NSR Query Results
Output year order : Descending NSR database version of April 25, 2024. Search: Author = F.Myhrer Found 47 matches. 2024CH16 Eur.Phys.J. A 60, (2024) P.Choudhary, U.Raha, F.Myhrer, D.Chakrabarti Analytical evaluation of elastic lepton-proton two-photon exchange in chiral perturbation theory
doi: 10.1140/epja/s10050-023-01207-0
2018TA29 Eur.Phys.J. A 54, 195 (2018) P.Talukdar, F.Myhrer, G.Meher, U.Raha Low-energy lepton-proton bremsstrahlung via effective field theory
doi: 10.1140/epja/i2018-12629-8
2016BA27 Eur.Phys.J. A 52, 146 (2016) V.Baru, E.Epelbaum, A.A.Filin, C.Hanhart, H.Krebs, F.Myhrer Threshold pion production in proton-proton collisions at NNLO in chiral EFT
doi: 10.1140/epja/i2016-16146-6
2014PA37 Int.J.Mod.Phys. E23, 1430010 (2014) S.Pastore, F.Myhrer, K.Kubodera An update of muon capture on hydrogen NUCLEAR REACTIONS 1,2H(μ-, X), E not given; analyzed available data; deduced parameters for capture rate. Chiral perturbation theory.
doi: 10.1142/S0218301314300100
2013FI10 Phys.Rev. C 88, 064003 (2013) A.A.Filin, V.Baru, E.Epelbaum, H.Krebs, C.Hanhart, F.Myhrer Pion production in nucleon-nucleon collisions in chiral effective field theory with Δ(1232) degrees of freedom
doi: 10.1103/PhysRevC.88.064003
2013PA40 Phys.Rev. C 88, 058501 (2013) S.Pastore, F.Myhrer, K.Kubodera Muon capture rate on hydrogen and the values of gA and gπNN
doi: 10.1103/PhysRevC.88.058501
2013RA07 Phys.Rev. C 87, 055501 (2013) Ordinary muon capture in hydrogen reexamined
doi: 10.1103/PhysRevC.87.055501
2012FI05 Phys.Rev. C 85, 054001 (2012) A.A.Filin, V.Baru, E.Epelbaum, H.Krebs, C.Hanhart, A.E.Kudryavtsev, F.Myhrer Pion production in nucleon-nucleon collisions in chiral effective field theory: Next-to-next-to-leading order contributions
doi: 10.1103/PhysRevC.85.054001
2012RA11 Phys.Rev. C 85, 045502 (2012), Erratum Phys.Rev. C 86, 039903 (2012) Radiative corrections to antineutrino-proton scattering at low energies
doi: 10.1103/PhysRevC.85.045502
2009KI06 Phys.Rev. C 80, 015206 (2009) Y.Kim, T.Sato, F.Myhrer, K.Kubodera Two-pion-exchange and other higher-order contributions to the pp → ppπ0 reaction NUCLEAR REACTIONS p(p, p)pπ0, E not given; calculated contributions to the threshold reaction amplitude with the use of the momentum coupling scheme (MCS) in the plane-wave approximation and in the frozen kinematics approximation (FKA). Comparison with the Weinberg scheme.
doi: 10.1103/PhysRevC.80.015206
2007GA32 Phys.Rev. C 76, 014005 (2007) A.Gardestig, K.Kubodera, F.Myhrer Comparison of the heavy-fermion and Foldy-Wouthuysen formalisms at third order
doi: 10.1103/PhysRevC.76.014005
2007KI14 Nucl.Phys. A792, 249 (2007) Y.Kim, K.Kubodera, D.-P.Min, F.Myhrer, M.Rho The effect of kaon condensation on quark-antiquark condensate in dense matter
doi: 10.1016/j.nuclphysa.2007.05.005
2007KI18 Phys.Lett. B 657, 187 (2007) Y.Kim, T.Sato, F.Myhrer, K.Kubodera Two-pion-exchange contributions to the pp → ppπ0 reaction
doi: 10.1016/j.physletb.2007.10.023
2006KI01 Phys.Rev. C 73, 025202 (2006) Y.Kim, I.Danchev, K.Kubodera, F.Myhrer, T.Sato Use of Vlow-k in a chiral-perturbation-theory description of the pp → ppπ0 reaction NUCLEAR REACTIONS 1H(p, p'π0), E=280-320 MeV; calculated σ. Chiral perturbation theory, comparison with data.
