NSR Query Results
Output year order : Descending NSR database version of April 11, 2024. Search: Author = K.Hebeler Found 52 matches. 2024CO02 Phys.Rev. C 109, 024311 (2024) M.Companys Franzke, A.Tichai, K.Hebeler, A.Schwenk Eigenvector continuation for the pairing Hamiltonian
doi: 10.1103/PhysRevC.109.024311
2023HE04 Phys.Rev. C 107, 024310 (2023) K.Hebeler, V.Durant, J.Hoppe, M.Heinz, A.Schwenk, J.Simonis, A.Tichai Normal ordering of three-nucleon interactions for ab initio calculations of heavy nuclei NUCLEAR STRUCTURE 18O, 48Ca, 78Ni, 132Sn, 208Pb; calculated ground-state energies. 132Sn, 208Pb; calculated charge radii. Jacobi normal-ordering (NO) framework to include three-nucleon (3N) interactions in ab initio many-body calculations up to heavy nuclei at the two-body operator level. Comparison to experimental data.
doi: 10.1103/PhysRevC.107.024310
2023KE02 Phys.Rev.Lett. 130, 072701 (2023) J.Keller, K.Hebeler, A.Schwenk Nuclear Equation of State for Arbitrary Proton Fraction and Temperature Based on Chiral Effective Field Theory and a Gaussian Process Emulator
doi: 10.1103/PhysRevLett.130.072701
2023SE18 Phys.Rev. C 108, 054005 (2023) R.Seutin, O.J.Hernandez, T.Miyagi, S.Bacca, K.Hebeler, S.Konig, A.Schwenk Magnetic dipole operator from chiral effective field theory for many-body expansion methods
doi: 10.1103/PhysRevC.108.054005
2022HO06 Phys.Rev. C 105, 034324 (2022) J.Hoppe, A.Tichai, M.Heinz, K.Hebeler, A.Schwenk Importance truncation for the in-medium similarity renormalization group NUCLEAR STRUCTURE 4He, 40,48,52,60Ca, 56,68,78Ni; calculated ground state energy. Importance truncation (IT) methods in the nonperturbative in-medium similarity renormalization group (IMSRG) approach. Investigated the effect of truncation in different sub-blocks of the two-body Hamiltonian on the solution error.
doi: 10.1103/PhysRevC.105.034324
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
2022MI01 Phys.Rev. C 105, 014302 (2022) T.Miyagi, S.R.Stroberg, P.Navratil, K.Hebeler, J.D.Holt Converged ab initio calculations of heavy nuclei NUCLEAR STRUCTURE 132Sn; calculated ground-state energy, rms point-proton and point-neutron radii, and neutron skin thickness using many-body perturbation theory (MBPT(2)), Hartree-Fock based many-body perturbation theory (HF-MBPT(3)) to second and third order, and in-medium similarity renormalization group (IMSRG(2)). 127Cd; calculated excitation spectrum computed in valence-space (VS)IMSRG(2) approximation. 126,128,130,132,134,136Sn; calculated energies of the first 2+ states using (VS)IMSRG(2) approximation, and compared with experimental data. Ab initio calculations of atomic nuclei with a proposed novel storage scheme for three-nucleon (3N) interaction matrix elements for the normal-ordered two-body (NO2B) approximation. Relevance to neutron skin of 208Pb, neutrinoless double-β decays and dark matter searches in germanium, selenium, xenon and tellurium.
doi: 10.1103/PhysRevC.105.014302
2022MI12 Phys.Rev. C 106, 024001 (2022) S.B.S.Miller, A.Ekstrom, K.Hebeler Neutron-deuteron scattering cross sections with chiral NN interactions using wave-packet continuum discretization NUCLEAR REACTIONS 2H(n, n), E<90 MeV; calculated phase shifts, σ(θ), total σ, neutron analyzing power. Faddeev equations for elastic Nd scattering solved with wavepacket continuum-discretization (WPCD) method. Chiral nucleon-nucleon interactions up to next-to-next-to-leading order. Comparison to experimental data.
