NSR Query Results
Output year order : Descending NSR database version of April 27, 2024. Search: Author = A.Buchmann Found 55 matches. 2014BU11 Few-Body Systems 55, 749 (2014) Three-Quark Currents and Baryon Spin
doi: 10.1007/s00601-014-0864-9
2013BU03 Phys.Rev. C 87, 028203 (2013) Pion couplings of the Δ(1232)
doi: 10.1103/PhysRevC.87.028203
2008BU09 Eur.Phys.J. A 35, 267 (2008) Baryon octupole moments
doi: 10.1140/epja/i2007-10565-4
2007BA46 Phys.Rev. C 75, 065203 (2007); Erratum Phys.Rev. C 77, 019903 (2008) D.Barquilla-Cano, A.J.Buchmann, E.Hernandez Axial N → Δ(1232) and N → N*(1440) transition form factors
doi: 10.1103/PhysRevC.75.065203
2006BA26 Eur.Phys.J. A 27, 365 (2006) D.Barquilla-Cano, A.J.Buchmann, E.Hernandez Axial exchange currents and nucleon spin NUCLEAR STRUCTURE A=1; calculated axial form factors, one- and two-body axial exchange currents. Constituent quark model.
doi: 10.1140/epja/i2005-10270-4
2005BU30 Can.J.Phys. 83, 455 (2005) Nucleon deformation and atomic spectroscopy NUCLEAR MOMENTS 1n, 1H; analyzed data; deduced quadrupole moments.
doi: 10.1139/P05-009
2004BU23 Phys.Rev.Lett. 93, 212301 (2004) Electromagnetic N → Δ Transition and Neutron Form Factors NUCLEAR REACTIONS 1n, 1H(e, e'X), E not given; analyzed Δ-resonance production form factors.
doi: 10.1103/PhysRevLett.93.212301
2003BA11 Nucl.Phys. A714, 611 (2003) D.Barquilla-Cano, A.J.Buchmann, E.Hernandez Partial conservation of the axial current and axial exchange currents in the nucleon
doi: 10.1016/S0375-9474(02)01389-1
2003BA94 Nucl.Phys. A721, 429c (2003) D.Barquilla-Cano, A.J.Buchmann, E.Hernandez Axial exchange currents and the spin content of the nucleon in a nonrelativistic chiral quark model NUCLEAR STRUCTURE 1n, 1H; calculated axial form factors. Nonrelativistic chiral quark model.
doi: 10.1016/S0375-9474(03)01089-3
2002BU26 Phys.Rev. D66, 056002 (2002) A.J.Buchmann, J.A.Hester, R.F.Lebed Quadrupole moments of N and Δ in the 1/Nc expansion
doi: 10.1103/PhysRevD.66.056002
2001BU03 Phys.Rev. C63, 015202 (2001) Intrinsic Quadrupole Moment of the Nucleon NUCLEAR STRUCTURE 1H; calculated intrinsic quadrupole moment for proton, Δ resonance; deduced deformation.
doi: 10.1103/PhysRevC.63.015202
2001GR08 Phys.Rev.Lett. 86, 2237 (2001) Moments of the Neutron Charge Form Factor and the N → Δ Quadrupole Transition NUCLEAR STRUCTURE 1n; analyzed form factor data; deduced N to Δ quadrupole transition features.
doi: 10.1103/PhysRevLett.86.2237
2001ME21 Phys.Rev. C64, 035203 (2001) U.Meyer, E.Hernandez, A.J.Buchmann Exchange Currents in Nucleon Electroexcitation NUCLEAR REACTIONS 1n, 1H(γ, X), E not given; calculated scalar and transverse helicity amplitudes for resonance excitation vs momentum transfer.
doi: 10.1103/PhysRevC.64.035203
2001SH05 Phys.Rev. C63, 025212 (2001) K.Shimizu, Y.B.Dong, A.Faessler, A.J.Buchmann Relativistic Description of Constituent Quarks
doi: 10.1103/PhysRevC.63.025212
2000BU12 Nucl.Phys. A670, 174c (2000) Relations between Electromagnetic Form Factors of Baryons
doi: 10.1016/S0375-9474(00)00090-7
2000SH27 Prog.Theor.Phys.(Kyoto), Suppl. 137, 43 (2000) K.Shimizu, S.Takeuchi, A.J.Buchmann Study of Nucleon-Nucleon and Hyperon-Nucleon Interaction
doi: 10.1143/PTPS.137.43
2000WA05 J.Phys.(London) G26, 267 (2000) G.Wagner, A.J.Buchmann, A.Faessler Electromagnetic Properties of Decuplet Hyperons in a Chiral Quark Model with Exchange Currents
doi: 10.1088/0954-3899/26/3/306
1999DO10 J.Phys.(London) G25, 1115 (1999) Y.B.Dong, K.Shimizu, A.Faessler, A.J.Buchmann Spin Content of the Nucleon in a Relativistic Quark Model NUCLEAR STRUCTURE 1n, 1H; calculated wavefunction pion admixtures, nucleon spin content related features. Relativistic quark model, comparison with chiral quark model.
