NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = H.Kamada Found 200 matches. Showing 1 to 100. [Next]2024KO03 Phys.Rev. C 109, 024003 (2024) Contributions of 2π exchange, 1π exchange, and contact three-body forces in NNLO chiral effective field theory to 3ΛH
doi: 10.1103/PhysRevC.109.024003
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
2023KA18 Phys.Rev. C 108, 024004 (2023) Faddeev calculation of 3ΛH incorporating the 2π-exchange ΛNN interaction NUCLEAR STRUCTURE 3H; calculated binding energies for Λ hypernuclei, hypertriton separation energies with and without 2π-exchange ΛNN 3-baryon force. Faddeev calculations of hypertriton performed, incorporating 2π-exchange ΛNN three-baryon force.
doi: 10.1103/PhysRevC.108.024004
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
2022KO27 Phys.Rev. C 106, 054004 (2022) Partial-wave expansion of ΛNN three-baryon interactions in chiral effective field theory NUCLEAR STRUCTURE 2H; calculated s- and d-wave functions in momentum space, folding potential of ΛNN hypernuclei. Partial-wave decomposition of three-body forces concerning the relevant Jacobi momenta, which allows to systematically treat the higher-rank spin and angular-momentum tensor-product structure.
doi: 10.1103/PhysRevC.106.054004
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
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
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
2020KE02 Nucl.Phys. A996, 121698 (2020) N.G.Kelkar, D.Bedoya Fierro, H.Kamada, M.Skurzok Study of the N* momentum distribution for experimental η-mesic 3He searches
doi: 10.1016/j.nuclphysa.2020.121698
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
2019KE07 Int.J.Mod.Phys. E28, 1950066 (2019) N.G.Kelkar, H.Kamada, M.Skurzok N-N-N* model calculations for experimental η-mesic 3He searches NUCLEAR STRUCTURE 3He; calculated momentum distributions, N*NN bound states parameters.
doi: 10.1142/S0218301319500666
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
2018MI04 Phys.Rev. C 97, 055209 (2018) K.Miyagawa, J.Haidenbauer, H.Kamada Faddeev approach to the reaction K- d → πΖn at pK = 1 GeV /c NUCLEAR REACTIONS 2H(K-, nπ-Σ+), (K-, nπ+Σ-), (K-, pπ-Σ0), (K-, nπ0Σ0), E at 1 GeV/c; calculated double differential σ(E, θ) by Faddeev-type approach using TW1, VE-dep, and ORB potentials with and without three-step processes. Comparison with preliminary data from E31 experiment performed at J-PARC facility.
doi: 10.1103/PhysRevC.97.055209
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
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
2017KA38 Few-Body Systems 58, 70 (2017) H.Kamada, O.Shebeko, A.Arslanaliev Triton Binding Energy of Kharkov Potential NUCLEAR STRUCTURE 3H; calculated binding energy, Q using relativistic and non-relativistic Faddeev equation with Kharkov potential. Compared with other calculations.
doi: 10.1007/s00601-017-1241-2
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
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
2016KA14 Few-Body Systems 57, 255 (2016) H.Kamada, J.Furuya, M.Yamaguchi, S.Oryu Neutron Pairing Correlations in an α-n-n Three-Cluster Model of the 6He Nucleus NUCLEAR STRUCTURE 6He; calculated form factors, binding and resonance energies, J, π, angle density matrix. Comparison with available data.
doi: 10.1007/s00601-016-1050-z
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
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
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
2014KA44 Few-Body Systems 55, 935 (2014) H.Kamada, J.Furuya, M.Yamaguchi, E.Uzu Core-Excitation Three-Cluster Model of Borromean Nuclei NUCLEAR STRUCTURE 6,7,8,9,10He, 9,10,11Li; calculated energy levels, J, π, reduced wave functions. Faddeev three-cluster equations.
doi: 10.1007/s00601-013-0799-6
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
2013KA34 Phys.Rev. C 88, 014005 (2013) Core-excitation three-cluster model description of 8He and 10He NUCLEAR STRUCTURE 6He, 8,10He; calculated low-lying levels, J, π, width by solving Faddeev equations of 6He-n-n and 8He-n-n systems in a new three-cluster model. Comparison with experimental data.