doi: 10.1103/PhysRevC.73.025202
2006MY01 Phys.Rev.C 74, 065202 (2006) Electromagnetic decay of Λ(1520)
doi: 10.1103/PhysRevC.74.065202
2005AL36 Phys.Rev. C 72, 038201 (2005) W.P.Alvarez, K.Kubodera, F.Myhrer Comparison of the extended linear σ model and chiral perturbation theory
doi: 10.1103/PhysRevC.72.038201
2005GU24 J.Res.Natl.Inst.Stand.Technol. 110, 315 (2005) V.Gudkov, K.Kubodera, F.Myhrer Radiative Corrections for Neutron Decay and Search for New Physics RADIOACTIVITY 1n(β-); calculated radiative corrections.
doi: 10.6028/jres.110.046
2005KO06 Phys.Rev. C 71, 028201 (2005) S.Kondratyuk, K.Kubodera, F.Myhrer Ratio of the proton electromagnetic form factors from meson dressing NUCLEAR STRUCTURE 1H; calculated electromagnetic form factor ratio. Dressed K-matrix model, comparison with data.
doi: 10.1103/PhysRevC.71.028201
2004AN13 Phys.Lett. B 595, 250 (2004) S.Ando, H.W.Fearing, V.Gudkov, K.Kubodera, F.Myhrer, S.Nakamura, T.Sato Neutron beta-decay in effective field theory RADIOACTIVITY 1n(β-); calculated T1/2, angular correlation coefficients, radiative corrections. Effective field theory.
doi: 10.1016/j.physletb.2004.06.037
2004KI20 Prog.Theor.Phys.(Kyoto) 112, 289 (2004) Fixed-Point Analysis of the Low-Energy Constants in the Pion-Nucleon Chiral Lagrangian
doi: 10.1143/PTP.112.289
2004KO25 Nucl.Phys. A736, 339 (2004) S.Kondratyuk, K.Kubodera, F.Myhrer, O.Scholten The Adler-Weisberger and Goldberger-Miyazawa-Oehme sum rules as probes of constraints from analyticity and chiral symmetry in dynamical models for pion-nucleon scattering
doi: 10.1016/j.nuclphysa.2004.03.003
2004TS09 Phys.Lett. B 602, 60 (2004) K.Tsuji, S.Nakamura, T.Sato, K.Kubodera, F.Myhrer Neutrino magnetic moment contribution to the neutrino-deuteron reaction NUCLEAR REACTIONS 2H(ν, ν'n), E=2.4-20.0 MeV; calculated breakup σ, effect of neutrino magnetic moment.
doi: 10.1016/j.physletb.2004.09.064
2003KO55 Phys.Rev. C 68, 044001 (2003) S.Kondratyuk, K.Kubodera, F.Myhrer In-medium meson properties and field transformations
doi: 10.1103/PhysRevC.68.044001
2003NA32 Nucl.Phys. A721, 549c (2003) S.Nakamura, T.Sato, S.Ando, T.-S.Park, F.Myhrer, V.Gudkov, K.Kubodera Neutrino-deuteron reactions at solar neutrino energies NUCLEAR REACTIONS 2H(ν, ep), (ν, νn), E=5, 10, 20 MeV; calculated σ. 2H(ν, X), E=0-20 MeV; calculated total charged-current σ.
doi: 10.1016/S0375-9474(03)01121-7
2002AN08 Phys.Rev. C65, 048501 (2002) S.-I.Ando, F.Myhrer, K.Kubodera Ordinary and Radiative Muon Capture in Liquid Hydrogen Reexamined NUCLEAR REACTIONS 1H(μ, ν), E at rest; analyzed ordinary and radiative capture rates.
