, P.Maris, Ulf-G.Meissner, A.Nogga, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, K.Vobig, H.Witala, at the LENPIC Collaboration

Few-nucleon and many-nucleon systems with semilocal coordinate-space regularized chiral nucleon-nucleon forces

NUCLEAR REACTIONS 2H(n, n), E=5, 10, 14.1 MeV; 2H(n, 2np), E=13, 65 MeV; calculated differential σ(θ), Ay analyzing powers, nucleon and deuteron vector analyzing powers, phase shifts, polarization-transfer coefficient, breakup cross sections, and pd analyzing powers.

NUCLEAR STRUCTURE 3H, 3,4He, 6Li; calculated binding energies, ground-state energies of 4He and 6Li, proton rms radii. 3H, 4,6,8He, 6,7,8,9Li, 8,9Be, 10B, 16,24O, 40,48Ca; calculated ground state energies. 3H, 3He, 6,7,8,9Li, 7,9Be, 8,9,10B, 9C; calculated magnetic dipole moments. 16,24O, 40,48Ca; calculated charge radii. Faddeev-Yakubovsky equations, with no-core configuration interaction approach, coupled-cluster (CC) theory, and in-medium similarity renormalization group (IM-SRG)methods with SCS chiral nucleon-nucleon (NN) potentials. Comparison with experimental values, and with other theoretical predictions.

doi: 10.1103/PhysRevC.98.014002
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2018GO16      Phys.Rev. C 98, 015501 (2018)

J.Golak, R.Skibinski, K.Topolnicki, H.Witala, A.Grassi, H.Kamada, L.E.Marcucci

Momentum space treatment of inclusive neutrino scattering off the deuteron and trinucleons

NUCLEAR REACTIONS 3He(ν-bar, 3Heν-bar), (ν, 3Heν), 3H(ν-bar, tν-bar), (ν, tν), E<300 MeV; calculated total σ(E), inclusive response functions response functions for charged current (CC) antineutrino disintegration of 3He, and neutral current (NC) antineutrino disintegration of 3He and 3H using momentum-space approach with AV18 nucleon-nucleon interaction. Comparison with other theoretical predictions.

doi: 10.1103/PhysRevC.98.015501
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2018GO24      Phys.Rev. C 98, 054001 (2018)

J.Golak, R.Skibinski, K.Topolnicki, H.Witala, A.Grassi, H.Kamada, A.Nogga, L.E.Marcucci

Radiative pion capture in 2H, 3He, and 3H

NUCLEAR REACTIONS 2H(π-, 2nγ), E not given; 3He(π-, tγ), (π-, ndγ), (π-, 2npγ), E not given; 3H(π-, 3nγ), E not given; calculated relativistic and non-relativistic kinematically allowed region in the (Eγ, En) plane, and differential capture rate as a function of the photon energy and magnitude of the relative n-n momentum, total radiative pion capture rates using single-nucleon Kroll-Ruderman-type transition operator with the AV18 two-nucleon and Urbana IX three-nucleon potentials. Comparison with previous theoretical predictions, and with experimental data.

doi: 10.1103/PhysRevC.98.054001
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2018SK01      Phys.Rev. C 97, 014002 (2018)

R.Skibinski, J.Golak, K.Topolnicki, H.Witala, Yu.Volkotrub, H.Kamada, A.M.Shirokov, R.Okamoto, K.Suzuki, J.P.Vary

Nucleon-deuteron scattering with the JISP16 potential

NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, n), (n, p), (polarized p, 2p), 1H(polarized d, d), E=5, 13, 65, 135 MeV; calculated differential elastic σ(θ), deuteron vector and tensor analyzing powers iT11, T22, differential cross section for deuteron breakup process. Nucleon-nucleon J-matrix inverse scattering potential JISP16 for elastic nucleon-deuteron scattering and the deuteron breakup process using the formalism of Faddeev equations. Comparison with experimental data, and with theoretical calculations using CD Bonn, Argonne AV18, and the chiral forces.

