NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = J.Golak Found 192 matches. Showing 1 to 100. [Next]2023GR02 Phys.Rev. C 107, 024617 (2023) A.Grassi, J.Golak, W.N.Polyzou, R.Skibinski, H.Witala, H.Kamada Electron and neutrino scattering off the deuteron in a relativistic framework NUCLEAR REACTIONS 2H(e, e'p), E=1, 3 GeV; calculated scattered electron energy, angular distribution, structure functions, deuteron tenzor and vector analyzing power. 2H(e, e'p), E=100, 500 MeV; calculated differential σ. 2H(e, e'), E=85 MeV; calculated scattered electron energy, differential σ. 2H(ν, npν), (ν-bar, 2ne+);E<800 MeV; calculated total and differential breakup σ, polarization observables. Relativistic framework with dynamical Poincare generators constructed using a relativistic re-interpretation of the Argonne V18 interaction that is designed to reproduce the experimentally observable deuteron binding energy and nucleon-nucleon scattering observables. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.024617
2022AR07 Physics of Part.and Nuclei 53, 87 (2022) A.Arslanaliev, J.Golak, H.Kamada, A.V.Shebeko, R.Skibinski, M.M.Stepanova, H.Witala The Kharkov Potential in the Theory of 2N and 3N Systems with Solving the Relativistic Faddeev Equations NUCLEAR STRUCTURE 1,2,3H, 1NN; analyzed available data; deduced neutron-proton phase shifts, binding energies. NUCLEAR REACTIONS 2H(p, X), E=135 MeV; calculated σ(θ) for different potentials with and without inclusion of the 3NF. Comparison with experimental data.
doi: 10.1134/S1063779622020149
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
2022MA63 Phys.Rev. C 106, 064002 (2022) P.Maris, R.Roth, E.Epelbaum, R.J.Furnstahl, J.Golak, K.Hebeler, T.Huther, H.Kamada, H.Krebs, H.Le, Ulf-G.Meissner, J.A.Melendez, A.Nogga, P.Reinert, R.Skibinski, J.P.Vary, H.Witala, T.Wolfgruber Nuclear properties with semilocal momentum-space regularized chiral interactions beyond N2LO NUCLEAR STRUCTURE 14,16,18,20,22,24,26O, 40,48Ca; calculated ground-state energies, point-proton radii. 4,6,8He, 6Li, 10Be, 10,12B, 12C; calculated ground state energies. 10,12B, 12C; calculated low-lying levels, J, π. Chiral EFT calculations with semilocal momentum-space regularized NN potentials up to fourth leading order N4LO. NUCLEAR REACTIONS 2H(n, X), E=70, 135, 200 MeV; calculated σ(E), σ(θ), vector- and tensor analyzing power. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.064002
2022MO32 Eur.Phys.J. A 58, 173 (2022) M.Mohammadi-Dadkan, H.R.Amir-Ahmadi, M.T.Bayat, A.Deltuva, M.Eslami-Kalantari, J.Golak, N.Kalantar-Nayestanaki, St.Kistryn, A.Kozela, H.Mardanpour, A.A.Mehmandoost-Khajeh-dad, J.G.Messchendorp, A.Ramazani-Moghaddam-Arani, R.Ramazani-Sharifabadi, R.Skibinski, E.Stephan, H.Tavakoli-Zaniani, H.Witala Analyzing powers at low nucleon-nucleon relative energies in proton-deuteron breakup reaction NUCLEAR REACTIONS 2H(polarized p, 2p)1NN, E=190 MeV; measured reaction products, Ep, Ip; deduced analyzing powers. Comparison with theoretical calculations. AGOR (Accelerateur Groningen-ORsay) cyclotron at KVI.
doi: 10.1140/epja/s10050-022-00804-9
2022VO07 Phys.Rev. C 106, 034002 (2022) Yu.Volkotrub, R.Skibinski, J.Golak, H.Witala Correlations among neutron-proton and neutron-deuteron elastic scattering observables NUCLEAR REACTIONS 1,2H(n, n), E=10, 13, 65, 135 MeV; calculated σ(θ), polarization, asymmetry, correlation plots and coefficients between calculated elastic scattering observables. Ab-initio calculations with OPE-Gaussian force, chiral N4LO SMS and the N4LO+ SMS interactions.
doi: 10.1103/PhysRevC.106.034002
2022WI01 Phys.Rev. C 105, 054004 (2022) H.Witala, J.Golak, R.Skibinski Significance of chiral three-nucleon force contact terms for understanding of elastic nucleon-deuteron scattering NUCLEAR REACTIONS 2H(n, n), E=10, 70, 135, 190, 250 MeV; calculated σ(θ), deuteron tensor and vector analyzing powers, nd scattering length, 3H binding energy. Investigated the influence of the three-nucleon force contact terms by applying the N4LO+ chiral semilocal momentum space (SMS) regularized nucleon-nucleon chiral potential supplemented by N2LO and all subleading N4LO three-nucleon force contact terms. Comparison to experimental data.
doi: 10.1103/PhysRevC.105.054004
2021LA03 Phys.Rev. C 103, 034311 (2021) G.Laskaris, W.Ji, X.Yan, J.Zhou, W.R.Zimmerman, M.W.Ahmed, T.Averett, A.Deltuva, A.C.Fonseca, H.Gao, J.Golak, A.Kafkarkou, H.J.Karwowski, B.Lalremruata, J.Manfredi, J.M.Mueller, P.U.Sauer, R.Skibinski, A.P.Smith, M.B.Tsang, H.R.Weller, H.Witala, Y.K.Wu, Z.W.Zhao First measurement of the asymmetry and the Gerasimov-Drell-Hearn integrand from the 3He((pol)(γ(pol), p)2H reaction at an incident photon energy of 29 MeV NUCLEAR REACTIONS 3He(polarized γ, p)2H, E=29 MeV; measured Ep, Ip, p(θ), time-of-flight, spin-dependent asymmetry and total σ using a circularly polarized, monoenergetic γ-ray beam and a longitudinally polarized 3He target, and an array of depleted silicon surface barrier detectors at the High Intensity γ-ray Source (HIγS) facility at TUNL; deduced contribution from the two-body photo-disintegration to the 3He Gerasimov-Drell-Hearn (GDH) integrands, and compared with the state-of-the art three-nucleon system calculations.