doi: 10.1103/PhysRevC.65.048501
2002AN10 Phys.Lett. 533B, 25 (2002) S.Ando, T.-S.Park, K.Kubodera, F.Myhrer The μ-d Capture Rate in Effective Field Theory NUCLEAR REACTIONS 2H(μ-, ν), E at rest; calculated capture rate vs final-state energy. Heavy baryon chiral perturbation theory.
doi: 10.1016/S0370-2693(02)01619-2
2002NA19 Nucl.Phys. A707, 561 (2002) S.Nakamura, T.Sato, S.Ando, T.-S.Park, F.Myhrer, V.Gudkov, K.Kubodera Neutrino-Deuteron Reactions at Solar Neutrino Energies NUCLEAR REACTIONS 2H(ν, ep), (ν, νp), E=1.5-20.0 MeV; calculated σ. Effective field theory.
doi: 10.1016/S0375-9474(02)00993-4
2001AN01 Phys.Rev. C63, 015203 (2001) S.-I.Ando, F.Myhrer, K.Kubodera Capture Rate and Neutron Helicity Asymmetry for Ordinary Muon Capture on Hydrogen NUCLEAR REACTIONS 1H(μ-, ν), E at rest; calculated muon capture rate, neutron helicity asymmetry. Heavy-baryon chiral perturbation theory. ATOMIC PHYSICS, Mesic-atoms 1H(μ-, ν), E at rest; calculated muon capture rate, neutron helicity asymmetry. Heavy-baryon chiral perturbation theory.
doi: 10.1103/PhysRevC.63.015203
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
2000DM01 Phys.Rev. C61, 025205 (2000) Pion-Nucleon Scattering and the Nucleon Σ Term in an Extended Linear Σ Model
doi: 10.1103/PhysRevC.61.025205
2000DM02 Nucl.Phys. A663-664, 465c (2000) V.Dmitrasinovic, K.Kubodera, F.Myhrer, T.Sato A Next-to-Next-to-Leading-Order pp → ppπ0 Transition Operator in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(p, pπ0), E not given; calculated next-to-leading-order S-wave amplitude.
doi: 10.1016/S0375-9474(99)00632-6
1999DM03 Phys.Lett. 465B, 43 (1999) V.Dmitrasinovic, K.Kubodera, F.Myhrer, T.Sato A Next-to-Next-to-Leading-Order pp → ppπ0 Transition Operator in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated transition operators, corrections. Chiral perturbation theory.
doi: 10.1016/S0370-2693(99)01075-8
1998ME02 Phys.Lett. 416B, 36 (1998) T.Meissner, F.Myhrer, K.Kubodera Radiative Muon Capture by a Proton in Chiral Perturbation Theory NUCLEAR REACTIONS 1H(μ-, nγ), E not given; analyzed radiative muon capture rate; deduced pseudoscalar coupling related features. Chiral perturbation theory.
doi: 10.1016/S0370-2693(97)01330-0
1997KL02 Z.Phys. A358, 423 (1997) Comparing the p(bar)p → K-K+ and p(bar)p π-π+ Reactions NUCLEAR REACTIONS 1H(p-bar, X), E at 360-988 MeV/c; analyzed σ(θ), analyzing power vs θ for K-K+-, π-π+-production; deduced partial wave amplitude parameters.
doi: 10.1007/s002180050350
1997SA42 Phys.Rev. C56, 1246 (1997) T.Sato, T.-S.H.Lee, F.Myhrer, K.Kubodera Chiral Perturbation Theory and the pp → ppπ0 Reaction Near Threshold NUCLEAR REACTIONS 1H(p, p'X), E=280-320 MeV; analyzed pion production σ(E); deduced rescattering term contribution enhancement. Chiral perturbation theory, momentum-space representation.