NUCLEAR STRUCTURE 2H; calculated ground state energies, 3S1 and 3D1 state probabilities for deuteron, potential and kinetic energies for various NN interactions. 3H; calculated binding energy, potential and kinetic energies for various NN interactions.

doi: 10.1103/PhysRevC.97.014002
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2018SK05      Phys.Rev. C 98, 014001 (2018)

R.Skibinski, Yu.Volkotrub, J.Golak, K.Topolnicki, H.Witala

Theoretical uncertainties of the elastic nucleon-deuteron scattering observables

NUCLEAR REACTIONS 2H(n, n), (p, p), E=13, 65, 200 MeV; calculated differential σ(θ), Ay analyzing powers, nucleon to nucleon spin transfer coefficient, deuteron tensor analyzing power, and spin correlation coefficient. One-Pion-Exchange (OPE) Gaussian model Comparison with experimental values.

doi: 10.1103/PhysRevC.98.014001
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2018TE06      Phys.Rev.Lett. 121, 242501 (2018)

S.Terashima, L.Yu, H.J.Ong, I.Tanihata, S.Adachi, N.Aoi, P.Y.Chan, H.Fujioka, M.Fukuda, H.Geissel, G.Gey, J.Golak, E.Haettner, C.Iwamoto, T.Kawabata, H.Kamada, X.Y.Le, H.Sakaguchi, A.Sakaue, C.Scheidenberger, R.Skibinski, B.H.Sun, A.Tamii, T.L.Tang, D.T.Tran, K.Topolnicki, T.F.Wang, Y.N.Watanabe, H.Weick, H.Witala, G.X.Zhang, L.H.Zhu

Dominance of Tensor Correlations in High-Momentum Nucleon Pairs Studied by (p, pd) Reaction

NUCLEAR REACTIONS 16O(p, pd), E=392 MeV; measured reaction products; deduced σ, σ(θ, E), isospin character of p-n pairs at large relative momentum. Comparison with the DWIA calculations.

doi: 10.1103/PhysRevLett.121.242501
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2017GO02      Few-Body Systems 58, 16 (2017)

J.Golak, R.Skibinski, H.Witala, K.Topolnicki, H.Kamada, A.Nogga, L.E.Marcucci

Muon Capture on 3H

NUCLEAR REACTIONS 3H(μ-, X), E slow; calculated capture rate. AV18 nucleon-nucleon potential and the Urbana IX three-nucleon force.

doi: 10.1007/s00601-016-1162-5
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2017TO09      Phys.Rev. C 96, 014611 (2017)

K.Topolnicki, J.Golak, R.Skibinski, H.Witala

Operator form of the three-nucleon scattering amplitude

doi: 10.1103/PhysRevC.96.014611
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2017TO11      Eur.Phys.J. A 53, 181 (2017)

K.Topolnicki

General operator form of the non-local three-nucleon force

doi: 10.1140/epja/i2017-12376-4
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2016BI06      Phys.Rev. C 93, 044002 (2016)

S.Binder, A.Calci, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, H.Kamada, H.Krebs, J.Langhammer, S.Liebig, P.Maris, Ulf-G.Meissner, D.Minossi, A.Nogga, H.Potter, R.Roth, R.Skibinski, K.Topolnicki, J.P.Vary, H.Witala, for the LENPIC Collaboration

Few-nucleon systems with state-of-the-art chiral nucleon-nucleon forces

NUCLEAR STRUCTURE 3H, 4He, 6Li; calculated energies of ground-state and lowest two states, point-proton radius using improved NN chiral potentials LO, NLO, N2LO, N3LO and N4LO. Comparison with experimental data.

