NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = A.Nogga Found 150 matches. Showing 1 to 100. [Next]2024LE01 Eur.Phys.J. A 60, 3 (2024) H.Le, J.Haidenbauer, U.-G.Meissner, A.Nogga Separation energies of light Λ hypernuclei and their theoretical uncertainties NUCLEAR STRUCTURE 4,5He, 3H; calculated separation energies and uncertainties in Λ hypernuclei using few-body method within the Faddeev-Yakubovsky scheme and the no-core shell model. Comparison with available data.
doi: 10.1140/epja/s10050-023-01219-w
2023HA13 Eur.Phys.J. A 59, 63 (2023) J.Haidenbauer, U.-G.Meissner, A.Nogga, H.Le Hyperon-nucleon interaction in chiral effective field theory at next-to-next-to-leading order
doi: 10.1140/epja/s10050-023-00960-6
2023LE03 Phys.Rev. C 107, 024002 (2023) H.Le, J.Haidenbauer, U.-G.Meissner, A.Nogga Ab initio calculation of charge-symmetry breaking in A=7 and 8 Λ hypernuclei NUCLEAR STRUCTURE 4,5H, 5,7He, 7,8Li, 7,8Be; calculated Λ separation energies for the hypernuclei systems, charge-symmetry breaking splittings, contributions to charge-symmetry breaking. Calculations are based on a hyperon-nucleon potential derived from chiral EFT at next-to-leading order. Jacobi no-core shell model. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.024002
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
2021HA46 Few-Body Systems 62, 105 (2021) J.Haidenbauer, U.-G.Meissner, A.Nogga Constraints on the Λ-Neutron Interaction from Charge Symmetry Breaking in the 4ΛHe - 4ΛH Hypernuclei NUCLEAR STRUCTURE 4H, 4He; analyzed available data on separation energies of the mirror hypernuclei; deduced constrain on the Λ-neutron interaction, description of all low energy hyperon-nucleon scattering data, scattering lengths.
doi: 10.1007/s00601-021-01684-3
2021LE14 Eur.Phys.J. A 57, 217 (2021) H.Le, J.Haidenbauer, U.-G.Meissner, A.Nogga S-shell ΛΛ hypernuclei based on chiral interactions NUCLEAR STRUCTURE 5,6He, 4H; calculated hypernuclei ground state wave functions, binding and separation energies using the Jacobi no-core shell model (J-NCSM) to study double-strangeness.
doi: 10.1140/epja/s10050-021-00522-8
2021LE27 Eur.Phys.J. A 57, 339 (2021) H.Le, J.Haidenbauer, U.-G.Meissner, A.Nogga A=4-7 Ξ hypernuclei based on interactions from chiral effective field theory NUCLEAR STRUCTURE A=4-7; analyzed available data. 4NN, 4,5,7H; deduced hypernuclei bound states, separation energies, phase shifts.
doi: 10.1140/epja/s10050-021-00653-y
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
2020GR16 Few-Body Systems 61, 48 (2020) H.W.Griesshammer, J.A.McGovern, A.Nogga, D.R.Phillips Scattering Observables from One- and Two-body Densities: Formalism and Application to γ 3He Scattering
doi: 10.1007/s00601-020-01578-w
2020HA12 Eur.Phys.J. A 56, 91 (2020) J.Haidenbauer, U.-G.Meissner, A.Nogga Hyperon-nucleon interaction within chiral effective field theory revisited
doi: 10.1140/epja/s10050-020-00100-4
2020HA22 Eur.Phys.J. A 56, 195 (2020) J.Haidenbauer, A.Nogga, I.Vidana Predictions for charmed nuclei based on YcN forces inferred from lattice QCD simulations
doi: 10.1140/epja/s10050-020-00185-x
2020LE01 Phys.Lett. B 801, 135189 (2020) H.Le, J.Haidenbauer, U.-G.Meissner, A.Nogga Implications of an increased Λ-separation energy of the hypertriton NUCLEAR STRUCTURE 3H, 4,5He, 7Li; calculated hypernuclei energy spectra, separation and binding energies.