doi: 10.1103/PhysRevC.103.034311
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
2021TA10 Eur.Phys.J. A 57, 58 (2021) H.Tavakoli-Zaniani, M.Eslami-Kalantari, H.R.Amir-Ahmadi, M.T.Bayat, A.Deltuva, J.Golak, N.Kalantar-Nayestanaki, St.Kistryn, A.Kozela, H.Mardanpour, J.G.Messchendorp, M.Mohammadi-Dadkan, A.Ramazani-Moghaddam-Arani, R.Ramazani-Sharifabadi, R.Skibinski, E.Stephan, H.Witala A comprehensive analysis of differential cross sections and analyzing powers in the proton-deuteron breakup channel at 135 MeV NUCLEAR REACTIONS 2H(polarized p, n), E=135 MeV; analyzed available data; deduced σ(θ, E), analyzing powers.
doi: 10.1140/epja/s10050-021-00358-2
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
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
2021WI08 Eur.Phys.J. A 57, 241 (2021) H.Witala, J.Golak, R.Skibinski Efficient emulator for solving three-nucleon continuum Faddeev equations with chiral three-nucleon force comprising any number of contact terms
doi: 10.1140/epja/s10050-021-00555-z
2020BA54 Eur.Phys.J. A 56, 249 (2020) M.T.Bayat, H.Tavakoli-Zaniani, H.R.Amir-Ahmadi, A.Deltuva, M.Eslami-Kalantari, J.Golak, N.Kalantar-Nayestanaki, St.Kistryn, A.Kozela, H.Mardanpour, J.G.Messchendorp, M.Mohammadi-Dadkan, A.Ramazani-Moghaddam-Arani, R.Ramazani-Sharifabadi, R.Skibinski, E.Stephan, H.Witala A comprehensive study of analyzing powers in the proton-deuteron break-up channel at 135 MeV NUCLEAR REACTIONS 2H(polarized p, 2p), E=135 MeV; measured reaction products, Ep, Ip; deduced analyzing power. Comparison with theoretical calculations.
doi: 10.1140/epja/s10050-020-00255-0
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
2020MO13 Eur.Phys.J. A 56, 81 (2020) M.Mohammadi-Dadkan, H.R.Amir-Ahmadi, M.T.Bayat, A.Deltuva, M.Eslami-Kalantari, J.Golak, N.Kalantar-Nayestanaki, St.Kistryn, A.Kozela, H.Mardanpour, A.A.Mehmandoost-Khajeh-dad, J.G.Messchendorp, A.Ramazani-Moghaddam-Arani, R.Ramazani-Sharifabadi, R.Skibinski, E.Stephan, H.Tavakoli-Zaniani, H.Witala Analyzing powers in d(p(pol), pp)n at intermediate and large scattering angles at 190 MeV
doi: 10.1140/epja/s10050-020-00085-0
2020PA43 Phys.Rev. C 102, 054002 (2020) W.Parol, A.Kozela, K.Bodek, A.Deltuva, M.Eslami-Kalantari, J.Golak, N.Kalantar-Nayestanaki, G.Khatri, St.Kistryn, B.Klos, J.Kubos, P.Kulessa, A.Lobejko, A.Magiera, H.Mardanpour, J.G.Messchendorp, I.Mazumdar, R.Skibinski, I.Skwira-Chalot, E.Stephan, A.Ramazani-Moghaddam-Arani, D.Rozpedzik, A.Wilczek, H.Witala, B.Wloch, A.Wronska, J.Zejma Measurement of differential cross sections for the deuteron-proton breakup reaction at 160 MeV NUCLEAR REACTIONS 1H(d, 2p), E=80 MeV/nucleon; measured reaction products and charged particles using Big Instrument for Nuclear-polarization Analysis (BINA) at KVI-Groningen; deduced interpolated σ for deuteron-proton elastic scattering, luminosity integrated over time, differential cross sections for deuteron breakup process for 243 geometrical configurations. Comparison with theoretical calculations modeling nuclear interactions with and without the three-nucleon force (3NF) and the Coulomb interaction.
doi: 10.1103/PhysRevC.102.054002
2020TA04 Eur.Phys.J. A 56, 62 (2020) H.Tavakoli-Zaniani, M.Eslami-Kalantari, H.R.Amir-Ahmadi, M.T.Bayat, A.Deltuva, J.Golak, N.Kalantar-Nayestanaki, St.Kistryn, A.Kozela, H.Mardanpour, J.G.Messchendorp, M.Mohammadi-Dadkan, A.Ramazani-Moghaddam-Arani, R.Ramazani-Sharifabadi, R.Skibinski, E.Stephan, H.Witala Vector-analyzing powers in the d(p(pol), pp)n and d(p(pol), 2He)n channels at 135 MeV
doi: 10.1140/epja/s10050-020-00065-4
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
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
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
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
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
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
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
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
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
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
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
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
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
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
2017SE20 Phys.Rev. C 96, 064001 (2017) K.Sekiguchi, H.Witala, T.Akieda, D.Eto, H.Kon, Y.Wada, A.Watanabe, S.Chebotaryov, M.Dozono, J.Golak, H.Kamada, S.Kawakami, Y.Kubota, Y.Maeda, K.Miki, E.Milman, A.Ohkura, H.Sakai, S.Sakaguchi, N.Sakamoto, M.Sasano, Y.Shindo, R.Skibinski, H.Suzuki, M.Tabata, T.Uesaka, T.Wakasa, K.Yako, T.Yamamoto, Y.Yanagisawa, J.Yasuda Complete set of deuteron analyzing powers from d(pol)p elastic scattering at 190 MeV/nucleon NUCLEAR REACTIONS 1H(polarized d, d), E=186.6 MeV; measured deuteron spectra, deuteron vector and tensor analyzing powers iT11, T20, T21 and T22 as function of angle using BigDpol system at RIBF-RIKEN; analyzed with the previously measured data at E=70, 135 and 190 MeV. All data from 70-294 MeV compared with three-nucleon Faddeev calculations using nucleon-nucleon (NN) potentials alone or combined with three-nucleon force (3NF) models such as the Tucson-Melbourne 99 or Urbana IX, and to locally regularized chiral NN potentials.