doi: 10.1103/PhysRevC.88.014005
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
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
2011KU07 Few-Body Systems 50, 287 (2011) S.Kuroita, K.Sagara, Y.Eguchi, K.Yashima, T.Shishido, T.Yabe, M.Dozono, Y.Yamada, T.Wakasa, T.Noro, H.Matsubara, J.Zenihiro, A.Tamii, H.Okamura, K.Hatanaka, T.Saito, Y.Maeda, H.Kamada, Y.Tameshige Discrepancy of Cross Sections in pd Breakup Reactions at Ep = 250 MeV NUCLEAR REACTIONS 2H(p, 2p), (p, p), E=247 MeV; measured outgoing proton spectra; deduced σ(E, θ). Comparison with 3N calculations, other experimental data.
doi: 10.1007/s00601-011-0219-8
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
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
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
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
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
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
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
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
2007KA42 Nucl.Phys. A790, 398c (2007) H.Kamada, S.Fujii, E.Uzu, M.Yamaguchi, R.Okamoto, Y.Koike Low-momentum nucleon-nucleon potential and its separability NUCLEAR STRUCTURE 3H; calculated binding energy; analyzed dependence on cutoff parameter. Low-momentum effective potential.
doi: 10.1016/j.nuclphysa.2007.03.070
2007KO72 Phys.Rev. C 76, 064002 (2007) M.Kohno, R.Okamoto, H.Kamada, Y.Fujiwara Equivalent hyperon-nucleon interactions in low-momentum space
doi: 10.1103/PhysRevC.76.064002
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
2007MA61 Nucl.Phys. A790, 430c (2007) Y.Maeda, H.Sakai, K.Fujita, M.Hatano, J.Kamiya, T.Kawabata, H.Kuboki, K.Hatanaka, H.Okamura, T.Saito, Y.Sakemi, M.Sasano, K.Sekiguchi, Y.Shimizu, K.Suda, Y.Tameshige, A.Tamii, T.Wakasa, K.Yako, M.B.Greenfield, H.Kamada, H.Witala Measurements of the (n(pol)d) scattering at 250 MeV and three-nucleon forces NUCLEAR REACTIONS 2H(polarized n, n), E=250 MeV; measured σ(θ), vector analyzing powers. Comparison with Faddeev calculations using 3N forces and other data.
doi: 10.1016/j.nuclphysa.2007.03.138
2007SA39 Nucl.Phys. A790, 348c (2007) K.Sagara, M.Tomiyama, S.Shimomoto, T.Ishida, T.Kudoh, S.Kuroita, T.Morikawa, M.Shiota, H.Ohira, H.Kamada, H.Witala Discrepancy in pd breakup reaction at Ep=13 MeV NUCLEAR REACTIONS 2H(p, p), (p, 2p), E=13 MeV; measured Ep, pp-coin, σ(θ); calculated σ(θ). Watson-Migdal-Faddeev model.
doi: 10.1016/j.nuclphysa.2007.03.145
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
2007TA23 Nucl.Phys. A790, 446c (2007) Y.Tameshige, K.Sagara, T.Kudoh, M.Shiota, S.Shimomoto, T.Wakasa, K.Hatanaka, A.Tamii, Y.Sakemi, Y.Shimizu, H.P.Yoshida, H.Kamada, H.Witala Tensor analyzing powers of pd radiative capture at E d(pol) = 137 MeV NUCLEAR REACTIONS 1H(polarized d, γ), E=137 MeV; measured tensor analyzing powers. Comparison with meson exchange current calculations and other data.
doi: 10.1016/j.nuclphysa.2007.03.175
2007UZ02 Nucl.Phys. A790, 286c (2007) E.Uzu, M.Yamaguchi, H.Kamada, Y.Koike Faddeev calculation for neutron-rich nuclei NUCLEAR STRUCTURE 6,8,10He; calculated levels, J, π. Three-body Faddeev equations.
