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NSR database version of April 11, 2024.

Search: Author = U.van Kolck

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2023GR11      Eur.Phys.J. A 59, 289 (2023)

H.W.Griesshammer, U.van Kolck

Universality of three identical bosons with large, negative effective range

doi: 10.1140/epja/s10050-023-01196-0
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


2020VA02      Eur.Phys.J. A 56, 97 (2020)

U.van Kolck

Naturalness in nuclear effective field theories

doi: 10.1140/epja/s10050-020-00092-1
Citations: PlumX Metrics


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
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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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


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
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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
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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
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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
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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
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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
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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
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2011LO24      Nucl.Phys. A870-871, 72 (2011)

B.Long, U.van Kolck

The role of the Roper in chiral perturbation theory

doi: 10.1016/j.nuclphysa.2011.09.002
Citations: PlumX Metrics


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
Citations: PlumX Metrics


2010LO10      Nucl.Phys. A840, 39 (2010)

B.Long, U.van Kolck

πN scattering in the Λ(1232) region in an effective field theory

doi: 10.1016/j.nuclphysa.2010.03.008
Citations: PlumX Metrics


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
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2007VA12      Nucl.Phys. A787, 405c (2007)

U.van Kolck

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
Citations: PlumX Metrics


2007VA13      Nucl.Phys. A790, 39c (2007)

U.van Kolck

Nuclear effective field theory with pions

doi: 10.1016/j.nuclphysa.2007.03.053
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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


2006SE05      Phys.Rev. C 73, 044006 (2006)

R.Seki, U.van Kolck

Effective field theory of nucleon-nucleon scattering on large discrete lattices

doi: 10.1103/PhysRevC.73.044006
Citations: PlumX Metrics


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
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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
Citations: PlumX Metrics


2005HO01      Phys.Lett. B 605, 273 (2005)

W.H.Hockings, U.van Kolck

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
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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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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
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2005VA08      Int.J.Mod.Phys. E14, 11 (2005)

U.van Kolck

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
Citations: PlumX Metrics


2005VA15      Nucl.Phys. A752, 145c (2005)

U.van Kolck

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
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2005VA26      J.Phys.(London) G31, S1245 (2005)

U.van Kolck

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
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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
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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
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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
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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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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
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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
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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
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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
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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
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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
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2002BE90      Ann.Rev.Nucl.Part.Sci. 52, 339 (2002)

P.F.Bedaque, U.van Kolck

Effective Field Theory for Few-Nucleon Systems

doi: 10.1146/annurev.nucl.52.050102.090637
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2002VA06      Nucl.Phys. A699, 33c (2002)

U.van Kolck

Recent Developments in Nuclear Effective Field Theory

doi: 10.1016/S0375-9474(01)01467-1
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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
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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
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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)

U.van Kolck

Effective Field Theories for Strongly Interacting Systems

doi: 10.1016/S0375-9474(00)00382-1
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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
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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
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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
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2000MA19      Phys.Lett. 478B, 73 (2000)

C.M.Maekawa, U.van Kolck

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
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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
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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
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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
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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
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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
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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
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1999FR26      Phys.Rev. C60, 034006 (1999)

J.L.Friar, U.van Kolck

Charge-Independence Breaking in the Two-Pion-Exchange Nucleon-Nucleon Force

doi: 10.1103/PhysRevC.60.034006
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1999VA01      Nucl.Phys. A645, 273 (1999)

U.van Kolck

Effective Field Theory of Short-Range Forces

doi: 10.1016/S0375-9474(98)00612-5
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1999VA14      Prog.Part.Nucl.Phys. 43, 337 (1999)

U.Van Kolck

Effective Field Theory of Nuclear Forces

doi: 10.1016/S0146-6410(99)00097-6
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1998BE27      Phys.Lett. 428B, 221 (1998)

P.F.Bedaque, U.van Kolck

Nucleon-Deuteron Scattering from an Effective Field Theory

doi: 10.1016/S0370-2693(98)00430-4
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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
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1998VA04      Nucl.Phys. A631, 56c (1998)

U.van Kolck

Chiral Perturbation Theory in Few-Body Systems

doi: 10.1016/S0375-9474(98)00015-3
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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
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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
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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
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1996OR02      Phys.Rev. C53, 2086 (1996)

C.Ordonez, L.Ray, U.van Kolck

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
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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
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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
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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
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1994OR05      Phys.Rev.Lett. 72, 1982 (1994)

C.Ordonez, L.Ray, U.van Kolck

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
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1994VA11      Phys.Rev. C49, 2932 (1994)

U.van Kolck

Few-Nucleon Forces from Chiral Lagrangians

doi: 10.1103/PhysRevC.49.2932
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