doi: 10.1103/PhysRevC.96.064001
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
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
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
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(θdγ), 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
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
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
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
2015HE11 Phys.Rev. C 91, 044001 (2015) K.Hebeler, H.Krebs, E.Epelbaum, J.Golak, R.Skibinski Efficient calculation of chiral three-nucleon forces up to N3LO for ab initio studies NUCLEAR STRUCTURE 3H; calculated matrix elements of chiral three-nucleon forces at next-to-next-to-leading-order and next-to-next-to-next-to-leading-order in large basis spaces, partial-wave contributions to the energy per particle to neutron matter, and contributions of the individual topologies to the triton energy for three different NN interactions. Relevance to ab initio studies of few-nucleon scattering processes, nuclei, and nuclear matter based on higher-order chiral three-nucleon forces.
doi: 10.1103/PhysRevC.91.044001
2015LA22 Phys.Lett. B 750, 547 (2015) G.Laskaris, X.Yan, J.M.Mueller, W.R.Zimmerman, W.Xiong, M.W.Ahmed, T.Averett, P.-H.Chu, A.Deltuva, C.Flower, A.C.Fonseca, H.Gao, J.Golak, J.N.Heideman, H.J.Karwowski, M.Meziane, P.U.Sauer, R.Skibinski, I.I.Strakovsky, H.R.Weller, H.Witala, Y.K.Wu Measurement of the doubly-polarized 3He(pol)(γ(pol), n)pp reaction at 16.5 MeV and its implications for the GDH sum rule NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured reaction products, Eγ, Iγ, En, In; deduced σ(θ, E), σ, contribution from the three-body channel to the Gerasimov-Drell-Hearn (GDH) integrand. Comparison with available data, Monte Carlo simulations using GEANT4.
doi: 10.1016/j.physletb.2015.09.065
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
2014CI06 Few-Body Systems 55, 639 (2014) I.Ciepal, B.Klos, St.Kistryn, E.Stephan, A.Biegun, K.Bodek, A.Deltuva, E.Epelbaum, M.Eslami-Kalantari, A.C.Fonseca, J.Golak, V.Jha, N.Kalantar-Nayestanaki, H.Kamada, G.Khatri, Da.Kirillov, Di.Kirillov, St.Kliczewski, A.Kozela, M.Kravcikova, H.Machner, A.Magiera, G.Martinska, J.Messchendorp, A.Nogga, W.Parol, A.Ramazani-Moghaddam-Arani, B.J.Roy, H.Sakai, K.Sekiguchi, I.Sitnik, R.Siudak, R.Skibinski, R.Sworst, J.Urban, H.Witala, J.Zejma Investigation of the Three-Nucleon System Dynamics in the Deuteron-Proton Breakup Reaction NUCLEAR REACTIONS 1H(d, 2p), E=100, 130 MeV; measured reaction products, Ep, Ip; deduced σ, σ(θ). Comparison with available data.
doi: 10.1007/s00601-014-0841-3
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
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
2014LA04 Phys.Rev. C 89, 024002 (2014) G.Laskaris, Q.Ye, B.Lalremruata, Q.J.Ye, M.W.Ahmed, T.Averett, A.Deltuva, D.Dutta, A.C.Fonseca, H.Gao, J.Golak, M.Huang, H.J.Karwowski, J.M.Mueller, L.S.Myers, C.Peng, B.A.Perdue, X.Qian, P.U.Sauer, R.Skibinski, S.Stave, J.R.Tompkins, H.R.Weller, H.Witala, Y.K.Wu, Y.Zhang, W.Zheng Spin-dependent cross sections from the three-body photodisintegration of 3He at incident energies of 12.8 and 14.7 MeV NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured time-of-flight spectra, γ spectra, and neutron spectra from three-body breakup of 3He using 16 liquid scintillator detectors, spin-dependent double-differential σ(E, θ) at HiγS-TUNL facility. Monoenergetic circularly polarized γ beam, and longitudinally polarized 3He target. Comparison with previous experimental results, and with theoretical calculations.
doi: 10.1103/PhysRevC.89.024002
2014SE13 Phys.Rev. C 89, 064007 (2014) K.Sekiguchi, Y.Wada, J.Miyazaki, H.Witala, M.Dozono, U.Gebauer, J.Golak, H.Kamada, S.Kawase, Y.Kubota, C.S.Lee, Y.Maeda, T.Mashiko, K.Miki, A.Nogga, H.Okamura, T.Saito, H.Sakai, S.Sakaguchi, N.Sakamoto, M.Sasano, Y.Shimizu, R.Skibinski, H.Suzuki, T.Taguchi, K.Takahashi, T.L.Tang, T.Uesaka, T.Wakasa, K.Yako Complete set of deuteron analyzing powers for dp elastic scattering at 250-294 MeV/nucleon and the three-nucleon force NUCLEAR REACTIONS 1H(polarized d, d), E=250, 294 MeV/nucleon; measured scattered particle spectra, σ(θ, E), deuteron analyzing powers iT11(θ, E), T20(θ, E), T21(θ, E), T22(θ, E) using vector and tensor polarized deuteron beam, BigDpol system at RIBF-RIKEN facility. Comparison with three-nucleon Faddeev calculations based on modern nucleon-nucleon (NN) potentials.