doi: 10.1088/0954-3899/25/6/301
1999DO23 Phys.Rev. C60, 035203 (1999) Y.B.Dong, K.Shimizu, A.Faessler, A.J.Buchmann Description of the Electroproduction Amplitudes of the Roper Resonance in a Relativistic Quark Model NUCLEAR REACTIONS 1n, 1H(γ, X), E not given; calculated Roper resonance production amplitudes; deduced relativistic, meson cloud effects. Relativistic quark model.
doi: 10.1103/PhysRevC.60.035203
1999FA09 Yad.Fiz. 62, No 7, 1198 (1999); Phys.Atomic Nuclei 62, 1125 (1999) A.Faessler, A.Buchmann, U.Meyer, A.Valcarce, F.Fernandez, E.Hernandez Deformation of the Nucleon and Nucleon-Nucleon Interaction in the Quark Model
1999MA04 Nucl.Phys. A646, 231 (1999); Erratum Nucl.Phys. A686, 601 (2001) A.I.Machavariani, A.Faessler, A.J.Buchmann Field-Theoretical Description of Electromagnetic Δ Resonance Production and Determination of the Magnetic Moment of the Δ+(1232) Resonance by the ep → e'N'π'γ' and γp → N'π'γ' Reactions NUCLEAR REACTIONS 1H(e, e'π0γ), (γ, γ'π0), E ≈ resonance; calculated σ(Eγ, θ(1), θ(2)); deduced dependence on Δ+ magnetic dipole moment.
doi: 10.1016/S0375-9474(98)00611-3
1999OB02 Phys.Rev. C60, 035207 (1999) I.T.Obukhovsky, A.Faessler, G.Wagner, A.J.Buchmann πNN Decay of a Possible d' Dibaryon in the 3P0 Quark Pair Creation Model
doi: 10.1103/PhysRevC.60.035207
1998BU09 Phys.Rev. C57, 3340 (1998) A.J.Buchmann, G.Wagner, A.Faessler d' Dibaryon in a Colored Cluster Model
doi: 10.1103/PhysRevC.57.3340
1998BU20 Phys.Rev. C58, 2478 (1998) A.J.Buchmann, E.Hernandez, U.Meyer, A.Faessler N → Δ(1232) E2 Transition and Siegert's Theorem
doi: 10.1103/PhysRevC.58.2478
1998BU25 Nucl.Phys. A642, 102c (1998) d' Dibaryon in a Colored Cluster Model and Dibaryon Condensation
doi: 10.1016/S0375-9474(98)00505-3
1998FA01 Phys.Rev. C57, 1458 (1998) A.Faessler, A.J.Buchmann, M.I.Krivoruchenko Nuclear Matter with a Bose Condensate of Dibaryons in a Relativistic Hartree Approximation
doi: 10.1103/PhysRevC.57.1458
1998FA06 J.Phys.(London) G24, 791 (1998) A.Faessler, A.J.Buchmann, M.I.Krivoruchenko, B.V.Martemyanov Dibaryons in Nuclear Matter
doi: 10.1088/0954-3899/24/4/011
1998KU03 Phys.Rev. C57, 535 (1998) V.I.Kukulin, V.N.Pomerantsev, A.Faessler, A.J.Buchmann, E.M.Tursunov Moscow-Type NN Potentials and Three-Nucleon Bound States NUCLEAR STRUCTURE 3H, 3He; calculated binding energies, Coulomb displacement energies, charge radii. Moscow potentials. Comparison with experiment.
