NSR Query Results
Output year order : Descending NSR database version of April 24, 2024. Search: Author = U.van Kolck Found 82 matches. 2023GR11 Eur.Phys.J. A 59, 289 (2023) Universality of three identical bosons with large, negative effective range
doi: 10.1140/epja/s10050-023-01196-0
2023YA29 Eur.Phys.J. A 59, 233 (2023) C.-J.Yang, A.Ekstrom, C.Forssen, G.Hagen, G.Rupak, U.van Kolck The importance of few-nucleon forces in chiral effective field theory NUCLEAR STRUCTURE 3H, 4He, 16O, 40Ca; calculated binding energy per nucleon with NN-only and NN+NNN interactions at leading order (LO) with coupled-cluster model of the equation of state for symmetric nuclear matter; deduced LO four-nucleon forces could play a crucial role for describing heavy-mass nuclei.
doi: 10.1140/epja/s10050-023-01149-7
2022TE06 Few-Body Systems 63, 67 (2022) I.Tews, Z.Davoudi, A.Ekstrom, J.D.Holt, K.Becker, R.Briceno, D.J.Dean, W.Detmold, C.Drischler, T.Duguet, E.Epelbaum, A.Gasparyan, J.Gegelia, J.R.Green, H.W.Griesshammer, A.D.Hanlon, M.Heinz, H.Hergert, M.Hoferichter, M.Illa, D.Kekejian, A.Kievsky, S.Konig, H.Krebs, K.D.Launey, D.Lee, P.Navratil, A.Nicholson, A.Parreno, D.R.Phillips, M.Ploszajczak, X.-L.Ren, T.R.Richardson, C.Robin, G.H.Sargsyan, M.J.Savage, M.R.Schindler, P.E.Shanahan, R.P.Springer, A.Tichai, U.van Kolck, M.L.Wagman, A.Walker-Loud, C.-J.Yang, X.Zhang Nuclear Forces for Precision Nuclear Physics: A Collection of Perspectives
doi: 10.1007/s00601-022-01749-x
2022ZH26 Phys.Rev. C 105, 054005 (2022) D.Zhou, B.Long, R.G.E.Timmermans, U.van Kolck Renormalization of one-pion exchange in chiral effective field theory for antinucleon-nucleon scattering
doi: 10.1103/PhysRevC.105.054005
2021HA24 Eur.Phys.J. A 57, 169 (2021) J.B.Habashi, S.Fleming, U.van Kolck Nonrelativistic effective field theory with a resonance field
doi: 10.1140/epja/s10050-021-00452-5
2021OO01 Phys.Lett. B 820, 136525 (2021) F.Oosterhof, J.de Vries, R.G.E.Timmermans, U.van Kolck Nucleon decay in the deuteron
doi: 10.1016/j.physletb.2021.136525
2020RY02 Eur.Phys.J. A 56, 7 (2020) E.Ryberg, C.Forssen, D.R.Phillips, U.van Kolck Finite-size effects in heavy halo nuclei from effective field theory
doi: 10.1140/epja/s10050-019-00001-1
2020VA02 Eur.Phys.J. A 56, 97 (2020) Naturalness in nuclear effective field theories
doi: 10.1140/epja/s10050-020-00092-1
2019CI06 Phys.Rev. C 100, 055504 (2019) V.Cirigliano, W.Dekens, J.de Vries, M.L.Graesser, E.Mereghetti, S.Pastore, M.Piarulli, U.van Kolck, R.B.Wiringa Renormalized approach to neutrinoless double-β decay RADIOACTIVITY 6He, 12Be(2β-); calculated Fermi (F), Gamow-Teller (GT), and tensor (T) densities, variational Monte Carlo (VMC) for the dimensionless matrix elements of the long-range and short-range neutrino-exchange potentials and short-range transition densities for 0νββ decay modes; deduced that a short-range operator is only needed in spin-singlet s-wave transitions, while leading-order transitions involving higher partial waves depend solely on long-range currents.Ab initio calculations of the matrix elements for 0νββ decay using pionless and chiral effective field theory, extended to include next-to-leading-order corrections.