doi: 10.1103/PhysRevC.89.064007
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
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
2013KL01 Acta Phys.Pol. B44, 345 (2013) B.Klos, I.Ciepal, St.Kistryn, E.Stephan, A.Biegun, K.Bodek, A.Deltuva, E.Epelbaum, M.Eslami-Kalantari, A.C.Fonseca, J.Golak, B.Jamroz, V.Jha, N.Kalantar-Nayestanaki, H.Kamada, G.Khatri, Da.Kirillov, Di.Kirillov, St.Kliczewski, A.Kozela, M.Kravcikova, H.Machner, A.Magiera, G.Martinska, J.Messchendorp, A.Nogga, W.Parol, A.Ramazani-Moghaddam-Arani, B.J.Roy, H.Sakai, K.Sekiguchi, I.Sitnik, R.Siudak, R.Skibinski, R.Sworst, J.Urban, H.Witala, A.Wronska, J.Zejma Systematic Studies of the Three-nucleon System Dynamics in the Deuteron-Proton Breakup Reaction NUCLEAR REACTIONS 1H(pol d, 2p), E=100, 130, 160 MeV; analyzed available data; deduced 3N system dynamics, 3NF effects.
doi: 10.5506/APhysPolB.44.345
2013LA14 Phys.Rev.Lett. 110, 202501 (2013) G.Laskaris, Q.Ye, B.Lalremruata, Q.J.Ye, M.W.Ahmed, T.Averett, A.Deltuva, D.Dutta, A.C.Fonseca, H.Gao, J.Golak, M.Huang, H.J.Karwowski, J.M.Mueller, L.S.Myers, C.Peng, B.A.Perdue, X.Qian, P.U.Sauer, R.Skibinski, S.Stave, J.R.Tompkins, H.R.Weller, H.Witala, Y.K.Wu, Y.Zhang, W.Zheng First Measurements of Spin-Dependent Double-Differential Cross Sections and the Gerasimov-Drell-Hearn Integrand from 3He(pol) (γ(pol), n)pp at Incident Photon Energies of 12.8 and 14.7 MeV NUCLEAR REACTIONS 3He(polarized γ, n), E=12.8, 14.7 MeV; measured reaction products, En, In; deduced σ, σ(θ, E) and their uncertainties, contributions from the three-body photodisintegration to the 3He Gerasimov-Drell-Hearn integrand. Comparison with available data.
doi: 10.1103/PhysRevLett.110.202501
2013ST06 Eur.Phys.J. A 49, 36 (2013) E.Stephan, St.Kistryn, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, M.Eslami-Kalantari, A.C.Fonseca, I.Gasparic, J.Golak, L.Joulaeizadeh, N.Kalantar-Nayestanaki, H.Kamada, B.Klos, A.Kozela, J.G.Messchendorp, H.Moeini, A.Nogga, W.Parol, A.Ramazani-Moghaddam-Arani, R.Skibinski, R.Sworst, A.Wilczek, H.Witala, J.Zejma Vector analyzing powers of the deuteron-proton elastic scattering and breakup at 100 MeV NUCLEAR REACTIONS 1H(polarized d, d), (polarized d, pn), E=100 MeV; measured charged reaction products using BINA (Big Instrument for Nuclear Polarization Analysis) with vector and tensor polarized incident deuterons; deduced asymmetry, analyzing power; calculated asymmetry, analyzing power using charge-dependent Bonn potential alone and with TM99 three-nucleon force and coupled channels.
doi: 10.1140/epja/i2013-13036-5
2012CI01 Phys.Rev. C 85, 017001 (2012) I.Ciepal, St.Kistryn, E.Stephan, A.Biegun, K.Bodek, A.Deltuva, E.Epelbaum, M.Eslami-Kalantari, A.Fonseca, J.Golak, V.Jha, N.Kalantar-Nayestanaki, H.Kamada, G.Khatri, Da.Kirillov, Di.Kirillov, M.Kis, St.Kliczewski, B.Klos, A.Kozela, M.Kravcikova, M.Lesiak, H.Machner, A.Magiera, G.Martinska, J.Messchendorp, A.Nogga, W.Parol, A.Ramazani-Moghaddam-Arani, B.J.Roy, H.Sakai, K.Sekiguchi, I.Sitnik, R.Siudak, R.Skibinski, R.Sworst, J.Urban, H.Witala, A.Wronska, J.Zejma Vector analyzing powers of deuteron-proton elastic scattering and breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, d), (polarized d, 2p), E=130 MeV; measured Ep, Ip, Ed, Id, pp-coin, vector analyzing powers of the elastic reaction iT11 and breakup process; deduced effects of three nucleon force and Coulomb interaction. COSY accelerator and GwWall detector at Julich. Comparison with theoretical predictions from realistic NN potential, NN potential combined with a three-nucleon force model, and ChPT framework.
doi: 10.1103/PhysRevC.85.017001
2012PH01 Prog.Theor.Phys.(Kyoto) 127, 1033 (2012) A.M.Phyu, H.Kamada, J.Golak, H.H.Oo, H.Witala, W.Glockle The Complex Energy Method Applied to the Nd Scattering with a Model Three-Body Force NUCLEAR REACTIONS 2H(n, n), E=14.1 MeV; calculated σ(θ), doublet scattering length. Comparison with available data.
doi: 10.1143/PTP.127.1033
2011RO19 Phys.Rev. C 83, 064004 (2011) D.Rozpedzik, J.Golak, S.Kolling, E.Epelbaum, R.Skibinski, H.Witala, H.Krebs Signatures of the chiral two-pion exchange electromagnetic currents in the 2H and 3He photodisintegration reactions NUCLEAR REACTIONS 2H(γ, n)p, E=10, 30, 60 MeV; calculated unpolarized differential cross section, total σ(E), photon and proton analyzing powers, deuteron tensor analyzing powers. 3He(γ, p)np, E=20, 20.5, 50 MeV; calculated differential cross sections, analyzing powers for photons, spin correlation coefficients. Long-range two-pion exchange (TPE) contributions in the framework of Chiral effective field theory (ChEFT) using five different parameterization of the next-to-next-to leading order (N2LO) nucleon-nucleon (NN) potential. Comparison with experimental data.