doi: 10.1016/j.nuclphysa.2007.03.046
2007WA10 Phys.Lett. B 645, 402 (2007) T.Wakasa, Y.Hagihara, T.Noro, T.Ishida, S.Asaji, Y.Nagasue, K.Hatanaka, Y.Sakemi, A.Tamii, Y.Shimizu, K.Fujita, Y.Tameshige, H.Sakai, H.Kuboki, M.Sasano, M.Ichimura, H.Kamada, M.Yamaguchi Isovector effective NN interaction in 28Si(p(pol), n(pol))28P(6-) at 198 MeV NUCLEAR REACTIONS 28Si(polarized p, n), E=198 MeV; measured excitation energy spectrum, σ; analysed spin-longitudinal and spin-transverse polarized σ. Distorted-wave impulse approximation.
doi: 10.1016/j.physletb.2006.12.069
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.
2006KA18 Prog.Theor.Phys.(Kyoto) 115, 839 (2006) H.Kamada, S.Fujii, E.Uzu, M.Yamaguchi, R.Okamoto, Y.Koike Separability of a Low-Momentum Effective Nucleon-Nucleon Potential NUCLEAR STRUCTURE 3H; calculated binding energy.
doi: 10.1143/PTP.115.839
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.
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
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
2005OO01 Prog.Theor.Phys.(Kyoto) 113, 809 (2005) H.H.Oo, K.W.Myint, H.Kamada, W.Glockle Does Σ-Σ-α Form a Quasi-Bound State?
doi: 10.1143/PTP.113.809
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
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
2004FU20 Phys.Rev. C 70, 024003 (2004) S.Fujii, E.Epelbaum, H.Kamada, R.Okamoto, K.Suzuki, W.Glockle Low-momentum nucleon-nucleon interaction and its application to few-nucleon systems NUCLEAR STRUCTURE 2H; calculated binding energy, D-state probability. 3H, 4He; calculated binding energies, cutoff parameter dependences.
doi: 10.1103/PhysRevC.70.024003
2004GL05 Eur.Phys.J. A 19, Supplement 1, 159 (2004) W.Glockle, E.Epelbaum, H.Kamada, U.-G.Meissner, A.Nogga, H.Witala Few-nucleon physics based on chiral dynamics NUCLEAR STRUCTURE 3H, 4,6He, 6,8Li, 8Be; calculated binding energies. Several nucleon-nucleon forces compared. NUCLEAR REACTIONS 2H(n, n), E=65, 135 MeV; calculated σ(θ), analyzing powers. Effective field theory approach.
doi: 10.1140/epjad/s2004-03-026-8
2004GL08 Eur.Phys.J. A 21, 335 (2004) W.Glockle, J.Golak, R.Skibinski, H.Witala, H.Kamada, A.Nogga Electron scattering on 3He - A playground to test nuclear dynamics NUCLEAR REACTIONS 3He(e, e), (e, e'), E not given; calculated form factors, response functions. 3He(e, e'p), (e, e'np), E not given; calculated σ(E, θ), spectral functions. Faddeev formalism, two- and three-nucleon forces.
doi: 10.1140/epja/i2004-10001-5
2004GO45 Phys.Rev. C 70, 034005 (2004) J.Golak, H.Witala, R.Skibinski, W.Glockle, A.Nogga, H.Kamada Limitations for the use of the spectral function in the semiexclusive 3He(e, e'N) process NUCLEAR REACTIONS 3He(e, e'p), (e, e'n), E ≈ 0-160 MeV; analyzed spectral functions; deduced limits on validity of approximation. Faddeev calculations.
doi: 10.1103/PhysRevC.70.034005
2004KU12 Few-Body Systems 34, 259 (2004) J.Kuros-Zolnierczuk, P.Thorngren Engblom, H.-O.Meyer, T.J.Whitaker, H.Witala, J.Golak, H.Kamada, A.Nogga, R.Skibinski Faddeev Calculations of Breakup Reactions with Realistic Experimental Constraints NUCLEAR REACTIONS 1H(polarized d, np), E=270 MeV; calculated analyzing powers, spin correlation coefficients. Faddeev framework.