doi: 10.1103/PhysRevC.57.535
1998WA24 Phys.Rev. C58, 1745 (1998) G.Wagner, A.J.Buchmann, A.Faessler Radiative Decays of Decuplet Hyperons
doi: 10.1103/PhysRevC.58.1745
1998WA32 Phys.Rev. C58, 3666 (1998) G.Wagner, A.J.Buchmann, A.Faessler Exchange Currents in Octet Hyperon Charge Radii
doi: 10.1103/PhysRevC.58.3666
1997BU01 Phys.Rev. C55, 448 (1997) A.J.Buchmann, E.Hernandez, A.Faessler Electromagnetic Properties of the Δ(1232) NUCLEAR STRUCTURE 1n, 1H; calculated magnetic radii. Nonrelativistic quark model, two-body exchange currents.
doi: 10.1103/PhysRevC.55.448
1997FA03 Phys.Lett. 391B, 255 (1997) A.Faessler, A.J.Buchmann, M.I.Krivoruchenko, B.V.Martemyanov Nuclear Matter with a Bose Condensate of Dibaryons in Relativistic Mean-Field Theory
doi: 10.1016/S0370-2693(96)01482-7
1997FA13 Phys.Rev. C56, 1576 (1997) A.Faessler, A.J.Buchmann, M.I.Krivoruchenko Constraints on the ω- and σ-Meson Coupling Constants with Dibaryons
doi: 10.1103/PhysRevC.56.1576
1997MA41 Ann.Phys.(New York) 253, 332 (1997) A.I.Machavariani, A.J.Buchmann, A.Faessler, G.A.Emelyanenko Three-Dimensional Field-Theoretical Construction of the Nucleon-Nucleon Potential from Quark Degrees of Freedom
doi: 10.1006/aphy.1996.5629
1997ME15 Phys.Lett. 408B, 19 (1997) U.Meyer, A.J.Buchmann, A.Faessler Exchange Currents in Photoproduction of Baryon Resonances
doi: 10.1016/S0370-2693(97)00840-X
1997OB01 Phys.Rev. C56, 3295 (1997) I.T.Obukhovsky, K.Itonaga, G.Wagner, A.J.Buchmann, A.Faessler Pionic Decay of a Possible d' Dibaryon and the Short-Range NN Interaction
doi: 10.1103/PhysRevC.56.3295
1997SA59 Nucl.Phys. A625, 192 (1997) T.Sakai, J.Mori, A.J.Buchmann, K.Shimizu, K.Yazaki The Interaction between H-Dibaryons
doi: 10.1016/S0375-9474(97)00492-2
1996BU52 Few-Body Systems 21, 149 (1996) A.J.Buchmann, H.Henning, P.U.Sauer Meson and Quark Degrees of Freedom and the Radius of the Deuteron NUCLEAR STRUCTURE 2H; analyzed longitudinal structure function, charge radius; deduced meson exchange contributions.
doi: 10.1007/s006010050045
1996EN04 Nucl.Phys. A602, 308 (1996) D.R.Entem, A.I.Machavariani, A.Valcarce, A.J.Buchmann, A.Faessler, F.Fernandez A Chiral Quark Model and the Spin Observables in Nucleon-Nucleon Scattering NUCLEAR REACTIONS 1n, 1H(p, p), E=25-250 MeV; analyzed σ(θ), polarization observables data; deduced sensitivity to phase shifts modifications. Nonrelativistic constituent quark model.
doi: 10.1016/0375-9474(96)00111-X
1996IT01 Nucl.Phys. A609, 422 (1996) K.Itonaga, A.J.Buchmann, G.Wagner, A.Faessler Pionic Decay of a Possible d' Dibaryon
doi: 10.1016/S0375-9474(96)00278-3
1996SZ07 J.Phys.(London) G22, 1741 (1996) A.Szczurek, A.J.Buchmann, A.Faessler On the Flavour Structure of the Constituent Quark
doi: 10.1088/0954-3899/22/12/004
1995VA02 Phys.Rev. C51, 1480 (1995) A.Valcarce, A.Buchmann, F.Fernandez, A.Faessler Spin-Orbit Force in a Quark Model Based Nucleon-Nucleon Potential
doi: 10.1103/PhysRevC.51.1480
1995WA22 Nucl.Phys. A594, 263 (1995) G.Wagner, L.Ya.Glozman, A.J.Buchmann, A.Faessler Constituent Quark Model Calculation for a Possible J(P) = 0-, T = 0 Dibaryon
doi: 10.1016/0375-9474(95)00351-Z
1995WA26 Phys.Lett. 359B, 288 (1995) G.Wagner, A.J.Buchmann, A.Faessler Magnetic Moments of the Octet Baryons in a Chiral Quark Potential Model NUCLEAR STRUCTURE 1H, 1n; calculated two-body current contributions to μ, magnetic radii. Chiral quark potential model.