doi: 10.1103/PhysRevC.83.064004
2011SE06 Phys.Rev. C 83, 061001 (2011) K.Sekiguchi, H.Okamura, N.Sakamoto, H.Suzuki, M.Dozono, Y.Maeda, T.Saito, S.Sakaguchi, H.Sakai, M.Sasano, Y.Shimizu, T.Wakasa, K.Yako, H.Witala, W.Glockle, J.Golak, H.Kamada, A.Nogga Three nucleon force effects in intermediate-energy deuteron analyzing powers for dp elastic scattering NUCLEAR REACTIONS 1H(polarized d, d), E=250 MeV/nucleon; measured deuteron and proton spectra, dp-coin, deuteron analyzing powers. 1H(polarized d, d), E=70, 100, 135, 200 MeV/nucleon; analyzed previous analyzing powers data. Comparison with three-nucleon Faddeev calculations based on nucleon-nucleon (NN) potentials alone or combined with two models of three nucleon forces: the Tucson-Melbourne 99 (TM99) and Urbana IX.
doi: 10.1103/PhysRevC.83.061001
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
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
2011TO06 Phys.Lett. B 702, 121 (2011) W.Tornow, H.J.Karwowski, J.H.Kelley, R.Raut, G.Rusev, S.C.Stave, A.P.Tonchev, A.Deltuva, A.C.Fonseca, L.E.Marcucci, M.Viviani, A.Kievsky, J.Golak, R.Skibinski, H.Witala, R.Schiavilla Two-body photodisintegration of 3He between 7 and 16 MeV NUCLEAR REACTIONS 3He(γ, p), E=7-16 MeV; measured reaction products, Ep, Ip; deduced σ. Comparison with theoretical calculations and experimental data.
doi: 10.1016/j.physletb.2011.06.080
2011WI02 Few-Body Systems 49, 61 (2011) H.Witala, J.Golak, R.Skibinski, W.Glockle, W.N.Polyzou, H.Kamada Relativistic Effects in Neutron-Deuteron Elastic Scattering and Breakup NUCLEAR REACTIONS 2H(n, n), E=5, 65, 70, 200, 250 MeV; calculated σ, σ(θ), σ(θ, E). Faddeev equation, AV 18 CD Bonn potentials.
doi: 10.1007/s00601-010-0098-4
2011WI04 Eur.Phys.J. A 47, 30 (2011) H.Witala, R.Skibinski, J.Golak, W.Glockle Momentum space 3N Faddeev calculations of hadronic and electromagnetic reactions with proton-proton Coulomb and three-nucleon forces included
doi: 10.1140/epja/i2011-11030-7
2011WI07 Phys.Rev. C 83, 044001 (2011); Erratum Phys.Rev. C 88, 069904 (2013) H.WitaLa, J.Golak, R.Skibinski, W.Glockle, H.Kamada, W.N.Polyzou Three-nucleon force in relativistic three-nucleon Faddeev calculations NUCLEAR REACTIONS 2H(n, n), E=70, 135, 200, 250 MeV; calculated σ(θ, E), vector (deuteron) and tensor analyzing powers, spin correlation coefficients, neutron analyzing powers, neutron-to-neutron polarization transfer coefficients. 2H(n, np), E=200 MeV; calculated differential cross section for breakup. 1n(d, 2n), E=270 MeV; calculated polarization transfer coefficient and deuteron analyzing powers. Comparison with experimental data. Relativistic three-nucleon Faddeev equations with a three-nucleon force included.
doi: 10.1103/PhysRevC.83.044001
2010GL04 Eur.Phys.J. A 43, 339 (2010) W.Glockle, I.Fachruddin, Ch.Elster, J.Golak, R.Skibinski, H.Witala 3N scattering in a three-dimensional operator formulation
doi: 10.1140/epja/i2010-10920-4
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
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
2010SK01 Acta Phys.Pol. B41, 875 (2010) R.Skibinski, J.Golak, H.Witala Numerical Investigations of the Three-dimensional Proton-Proton Screened Coulomb t-matrix
2010ST08 Phys.Rev. C 82, 014003 (2010) E.Stephan, St.Kistryn, R.Sworst, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, A.C.Fonseca, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, B.Klos, A.Kozela, M.Mahjour-Shafiei, A.Micherdzinska, A.Nogga, R.Skibinski, H.Witala, A.Wronska, J.Zejma, W.Zipper Vector and tensor analyzing powers in deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured proton and deuteron spectra, vector and tensor analyzing powers; deduced asymmetry distributions. Vector- and tensor-polarized deuteron beam. Comparison with coupled-channels calculations and with Chiral perturbed theory.
doi: 10.1103/PhysRevC.82.014003
2009GL01 Phys.Rev. C 79, 044003 (2009) W.Glockle, J.Golak, R.Skibinski, H.Witala Exact three-dimensional wave function and the on-shell t matrix for the sharply cut-off Coulomb potential: Failure of the standard renormalization factor
doi: 10.1103/PhysRevC.79.044003
2009MI18 Phys.Rev.Lett. 103, 152501 (2009) D.G.Middleton, J.R.M.Annand, M.A.Antelo, C.Ayerbe, P.Barneo, D.Baumann, J.Bermuth, J.Bernauer, H.P.Blok, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.Garcia Llongo, D.I.Glazier, J.Golak, W.Glockle, P.Grabmayr, T.Hehl, J.Heim, W.H.A.Hesselink, E.Jans, H.Kamada, G.J.Manas, M.Kohl, L.Lapikas, I.J.D.MacGregor, I.Martin, J.C.McGeorge, H.Merkel, P.Merle, K.Monstad, F.Moschini, U.Muller, A.Nogga, R.Perez-Benito, Th.Pospischil, M.Potokar, G.Rosner, M.Seimetz, R.Skibinski, H.de Vries, Th.Walcher, D.P.Watts, M.Weinriefer, M.Weiss, H.Witala, B.Zihlmann Investigation of the Exclusive 3He(e, e'pn)1H Reaction NUCLEAR REACTIONS 3He(e, e'np), E=220-270 MeV; measured Ee, Ie, Ep, Ip and En, In; deduced σ. Continuum Fadeev calculations.