doi: 10.1007/s00601-004-0055-1
2004NO11 Nucl.Phys. A737, 236 (2004) A.Nogga, E.Epelbaum, P.Navratil, W.Glockle, H.Kamada, U.-G.Meissner, H.Witala, B.R.Barrett, J.P.Vary Probing chiral interactions in light nuclei NUCLEAR STRUCTURE 6Li; calculated binding energy, level energies, three-nucleon force effects. Chiral perturbation theory, no-core shell model.
doi: 10.1016/j.nuclphysa.2004.03.082
2004SE07 Phys.Rev. C 70, 014001 (2004) K.Sekiguchi, H.Sakai, H.Witala, K.Ermisch, W.Glockle, J.Golak, M.Hatano, H.Kamada, N.Kalantar-Nayestanaki, H.Kato, Y.Maeda, J.Nishikawa, A.Nogga, T.Ohnishi, H.Okamura, T.Saito, N.Sakamoto, S.Sakoda, Y.Satou, K.Suda, A.Tamii, T.Uchigashima, T.Uesaka, T.Wakasa, K.Yako Polarization transfer measurement for 1H((d(pol), (p(pol))2H elastic scattering at 135 MeV/nucleon and three-nucleon force effects NUCLEAR REACTIONS 1H(polarized d, p), E=135 MeV/nucleon; measured analyzing powers, polarization-transfer coefficients; deduced three-nucleon force effects. Several three-nucleon force models compared.
doi: 10.1103/PhysRevC.70.014001
2003BE39 Phys.Lett. B 564, 199 (2003) J.Bermuth, P.Merle, C.Carasco, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, J.Golak, W.Glockle, M.Hauger, W.Heil, P.Jennewein, J.Jourdan, H.Kamada, A.Klein, M.Kohl, B.Krusche, K.W.Krygier, H.Merkel, U.Muller, R.Neuhausen, A.Nogga, Ch.Normand, E.Otten, Th.Pospischil, M.Potokar, D.Rohe, H.Schmieden, J.Schmiedeskamp, M.Seimetz, I.Sick, S.Sirca, R.Skibinski, G.Testa, Th.Walcher, G.Warren, M.Weis, H.Witala, H.Wohrle, M.Zeier The neutron charge from factor and target analyzing powers from 3He(pol)(e(pol), e'n) scattering NUCLEAR REACTIONS 3He(polarized e, e'n), E=854.5 MeV; measured particle spectra, asymmetries, analyzing power; deduced final state interaction effects. 1n deduced charge form factor. Polarized target.
doi: 10.1016/S0370-2693(03)00725-1
2003CA09 Phys.Lett. B 559, 41 (2003) C.Carasco, J.Bermuth, P.Merle, P.Bartsch, D.Baumann, R.Bohm, D.Bosnar, M.Ding, M.O.Distler, J.Friedrich, J.M.Friedrich, J.Golak, W.Glockle, M.Hauger, W.Heil, P.Jennewein, J.Jourdan, H.Kamada, A.Klein, M.Kohl, K.W.Krygier, H.Merkel, U.Muller, R.Neuhausen, A.Nogga, Ch.Normand, E.Otten, Th.Pospischil, M.Potokar, D.Rohe, H.Schmieden, J.Schmiedeskamp, M.Seimetz, I.Sick, S.Sirca, R.Skibinski, G.Testa, Th.Walcher, G.Warren, M.Weis, H.Witala, H.Wohrle, M.Zeier Final state interaction effects in 3He(pol)(e(pol), e'p) NUCLEAR REACTIONS 3He(polarized e, e'p), E=854.5 MeV; measured Ep, σ(θ), asymmetries; deduced final-state interaction effects. Polarized target, comparison with model predictions.
doi: 10.1016/S0370-2693(03)00306-X
2003EP03 Eur.Phys.J. A 17, 415 (2003) E.Epelbaum, A.Nogga, H.Witala, H.Kamada, W.Glockle, U.-G.Meissner Neutron-deuteron scattering in chiral effective field theory NUCLEAR REACTIONS 2H(n, n), E=65 MeV; calculated tensor analyzing powers, spin transfer coefficients. 2H(p, np), E=65 MeV; calculated σ(θ). Chiral effective field theory, comparison with data and other models.
