NSR Query Results
Output year order : Descending NSR database version of May 6, 2024. Search: Author = K.Goeke Found 125 matches. Showing 1 to 100. [Next]2009GO10 Phys.Rev. C 79, 035210 (2009) Leading twist nuclear shadowing, nuclear generalized parton distributions, and nuclear deeply virtual Compton scattering at small x
doi: 10.1103/PhysRevC.79.035210
2008GO13 Eur.Phys.J. A 36, 49 (2008) Deeply Virtual Compton Scattering on nucleons and nuclei in the Generalized Vector Meson Dominance model
doi: 10.1140/epja/i2008-10549-x
2008LE22 Nucl.Phys. A811, 353 (2008) Vector transition form factors of the NK* → Θ+ and N(K-bar)* → Σ*-10-bar in the SU(3) chiral quark-solition model
doi: 10.1016/j.nuclphysa.2008.08.002
2007CE05 Nucl.Phys. A794, 87 (2007) C.Cebulla, K.Goeke, J.Ossmann, P.Schweitzer The nucleon form-factors of the energy-momentum tensor in the Skyrme model
doi: 10.1016/j.nuclphysa.2007.08.004
2007GO17 Phys.Rev. C 75, 055207 (2007) K.Goeke, J.Grabis, J.Ossmann, P.Schweitzer, A.Silva, D.Urbano Pion mass dependence of the nucleon form factors of the energy-momentum tensor in the chiral quark-soliton model
doi: 10.1103/PhysRevC.75.055207
2007GO33 Eur.Phys.J. A 32, 393 (2007) K.Goeke, H.-C.Kim, A.Silva, D.Urbano Strange nucleon form factors: Solitonic approach GsM, GsE, (G-∼)pA and (G-∼)nA and comparison with world data
doi: 10.1140/epja/i2006-10398-7
2006CO10 Phys.Rev. D 73, 094023 (2006) J.C.Collins, A.V.Efremov, K.Goeke, M.Grosse Perdekamp, S.Menzel, B.Meredith, A.Metz, P.Schweitzer Sivers effect in the Drell-Yan process at BNL RHIC NUCLEAR REACTIONS 1H(polarized p, X), E(cm)=200 GeV; calculated single-spin asymmetries in lepton pair production.
doi: 10.1103/PhysRevD.73.094023
2006GO09 Eur.Phys.J. A 27, 77 (2006) K.Goeke, J.Ossmann, P.Schweitzer, A.Silva Pion mass dependence of the nucleon mass in the chiral quark soliton model
doi: 10.1140/epja/i2005-10229-5
2006SI29 Phys.Rev. D 74, 054011 (2006) A.Silva, H.-C.Kim, D.Urbano, K.Goeke Parity-violating asymmetries in elastic (e(pol)p) scattering in the chiral quark-soliton model: Comparison with the A4, G0, HAPPEX and SAMPLE experiments NUCLEAR REACTIONS 1H(polarized e, e), E=high; analyzed parity-violating asymmetries. Chiral quark-soliton model.
doi: 10.1103/PhysRevD.74.054011
2005AZ10 Eur.Phys.J. A 26, 79 (2005) Ya.I.Azimov, R.A.Arndt, I.I.Strakovsky, R.L.Workman, K.Goeke Search for higher flavor multiplets in partial-wave analyses
doi: 10.1140/epja/i2005-10150-y
2005EF01 Phys.Lett. B 612, 233 (2005) A.V.Efremov, K.Goeke, S.Menzel, A.Metz, P.Schweitzer Sivers effect in semi-inclusive DIS and in the Drell-Yan process
doi: 10.1016/j.physletb.2005.03.010
2005KI12 Nucl.Phys. A755, 419c (2005) H.-Ch.Kim, Gh.-S.Yang, M.Praszalowicz, K.Goeke Magnetic moments of exotic pentaquark baryons
doi: 10.1016/j.nuclphysa.2005.03.133
2005SI04 Eur.Phys.J. A 24, Supplement 2, 93 (2005) A.Silva, D.Urbano, H.-C.Kim, K.Goeke Strange form factors of the nucleon in the chiral quark-soliton model NUCLEAR STRUCTURE 1n, 1H; calculated strange form factors. Chiral quark-soliton model.
doi: 10.1140/epjad/s2005-04-020-4
2005SI18 Nucl.Phys. A755, 290c (2005) Baryon form factors in the chiral quark-soliton model NUCLEAR MOMENTS 1n, 1H; calculated radii, μ, form factors. Chiral quark-soliton model.
doi: 10.1016/j.nuclphysa.2005.03.030
2004AZ03 Eur.Phys.J. A 21, 501 (2004) Decay properties of new D-mesons
doi: 10.1140/epja/i2004-10010-4
2004EF02 Eur.Phys.J. C 35, 207 (2004) A.V.Efremov, K.Goeke, P.Schweitzer Transversity distribution function in hard scattering of polarized protons and antiprotons in the PAX experiment NUCLEAR REACTIONS 1H(polarized p-bar, X), E ≈ 15-25 GeV; calculated lepton pair production double spin asymmetry.
doi: 10.1140/epjc/s2004-01854-9
2004SI31 Eur.Phys.J. A 22, 481 (2004) Strange and singlet form factors of the nucleon: Predictions for G0, A4, and HAPPEX II experiments NUCLEAR STRUCTURE 1n, 1H; calculated electric and magnetic form factors. SU(3) chiral quark-soliton model.