doi: 10.1103/PhysRevLett.103.152501
2009SE05 Phys.Rev. C 79, 054008 (2009) K.Sekiguchi, H.Sakai, H.Witala, W.Glockle, J.Golak, K.Itoh, H.Kamada, T.Kawabata, H.Kuboki, Y.Maeda, A.Nogga, H.Okamura, S.Sakaguchi, N.Sakamoto, Y.Sasamoto, M.Sasano, R.Skibinski, K.Suda, Y.Takahashi, T.Uesaka, T.Wakasa, K.Yako Three-nucleon force effects in the1H(d(pol), p(pol)p)n reaction at 135 MeV/nucleon NUCLEAR REACTIONS 1H(polarized d, 2p), E=135 MeV/nucleon; measured Ep, Ip, polarization transfer coefficients and vector analyzing powers of outgoing proton. Comparison with calculations using three-nucleon Faddeev equation.
doi: 10.1103/PhysRevC.79.054008
2009SK06 Eur.Phys.J. A 40, 215 (2009) R.Skibinski, J.Golak, H.Witala, W.Glockle Proton-proton scattering without Coulomb force renormalization NUCLEAR REACTIONS 1H(polarized p, p), E=13, 50 MeV; calculated σ(θ), analyzing power and other observables using a screened Coulomb force without renormalization and the Lippmann-Schwinger equation.
doi: 10.1140/epja/i2009-10752-3
2009ST27 Eur.Phys.J. A 42, 13 (2009) E.Stephan, St.Kistryn, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, A.C.Fonseca, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, B.Klos, A.Kozela, M.Mahjour-Shafiei, A.Micherdzinska, A.Nogga, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Precise set of tensor analyzing power T20 data for the deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured proton spectra, charged-particle spectra, proton(charged-particle)-coin for several polarization states; deduced tensor analyzing powers. Comparison with various models.
doi: 10.1140/epja/i2009-10865-7
2009WI08 Nucl.Phys. A827, 222c (2009) H.Witala, J.Golak, R.Skibinski, W.Glockle, H.Kamada, A.Nogga Testing nucleonic forces with three nucleon reactions NUCLEAR REACTIONS 2H(polarized p, p), (polarized n, n), E=250 MeV; analyzed σ(θ), analyzing power using a three-nucleon force model.
doi: 10.1016/j.nuclphysa.2009.05.042
2009WI16 Eur.Phys.J. A 41, 369 (2009) H.Witala, R.Skibinski, J.Golak, W.Glockle A novel treatment of the proton-proton Coulomb force in proton-deuteron Faddeev calculations: Elastic scattering NUCLEAR REACTIONS 2H(p, p), E=13 MeV; calculated σ(θ) using 3-dimensional screened pp Coulomb t-matrix in 3N Faddeev calculations.
doi: 10.1140/epja/i2009-10843-1
2009WI17 Eur.Phys.J. A 41, 385 (2009) H.Witala, R.Skibinski, J.Golak, W.Glockle A novel treatment of the proton-proton Coulomb force in proton-deuteron Faddeev calculations: Breakup NUCLEAR REACTIONS 2H(p, 2p), E=13 MeV; calculated σ(θ) using 3-dimensional screened pp Coulomb t-matrix in 3N Faddeev calculations.
doi: 10.1140/epja/i2009-10842-2
2008KI21 Few-Body Systems 44, 11 (2008) St.Kistryn, E.Stephan, N.Kalantar-Nayestanaki, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, A.C.Fonseca, W.Glockle, J.Golak, H.Kamada, M.Kis, B.Klos, A.Kozela, A.Nogga, M.Mahjour-Shafiei, A.Micherdzinska, P.U.Sauer, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Studies of the three-nucleon system dynamics: Cross sections of the deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured particle spectra, break-up cross sections.
doi: 10.1007/s00601-008-0245-3
2008WI02 Phys.Rev. C 77, 034004 (2008) H.Witala, J.Golak, R.Skibinski, W.Glockle, W.N.Polyzou, H.Kamada Relativity and the low-energy nd Ay puzzle NUCLEAR REACTIONS 2H(n, n), E=5, 8, 8.5, 13, 35, 65 MeV; calculated analyzing power. Faddeev equations in Poincare invariant formalism. Comparison with experimental data.
doi: 10.1103/PhysRevC.77.034004
2007MA46 Phys.Rev. C 76, 014004 (2007) Y.Maeda, H.Sakai, K.Fujita, M.B.Greenfield, K.Hatanaka, M.Hatano, J.Kamiya, T.Kawabata, H.Kuboki, H.Okamura, J.Rapaport, T.Saito, Y.Sakemi, M.Sasano, K.Sekiguchi, Y.Shimizu, K.Suda, Y.Tameshige, A.Tamii, T.Wakasa, K.Yako, J.Blomgren, P.Mermod, A.Ohrn, M.Osterlund, H.Witala, A.Deltuva, A.C.Fonseca, P.U.Sauer, W.Glockle, J.Golak, H.Kamada, A.Nogga, R.Skibinski Differential cross section and analyzing power measurements for (n-pol, d) elastic scattering at 248 MeV NUCLEAR REACTIONS 2H(n, n), E=248 MeV; measured En, σ and vector analyzing power.
doi: 10.1103/PhysRevC.76.014004
2007ST29 Phys.Rev. C 76, 057001 (2007) E.Stephan, St.Kistryn, R.Sworst, A.Biegun, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, A.Fonseca, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, A.Kozela, M.Mahjour-Shafiei, A.Micherdzinska, A.Nogga, P.U.Sauer, R.Skibinski, H.Witala, J.Zejma, W.Zipper Vector and tensor analyzing powers of elastic deuteron-proton scattering at 130 MeV deuteron beam energy NUCLEAR REACTIONS 1H(polarized d, d), E=130 MeV; measured cross sections, angular distributions, vector and tensor analyzing powers.
doi: 10.1103/PhysRevC.76.057001
2006BI03 Acta Phys.Pol. B37, 213 (2006) A.Biegun, E.Stephan, St.Kistryn, K.Bodek, I.Ciepal, A.Deltuva, E.Epelbaum, W.Gloeckle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, B.Klos, A.Kozela, J.Kuros-Zolnierczuk, M.Mahjour-Shafiei, U.-G.Meissner, A.Micherdzinska, A.Nogga, P.U.Sauer, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Three-nucleon force effects in the analyzing powers of the d(pol)p breakup at 130 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=130 MeV; measured analyzing powers; deduced no three-nucleon force effects.