doi: 10.1140/epja/i2002-10200-0
2003ER04 Phys.Rev. C 68, 051001 (2003) K.Ermisch, H.R.Amir-Ahmadi, A.M.van den Berg, R.Castelijns, B.Davids, E.Epelbaum, E.van Garderen, 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, R.Skibinski, H.Witala, H.J.Wortche Systematic investigation of the elastic proton-deuteron differential cross section at intermediate energies NUCLEAR REACTIONS 2H(p, p), E=108-190 MeV; measured σ(θ); deduced three-nucleon force effects.
doi: 10.1103/PhysRevC.68.051001
2003HI05 Phys.Rev. C 67, 064004 (2003) R.S.Hicks, A.Hotta, S.Churchwell, X.Jiang, G.A.Peterson, J.Shaw, B.Asavapibhop, M.C.Berisso, P.E.Bosted, K.Burchesky, R.A.Miskimen, S.E.Rock, I.Nakagawa, T.Tamae, T.Suda, J.Golak, R.Skibinski, H.Witala, F.Casagrande, W.Turchinetz, A.Cichocki, K.Wang, W.Glockle, H.Kamada, T.Kobayashi, A.Nogga Threshold electrodisintegration of 3He NUCLEAR REACTIONS 3He(e, e'), E=263, 506, 549 MeV; measured σ(E, σ=160°); deduced transverse and longitudinal response functions. Faddeev-type calculations including meson exchange currents and continuum final states with final-state interactions.
doi: 10.1103/PhysRevC.67.064004
2003KA59 Nucl.Phys. A721, 987c (2003) The hypernuclei 4ΛHe and 4ΛH with Modern YN Interactions NUCLEAR STRUCTURE 4H, 4He; calculated hypernucleus levels separation energies. Comparison with data.
doi: 10.1016/S0375-9474(03)01266-1
2003KA73 Mod.Phys.Lett. A 18, 124 (2003) H.Kamada, W.Glockle, J.Golak, Ch.Elster Lorentz boosted NN potential for few-body systems: application to the three-nucleon bound state NUCLEAR STRUCTURE 3H; calculated binding energy, relativistic effects.
doi: 10.1142/S0217732303010089
2003KI21 Phys.Rev. C 68, 054004 (2003) St.Kistryn, A.Micherdzinska, R.Bieber, A.Biegun, K.Bodek, K.Ermisch, W.Glockle, J.Golak, N.Kalantar-Nayestanaki, H.Kamada, M.Kis, A.Kozela, J.Kuros-Zolnierczuk, A.Nogga, M.Mahjour-Shafiei, R.Skibinski, E.Stephan, H.Witala, J.Zejma, W.Zipper Evidence of three-nucleon force effects from 130 MeV deuteron-proton breakup cross section measurement NUCLEAR REACTIONS 1H(polarized d, 2p), (polarized d, d), E=130 MeV; measured particle spectra, σ(θ, φ); deduced three-nucleon force effects. Comparisons with model predictions.
doi: 10.1103/PhysRevC.68.054004
2003MB06 Mod.Phys.Lett. A 18, 298 (2003) Y.Maeda, H.Sakai, A.Tamii, S.Sakoda, H.Kato, M.Hatano, T.Saito, N.Uchigashima, H.Kuboki, K.Hatanaka, D.Hirooka, Y.Shimizu, Y.Kitamura, K.Fujita, N.Sakamoto, H.Okamura, K.Suda, T.Ikeda, K.Itoh, Y.Sakemi, T.Wakasa, J.Kamiya, K.Yako, K.Sekiguchi, Y.Sato, M.B.Greenfield, J.Rapaport, H.Kamada Measurement of differential cross sections and vector analyzing powers for the (n(pol))d reaction at 250 MeV NUCLEAR REACTIONS 2H(polarized n, n), E=245 MeV; measured σ(θ), Ay(θ).
doi: 10.1142/S0217732303010387
2003NO01 Phys.Rev. C 67, 034004 (2003) A.Nogga, A.Kievsky, H.Kamada, W.Glockle, L.E.Marcucci, S.Rosati, M.Viviani Three-nucleon bound states using realistic potential models NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, mass difference, wave functions. Three-nucleon potential, Fadeev and hyperspherical harmonics calculations.