doi: 10.1103/PhysRevC.100.055504
2019OO01 Phys.Rev.Lett. 122, 172501 (2019) F.Oosterhof, B.Long, J.de Vries, R.G.E.Timmermans, U.van Kolck Baryon-Number Violation by Two Units and the Deuteron Lifetime NUCLEAR STRUCTURE 2H; calculated the lifetime of the deuteron with dimension-nine quark operators that violate baryon number by two units.
doi: 10.1103/PhysRevLett.122.172501
2018SA09 Phys.Rev. C 97, 024001 (2018) M.Sanchez Sanchez, C.-J.Yang, B.Long, U.van Kolck Two-nucleon 1S0 amplitude zero in chiral effective field theory
doi: 10.1103/PhysRevC.97.024001
2017KO17 Phys.Rev.Lett. 118, 202501 (2017) S.Konig, H.W.Griesshammer, H.-W.Hammer, U.van Kolck Nuclear Physics Around the Unitarity Limit
doi: 10.1103/PhysRevLett.118.202501
2017PA16 Phys.Rev. C 95, 054001 (2017) M.Pavon Valderrama, M.Sanchez Sanchez, C.-J.Yang, B.Long, J.Carbonell, U.van Kolck Power counting in peripheral partial waves: The singlet channels
doi: 10.1103/PhysRevC.95.054001
2017SO16 Phys.Rev. C 96, 024002 (2017); Erratum Phys.Rev. C 100, 019901 (2019) Y.-H.Song, R.Lazauskas, U.van Kolck Triton binding energy and neutron-deuteron scattering up to next-to-leading order in chiral effective field theory NUCLEAR REACTIONS 2H(n, X), E=5 MeV-10 GeV; analyzed cutoff dependence of three-nucleon observables: the quartet and doublet neutron-deuteron scattering lengths, phase shifts, and the triton binding energy at the leading and next-to-leading orders using Chiral Effective Field Theory. 3H; analyzed triton binding energy.
doi: 10.1103/PhysRevC.96.024002
2017YA15 Phys.Rev. C 95, 054325 (2017) C.J.Yang, M.Grasso, K.Moghrabi, U.van Kolck Renormalizability of the nuclear many-body problem with the Skyrme interaction beyond mean field
doi: 10.1103/PhysRevC.95.054325
2016GR16 Phys.Scr. 91, 063005 (2016) M.Grasso, D.Lacroix, U.van Kolck From effective field theories to effective density functionals in and beyond the mean field
doi: 10.1088/0031-8949/91/6/063005
2016KO17 J.Phys.(London) G43, 055106 (2016) S.Konig, H.W.Griesshammer, H.-W.Hammer, U.van Kolck Effective theory of3H and 3He NUCLEAR STRUCTURE 3H, 3He; calculated binding energy splitting; deduced Coulomb force in pionless EFT is a completely perturbative effect in the trinucleon bound-state regime.
doi: 10.1088/0954-3899/43/5/055106
2015BA05 Phys.Rev.Lett. 114, 052501 (2015) N.Barnea, L.Contessi, D.Gazit, F.Pederiva, U.van Kolck Effective Field Theory for Lattice Nuclei NUCLEAR STRUCTURE 3H, 3,4,5He, 5,6Li; calculated binding energies. Comparison with available data.