doi: 10.1016/j.physletb.2019.135189
2020LE18 Eur.Phys.J. A 56, 301 (2020) H.Le, J.Haidenbauer, U.-G.Meissner, A.Nogga Jacobi no-core shell model for p-shell hypernuclei NUCLEAR STRUCTURE 4H, 4,5,6He, 6,7Li; calculated hypernuclei ground states, the similarity renormalization group (SRG) to soften the nucleon-nucleon and hyperon-nucleon interactions; deduced basis states and the transition coefficients.
doi: 10.1140/epja/s10050-020-00314-6
2019BU09 Phys.Rev. C 99, 044603 (2019) M.Burrows, Ch.Elster, S.P.Weppner, K.D.Launey, P.Maris, A.Nogga, G.Popa Ab initio folding potentials for nucleon-nucleus scattering based on no-core shell-model one-body densities NUCLEAR REACTIONS 4,6He, 12C, 16O(p, p), (polarized p, p), E=100, 122, 135, 150, 160, 200 MeV; 16O(n, n), E=60-200 MeV; calculated σ(E, θ), Ay(θ, E), and point-proton rms radii using Lippmann-Schwinger equation with folding potential obtained from translationally invariant no-core shell model (NCSM) one-body density and the off-shell Wolfenstein amplitudes, with chiral next-to-next-to-leading order (NNLO) interaction. Comparison with experimental data.
doi: 10.1103/PhysRevC.99.044603
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
2019HL01 Phys.Rev. C 100, 034609 (2019) L.Hlophe, J.Lei, Ch.Elster, A.Nogga, F.M.Nunes, D.Jurciukonis, A.Deltuva Deuteron-α scattering: Separable versus nonseparable Faddeev approach NUCLEAR REACTIONS 4He(d, d), (d, np), E=10, 20, 50 MeV; calculated differential σ(E) for elastic and breakup reactions using the momentum-space Faddeev Alt-Grassberger-Sandhas (AGS) framework.
doi: 10.1103/PhysRevC.100.034609
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
2018BU04 Phys.Rev. C 97, 024325 (2018) M.Burrows, Ch.Elster, G.Popa, K.D.Launey, A.Nogga, P.Maris Ab initio translationally invariant nonlocal one-body densities from no-core shell-model theory NUCLEAR STRUCTURE 4He, 6Li, 12C, 16O; calculated translationally invariant local one-body densities, and K=0 components of the translationally invariant nonlocal one-body density from ab initio no-core shell-model (NCSM) and symmetry-adapted NCSM (SA-NCSM) calculations using the JISP16 nucleon-nucleon interaction; formulation for removing center-of-mass contributions from nonlocal one-body densities.
doi: 10.1103/PhysRevC.97.024325
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
2018LE16 Phys.Rev. C 98, 051001 (2018) J.Lei, L.Hlophe, Ch.Elster, A.Nogga, F.M.Nunes, D.R.Phillips Few-body universality in the deuteron-α system NUCLEAR STRUCTURE 6Li; calculated d-α S-wave scattering length and absolute value of the n-p-α three body separation energy using variety of phase-shift equivalent nucleon-nucleon and α-nucleon interactions; interpreted as a deuteron or two-nucleon halo nucleus from dα and 6Li correlation.
doi: 10.1103/PhysRevC.98.051001
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
2017HL02 Phys.Rev. C 96, 064003 (2017) L.Hlophe, J.Lei, C.Elster, A.Nogga, F.M.Nunes 6Li in a three-body model with realistic Forces: Separable versus nonseparable approach NUCLEAR STRUCTURE 6Li; calculated three-body binding energies for the ground state, momentum distributions of different pairs in the ground state of 6Li, by solving momentum-space Faddeev equations using separable interactions based on the Ernst-Shakin-Thaler (EST) scheme, and with CD-Bonn interaction for the np pair and Bang potential for the n(p)-α subsystems.
doi: 10.1103/PhysRevC.96.064003
2017KO32 Phys.Rev. C 96, 035805 (2017) First-principle calculations of dark matter scattering off light nuclei NUCLEAR STRUCTURE 2,3H, 3He; calculated nuclear wave functions for scattering of dark matter from light particles for scalar interactions and one- and two-nucleon scattering processes in the framework of chiral effective field theory.
