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NSR database version of April 11, 2024.

Search: Author = A.Nogga

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

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

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

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

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

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

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

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

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

doi: 10.1103/PhysRevC.103.054001
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2020EP01      Eur.Phys.J. A 56, 92 (2020)

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

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

doi: 10.1140/epja/s10050-020-00102-2
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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
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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
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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
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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
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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
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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
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2019EP01      Phys.Rev. C 99, 024313 (2019)

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

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

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

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

doi: 10.1103/PhysRevC.99.024313
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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
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2018BI08      Phys.Rev. C 98, 014002 (2018)

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

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

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

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

doi: 10.1103/PhysRevC.98.014002
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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
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2018GO24      Phys.Rev. C 98, 054001 (2018)

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

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

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

doi: 10.1103/PhysRevC.98.054001
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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
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2017GO02      Few-Body Systems 58, 16 (2017)

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

Muon Capture on 3H

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

doi: 10.1007/s00601-016-1162-5
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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
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2017KO32      Phys.Rev. C 96, 035805 (2017)

C.Korber, A.Nogga, J.de Vries

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
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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
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2016BI06      Phys.Rev. C 93, 044002 (2016)

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

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

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

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

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

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

Muon capture on 3H

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

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

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

Testing semilocal chiral two-nucleon interaction in selected electroweak processes

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

doi: 10.1103/PhysRevC.93.064002
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2016WI09      Few-Body Systems 57, 1213 (2016)

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

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

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

doi: 10.1007/s00601-016-1156-3
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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
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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
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2014GO19      Phys.Rev. C 90, 024001 (2014)

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

Break-up channels in muon capture on 3He

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

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

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

Low-energy neutron-deuteron reactions with N3LO chiral forces

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

doi: 10.1140/epja/i2014-14177-7
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2014NO10      Few-Body Systems 55, 757 (2014)

A.Nogga

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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2452.


2014TO12      Few-Body Systems 55, 835 (2014)

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

2N and 3N Systems in a Three Dimensional Formalism

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

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

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

doi: 10.1007/s00601-012-0480-5
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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
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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
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2013NO08      Nucl.Phys. A914, 140c (2013)

A.Nogga

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 hyperon┬Łnucleon and nucleon┬Łnucleon interactions including Λ-Σ conversion.

doi: 10.1016/j.nuclphysa.2013.02.053
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1974.


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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2346.


2011SK04      Eur.Phys.J. A 47, 48 (2011)

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

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

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

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

Triton with long-range chiral N3LO three-nucleon forces

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

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

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

Two-nucleon systems in three dimensions

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

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

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

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

doi: 10.1140/epja/i2009-10903-6
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE2148.


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
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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
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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
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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
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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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22983.


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
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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
Citations: PlumX Metrics

Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1434.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1432.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetK2005.


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
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Data from this article have been entered in the EXFOR database. For more information, access X4 dataset22943.


2006NO02      Phys.Lett. B 634, 210 (2006)

A.Nogga, C.Hanhart

Can one extract the π-neutron scattering length from π-deuteron scattering?

doi: 10.1016/j.physletb.2005.12.071
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetD0553.


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
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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
Citations: PlumX Metrics


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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetO1518.


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
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2005NO09      Nucl.Phys. A754, 36c (2005)

A.Nogga

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
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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
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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
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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1958.


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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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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Data from this article have been entered in the EXFOR database. For more information, access X4 datasetE1907.


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