NSR Query Results
Output year order : Descending NSR database version of March 21, 2024. Search: Author = S.Scherer Found 55 matches. 2018HI03 Phys.Rev. C 97, 035205 (2018) M.Hilt, T.Bauer, S.Scherer, L.Tiator Nucleon-to-Δ transition form factors in chiral effective field theory using the complex-mass scheme
doi: 10.1103/PhysRevC.97.035205
2017BA30 Phys.Rev. C 96, 025203 (2017) T.Bauer, Y.Unal, A.Kucukarslan, S.Scherer Mass and width of the Λ(1232) resonance using complex-mass renormalization
doi: 10.1103/PhysRevC.96.025203
2015UN02 Phys.Rev. C 92, 055208 (2015) Y.Unal, A.Kucukarslan, S.Scherer Interaction of the vector-meson octet with the baryon octet in effective field theory
doi: 10.1103/PhysRevC.92.055208
2014BA26 Phys.Rev. C 90, 015201 (2014) Electromagnetic transition form factors of the Roper resonance in a phenomenological field theory
doi: 10.1103/PhysRevC.90.015201
2013HI02 Phys.Rev. C 87, 045204 (2013) Threshold π0 photoproduction in relativistic chiral perturbation theory
doi: 10.1103/PhysRevC.87.045204
2013HI11 Phys.Rev. C 88, 055207 (2013) M.Hilt, B.C.Lehnhart, S.Scherer, L.Tiator Pion photo- and electroproduction in relativistic baryon chiral perturbation theory and the chiral MAID interface
doi: 10.1103/PhysRevC.88.055207
2012BA59 Phys.Rev. C 86, 065206 (2012) T.Bauer, J.C.Bernauer, S.Scherer Electromagnetic form factors of the nucleon in effective field theory
doi: 10.1103/PhysRevC.86.065206
2010GE07 Eur.Phys.J. A 44, 425 (2010) How to define physical properties of unstable particles
doi: 10.1140/epja/i2010-10955-5
2010PA04 Phys.Rev. C 81, 029802 (2010) B.Pasquini, D.Drechsel, S.Scherer Reply to "Comment on 'Polarizability of the pion: No conflict between dispersion theory and chiral perturbation theory'"
doi: 10.1103/PhysRevC.81.029802
2008CA12 Eur.Phys.J. A 35, 253 (2008) S.Capstick, A.Svarc, L.Tiator, J.Gegelia, M.M.Giannini, E.Santopinto, C.Hanhart, S.Scherer, T.-S.H.Lee, T.Sato, N.Suzuki The physical meaning of scattering matrix singularities in coupled-channel formalisms BRAG 2007 Workshop summary
doi: 10.1140/epja/i2007-10576-1
2008PA13 Phys.Rev. C 77, 065211 (2008) B.Pasquini, D.Drechsel, S.Scherer Polarizability of the pion: No conflict between dispersion theory and chiral perturbation theory
doi: 10.1103/PhysRevC.77.065211
2008SC04 Nucl.Phys. A803, 68 (2008); Erratum Nucl.Phys. A1010, 122175 (2021) M.R.Schindler, D.Djukanovic, J.Gegelia, S.Scherer Infrared renormalization of two-loop integrals and the chiral expansion of the nucleon mass
doi: 10.1016/j.nuclphysa.2008.01.023
2007DJ03 Few-Body Systems 41, 141 (2007) D.Djukanovic, J.Gegelia, S.Scherer, M.R.Schindler NN scattering in higher-derivative formulation of baryon chiral perturbation theory
doi: 10.1007/S00601-007-0194-2
2007SC04 Phys.Rev. C 75, 025202 (2007) M.R.Schindler, T.Fuchs, J.Gegelia, S.Scherer Axial, induced pseudoscalar, and pion-nucleon form factors in manifestly Lorentz-invariant chiral perturbation theory
doi: 10.1103/PhysRevC.75.025202
2007SC40 Phys.Lett. B 649, 390 (2007) M.R.Schindler, D.Djukanovic, J.Gegelia, S.Scherer Chiral expansion of the nucleon mass to order O(q6)
doi: 10.1016/j.physletb.2007.04.034
2007SC42 Eur.Phys.J. A 32, 429 (2007) Nucleon form factors of the isovector axial-vector current Situation of experiments and theory
doi: 10.1140/epja/i2006-10403-3
2006DJ03 Eur.Phys.J. A 29, 337 (2006) D.Djukanovic, J.Gegelia, S.Scherer Probing the convergence of perturbative series in baryon chiral perturbation theory NUCLEAR REACTIONS 1H(π-, π0), (π+, π+), (π-, π-), E(cm)=1.1-1.35 GeV; calculated σ(θ).