NUCLEAR REACTIONS 3H, 4He, 6Li(d, X), (polarized d, d), E=10, 70, 135, 200 MeV; total σ(E), differential cross section and tensor analyzing powers for elastic scattering based on NN chiral potentials LO, NLO, N2LO, N3LO and N4LO. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.044002
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2016GO22      Phys.Rev. C 94, 034002 (2016)

J.Golak, R.Skibinski, H.Witala, K.Topolnicki, H.Kamada, A.Nogga, L.E.Marcucci

Muon capture on 3H

NUCLEAR REACTIONS 3H(μ-, 3nν), E at rest; calculated total and differential rates for muon capture as function of muonic or neutron energy, predictions for three-body breakup of 3H using two- and three-nucleon potentials AV18 and Urbana-IX. Comparison with previous theoretical calculations.

doi: 10.1103/PhysRevC.94.034002
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2016SK02      Phys.Rev. C 93, 064002 (2016)

R.Skibinski, J.Golak, K.Topolnicki, H.Witala, E.Epelbaum, H.Krebs, H.Kamada, Ulf-G.Meissner, A.Nogga

Testing semilocal chiral two-nucleon interaction in selected electroweak processes

NUCLEAR REACTIONS 2H(γ, np), E<80 MeV; calculated total σ(E). 2H(γ, np), E<150 MeV; calculated deuteron analyzing powers. 2H(γ, np), E=30, 100 MeV; calculated differential σ(qp) for LO, NLO, N2LO, N3LO, and N4LO chiral interactions. 2H(γ, np), E=2-4 MeV; calculated photon asymmetry as function of proton center-of-mass scattering angle. 2H(γ, np), E=19.8, 60.8 MeV; calculated photon asymmetry as function of neutron center-of-mass scattering angle. 2H(n, 3H), E=9.0 MeV; 2H(p, 3He), E=17.5, 29, 95 MEV; calculated differential σ(θ), deuteron analyzing power Ay(d). 3He(γ, p), E=40, 120 MeV; calculated differential σ(Ep, θ), three-body 3He photodisintegration rates. 2H(μ-, 2nν); 3He(μ-,3Hν); 3He(μ-, ndν); 3He(μ-, 2npν); calculated differential capture rates for two- and three-nucleon breakup channels, doublet and total capture rates. Single nucleon current (SNC+Siegert), and SNC+meson exchange currents (MEC) models using 3N Lippmann-Schwinger and Faddeev equations, Argonne V18 potential and improved chiral NN forces. Comparison with experimental data.

doi: 10.1103/PhysRevC.93.064002
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2016TO04      Eur.Phys.J. A 52, 22 (2016)

K.Topolnicki, J.Golak, R.Skibinski, H.Witala

Orthogonal polynomial approach to calculate the two-nucleon transition operator in three dimensions

NUCLEAR REACTIONS 1n, 1H(n, n), E=300 MeV; calculated σ(θ) using orthogonal polynomials to calculate two-nucleon transition operator. Compared with other calculations.

doi: 10.1140/epja/i2016-16022-5
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2016TO09      Eur.Phys.J. A 52, 188 (2016)

K.Topolnicki, J.Golak, R.Skibinski, H.Witala

The general operator form for the total-momentum-dependent nucleon-nucleon potential

doi: 10.1140/epja/i2016-16188-8
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2016WI09      Few-Body Systems 57, 1213 (2016)

H.Witala, J.Golak, R.Skibinski, K.Topolnicki, E.Epelbaum, K.Hebeler, H.Kamada, H.Krebs, U.-G.Meissner, A.Nogga

Role of the Total Isospin 3/2 Component in Three-Nucleon Reactions

NUCLEAR REACTIONS 2H(n, n), E=13, 250 MeV; calculated σ(θ), σ(θ, E). Comparison with available data.

doi: 10.1007/s00601-016-1156-3
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2015TO15      Eur.Phys.J. A 51, 132 (2015)

K.Topolnicki, J.Golak, R.Skibinski, H.Witala, C.A.Bertulani

First-order neutron-deuteron scattering in a three-dimensional approach

NUCLEAR REACTIONS 2H(n, 2n), E=25, 190 MeV; calculated energy correlation between the first and the second neutron (coming from deuteron breakup), σ(θ) vs "kinematic S parameter", analyzing power using co-called "3D" formalism.