doi: 10.1103/PhysRevC.67.034004
2003SK02 Phys.Rev. C 67, 054001 (2003) R.Skibinski, J.Golak, H.Kamada, H.Witala, W.Glockle, A.Nogga Search for three-nucleon force effects in two-body photodisintegration of 3He(3H) and in the time reversed proton-deuteron radiative capture process NUCLEAR REACTIONS 3H, 3He(γ, d), E ≈ 10-240 MeV; calculated σ, σ(θ); deduced three-nucleon force effects. Fadeev calculations, comparison with data.
doi: 10.1103/PhysRevC.67.054001
2003SK03 Phys.Rev. C 67, 054002 (2003) R.Skibinski, J.Golak, H.Witala, W.Glockle, H.Kamada, A.Nogga Three-nucleon photodisintegration of 3He NUCLEAR REACTIONS 3He(γ, np), (γ, 2p), E=12, 40, 120 MeV; calculated σ, σ(E, θ); deduced three-nucleon force effects. Fadeev calculations, comparison with data.
doi: 10.1103/PhysRevC.67.054002
2003UZ03 Phys.Rev. C 68, 061001 (2003) Complex energy method in four-body Faddeev-Yakubovsky equations
doi: 10.1103/PhysRevC.68.061001
2003WI08 Phys.Rev. C 68, 034002 (2003) H.Witala, A.Nogga, H.Kamada, W.Glockle, J.Golak, R.Skibinski Modern nuclear force predictions for the neutron-deuteron scattering lengths NUCLEAR REACTIONS 2H(n, n), E=low; calculated scattering lengths. Comparison with data. Several two- and three-nucleon force models compared. NUCLEAR STRUCTURE 3H; calculated binding energy. Several two- and three-nucleon force models compared.
doi: 10.1103/PhysRevC.68.034002
2003XU02 Phys.Rev. C 67, 012201 (2003) W.Xu, B.Anderson, L.Auberbach, T.Averett, W.Bertozzi, T.Black, J.Calarco, L.Cardman, G.D.Cates, Z.W.Chai, J.P.Chen, S.Choi, E.Chudakov, S.Churchwell, G.S.Corrado, C.Crawford, D.Dale, A.Deur, P.Djawotho, T.W.Donnelly, D.Dutta, J.M.Finn, H.Gao, R.Gilman, A.V.Glamazdin, C.Glashausser, W.Glockle, J.Golak, J.Gomez, V.G.Gorbenko, J.-O.Hansen, F.W.Hersman, D.W.Higinbotham, R.Holmes, C.R.Howell, E.Hughes, B.Humensky, S.Incerti, C.W.de Jager, J.S.Jensen, X.Jiang, C.E.Jones, M.Jones, R.Kahl, H.Kamada, A.Kievsky, I.Kominis, W.Korsch, K.Kramer, G.Kumbartzki, M.Kuss, E.Lakuriqi, M.Liang, N.Liyanage, J.LeRose, S.Malov, D.J.Margaziotis, J.W.Martin, K.McCormick, R.D.McKeown, K.McIlhany, Z.-E.Meziani, R.Michaels, G.W.Miller, J.Mitchell, S.Nanda, E.Pace, T.Pavlin, G.G.Petratos, R.I.Pomatsalyuk, D.Pripstein, D.Prout, R.D.Ransome, Y.Roblin, M.Rvachev, A.Saha, G.Salme, M.Schnee, T.Shin, K.Slifer, P.A.Souder, S.Strauch, R.Suleiman, M.Sutter, B.Tipton, L.Todor, M.Viviani, B.Vlahovic, J.Watson, C.F.Williamson, H.Witala, B.Wojtsekhowski, F.Xiong, J.Yeh, P.Zolnierczuk Plane-wave impulse approximation extraction of the neutron magnetic form factor from quasielastic 3He(pol)(e(pol), e') at Q2 = 0.3 to 0.6 (GeV/c)2 NUCLEAR REACTIONS 3He(polarized e, e'), E=0.778, 1.727 GeV; measured transverse spin-dependent asymmetry. 1n deduced magnetic form factor. Polarized target.
doi: 10.1103/PhysRevC.67.012201
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