doi: 10.1140/epja/i2006-10096-6
2006HA19 Eur.Phys.J. A 28, 5 (2006) C.Hacker, N.Wies, J.Gegelia, S.Scherer Magnetic dipole moment of the Δ(1232) in chiral perturbation theory
doi: 10.1140/epja/i2006-10043-7
2006SC24 Eur.Phys.J. A 28, Supplement 1, 59 (2006) Chiral perturbation theory: Success and challenge NUCLEAR REACTIONS 1H(γ, π+γ), E=537-817 MeV; analysed σ, σ(E); deduced pion polarizabilities. 1H(e, e'γ), E not given; deduced proton magnetic polarizability. NUCLEAR STRUCTURE A=1; calculated form factors. Extended on-mass-shell renormalization scheme.
doi: 10.1140/epja/i2006-09-007-4
2005AH01 Eur.Phys.J. A 23, 113 (2005) J.Ahrens, V.M.Alexeev, J.R.M.Annand, H.J.Arends, R.Beck, G.Caselotti, S.N.Cherepnya, D.Drechsel, L.V.Filkov, K.Fohl, I.Giller, P.Grabmayr, T.Hehl, D.Hornidge, V.L.Kashevarov, M.Kotulla, D.Krambrich, B.Krusche, M.Lang, J.C.McGeorge, I.J.D.MacGregor, V.Metag, M.Moinester, R.Novotny, M.Pfeiffer, M.Rost, S.Schadmand, S.Scherer, A.Thomas, C.Unkmeir, Th.Walcher Measurement of the π+-meson polarizabilities via the γp → γπ+n reaction NUCLEAR REACTIONS 1H(γ, π+γ), E=537-817 MeV; measured Eγ, En, (pion)nγ-coin, σ(θ); deduced pion polarizabilities. Tagged photon beam, comparison with model predictions.
doi: 10.1140/epja/i2004-10056-2
2005GI11 Eur.Phys.J. A 25, 229 (2005) I.Giller, A.Ocherashvili, T.Ebertshauser, M.A.Moinester, S.Scherer A new determination of the γπ → ππ anomalous amplitude via π-e- → π-e-π0 data
doi: 10.1140/epja/i2005-10116-1
2005HA62 Phys.Rev. C 72, 055203 (2005) C.Hacker, N.Wies, J.Gegelia, S.Scherer Including the Δ(1232) resonance in baryon chiral perturbation theory
doi: 10.1103/PhysRevC.72.055203
2005LE03 J.Phys.(London) G31, 89 (2005) B.C.Lehnhart, J.Gegelia, S.Scherer Baryon masses and nucleon sigma terms in manifestly Lorentz-invariant baryon chiral perturbation theory
doi: 10.1088/0954-3899/31/2/002
2005SC07 J.Phys.(London) G31, S1199 (2005) Exotic hadrons from dynamical clustering of quarks in ultrarelativistic heavy ion collisions NUCLEAR REACTIONS Pb(Pb, X), E=30-160 GeV/nucleon; calculated quark cluster rapidity distributions, pentaquark yields. Dynamical quark molecular dynamics model.
doi: 10.1088/0954-3899/31/6/087
2005SC23 Eur.Phys.J. A 26, 1 (2005) M.R.Schindler, J.Gegelia, S.Scherer Electromagnetic form factors of the nucleon in chiral perturbation theory including vector mesons NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors. Lorentz-invariant chiral perturbation theory with vector mesons.
doi: 10.1140/epja/i2005-10145-8
2004FU03 Eur.Phys.J. A 19, Supplement 1, 35 (2004) Structure of the nucleon in chiral perturbation theory NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors, renormalization. Baryon chiral perturbation theory.
doi: 10.1140/epjad/s2004-03-006-0
2004FU23 J.Phys.(London) G30, 1407 (2004) Electromagnetic form factors of the nucleon in chiral perturbation theory NUCLEAR STRUCTURE 1n, 1H; calculated electromagnetic form factors. Chiral perturbation theory.