doi: 10.1103/PhysRevLett.114.052501
2015KI10 Phys.Rev. C 92, 054002 (2015) J.Kirscher, N.Barnea, D.Gazit, F.Pederiva, U.van Kolck Spectra and scattering of light lattice nuclei from effective field theory
doi: 10.1103/PhysRevC.92.054002
2013EN01 Prog.Part.Nucl.Phys. 71, 21 (2013) J.Engel, M.J.Ramsey-Musolf, U.van Kolck Electric dipole moments of nucleons, nuclei, and atoms: The Standard Model and beyond
doi: 10.1016/j.ppnp.2013.03.003
2013ME12 Phys.Rev. C 88, 034001 (2013) E.Mereghetti, J.de Vries, R.G.E.Timmermans, U.van Kolck Toroidal quadrupole form factor of the deuteron
doi: 10.1103/PhysRevC.88.034001
2012CO20 Phys.Rev. C 86, 054002 (2012) S.A.Coon, M.I.Avetian, M.K.G.Kruse, U.van Kolck, P.Maris, J.P.Vary Convergence properties of ab initio calculations of light nuclei in a harmonic oscillator basis NUCLEAR STRUCTURE 2,3H, 4,6He; calculated ground-state energy of light nuclei as function of momentum using shell model with the bare and soft NN interactions Idaho N3LO and JISP16.
doi: 10.1103/PhysRevC.86.054002
2012LI29 Phys.Lett. B 713, 447 (2012) C.-P.Liu, J.de Vries, E.Mereghetti, R.G.E.Timmermans, U.van Kolck Deuteron magnetic quadrupole moment from chiral effective field theory NUCLEAR STRUCTURE 2H; calculated magnetic quadrupole moment of the deuteron; QCD calculations, comparison with available data.
doi: 10.1016/j.physletb.2012.06.024
2012RO07 Phys.Rev. C 85, 034003 (2012); Pub.Note Phys.Rev. C 85, 039903 (2012) J.Rotureau, I.Stetcu, B.R.Barrett, U.van Kolck Two and three nucleons in a trap, and the continuum limit
doi: 10.1103/PhysRevC.85.034003
2011DE34 Phys.Rev. C 84, 065501 (2011) J.de Vries, R.Higa, C.-P.Liu, E.Mereghetti, I.Stetcu, R.G.E.Timmermans, U.van Kolck Electric dipole moments of light nuclei from chiral effective field theory NUCLEAR STRUCTURE 2,3H, 3He; calculated electric dipole moments by systematic expansion provided by chiral effective field theory (EFT) taking into account parity and time reversal violation.
doi: 10.1103/PhysRevC.84.065501
2011LO24 Nucl.Phys. A870-871, 72 (2011) The role of the Roper in chiral perturbation theory
doi: 10.1016/j.nuclphysa.2011.09.002
2011MA64 Nucl.Phys. A872, 117 (2011) C.M.Maekawa, E.Mereghetti, J.de Vries, U.van Kolck The time-reversal- and parity-violating nuclear potential in chiral effective theory
doi: 10.1016/j.nuclphysa.2011.09.020
2010LO10 Nucl.Phys. A840, 39 (2010) πN scattering in the Λ(1232) region in an effective field theory
doi: 10.1016/j.nuclphysa.2010.03.008
2008HI12 Nucl.Phys. A809, 171 (2008) R.Higa, H.-W.Hammer, U.van Kolck αα scattering in halo effective field theory NUCLEAR REACTIONS 4H(α, α'), E=0-3.5 MeV; calculated phase shifts. Effective field theory and effective-range expansion, halo and cluster nuclei discussed.
doi: 10.1016/j.nuclphysa.2008.06.003
2007VA12 Nucl.Phys. A787, 405c (2007) Nuclear Effective Field Theory Without Pion NUCLEAR REACTIONS 4He(n, X), E=0-5 MeV; calculated σ. Effective field theory. Comparison with data. NUCLEAR STRUCTURE 2,3H, 4He, 6Li; calculated binding energy. Effective field theory and no-core shell model.