2006LE23 Phys.Rev. C 73, 064001 (2006) J.Ley, C.Duweke, R.Emmerich, A.Imig, H.Paetz gen.Schieck, J.Golak, H.Witala, E.Epelbaum, A.Deltuva, A.C.Fonseca, W.Glockle, U.-G.Meissner, A.Nogga, P.U.Sauer Cross sections and tensor analyzing powers Ayy of the reaction 1H(d(pol), pp)n in "symmetric constant relative energy" geometries at Ed = 19 MeV NUCLEAR REACTIONS 1H(polarized d, 2p), E=19 MeV; measured σ(E, θ), tensor analyzing powers Ayy for four geometries. Comparisons with Faddeev calculations using phenomenological NN potentials with and without three-body forces, effect of Delta and Coulomb interaction, chiral forces.
doi: 10.1103/PhysRevC.73.064001
2006NA10 Phys.Rev. C 73, 034003 (2006) S.Naito, Y.Nagai, T.Shima, H.Makii, K.Mishima, K.Tamura, H.Toyokawa, H.Ohgaki, J.Golak, R.Skibinski, H.Witala, W.Glockle, A.Nogga, H.Kamada New data for total 3He(γ, p)D and 3He(γ, pp)n cross sections compared to current theory NUCLEAR REACTIONS 3He(γ, p), (γ, 2p), E=10.2, 16.0 MeV; measured charged particle spectra, σ. Comparison with model predictions.
doi: 10.1103/PhysRevC.73.034003
2006NA25 Phys.Rev. C 74, 025804 (2006) Y.Nagai, T.Kobayashi, T.Shima, T.Kikuchi, K.Takaoka, M.Igashira, J.Golak, R.Skibinski, H.Witala, A.Nogga, W.Glockle, H.Kamada Measurement of the 2H(n, γ)3H reaction cross section between 10 and 550 keV NUCLEAR REACTIONS 2H(n, γ), E=30.5, 54.2, 531 keV; measured Eγ, Iγ, σ; deduced astrophysical reaction rates. Comparison with model predictions.
doi: 10.1103/PhysRevC.74.025804
2006RO42 Acta Phys.Pol. B37, 2889 (2006) D.Rozpedzik, J.Golak, R.Skibinski, H.Witala, W.Glockle, E.Epelbaum, A.Nogga, H.Kamada A first estimation of chiral four-nucleon force effects in 4He NUCLEAR STRUCTURE 4He; calculated four-nucleon force effects.
2006SK06 Acta Phys.Pol. B37, 2905 (2006) R.Skibinski, J.Golak, H.Witala, W.Glockle, A.Nogga, E.Epelbaum Nucleon-deuteron capture with chiral potentials NUCLEAR REACTIONS 2H(n, γ), E=9, 10.8 MeV; calculated σ(θ). 1H(d, γ), E=17.5, 29, 45, 95 MeV; calculated σ(θ), Ay(θ), Ayy(θ).
2006SK08 Eur.Phys.J. A 30, 369 (2006) R.Skibinski, H.Witala, J.Golak Relativistic effects in exclusive neutron-deuteron breakup NUCLEAR REACTIONS 2H(n, 2n), E=65, 156, 200 MeV; calculated σ(E, θ1, θ2); deduced relativistic effects, related features. Comparison with data.
doi: 10.1140/epja/i2006-10115-8
2006WI05 Phys.Lett. B 634, 374 (2006) H.Witala, J.Golak, R.Skibinski Selectivity of the nucleon-induced deuteron breakup and relativistic effects NUCLEAR REACTIONS 2H(p, 2p), E=65 MeV; 2H(p, pn), E=200 MeV; calculated σ(θ, E). Three-nucleon Faddeev model, comparison with data.
doi: 10.1016/j.physletb.2006.01.070
2006WI09 Phys.Rev. C 73, 044004 (2006) H.Witala, J.Golak, R.Skibinski, W.Glockle, A.Nogga, E.Epelbaum, H.Kamada, A.Kievsky, M.Viviani Testing nuclear forces by polarization transfer coefficients in d(p(pol), p(pol))d and d(p(pol), d(pol))p reactions at Elabp = 22.7 MeV NUCLEAR REACTIONS 2H(polarized p, p), (polarized p, d), E=22.7 MeV; measured spin transfer coefficients. Comparison with model predictions using various potentials.
doi: 10.1103/PhysRevC.73.044004
2006WI16 Eur.Phys.J. A 29, 141 (2006) H.Witala, R.Skibinski, J.Golak, W.Glockle, A.Nogga, H.Kamada The elastic pd scattering analyzing powers and spin correlation coefficients at Elabp = 135 and 200 MeV: Three-nucleon force and relativistic effects NUCLEAR REACTIONS 2H(polarized p, p), E=135, 200 MeV; analyzed vector and tensor analyzing powers, spin correlation coefficients; deduced three-nucleon force and relativistic effects.
doi: 10.1140/epja/i2006-10069-9
2005DU14 Phys.Rev. C 71, 054003 (2005) C.Duweke, R.Emmerich, A.Imig, J.Ley, G.Tenckhoff, H.Paetz gen.Schieck, J.Golak, H.Witala, E.Epelbaum, W.Glockle, A.Nogga The reaction 2H(p, pp)n in three kinematical configurations at Ep= 16 MeV NUCLEAR REACTIONS 2H(p, 2p), E=16 MeV; measured σ(E, θ) for three kinematical configurations. Comparison with model predictions.