doi: 10.1140/epja/s2015-15132-x
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2014GO19      Phys.Rev. C 90, 024001 (2014)

J.Golak, R.Skibinski, H.Witala, K.Topolnicki, A.E.Elmeshneb, H.Kamada, A.Nogga, L.E.Marcucci

Break-up channels in muon capture on 3He

NUCLEAR REACTIONS 2H(μ-, ν)2n, 3He(μ-, ν)3H, (μ-, dν)n, (μ-, pν)2n, E not given; calculated total and differential rates for muon capture as function of muonic neutrino energy using two- and three-nucleon potentials AV18 and Urbana-IX. Comparison with experimental data.

doi: 10.1103/PhysRevC.90.024001
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2014GO30      Eur.Phys.J. A 50, 177 (2014)

J.Golak, R.Skibinski, K.Topolnicki, H.Witala, E.Epelbaum, H.Krebs, H.Kamada, Ulf-G.Meissner, V.Bernard, P.Maris, J.Vary, S.Binder, A.Calci, K.Hebeler, J.Langhammer, R.Roth, A.Nogga, S.Liebig, D.Minossi

Low-energy neutron-deuteron reactions with N3LO chiral forces

NUCLEAR REACTIONS 2H(n, n), E=6.5, 10 MeV; calculated analyzing power. 2H(n, x), E=13.0 MeV; calculated σ(θ). Three-nucleon Faddeev equations with different N3LO chiral forces. Compared to data.

doi: 10.1140/epja/i2014-14177-7
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2014TO12      Few-Body Systems 55, 835 (2014)

K.Topolnicki, J.Golak, R.Skibinski, A.E.Elmeshneb, H.Witala, A.Nogga, H.Kamada

2N and 3N Systems in a Three Dimensional Formalism

doi: 10.1007/s00601-013-0793-z
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2013GO08      Few-Body Systems 53, 237 (2013)

J.Golak, R.Skibinski, H.Witala, K.Topolnicki, W.Glockle, A.Nogga, H.Kamada

Different Methods for the Two-Nucleon T-Matrix in the Operator Form

doi: 10.1007/s00601-012-0480-5
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2011SK04      Eur.Phys.J. A 47, 48 (2011)

R.Skibinski, J.Golak, K.Topolnicki, H.Witala, H.Kamada, W.Glockle, A.Nogga

The Tucson-Melbourne three-nucleon force in the automatized partial-wave decomposition

doi: 10.1140/epja/i2011-11048-9
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2011SK08      Phys.Rev. C 84, 054005 (2011)

R.Skibinski, J.Golak, K.Topolnicki, H.Witala, E.Epelbaum, W.Glockle, H.Krebs, A.Nogga, H.Kamada

Triton with long-range chiral N3LO three-nucleon forces

NUCLEAR STRUCTURE 3H; calculated Long-range contributions to the three-nucleon force (3NF) matrix elements, expectation values for 3NF contributions, two-body correlation function. Chiral effective-field theory with N3LO, Faddeev calculations.

doi: 10.1103/PhysRevC.84.054005
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2010GO03      Phys.Rev. C 81, 034006 (2010)

J.Golak, W.Glockle, R.Skibinski, H.Witala, D.Rozpedzik, K.Topolnicki, I.Fachruddin, Ch.Elster, A.Nogga

Two-nucleon systems in three dimensions

NUCLEAR REACTIONS 1n(n, n'), 1n(p, p'), E=13, 150, 300 MeV; calculated σ, σ(θ) and other observables using chiral next-to-next leading order (NNLO) nucleon-nucleon force potential, and Bonn B potential.

doi: 10.1103/PhysRevC.81.034006
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2010GO17      Eur.Phys.J. A 43, 241 (2010)

J.Golak, D.Rozpedzik, R.Skibinski, K.Topolnicki, H.Witala, W.Glockle, A.Nogga, E.Epelbaum, H.Kamada, Ch.Elster, I.Fachruddin

A new way to perform partial-wave decompositions of few-nucleon forces

doi: 10.1140/epja/i2009-10903-6
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