NSR Query Results
Output year order : Descending NSR database version of April 29, 2024. Search: Author = B.Long Found 19 matches. 2023LI40 Phys.Rev. C 108, 024002 (2023) Effective field theory with resonant P-wave interaction NUCLEAR STRUCTURE 6He; calculated binding energy. Effective field theory with momentum-dependent nonlocal potential for shallow P-wave resonances applied to neutron-α and neutron-neutron-α systems.
doi: 10.1103/PhysRevC.108.024002
2022GU06 J.Phys.(London) G49, 055104 (2022) Nuclear reactions in artificial traps
doi: 10.1088/1361-6471/ac59d5
2022LI62 Phys.Rev. C 106, 055501 (2022) T.-X.Liu, R.Peng, S.Lyu, B.Long Renormalization of proton-proton fusion in chiral effective field theory NUCLEAR REACTIONS 1H(p, d);E(cm)<330 MeV/c; calculated pp 1S0 phase shift, radial matrix element as a function of cut-off value. Calculations in the framework of chiral effective field theory (ChEFT), with renormalization-group (RG) invariance performed up to next-to-next-to-leading order (N2LO).
doi: 10.1103/PhysRevC.106.055501
2022PE06 Phys.Rev. C 105, 054002 (2022) R.Peng, S.Lyu, S.Konig, B.Long Constructing chiral effective field theory around unnatural leading-order interactions NUCLEAR STRUCTURE 3H; calculated binding energy. Momentum-dependent formulation based on a stationary spin-0 and isospin-1 dibaryon field.
doi: 10.1103/PhysRevC.105.054002
2022SH32 Phys.Rev. C 106, 015505 (2022) W.Shi, R.Peng, T.X.Liu, S.Lyu, B.Long Perturbative calculations of deuteron form factors NUCLEAR STRUCTURE 2H; calculated charge, quadrupole, and magnetic form factors. Chiral effective field theory calculations up to next-to-next-to-leading (N2LO) with corrections arising from chiral nuclear forces in perturbation theory.
doi: 10.1103/PhysRevC.106.015505
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
2021LI55 Phys.Rev. C 104, 044001 (2021) C.Li, J.Yu, R.Peng, S.Lyu, B.Long Trapped two-nucleon system in energy-dependent effective field theory
doi: 10.1103/PhysRevC.104.044001
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
2019WU04 Phys.Rev. C 99, 024003 (2019) Perturbative NN scattering in chiral effective field theory
doi: 10.1103/PhysRevC.99.024003
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
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
2016LO05 Phys.Rev. C 93, 044003 (2016) Cutoff regulators in chiral nuclear effective field theory
doi: 10.1103/PhysRevC.93.044003
2013LO06 Phys.Rev. C 88, 014002 (2013) Improved convergence of chiral effective field theory for 1S0 of NN scattering
doi: 10.1103/PhysRevC.88.014002
2012LO03 Phys.Rev. C 85, 034002 (2012) Renormalizing chiral nuclear forces: Triplet channels
doi: 10.1103/PhysRevC.85.034002
2012LO09 Phys.Rev. C 86, 024001 (2012) Short-range nuclear forces in singlet channels
doi: 10.1103/PhysRevC.86.024001
2011LO11 Phys.Rev. C 83, 045206 (2011) Heavy-particle formalism with Foldy-Wouthuysen representation
doi: 10.1103/PhysRevC.83.045206
2011LO24 Nucl.Phys. A870-871, 72 (2011) The role of the Roper in chiral perturbation theory
doi: 10.1016/j.nuclphysa.2011.09.002
2011LO26 Phys.Rev. C 84, 057001 (2011) Renormalizing chiral nuclear forces: A case study of 3P0
doi: 10.1103/PhysRevC.84.057001
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
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