doi: 10.1103/PhysRevC.96.035805
2016BE30 Eur.Phys.J. A 52, 296 (2016) J.Behrendt, E.Epelbaum, J.Gegelia, Ulf-G.Meissner, A.Nogga Two-nucleon scattering in a modified Weinberg approach with a symmetry-preserving regularization
doi: 10.1140/epja/i2016-16296-5
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
2016LI23 Eur.Phys.J. A 52, 103 (2016) S.Liebig, U.-G.Meissner, A.Nogga Jacobi no-core shell model for p-shell nuclei NUCLEAR STRUCTURE 3H, 4,6He, 6,7Li; calculated mass excess, gs energy, excitation energy using fully antisymmetrized basis and two- and three-nucleon operators, dependence on the harmonic oscillator frequency. Compared to data.
doi: 10.1140/epja/i2016-16103-5
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
2014GE06 Phys.Rev. C 90, 054323 (2014) A.Gezerlis, I.Tews, E.Epelbaum, M.Freunek, S.Gandolfi, K.Hebeler, A.Nogga, A.Schwenk Local chiral effective field theory interactions and quantum Monte Carlo applications NUCLEAR STRUCTURE 2H; calculated binding energy, quadrupole moment, magnetic moment, asymptotic D/S ratio, rms radius, asymptotic s-wave factor, and the d-state probability using the local chiral potentials. Calculated ground-state energy for a 66-neutron matter system. Local chiral effective field theory interactions to next-to-next-to-leading order and Monte Carlo calculations for neutron matter.
doi: 10.1103/PhysRevC.90.054323
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
2014NO10 Few-Body Systems 55, 757 (2014) Light Hypernuclei Based on Chiral Interactions at Next-to-Leading Order NUCLEAR STRUCTURE 3,4H, 4He; calculated hypernuclei binding and separation energies. Faddeev and Yakubovsky equations in momentum space.
doi: 10.1007/s00601-014-0873-8
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
2013BS01 Eur.Phys.J. A 49, 31 (2013) J.Bsaisou, C.Hanhart, S.Liebig, U.-G.Meissner, A.Nogga, A.Wirzba The electric dipole moment of the deuteron from the QCD Θ-term NUCLEAR STRUCTURE 2H; calculated electric dipole moment using effective field theory with QCD θ-term.
doi: 10.1140/epja/i2013-13031-x
2013GE03 Phys.Rev.Lett. 111, 032501 (2013) A.Gezerlis, I.Tews, E.Epelbaum, S.Gandolfi, K.Hebeler, A.Nogga, A.Schwenk Quantum Monte Carlo Calculations with Chiral Effective Field Theory Interactions
doi: 10.1103/PhysRevLett.111.032501
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
2013HA23 Nucl.Phys. A915, 24 (2013) J.Haidenbauer, S.Petschauer, N.Kaiser, U.-G.Meissner, A.Nogga, W.Weise Hyperon-nucleon interaction at next-to-leading order in chiral effective field theory NUCLEAR REACTIONS 1H(Λ, Λ), E at 100-900 MeV/c;1n(Σ+, Σ0), E at 500-800 MeV/c;1H(Σ-, Λ), E at 100-600 MeV/c;1H(Σ-, Σ0), (Σ-, Σ-), E at 100-600 MeV/c;1H(Σ+, Σ+), (Σ-, Σ-), E at 100-730 MeV/c; calculated σ. 1H(Σ-, Λ), E at 135, 160 MeV/c;1H(Σ-, Σ-), E at 160, 550 MeV/c;1H(Σ+, Σ+), E at 170, 450 MeV/c; calculated σ(θ). 1H(Λ, Λ), E at 0-900 MeV/c;1H, 1n(Σ+, Σ+), E at 0-600 MeV/c; calculated phase shifts for specified partial waves. Next-to-leading order chiral effective field theory, compared with data.