doi: 10.1103/PhysRevC.106.024001
2022TI04 Phys.Rev. C 106, 024320 (2022) A.Tichai, P.Arthuis, K.Hebeler, M.Heinz, J.Hoppe, A.Schwenk, L.Zurek Least-square approach for singular value decompositions of scattering problems
doi: 10.1103/PhysRevC.106.024320
2021FR01 Phys.Rev.Lett. 126, 102501 (2021) U.Friman-Gayer, C.Romig, T.Huther, K.Albe, S.Bacca, T.Beck, M.Berger, J.Birkhan, K.Hebeler, O.J.Hernandez, J.Isaak, S.Konig, N.Pietralla, P.C.Ries, J.Rohrer, R.Roth, D.Savran, M.Scheck, A.Schwenk, R.Seutin, V.Werner Role of Chiral Two-Body Currents in 6Li Magnetic Properties in Light of a New Precision Measurement with the Relative Self-Absorption Technique RADIOACTIVITY 6Li(IT) [from 6Li(γ, γ'), E<7.1 MeV]; measured decay products, Eγ, Iγ; deduced B(M1), decay width. Comparison with ab initio calculations based on chiral effective field theory that take into account contributions to the magnetic dipole operator beyond leading order.
doi: 10.1103/PhysRevLett.126.102501
2021HE01 Phys.Rep. 890, 1 (2021) Three-nucleon forces: Implementation and applications to atomic nuclei and dense matter
doi: 10.1016/j.physrep.2020.08.009
2021HE11 Phys.Rev. C 103, 044318 (2021) M.Heinz, A.Tichai, J.Hoppe, K.Hebeler, A.Schwenk In-medium similarity renormalization group with three-body operators NUCLEAR STRUCTURE 4He, 16O; calculated ground-state energies using various truncation schemes. Full and approximate in-medium similarity renormalization group (IMSRG(3)) truncations applied to the closed-shell nuclei using nucleon-nucleon and nucleon-nucleon+3N-chiral Hamiltonians with the Hartree-Fock and natural orbital single-particle bases.
doi: 10.1103/PhysRevC.103.044318
2021HO03 Phys.Rev. C 103, 014321 (2021) J.Hoppe, A.Tichai, M.Heinz, K.Hebeler, A.Schwenk Natural orbitals for many-body expansion methods NUCLEAR STRUCTURE 16,22O, 40Ca, 78Ni; calculated one-body proton density matrix, occupation numbers of the single-particle proton orbitals, and absolute value of the radial wave function for 16O, negative occupations of the p orbitals for 16O and 22O, ground-state energies and charge radii of 16O, 40Ca and 78Ni. Nonperturbative many-body calculations using the in-medium similarity renormalization group (IMSRG) approach, with large single-particle basis. Comparison with experimental data for 78Ni.
doi: 10.1103/PhysRevC.103.014321
2021KE06 Phys.Rev. C 103, 055806 (2021) J.Keller, C.Wellenhofer, K.Hebeler, A.Schwenk Neutron matter at finite temperature based on chiral effective field theory interactions
doi: 10.1103/PhysRevC.103.055806
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
2020DE11 Phys.Rev. C 101, 041302 (2020) P.Demol, T.Duguet, A.Ekstrom, M.Frosini, K.Hebeler, S.Konig, D.Lee, A.Schwenk, V.Soma, A.Tichai Improved many-body expansions from eigenvector continuation NUCLEAR STRUCTURE 3H, 18O; calculated ground state energies using many-body perturbation theory (MBPT)-based eigenvector continuation (EC) resummation method for 3He, and Bogoliubov many-body perturbation theory (BMBPT)-based EC resummation method for 16O, using realistic nuclear two-body interaction derived from chiral effective field theory. Comparison with MBPT, BMBPT, and MBPT-based Pade approximation calculations.
doi: 10.1103/PhysRevC.101.041302
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
2020LE14 Phys.Rev.Lett. 125, 142502 (2020) M.Leonhardt, M.Pospiech, B.Schallmo, J.Braun, C.Drischler, K.Hebeler, A.Schwenk Symmetric Nuclear Matter from the Strong Interaction
doi: 10.1103/PhysRevLett.125.142502
2019DR01 Phys.Rev.Lett. 122, 042501 (2019) C.Drischler, K.Hebeler, A.Schwenk Chiral Interactions up to Next-to-Next-to-Next-to-Leading Order and Nuclear Saturation
doi: 10.1103/PhysRevLett.122.042501
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
2019HO09 Phys.Rev. C 100, 024318 (2019) J.Hoppe, C.Drischler, K.Hebeler, A.Schwenk, J.Simonis Probing chiral interactions up to next-to-next-to-next-to-leading order in medium-mass nuclei NUCLEAR STRUCTURE 3H, 16,24O, 40,48,52,60Ca, 56,68Ni; calculated binding energies, charge radii, and ground-state energies per nucleon. Ab initio calculations using in-medium similarity renormalization group (IM-SRG) based on chiral interactions at next-to-leading order (NLO), N2LO, and N3LO. Comparison with experimental data.