doi: 10.1016/j.nuclphysa.2006.12.062
2007VA13 Nucl.Phys. A790, 39c (2007) Nuclear effective field theory with pions
doi: 10.1016/j.nuclphysa.2007.03.053
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
2006SE05 Phys.Rev. C 73, 044006 (2006) Effective field theory of nucleon-nucleon scattering on large discrete lattices
doi: 10.1103/PhysRevC.73.044006
2005BE08 Nucl.Phys. A747, 311 (2005) S.R.Beane, M.Malheiro, J.A.McGovern, D.R.Phillips, U.van Kolck Compton scattering on the proton, neutron, and deuteron in chiral perturbation theory to O(Q4) NUCLEAR REACTIONS 1n, 1,2H(γ, γ'), E ≈ 40-200 MeV; calculated σ(θ). Chiral perturbation theory, comparison with data.
doi: 10.1016/j.nuclphysa.2004.09.068
2005FR02 Phys.Rev. C 71, 024003 (2005) J.L.Friar, G.L.Payne, U.van Kolck Charge-symmetry-breaking three-nucleon forces NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference, role of charge-symmetry-breaking three-nucleon forces.
doi: 10.1103/PhysRevC.71.024003
2005HO01 Phys.Lett. B 605, 273 (2005) The electric dipole form factor of the nucleon NUCLEAR STRUCTURE 1n, 1H; calculated electric dipole form factor.
doi: 10.1016/j.physletb.2004.11.043
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
2005PA34 Phys.Rev. C 71, 064002 (2005) V.R.Pandharipande, D.R.Phillips, U.van Kolck Δ effects in pion-nucleon scattering and the strength of the two-pion-exchange three-nucleon interaction
doi: 10.1103/PhysRevC.71.064002
2005VA08 Int.J.Mod.Phys. E14, 11 (2005) Halo effective field theory NUCLEAR REACTIONS 4He(n, n), E=0-5 MeV; calculated σ, σ(θ). Effective field theories, halo systems.
doi: 10.1142/S0218301305002722
2005VA15 Nucl.Phys. A752, 145c (2005) Effective Field Theories of Light Nuclei NUCLEAR REACTIONS 4He(n, n), E ≈ 0.1-5 MeV; calculated σ, σ(θ). Effective field theory approach.
doi: 10.1016/j.nuclphysa.2005.02.030
2005VA26 J.Phys.(London) G31, S1245 (2005) Effective field theories for weakly bound nuclei NUCLEAR STRUCTURE 2,3H; calculated binding energies. Effective field theory approach. NUCLEAR REACTIONS 4He(n, n), E ≈ 0-4 MeV; calculated σ, σ(θ). Effective field theory approach.
doi: 10.1088/0954-3899/31/8/002
2005ZH05 Nucl.Phys. A748, 435 (2005) S.-L.Zhu, C.M.Maekawa, B.R.Holstein, M.J.Ramsey-Musolf, U.van Kolck Nuclear parity violation in effective field theory
doi: 10.1016/j.nuclphysa.2004.10.032
2004CO08 Phys.Lett. B 588, 57 (2004) T.D.Cohen, B.A.Gelman, U.van Kolck An effective field theory for coupled-channel scattering
doi: 10.1016/j.physletb.2004.03.020
2004FR29 Phys.Rev. C 70, 044001 (2004) J.L.Friar, U.van Kolck, M.C.M.Rentmeester, R.G.E.Timmermans Nucleon-mass difference in chiral perturbation theory and nuclear forces
doi: 10.1103/PhysRevC.70.044001
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
2003BE40 Phys.Lett. B 567, 200 (2003); Erratum Phy.Lett. B 607, 320 (2005) S.R.Beane, M.Malheiro, J.A.McGovern, D.R.Phillips, U.van Kolck Nucleon polarizabilities from low-energy Compton scattering NUCLEAR REACTIONS 1,2H(γ, γ), E ≈ 40-200 MeV; analyzed σ(θ). 1n, 1H deduced polarizabilities.
doi: 10.1016/j.physletb.2003.06.040
2003BE42 Phys.Lett. B 569, 159 (2003) P.F.Bedaque, H.-W.Hammer, U.van Kolck Narrow resonances in effective field theory NUCLEAR REACTIONS 4He(n, n), E=0-1 MeV; calculated total σ. 4He(n, n), E(cm)=15.5 MeV; calculated σ(θ). Effective field theory.