doi: 10.1016/j.nuclphysa.2013.06.008
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
2013NO08 Nucl.Phys. A914, 140c (2013) FLight hypernuclei based on chiral and phenomenological interactions NUCLEAR STRUCTURE 3,4H, 4He; calculated Λ hypernuclei biding energies, mass excess, low-lying levels, J, π, Λ separation energy, scattering length; deduced charge symmetry breaking of Λ separation energy from 4H and 4He Λ hypernuclei using realistic hyperonnucleon and nucleonnucleon interactions including Λ-Σ conversion.
doi: 10.1016/j.nuclphysa.2013.02.053
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
2011BA43 Nucl.Phys. A872, 69 (2011) V.Baru, C.Hanhart, M.Hoferichter, B.Kubis, A.Nogga, D.R.Phillips Precision calculation of threshold π-d scattering, πN scattering lengths, and the GMO sum rule NUCLEAR REACTIONS 2H(π-, π-), (π-, π-'), E≈threshold; calculated matrix elements, πN scattering lengths using chiral perturbation theory including isospin-violating corrections; deduced charged-pion-nucleon coupling constant from discussion of validity of Goldberger-Miyazawa-Oehme sum rule in the presence of isospin violation.
doi: 10.1016/j.nuclphysa.2011.09.015
2011HE06 Phys.Rev. C 83, 031301 (2011) K.Hebeler, S.K.Bogner, R.J.Furnstahl, A.Nogga, A.Schwenk Improved nuclear matter calculations from chiral low-momentum interactions
doi: 10.1103/PhysRevC.83.031301
2011LI20 Eur.Phys.J. A 47, 69 (2011) S.Liebig, V.Baru, F.Ballout, C.Hanhart, A.Nogga Towards a high-precision calculation for the pion-nucleus scattering lengths NUCLEAR STRUCTURE 2H, 3He, 4He; calculated π-2H, π-3He, π-4He scattering length, mass excess.
doi: 10.1140/epja/i2011-11069-4
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
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
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
2009SH09 Nucl.Phys. A819, 98 (2009) D.Shukla, A.Nogga, D.R.Phillips Analyzing the effects of neutron polarizabilities in elastic Compton scattering off 3He NUCLEAR REACTIONS 3He(γ, γ), (polarized γ, γ), E(cm)=60, 80, 100, 120 MeV; calculated σ(θ), double-polarization observables; deduced sensitivity to neutron spin polarizabilities. Heavy-baryon chiral perturbation theory. Polarized target.
doi: 10.1016/j.nuclphysa.2009.01.003
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
2008PA19 Eur.Phys.J. A 36, 315 (2008) M.Pavon Valderrama, A.Nogga, E.Ruiz Arriola, D.R.Phillips Deuteron form factors in chiral effective theory: Regulator-independent results and the role of two-pion exchange NUCLEAR STRUCTURE 2H; calculated wave function, quadrupole moment, form factors, radius using effective field theory with one-pion and chiral two-pion exchange potentials.
doi: 10.1140/epja/i2007-10581-4
2007HA33 Phys.Rev. C 76, 034302 (2007) G.Hagen, T.Papenbrock, D.J.Dean, A.Schwenk, A.Nogga, M.Wloch, P.Piecuch Coupled-cluster theory for three-body Hamiltonians
doi: 10.1103/PhysRevC.76.034302
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
2007NA16 Phys.Rev.Lett. 99, 042501 (2007) P.Navratil, V.G.Gueorguiev, J.P.Vary, W.E.Ormand, A.Nogga Structure of A=10-13 Nuclei with Two- Plus Three-Nucleon Interactions from Chiral Effective Field Theory NUCLEAR STRUCTURE 4He, 6Li, 10,11B, 12,13C; calculated level energies, B(E2), B(M1), B(GT) using effective field theory.
doi: 10.1103/PhysRevLett.99.042501
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
2006NO02 Phys.Lett. B 634, 210 (2006) Can one extract the π-neutron scattering length from π-deuteron scattering?
doi: 10.1016/j.physletb.2005.12.071
2006NO04 Phys.Rev. C 73, 064002 (2006) A.Nogga, P.Navratil, B.R.Barrett, J.P.Vary Spectra and binding energy predictions of chiral interactions for 7Li NUCLEAR STRUCTURE 7Li; calculated ground and excited states energies; deduced sensitivity to chiral interactions, three-nucleon force. No-core shell model approach.