doi: 10.1103/PhysRevC.100.024318
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
2017DR02 Phys.Rev. C 95, 024302 (2017) C.Drischler, T.Kruger, K.Hebeler, A.Schwenk Pairing in neutron matter: New uncertainty estimates and three-body forces
doi: 10.1103/PhysRevC.95.024302
2017HO24 Phys.Rev. C 96, 054002 (2017) J.Hoppe, C.Drischler, R.J.Furnstahl, K.Hebeler, A.Schwenk Weinberg eigenvalues for chiral nucleon-nucleon interactions
doi: 10.1103/PhysRevC.96.054002
2017KL03 Eur.Phys.J. A 53, 168 (2017); Erratum Eur.Phys.J. A 54, 76 (2018) P.Klos, A.Carbone, K.Hebeler, J.Menendez, A.Schwenk Uncertainties in constraining low-energy constants from 3H β decay RADIOACTIVITY 3H(β-); calculated low-energy constants of chiral effective field theory from T1/2; deduced uncertainty.
doi: 10.1140/epja/i2017-12357-7
2017SI17 Phys.Rev. C 96, 014303 (2017) J.Simonis, S.R.Stroberg, K.Hebeler, J.D.Holt, A.Schwenk Saturation with chiral interactions and consequences for finite nuclei NUCLEAR STRUCTURE 40,54Ca, 56,78Ni; calculated ground-state energies and charge radii using the closed-shell IM-SRG, and compared with evaluated experimental data. 4He, 16,22,24O, 36,40,48,52,54,60Ca, 48,56,68,78Ni; calculated binding energies and charge radii using the IM-SRG for the four Hamiltonians, and compared with evaluated data. 19,20,21,22,23,24,25,26,27,28,29,30,31,32Na, 28,29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45S, 40,41,42,43,44,45,46,47,48,49,50,51,52,53,54Ca, 48,49,50,51,52,53,54,55,56,57,58,59,60,61,62,63,64Mn, 53,54,55,56,57,58,59,60,61,62,63,64,65,66,67,68,69,70,71,72Ni; calculated ground-state energies and S(2n), charge radii of Mn isotopes, first excited 2+ states of Ca, S and Ni isotopes using the VS-IM-SRG, and compared with experimental data. Calculations used ab initio in-medium similarity renormalization group (IM-SRG) method, and valence-space (VS) IM-SRG for charge radii.
doi: 10.1103/PhysRevC.96.014303
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
2016DR06 Phys.Rev. C 93, 054314 (2016) C.Drischler, K.Hebeler, A.Schwenk Asymmetric nuclear matter based on chiral two- and three-nucleon interactions
doi: 10.1103/PhysRevC.93.054314
2016DR13 Phys.Rev. C 94, 054307 (2016) C.Drischler, A.Carbone, K.Hebeler, A.Schwenk Neutron matter from chiral two- and three-nucleon calculations up to N3 LO
doi: 10.1103/PhysRevC.94.054307
2016DY01 Phys.Rev. C 94, 034001 (2016) A.Dyhdalo, R.J.Furnstahl, K.Hebeler, I.Tews Regulator artifacts in uniform matter for chiral interactions
doi: 10.1103/PhysRevC.94.034001
2016GA34 Nat.Phys. 12, 594 (2016) R.F.Garcia Ruiz, M.L.Bissell, K.Blaum, A.Ekstrom, N.Frommgen, G.Hagen, M.Hammen, K.Hebeler, J.D.Holt, G.R.Jansen, M.Kowalska, K.Kreim, W.Nazarewicz, R.Neugart, G.Neyens, W.Nortershauser, T.Papenbrock, J.Papuga, A.Schwenk, J.Simonis, K.A.Wendt, D.T.Yordanov Unexpectedly large charge radii of neutron-rich calcium isotopes NUCLEAR REACTIONS U(p, X)43Ca/44Ca/45Ca/46Ca/47Ca/48Ca/49Ca/50Ca/51Ca/52Ca, E=1.4GeV; measured hyperfine structure spectra; deduced charge radii. Comparison with available data.