doi: 10.1016/j.physletb.2003.07.049
2003FR20 Phys.Rev. C 68, 024003 (2003) J.L.Friar, U.van Kolck, G.L.Payne, S.A.Coon Charge-symmetry breaking and the two-pion-exchange two-nucleon interaction NUCLEAR STRUCTURE 3H, 3He; calculated binding energy difference, charge-symmetry breaking effects. Effective field theory.
doi: 10.1103/PhysRevC.68.024003
2003ST16 Phys.Rev.Lett. 91, 142302 (2003) E.J.Stephenson, A.D.Bacher, C.E.Allgower, A.Gardestig, C.M.Lavelle, G.A.Miller, H.Nann, J.Olmsted, P.V.Pancella, M.A.Pickar, J.Rapaport, T.Rinckel, A.Smith, H.M.Spinka, U.van Kolck Observation of the Charge Symmetry Breaking d + d → 4He + π0 Reaction Near Threshold NUCLEAR REACTIONS 2H(d, π0), (d, 2γ), E=228.5, 231.8 MeV; measured missing mass spectra, pion production total σ; deduced charge symmetry breaking features.
doi: 10.1103/PhysRevLett.91.142302
2002BE22 Nucl.Phys. A700, 377 (2002) S.R.Beane, P.F.Bedaque, M.J.Savage, U.van Kolck Towards a Perturbative Theory of Nuclear Forces
doi: 10.1016/S0375-9474(01)01324-0
2002BE83 Nucl.Phys. A712, 37 (2002) C.A.Bertulani, H.-W.Hammer, U.van Kolck Effective field theory for halo nuclei: shallow p-wave states NUCLEAR REACTIONS 4H(n, n'), E=0-4 MeV; calculated phase shifts, σ, σ(θ). Effective field theory, application to halo nuclei discussed.
doi: 10.1016/S0375-9474(02)01270-8
2002BE90 Ann.Rev.Nucl.Part.Sci. 52, 339 (2002) Effective Field Theory for Few-Nucleon Systems
doi: 10.1146/annurev.nucl.52.050102.090637
2002VA06 Nucl.Phys. A699, 33c (2002) Recent Developments in Nuclear Effective Field Theory
doi: 10.1016/S0375-9474(01)01467-1
2001DI07 Phys.Rev. C63, 044007 (2001) L.Diaconescu, R.Schiavilla, U.van Kolck Parity-Violating Electron-Deuteron Scattering NUCLEAR REACTIONS 2H(e, e'), E=193 MeV calculated σ(θ), asymmetry. Model including Z0 exchange and 1-, 2-body contributions.
doi: 10.1103/PhysRevC.63.044007
2001HA17 Phys.Rev. C63, 044002 (2001) C.Hanhart, G.A.Miller, F.Myhrer, T.Sato, U.van Kolck Toy Model for Pion Production in Nucleon-Nucleon Collisions
doi: 10.1103/PhysRevC.63.044002
2001HU13 Few-Body Systems 30, 95 (2001) D.Huber, J.L.Friar, A.Nogga, H.Witala, U.van Kolck Novel Three-Nucleon-Force Terms in the Three-Nucleon System NUCLEAR REACTIONS 2H(polarized n, n), E=3, 10, 50 MeV; calculated Ay(θ). Three-nucleon force, comparisons with data.