doi: 10.1088/0954-3899/30/10/008
2004SC13 Phys.Lett. B 586, 258 (2004) M.R.Schindler, J.Gegelia, S.Scherer Infrared regularization of baryon chiral perturbation theory reformulated
doi: 10.1016/j.physletb.2004.02.056
2003FU15 Phys.Rev. C 68, 055501 (2003) Pion electroproduction, partially conserved axial-vector current, chiral Ward identities, and the axial form factor revisited
doi: 10.1103/PhysRevC.68.055501
2002KO20 Phys.Rev. C65, 045202 (2002) J.H.Koch, V.Pascalutsa, S.Scherer Hadron Structure in the Description of Electromagnetic Reactions
doi: 10.1103/PhysRevC.65.045202
2002UN01 Phys.Rev. C65, 015206 (2002) C.Unkmeir, A.Ocherashvili, T.Fuchs, M.A.Moinester, S.Scherer Pion Generalized Dipole Polarizabilities by Virtual Compton Scattering πe → πeγ
doi: 10.1103/PhysRevC.65.015206
2001LV01 Phys.Rev. C64, 015203 (2001) A.I.Lvov, S.Scherer, B.Pasquini, C.Unkmeir, D.Drechsel Generalized Dipole Polarizabilities and the Spatial Structure of Hadrons
doi: 10.1103/PhysRevC.64.015203
2001PA04 Phys.Rev. C63, 025205 (2001) B.Pasquini, S.Scherer, D.Drechsel Generalized Polarizabilities of the Proton in a Constituent Quark Model Revisited NUCLEAR STRUCTURE 1H; calculated generalized polarizabilities for low-energy virtual Compton scattering. Constituent quark model.
doi: 10.1103/PhysRevC.63.025205
2001SC20 Nucl.Phys. A684, 499c (2001) A Simple Model Illustrating the Impossibility of Measuring Off-Shell Effects
doi: 10.1016/S0375-9474(01)00476-6
2001ZS03 Acta Phys.Hung.N.S. 14, 425 (2001) D.Zschiesche, S.Bass, M.Bleicher, J.Brachmann, L.Gerland, K.Paech, S.Scherer, S.Soff, C.Spieles, H.Weber, H.Stocker, W.Greiner Current Status of Quark-Gluon Plasma Signals
doi: 10.1556/APH.14.2001.1-4.40
2000FE12 Phys.Rev. C62, 034003 (2000) Field Transformations and Simple Models Illustrating the Impossibility of Measuring Off-Shell Effects
doi: 10.1103/PhysRevC.62.034003
2000HO08 Phys.Lett. 478B, 161 (2000) M.Hofmann, M.Bleicher, S.Scherer, L.Neise, H.Stocker, W.Greiner Statistical Mechanics of Colored Objects
doi: 10.1016/S0370-2693(00)00257-4
1999SC23 Prog.Part.Nucl.Phys. 42, 279 (1999) S.Scherer, S.A.Bass, M.Bleicher, M.Belkacem, L.Bravina, J.Brachmann, A.Dumitru, C.Ernst, L.Gerland, M.Hofmann, L.Neise, M.Reiter, S.Soff, C.Spieles, H.Weber, E.Zabrodin, D.Zschiesche, J.A.Maruhn, H.Stocker, W.Greiner Critical Review of Quark Gluon Plasma Signatures
doi: 10.1016/S0146-6410(99)00083-6
1999SC31 Czech.J.Phys. 49, 1307 (1999) Real and Virtual Compton Scattering at Low Energies
doi: 10.1023/A:1022872211333
1998DR01 Phys.Rev. C57, 941 (1998) D.Drechsel, G.Knochlein, A.Yu.Korchin, A.Metz, S.Scherer Structure Analysis of the Virtual Compton Scattering Amplitude at Low Energies
doi: 10.1103/PhysRevC.57.941
1998DR08 Phys.Rev. C58, 1751 (1998) D.Drechsel, G.Knochlein, A.Yu.Korchin, A.Metz, S.Scherer Low-Energy and Low-Momentum Representation of the Virtual Compton Scattering Amplitude
doi: 10.1103/PhysRevC.58.1751
1998FE02 Nucl.Phys. A631, 735c (1998) H.W.Fearing, R.Lewis, N.Mobed, S.Scherer Radiative and Non Radiative Muon Capture on the Proton in Heavy Baryon Chiral Perturbation Theory
doi: 10.1016/S0375-9474(98)00101-8
1998HE10 Nucl.Phys. A631, 607c (1998) T.R.Hemmert, B.R.Holstein, G.Knochlein, S.Scherer Generalized Polarizabilities and the Chiral Structure of the Nucleon
doi: 10.1016/S0375-9474(98)00076-1
1998LV01 Phys.Rev. C57, 312 (1998) A.I.Lvov, S.Scopetta, D.Drechsel, S.Scherer Polarization Phenomena in Small-Angle Photoproduction of e+e- Pairs and the Gerasimov-Drell-Hearn Sum Rule NUCLEAR REACTIONS 1H(polarized γ, e-e+), E < 1.2 GeV; calculated σ, asymmetries; deduced sum rule test.