doi: 10.1038/nphys3645
2016HA27 Nat.Phys. 12, 186 (2016) G.Hagen, A.Ekstrom, C.Forssen, G.R.Jansen, W.Nazarewicz, T.Papenbrock, K.A.Wendt, S.Bacca, N.Barnea, B.Carlsson, C.Drischler, K.Hebeler, M.Hjorth-Jensen, M.Miorelli, G.Orlandini, A.Schwenk, J.Simonis Neutron and weak-charge distributions of the 48Ca nucleus NUCLEAR STRUCTURE 48Ca; calculated neutron skin parameters, radii. Ab initio calculations.
doi: 10.1038/nphys3529
2016SI02 Phys.Rev. C 93, 011302 (2016) J.Simonis, K.Hebeler, J.D.Holt, J.Menendez, A.Schwenk Exploring sd-shell nuclei from two- and three-nucleon interactions with realistic saturation properties NUCLEAR STRUCTURE 18,19,20,21,22,23,24,25,26,27,28O, 19,20,21,22,23,24,25,26,27,28,29F, 20,21,22,23,24,25,26,27,28,29,30Ne, 21,22,23,24,25,26,27,28,29,30,31Na, 22,23,24,25,26,27,28,29,30,31,32Mg, 23,24,25,26,27,28,29,30,31,32,33Al, 24,25,26,27,28,29,30,31,32,33,34Si, 25,26,27,28,29,30,31,32,33,34,35P, 26,27,28,29,30,31,32,33,34,35,36S, 27,28,29,30,31,32,33,34,35,36,37Cl, 28,29,30,31,32,33,34,35,36,37,38Ar, 29,30,31,32,33,34,35,36,37,38,39K, 30,31,32,33,34,35,36,37,38,39,40Ca; calculated S(2n), S(2p), energies of first 2+ states in even-even nuclei, and theoretical uncertainty estimates from variation of the resolution scale, the low-energy couplings, and from the many-body method. 22,23,24,25,26,27,28,29,30,31,32Mg, 27,28,29,30,31,32,33,34,35,36,37Cl; calculated ground-state energies relative to that of 16O, and theoretical uncertainties. Comparison to AME-12 data.
doi: 10.1103/PhysRevC.93.011302
2016WI09 Few-Body Systems 57, 1213 (2016) H.Witala, J.Golak, R.Skibinski, K.Topolnicki, E.Epelbaum, K.Hebeler, H.Kamada, H.Krebs, U.-G.Meissner, A.Nogga Role of the Total Isospin 3/2 Component in Three-Nucleon Reactions NUCLEAR REACTIONS 2H(n, n), E=13, 250 MeV; calculated σ(θ), σ(θ, E). Comparison with available data.
doi: 10.1007/s00601-016-1156-3
2015HE11 Phys.Rev. C 91, 044001 (2015) K.Hebeler, H.Krebs, E.Epelbaum, J.Golak, R.Skibinski Efficient calculation of chiral three-nucleon forces up to N3LO for ab initio studies NUCLEAR STRUCTURE 3H; calculated matrix elements of chiral three-nucleon forces at next-to-next-to-leading-order and next-to-next-to-next-to-leading-order in large basis spaces, partial-wave contributions to the energy per particle to neutron matter, and contributions of the individual topologies to the triton energy for three different NN interactions. Relevance to ab initio studies of few-nucleon scattering processes, nuclei, and nuclear matter based on higher-order chiral three-nucleon forces.
doi: 10.1103/PhysRevC.91.044001
2015MO26 Phys.Rev. C 92, 064002 (2015) S.N.More, S.Konig, R.J.Furnstahl, K.Hebeler Deuteron electrodisintegration with unitarily evolved potentials NUCLEAR REACTIONS 2H(e, X), E not given; calculated momentum distributions for various potentials. Electrodisintegration of deuteron. Similarity renormalization-group (SRG) method for investigation of RG evolution of structure and reaction components. Unitary transformation matrices.