2001VA05 Nucl.Phys. A680, 17c (2001) Effective Field Theories for Strongly Interacting Systems
doi: 10.1016/S0375-9474(00)00382-1
2000BE39 Nucl.Phys. A676, 357 (2000) P.F.Bedaque, H.-W.Hammer, U.van Kolck Effective Theory of the Triton NUCLEAR STRUCTURE 3H; calculated phase shifts, three-nucleon bound state spectrum, scattering lengths. Three-body forces discussed. Effective field theory calculations. NUCLEAR REACTIONS 2H(n, X), E=low; calculated phase shifts, three-nucleon bound state spectrum, scattering lengths. Three-body forces discussed. Effective field theory calculations.
doi: 10.1016/S0375-9474(00)00205-0
2000DA04 Phys.Rev. C61, 034613 (2000) C.A.da Rocha, G.A.Miller, U.van Kolck NN → NNπ+ Reaction Near Threshold in a Chiral Power Counting Approach NUCLEAR REACTIONS 1H(p, π+), (p, nπ+), E ≈ threshold; calculated σ; deduced contributions. Chiral power counting approach.
doi: 10.1103/PhysRevC.61.034613
2000HA48 Phys.Rev.Lett. 85, 2905 (2000) C.Hanhart, U.van Kolck, G.A.Miller Chiral Three-Nucleon Forces from p-Wave Pion Production NUCLEAR REACTIONS 1H(p, pπ0), E not given; calculated partial σ vs pion momentum. 1H(p, pπ+), E not given; calculated transition amplitude vs pion momentum. Chiral perturbation theory, three-nucleon forces.
doi: 10.1103/PhysRevLett.85.2905
2000MA19 Phys.Lett. 478B, 73 (2000) The Anapole Form Factor of the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated anapole form factor. Chiral perturbation theory.
doi: 10.1016/S0370-2693(00)00249-5
2000MA67 Phys.Lett. 488B, 167 (2000) C.M.Maekawa, J.S.Veiga, U.van Kolck The Nucleon Anapole Form Factor in Chiral Perturbation Theory to Sub-Leading Order NUCLEAR STRUCTURE 1n, 1H; calculated anapole form factors.
doi: 10.1016/S0370-2693(00)00851-0
2000MU07 Phys.Rev. C61, 044320 (2000) H.-M.Muller, S.E.Koonin, R.Seki, U.van Kolck Nuclear Matter on a Lattice
doi: 10.1103/PhysRevC.61.044320
2000VA26 Phys.Lett. 493B, 65 (2000) U.van Kolck, J.A.Niskanen, G.A.Miller Charge Symmetry Violation in pn → dπ0 and Chiral Effective Field Theory NUCLEAR REACTIONS 1H(n, π0), E(cm)=279.5 MeV; calculated integrated forward-backward asymmetry in σ(θ) near threshold. Charge symmetry violation discussed in connection with future experiments.
doi: 10.1016/S0370-2693(00)01133-3
1999BE06 Nucl.Phys. A646, 444 (1999) P.F.Bedaque, H.-W.Hammer, U.van Kolck The Three-Boson System with Short-Range Interactions
doi: 10.1016/S0375-9474(98)00650-2
1999BE42 Nucl.Phys. A656, 367 (1999) S.R.Beane, M.Malheiro, D.R.Phillips, U.van Kolck Compton Scattering on the Deuteron in Baryon Chiral Perturbation Theory NUCLEAR REACTIONS 2H(γ, γ'), E=49, 69, 95 MeV; calculated Compton scattering σ(θ). Baryon chiral perturbation theory, comparisons with data.
doi: 10.1016/S0375-9474(99)00312-7
1999FR02 Phys.Rev. C59, 53 (1999) J.L.Friar, D.Huber, U.van Kolck Chiral Symmetry and Three-Nucleon Forces
doi: 10.1103/PhysRevC.59.53
1999FR26 Phys.Rev. C60, 034006 (1999) Charge-Independence Breaking in the Two-Pion-Exchange Nucleon-Nucleon Force
doi: 10.1103/PhysRevC.60.034006
1999VA01 Nucl.Phys. A645, 273 (1999) Effective Field Theory of Short-Range Forces
doi: 10.1016/S0375-9474(98)00612-5
1999VA14 Prog.Part.Nucl.Phys. 43, 337 (1999) Effective Field Theory of Nuclear Forces
doi: 10.1016/S0146-6410(99)00097-6
1998BE27 Phys.Lett. 428B, 221 (1998) Nucleon-Deuteron Scattering from an Effective Field Theory
doi: 10.1016/S0370-2693(98)00430-4
1998BE37 Phys.Rev. C58, R641 (1998) P.F.Bedaque, H.-W.Hammer, U.van Kolck Effective Theory for Neutron-Deuteron Scattering: Energy dependence NUCLEAR REACTIONS 2H(n, X), E not given; calculated phase shifts.