doi: 10.1103/PhysRevC.73.064002
2006NO08 Phys.Lett. B 639, 465 (2006) A.Nogga, A.C.Fonseca, A.Gardestig, C.Hanhart, C.J.Horowitz, G.A.Miller, J.A.Niskanen, U.van Kolck Realistic few-body physics in the dd → απ0 NUCLEAR REACTIONS 2H(d, π0), E=293 MeV; calculated σ, related matrix elements. Effective field theory with four-body theory.
doi: 10.1016/j.physletb.2006.04.058
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).
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
2005BO48 Nucl.Phys. A763, 59 (2005) S.K.Bogner, A.Schwenk, R.J.Furnstahl, A.Nogga Is nuclear matter perturbative with low-momentum interactions?
doi: 10.1016/j.nuclphysa.2005.08.024
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
2005NO09 Nucl.Phys. A754, 36c (2005) Faddeev-Yakubovsky calculations for A=4 hypernuclear systems NUCLEAR STRUCTURE 4H, 4He; calculated hyperon separation energies. Faddeev-Yakubovsky equations, several hyperon-nucleon interactions compared.
doi: 10.1016/j.nuclphysa.2005.01.013
2005NO14 Phys.Rev. C 72, 054006 (2005) A.Nogga, R.G.E.Timmermans, U.van Kolck Renormalization of one-pion exchange and power counting
doi: 10.1103/PhysRevC.72.054006
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
2005VA32 Eur.Phys.J. A 25, Supplement 1, 475 (2005) J.P.Vary, O.V.Atramentov, B.R.Barrett, M.Hasan, A.C.Hayes, R.Lloyd, A.I.Mazur, P.Navratil, A.G.Negoita, A.Nogga, W.E.Ormand, S.Popescu, B.Shehadeh, A.M.Shirokov, J.R.Spence, I.Stetcu, S.Stoica, T.A.Weber, S.A.Zaytsev Ab initio No-Core Shell Model -- Recent results and future prospects NUCLEAR STRUCTURE 4He; calculated radius. 6Li, 16O, 48Ar, 48K, 48Ca, 48Sc, 48Ti, 48V, 48Cr, 48Mn; calculated ground-state energies. 16O, 47Ca; calculated excited states energies. No-core shell model.
doi: 10.1140/epjad/i2005-06-214-x
2004BB09 Nucl.Phys. A746, 579c (2004) B.R.Barrett, P.Navratil, A.Nogga, W.E.Ormand, J.P.Vary No-core shell-model calculations in light nuclei with three-nucleon forces NUCLEAR STRUCTURE 6,7Li, 10B; calculated levels, J, π, three-nucleon force effects. No-core shell model.
doi: 10.1016/j.nuclphysa.2004.09.137
2004FA15 Phys.Rev. C 69, 064002 (2004) I.Fachruddin, W.Glockle, Ch.Elster, A.Nogga Operator form of 3H (3He) and its spin structure NUCLEAR STRUCTURE 3H, 3He; calculated wave functions, nucleon momentum distributions. Operator form.
doi: 10.1103/PhysRevC.69.064002
2004GA22 Phys.Rev. C 69, 044606 (2004) A.Gardestig, C.J.Horowitz, A.Nogga, A.C.Fonseca, C.Hanhart, G.A.Miller, J.A.Niskanen, U.van Kolck Survey of charge symmetry breaking operators for dd → απ0 NUCLEAR REACTIONS 2H(d, π0), E=228.5, 231.8 MeV; calculated pion production total σ, charge symmetry breaking amplitudes; deduced reaction mechanism features. Effective field theory approach.
doi: 10.1103/PhysRevC.69.044606
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
2004NO19 Phys.Rev. C 70, 061002 (2004) A.Nogga, S.K.Bogner, A.Schwenk Low-momentum interaction in few-nucleon systems NUCLEAR STRUCTURE 3H, 3,4He; calculated binding energies, three-nucleon force effects, related features. Low-momentum interactions.
doi: 10.1103/PhysRevC.70.061002
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
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