doi: 10.1016/0370-2693(95)01103-W
1994BU03 Nucl.Phys. A569, 661 (1994) A.Buchmann, E.Hernandez, K.Yazaki Gluon, Pion and Confinement Exchange Currents in the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated μ. Constituent quark model, gluon, pion exchange currents.
doi: 10.1016/0375-9474(94)90379-4
1994GL03 J.Phys.(London) G20, L49 (1994) L.Ya.Glozman, A.Buchmann, A.Faessler Constituent Quark Model and a Possible J(p) = 0-, T = 0 Dibaryon
doi: 10.1088/0954-3899/20/5/001
1994VA22 Phys.Rev. C50, 2246 (1994) A.Valcarce, A.Buchmann, F.Fernandez, A.Faessler Can One Simultaneously Describe the Deuteron Properties and the Nucleon-Nucleon Phase Shifts in the Quark Cluster Model ( Question ) NUCLEAR STRUCTURE 2H; calculated structure function, D-state observables, wave function. Quark cluster model.
doi: 10.1103/PhysRevC.50.2246
1993FA14 Int.J.Mod.Phys. E2, 39 (1993) A.Faessler, A.Buchmann, Y.Yamauchi The Quark Model, Deuteron Form Factors and Nuclear Magnetic Moments NUCLEAR STRUCTURE 2H; calculated various form factors, structure functions. 15N, 17O, 39K; calculated quark exchange contributions to magnetic moment, magnetic form factors. Quark cluster model.
doi: 10.1142/S0218301393000030
1991BU11 Phys.Lett. 269B, 35 (1991) A.Buchmann, E.Hernandez, K.Yazaki Gluon and Pion Exchange Currents in the Nucleon NUCLEAR STRUCTURE 1n, 1H; calculated proton, neutron charge form factor. Constituent quark model, gluon, pion exchange currents.
doi: 10.1016/0370-2693(91)91448-5
1991YA03 Nucl.Phys. A526, 495 (1991) Y.Yamauchi, A.Buchmann, A.Faessler, A.Arima Quark Exchange Currents in Nuclei Effective Operator Description NUCLEAR STRUCTURE 15N, 17O, 39K; calculated μ, elastic magnetic form factors; deduced quark exchange currents role. Quark cluster model.
doi: 10.1016/0375-9474(91)90431-5
1989BU11 Nucl.Phys. A496, 621 (1989) A.Buchmann, Y.Yamauchi, A.Faessler The Electromagnetic Form Factors of the Deuteron in the Quark Cluster Model NUCLEAR STRUCTURE 2H; calculated charge monopole, quadrupole, magnetic dipole form factors. Quark cluster model.
doi: 10.1016/0375-9474(89)90116-4
1989BU13 Phys.Lett. 225B, 301 (1989) A.Buchmann, Y.Yamauchi, A.Faessler The One-Gluon Exchange Current in the Quark Cluster Model of the Deuteron NUCLEAR STRUCTURE 2H; calculated magnetic form factor, M1 transition matrix element.
doi: 10.1016/0370-2693(89)90572-8
1989YA04 Nucl.Phys. A494, 401 (1989) Y.Yamauchi, A.Buchmann, A.Faessler Deuteron Threshold Electrodisintegration in a Microscopic Meson-Quark Cluster Model NUCLEAR REACTIONS 2H(e, e'n), E not given; calculated electrodisintegration σ(θ(e'), E(e')). Microscopic meson-quark cluster model.
doi: 10.1016/0375-9474(89)90184-X
1988BU10 J.Phys.(London) G14, 1037 (1988) A.Buchmann, Y.Yamauchi, H.Ito, A.Faessler The Pion Pair Current in the Quark Cluster Model NUCLEAR STRUCTURE 2H; calculated form factors, structure functions.
doi: 10.1088/0305-4616/14/8/007
1985BU17 Nucl.Phys. A443, 726 (1985) A.Buchmann, W.Leidemann, H.Arenhovel A Gauge-Invariant Exchange Current for the Paris Potential NUCLEAR REACTIONS 2H(γ, p), (polarized γ, p), (γ, n), E=100, 140 MeV; calculated σ(θ), γ-asymmetry, neutron polarization vs θ. 2H(e, e'), E not given; calculated breakup σ(θ, E(e')). Gauge invariant exchange current model.
doi: 10.1016/0375-9474(85)90221-0
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