doi: 10.1103/PhysRevC.58.R641
1998VA04 Nucl.Phys. A631, 56c (1998) Chiral Perturbation Theory in Few-Body Systems
doi: 10.1016/S0375-9474(98)00015-3
1998VA10 Phys.Rev.Lett. 80, 4386 (1998) U.van Kolck, M.C.M.Rentmeester, J.L.Friar, T.Goldman, J.J.de Swart Electromagnetic Corrections to the One-Pion-Exchange Potential
doi: 10.1103/PhysRevLett.80.4386
1997BE19 Nucl.Phys. A618, 381 (1997) S.R.Beane, V.Bernard, T.-S.H.Lee, Ulf.-G.Meissner, U.van Kolck Neutral Pion Photoproduction on Deuterium in Baryon Chiral Perturbation Theory to Order q4 NUCLEAR REACTIONS 2H(γ, X), E ≈ threshold; calculated π0 production σ related features; deduced sensitivity to γn → π0n amplitude. Baryon chiral perturbation theory to order q4.
doi: 10.1016/S0375-9474(97)00133-4
1996CO07 Phys.Rev. C53, 2661 (1996) T.D.Cohen, J.L.Friar, G.A.Miller, U.van Kolck pp → ppπ0 Reaction Near Threshold: A chiral power counting approach NUCLEAR REACTIONS 1H(p, X), E ≈ threshold; calculated amplitude characteristics for different mechanisms in pp → ppπ0 reaction. Power-counting scheme.
doi: 10.1103/PhysRevC.53.2661
1996OR02 Phys.Rev. C53, 2086 (1996) Two-Nucleon Potential from Chiral Lagrangians NUCLEAR STRUCTURE 2H; calculated binding energy, μ, electric quadrupole moment, D-state probability, asymptotic D/S ratio. Effective chiral Lagrangian based NN-potential. NUCLEAR REACTIONS 1H(p, p), E ≤ 300 MeV; 1H(n, n), E ≤ 100 MeV; calculated phase shifts, mixing angle vs E. Effective chiral Lagrangian based NN-potential.
doi: 10.1103/PhysRevC.53.2086
1996VA08 Phys.Lett. 371B, 169 (1996) U.van Kolck, J.L.Friar, T.Goldman Phenomenological Aspects of Isospin Violation in the Nuclear Force
doi: 10.1016/0370-2693(96)00009-3
1996VA18 Phys.Lett. 388B, 679 (1996) U.van Kolck, G.A.Miller, D.O.Riska Meson Exchange and Pion Rescattering Contributions to the Cross Section for pp → ppπ0 NUCLEAR REACTIONS 1H(p, pπ0), E not given; analyzed σ. Meson exchange and pion rescattering included.
doi: 10.1016/S0370-2693(96)01225-7
1995BE53 Phys.Rev. C52, 2914 (1995) S.R.Beane, C.Y.Lee, U.van Kolck Neutral Pion Photoproduction on Nuclei in Baryon Chiral Perturbation Theory
doi: 10.1103/PhysRevC.52.2914
1994OR05 Phys.Rev.Lett. 72, 1982 (1994) Nucleon-Nucleon Potential from an Effective Chiral Lagrangian NUCLEAR REACTIONS 1H, 1n(p, p), E=100 MeV; calculated phase shifts vs E. Potential based on effective chiral Lagrangian.
doi: 10.1103/PhysRevLett.72.1982
1994VA11 Phys.Rev. C49, 2932 (1994) Few-Nucleon Forces from Chiral Lagrangians
doi: 10.1103/PhysRevC.49.2932
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