doi: 10.1103/PhysRevC.71.054003
2005ER03 Phys.Rev. C 71, 064004 (2005) K.Ermisch, H.R.Amir-Ahmadi, A.M.van den Berg, R.Castelijns, B.Davids, A.Deltuva, E.Epelbaum, W.Glockle, J.Golak, M.N.Harakeh, M.Hunyadi, M.A.de Huu, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, M.Mahjour-Shafiei, A.Nogga, P.U.Sauer, R.Skibinski, H.Witala, H.J.Wortche Systematic investigation of three-nucleon force effects in elastic scattering of polarized protons from deuterons at intermediate energies NUCLEAR REACTIONS 2H(polarized p, p), E=108, 120, 135, 150, 170, 190 MeV; measured σ(θ) and vector analyzing power; deduced three-nucleon forces contribution and necessity of inclusion. Comparisons with model predictions.
doi: 10.1103/PhysRevC.71.064004
2005GO26 Phys.Rep. 415, 89 (2005) J.Golak, R.Skibinski, H.Witala, W.Glockle, A.Nogga, H.Kamada Electron and photon scattering on three-nucleon bound states
doi: 10.1016/j.physrep.2005.04.005
2005GO38 Phys.Rev. C 72, 054005 (2005) J.Golak, R.Skibinski, H.Witala, W.Glockle, A.Nogga, H.Kamada Proton polarizations in polarized 3He studied with the 3He(pol)(e(pol), e'p)d and 3He(pol)(e(pol), e'p)pn processes NUCLEAR REACTIONS 3He(polarized e, e'p), (polarized e, e'np), E=735 MeV; calculated polarization observables, related features. Faddeev framework, polarized target.
doi: 10.1103/PhysRevC.72.054005
2005KI19 Phys.Rev. C 72, 044006 (2005) St.Kistryn, E.Stephan, A.Biegun, K.Bodek, A.Deltuva, E.Epelbaum, K.Ermisch, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, B.Klos, A.Kozela, J.Kuros-Zolnierczuk, M.Mahjour-Shafiei, U.-G.Meissner, A.Micherdzinska, A.Nogga, P.U.Sauer, R.Skibinski, R.Sworst, H.Witala, J.Zejma, W.Zipper Systematic study of three-nucleon force effects in the cross section of the deuteron-proton breakup at 130 MeV NUCLEAR REACTIONS 2H(p, 2p), E=130 MeV; measured Ep, pp-coin, σ(θ1, θ2); deduced three-nucleon force effects.
doi: 10.1103/PhysRevC.72.044006
2005ME09 Phys.Lett. B 617, 18 (2005) A.A.Mehmandoost-Khajeh-Dad, H.R.Amir-Ahmadi, J.C.S.Bacelar, A.M.van den Berg, R.Castelijns, A.Deltuva, E.D.van Garderen, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, R.Koohi-Fayegh-Dehkordi, H.Lohner, M.Mahjour-Shafiei, H.Mardanpour, J.G.Messchendorp, A.Nogga, P.Sauer, S.V.Shende, R.Skibinski, H.Witala, H.J.Wortche Spin observables in deuteron-proton radiative capture at intermediate energies NUCLEAR REACTIONS 1H(polarized d, γ), E=55, 66.5, 90 MeV/nucleon; measured Eγ, (particle)γ-coin, vector and tensor analyzing powers. Comparison with model predictions.
doi: 10.1016/j.physletb.2005.04.071
2005SE22 Phys.Rev.Lett. 95, 162301 (2005) K.Sekiguchi, H.Sakai, H.Witala, W.Glockle, J.Golak, K.Hatanaka, M.Hatano, K.Itoh, H.Kamada, H.Kuboki, Y.Maeda, A.Nogga, H.Okamura, T.Saito, N.Sakamoto, Y.Sakemi, M.Sasano, Y.Shimizu, K.Suda, A.Tamii, T.Uesaka, T.Wakasa, K.Yako Resolving the Discrepancy of 135 MeV pd Elastic Scattering Cross Section and Relativistic Effects NUCLEAR REACTIONS 2H(p, p), E=135 MeV; 1H(d, d), E=135 MeV/nucleon; measured σ(θ); deduced relativistic effects, three-nucleon force effects. Comparison with previous results.
doi: 10.1103/PhysRevLett.95.162301
2005SK01 Eur.Phys.J. A 24, 31 (2005) R.Skibinski, J.Golak, H.Witala, W.Glockle, A.Nogga Different formulations of 3He and 3H photodisintegration NUCLEAR REACTIONS 1H(d, γ), E=300 MeV; calculated σ(θ), analyzing powers. 3He(γ, 2p), E=100 MeV; calculated σ(E, θ). Different formulations of Fadeev-like equations compared.
doi: 10.1140/epja/i2004-10134-5
2005SK05 Phys.Rev. C 72, 044002 (2005) R.Skibinski, J.Golak, H.Witala, W.Glockle, A.Nogga, H.Kamada Polarization observables in the semiexclusive photoinduced three-body breakup of 3He NUCLEAR REACTIONS 3He(polarized γ, nX), (polarized γ, pX), E=12, 40, 120 MeV; calculated σ(E, θ), Ay(θ), spin correlation coefficients for three-body breakup.
doi: 10.1103/PhysRevC.72.044002
2005WI13 Phys.Rev. C 71, 054001 (2005) H.Witala, J.Golak, W.Glockle, H.Kamada Relativistic effects in neutron-deuteron elastic scattering NUCLEAR REACTIONS 2H(n, n), E=28, 65, 135, 250 MeV; calculated σ(θ), analyzing powers, relativistic effects. Three-nucleon Fadeev equation.
doi: 10.1103/PhysRevC.71.054001
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