doi: 10.1103/PhysRevC.56.1246
1996KL11 Acta Phys.Pol. B27, 2871 (1996) Comparing (p-bar)p → π-π+ and (p-bar)p → K-K+
1996PA10 Phys.Rev. C53, 1519 (1996) B.-Y.Park, F.Myhrer, J.R.Morones, T.Meissner, K.Kubodera Chiral Perturbation Approach to the pp → ppπ0 Reaction Near Threshold NUCLEAR REACTIONS 1H(p, pπ0), E ≈ threshold; calculated σ. Chiral perturbation approach.
doi: 10.1103/PhysRevC.53.1519
1994MY01 Yad.Fiz. 57, No 9, 1632 (1994); Phys.Atomic Nuclei 57, 1559 (1994) Exclusive Reactions at High Q2 and Polarization Phenomena NUCLEAR REACTIONS 1H(p-bar, X), E at 2.2 GeV/c; analyzed annihilation, multi-pion production data; deduced large angle scattering behavior.
1993TA14 Nucl.Phys. A556, 601 (1993) S.Takeuchi, F.Myhrer, K.Kubodera Maximum Asymmetry Phenomena in (p-bar)p → π-π+ and (p-bar)p → K-K+ Reactions NUCLEAR REACTIONS 1H(p-bar, p-bar), E at 988, 1550 MeV/c; calculated σ(θ), polarization. 1H(p-bar, X), E at 988, 1550 MeV/c; calculated σ(θ), asymmetry vs θ for (K-K+), (π-π+) production; deduced helicity-flip, helicity-nonflip amplitudes role.
doi: 10.1016/0375-9474(93)90472-A
1992CA34 Phys.Rev. D46, 2891 (1992) C.E.Carlson, M.Chachkhunashvili, F.Myhrer Elastic pp and pp-bar → ππ Reactions in Short- and Middle-Distance QCD NUCLEAR REACTIONS 1H(polarized p, p), E=high; calculated scaled σ(θ), spin correlation parameter; deduced implications to (p-bar)(p) interaction.
doi: 10.1103/PhysRevD.46.2891
1986TE04 Phys.Lett. 182B, 6 (1986) Low Energy p-p(bar) Scattering and the Quark Confinement Radius NUCLEAR REACTIONS H(p-bar, p-bar), (p-bar, n-bar), E=490 MeV/c; calculated σ(θ). New annihilation potential.
doi: 10.1016/0370-2693(86)91068-3
1982MY01 Phys.Lett. 110B, 353 (1982) Nucleon RMS Radii from Chiral Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated rms radii. Quark model.
doi: 10.1016/0370-2693(82)91271-0
1979MY01 Nucl.Phys. A326, 497 (1979) An Important Correction to πd Scattering in the Resonance Region NUCLEAR REACTIONS 2H(π+, π+), (π-, π-), E=142, 180, 256 MeV; calculated σ(θ). Nucleon-nucleon rescattering term, Faddeev calculations.
doi: 10.1016/0375-9474(79)90405-6
1978ER02 Phys.Lett. 74B, 163 (1978) Pion Bound States in Nuclei NUCLEAR STRUCTURE 16O, 28Si, 32Na, 208Pb; calculated pion-nucleus bound-state interaction.
doi: 10.1016/0370-2693(78)90543-9
1977KO25 Z.Phys. A283, 397 (1977) Theory of Pion-Nucleus Scattering Lengths NUCLEAR REACTIONS 4He, 11B, 12C, 14N, 16O(π-, π-); calculated contributions to scattering length.
doi: 10.1007/BF01409521
1976LO04 Helv.Phys.Acta 49, 123 (1976) A Remark on Pion Capture in Heavy Nuclei NUCLEAR REACTIONS 165Ho(π-, xn); calculated σ.
1969MY01 Phys.Norvegica 3, 191 (1969) Photo-Production of Positive Pions from 16O NUCLEAR REACTIONS 16O(γ, π+), E=150-300 MeV; calculated σ(E;θ).
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