doi: 10.1103/PhysRevC.57.312
1997DR01 Phys.Rev. C55, 424 (1997) D.Drechsel, G.Knochlein, A.Metz, S.Scherer Generalized Polarizabilities and the Spin-Averaged Amplitude in Virtual Compton Scattering Off the Nucleon
doi: 10.1103/PhysRevC.55.424
1997FE10 Phys.Rev. D56, 1783 (1997) H.W.Fearing, R.Lewis, N.Mobed, S.Scherer Muon Capture by a Proton in Heavy Baryon Chiral Perturbation Theory NUCLEAR REACTIONS 1H(μ-, n), E not given; calculated form factors. Chiral Perturbation Theory, Ecker-Mojzis Lagrangian.
doi: 10.1103/PhysRevD.56.1783
1997HE13 Phys.Rev.Lett. 79, 22 (1997) T.R.Hemmert, B.R.Holstein, G.Knochlein, S.Scherer Generalized Polarizabilities and the Chiral Structure of the Nucleon NUCLEAR STRUCTURE 1H; calculated generalized polarizabilities. Chiral perturbation theory. NUCLEAR REACTIONS 1H(e, e'), E not given; calculated response function. Chiral perturbation theory based proton generalized polarizabilities.
doi: 10.1103/PhysRevLett.79.22
1997SC28 Nucl.Phys. A623, 215c (1997) Chiral Dynamics of Rare η Decays and Virtual Compton Scattering Off the Nucleon
doi: 10.1016/S0375-9474(97)00440-5
1996SC15 Phys.Rev. C54, 904 (1996) S.Scherer, A.Yu.Korchin, J.H.Koch Virtual Compton Scattering Off the Nucleon at Low Energies
doi: 10.1103/PhysRevC.54.904
1995SC01 Phys.Rev. C51, 359 (1995) Compton Scattering by a Pion and Off-Shell Effects
doi: 10.1103/PhysRevC.51.359
1994FE07 Nucl.Phys. A570, 657 (1994) H.W.Fearing, G.I.Poulis, S.Scherer Effective Hamiltonians with Relativistic Corrections: The Foldy-Wouthuysen transformation versus the direct Pauli reduction NUCLEAR REACTIONS 1H(polarized p, γ), E=280 MeV; calculated σ(θp3, θp4, θγ), analyzing power vs θγ. Effective hamiltonians, relativistic corrections.
doi: 10.1016/0375-9474(94)90078-7
1994RU06 Phys.Rev. C50, 447 (1994) T.E.Rudy, H.W.Fearing, S.Scherer Off-Shell Electromagnetic Form Factors of Pions and Kaons in Chiral Perturbation Theory
doi: 10.1103/PhysRevC.50.447
1994SC09 Nucl.Phys. A570, 686 (1994) S.Scherer, G.I.Poulis, H.W.Fearing Low-Energy Compton Scattering by a Proton: Comparison of effective hamiltonians with relativistic corrections
doi: 10.1016/0375-9474(94)90079-5
1992BO27 Nucl.Phys. A547, 488 (1992) Hadron Structure and Gauge Invariance in Photo- and Electroproduction of Pions NUCLEAR REACTIONS 1H(γ, π0), E not given; calculated photoproduction σ(θ).
doi: 10.1016/0375-9474(92)90035-I
1991SC11 Nucl.Phys. A526, 733 (1991) Pion Photoproduction in the Skyrme Model and Low-Energy Theorems NUCLEAR REACTIONS 1H(γ, π+), (γ, π0), 1n(γ, π-), (γ, π0), E not given; calculated electric dipole pion photoproduction amplitude. Skyrme model.
doi: 10.1016/0375-9474(91)90441-8
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