doi: 10.1103/PhysRevC.92.064002
2014FO09 Phys.Rev. C 89, 041301 (2014) M.M.Forbes, A.Gezerlis, K.Hebeler, T.Lesinski, A.Schwenk Neutron polaron as a constraint on nuclear density functionals
doi: 10.1103/PhysRevC.89.041301
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
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
2014HE03 Eur.Phys.J. A 50, 11 (2014) Symmetry energy, neutron skin, and neutron star radius from chiral effective field theory interactions
doi: 10.1140/epja/i2014-14011-4
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
2013HE06 Phys.Rev. C 87, 031302 (2013) Neutron matter based on consistently evolved chiral three-nucleon interactions
doi: 10.1103/PhysRevC.87.031302
2013KR10 Phys.Rev. C 88, 025802 (2013) T.Kruger, I.Tews, K.Hebeler, A.Schwenk Neutron matter from chiral effective field theory interactions
doi: 10.1103/PhysRevC.88.025802
2013TE01 Phys.Rev.Lett. 110, 032504 (2013) I.Tews, T.Kruger, K.Hebeler, A.Schwenk Neutron Matter at Next-to-Next-to-Next-to-Leading Order in Chiral Effective Field Theory NUCLEAR STRUCTURE 208Pb; calculated neutron matter energy, energy per particle vs. density using N3LO potentials. Comparison with available data.
doi: 10.1103/PhysRevLett.110.032504
2012HE04 Phys.Rev. C 85, 021002 (2012) Momentum-space evolution of chiral three-nucleon forces NUCLEAR STRUCTURE 3H; calculated ground state energy as function of flow parameter for different next to-next to leading order (N2LO) interactions and similarity renormalization group (SRG) model sizes, contour plots of the evolved 3N potential, matrix elements of the initial 3N forces. Chiral 3N forces.
doi: 10.1103/PhysRevC.85.021002
2012LE01 J.Phys.(London) G39, 015108 (2012) T.Lesinski, K.Hebeler, T.Duguet, A.Schwenk Chiral three-nucleon forces and pairing in nuclei
doi: 10.1088/0954-3899/39/1/015108
2012TS04 Phys.Rev. C 86, 015803 (2012) M.B.Tsang, J.R.Stone, F.Camera, P.Danielewicz, S.Gandolfi, K.Hebeler, C.J.Horowitz, J.Lee, W.G.Lynch, Z.Kohley, R.Lemmon, P.Moller, T.Murakami, S.Riordan, X.Roca-Maza, F.Sammarruca, A.W.Steiner, I.Vidana, S.J.Yennello Constraints on the symmetry energy and neutron skins from experiments and theory NUCLEAR STRUCTURE 208Pb; analyzed neutron-skin thickness, symmetry energy constraints. Contributions of three-body forces in neutron matter models.
doi: 10.1103/PhysRevC.86.015803
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
2010HE07 Phys.Rev. C 82, 014314 (2010) Chiral three-nucleon forces and neutron matter
doi: 10.1103/PhysRevC.82.014314
2009DU13 Int.J.Mod.Phys. E18, 2007 (2009) T.Duguet, T.Lesinski, K.Hebeler, K.Bennaceur, A.Schwenk, J.Meyer Non-empirical energy density functional for nuclei: The pairing part
doi: 10.1142/S0218301309014172
2009HE17 Phys.Rev. C 80, 044321 (2009) K.Hebeler, T.Duguet, T.Lesinski, A.Schwenk Non-empirical pairing energy functional in nuclear matter and finite nuclei NUCLEAR STRUCTURE N=16-184, Z=20, 28, 50, 82; Z=18-94, N=28, 50, 82, 126; calculated neutron and proton lowest canonical state (LCS) pairing gaps in semi-magic nuclei using refitted Skyrme EDF. Comparison with experimental data.
doi: 10.1103/PhysRevC.80.044321
2007HE18 Phys.Lett. B 648, 176 (2007) K.Hebeler, A.Schwenk, B.Friman Dependence of the BCS 1S0 superfluid pairing gap on nuclear interactions
doi: 10.1016/j.physletb.2007.03.022
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