doi: 10.1140/epja/i2003-10240-x
2003EF01 Phys.Lett. B 568, 63 (2003) A.V.Efremov, K.Goeke, P.Schweitzer Sivers vs. Collins effect in azimuthal single spin asymmetries in pion production in SIDIS NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated pion production associated spin asymmetries from polarized targets; deduced relative influence of Sivers and Collins effects.
doi: 10.1016/j.physletb.2003.06.016
2003GO14 Phys.Lett. B 567, 27 (2003) K.Goeke, A.Metz, P.V.Pobylitsa, M.V.Polyakov Lorentz invariance relations among parton distributions revisited
doi: 10.1016/S0370-2693(03)00870-0
2003SI18 Nucl.Phys. A721, 417c (2003) Strange vector form factors in the context of the SAMPLE, A4, HAPPEX and G0 experiments NUCLEAR STRUCTURE 1n, 1H; analyzed strange form factors, related data.
doi: 10.1016/S0375-9474(03)01086-8
2002EF01 Eur.Phys.J. C 24, 407 (2002) A.V.Efremov, K.Goeke, P.Schweitzer Predictions for Azimuthal Asymmetries in Pion and Kaon Production in SIDIS Off a Longitudinally Polarized Deuterium Target at HERMES NUCLEAR REACTIONS 2H(e, X), E=high; calculated pion and kaon production azimuthal asymmetries. Polarized target, Collins fragmentation function.
doi: 10.1007/s100520200918
2002EF03 Nucl.Phys. A711, 84c (2002) A.V.Efremov, K.Goeke, P.Schweitzer Azimuthal asymmetries in SIDIS and Collins analysing power NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated pion production associated azimuthal asymmetries, analyzing powers. Comparison with data.
doi: 10.1016/S0375-9474(02)01199-5
2002EF04 Acta Phys.Pol. B33, 3755 (2002) A.V.Efremov, K.Goeke, P.Schweitzer Azimuthal Asymmetries and Collins Analyzing Power NUCLEAR REACTIONS 1,2H(e, e'X), (e+, e+'X), E=high; analyzed pion production associated azimuthal asymmetries, Collins fragmentation function, twist-3 distribution. Polarized targets.
2002FR03 Nucl.Phys. A699, 541 (2002) ΔS = 1, 2 Effective Weak Chiral Lagrangian from the Instanton Vacuum
doi: 10.1016/S0375-9474(01)01275-1
2001EF05 Phys.Lett. 522B, 37 (2001); Erratum Phys.Lett. 544B, 389 (2002) A.V.Efremov, K.Goeke, P.Schweitzer Azimuthal Asymmetry in Electro-Production of Neutral Pions in Semi-Inclusive DIS NUCLEAR REACTIONS 1H(e+, π+X), (e+, π0X), (e+, π-X), E not given; analyzed azimuthal asymmetry data; deduced proton transversivity distribution features. Polarized target.
doi: 10.1016/S0370-2693(01)01258-8
2001GO03 Nucl.Phys. A680, 308c (2001) K.Goeke, P.V.Pobylitsa, M.V.Polyakov, D.Urbano Polarized Antiquark Distributions from the Chiral Quark Soliton Model: Results and parametrization for Δ(u-bar)(x), Δ(d-bar)(x) and Δ(s-bar)(x)
doi: 10.1016/S0375-9474(00)00434-6
2001KI32 Nucl.Phys. A691, 403c (2001) H.-C.Kim, M.Praszalowicz, K.Goeke Hyperon Semileptonic Decay Constants and Quark-Spin Content of the Octet Baryons
doi: 10.1016/S0375-9474(01)01065-X
2001LE45 J.Phys.(London) G27, L127 (2001) N.-Y.Lee, P.V.Pobylitsa, M.V.Polyakov, K.Goeke Meson Twist-4 Parton Distributions in Terms of Twist-2 Distribution Amplitudes at Large Nc
doi: 10.1088/0954-3899/27/12/101
2001SC34 Phys.Rev. D64, 034013 (2001) P.Schweitzer, M.V.Polyakov, C.Weiss, P.V.Pobylitsa, K.Goeke Transversity Distributions in the Nucleon in the Large-Nc Limit NUCLEAR STRUCTURE 1n, 1H; calculated quark transversivity distributions. NUCLEAR REACTIONS 1H(polarized p, X), (polarized p-bar, X), E(cm)=40, 200 GeV; calculated transverse spin asymmetry.
doi: 10.1103/PhysRevD.64.034013
2000DR08 Prog.Part.Nucl.Phys. 44, 293 (2000) B.Dressler, K.Goeke, P.Schweitzer, C.Weiss, M.V.Polyakov Can We Measure Δ(u-bar)(x) - Δ(d-bar)(x) in Semi-Inclusive eN or NN Scattering ?
doi: 10.1016/S0146-6410(00)00078-8
2000DR18 Eur.Phys.J. C 14, 147 (2000) B.Dressler, K.Goeke, M.V.Polyakov, C.Weiss Flavor Asymmetry of Polarized Antiquark Distributions and Semi-Inclusive DIS NUCLEAR REACTIONS 1H(e, e'X), E=high; calculated pion, kaon spin asymmetries, contributions from flavor asymmetries.
doi: 10.1007/s100520050741
2000EF01 Phys.Lett. 478B, 94 (2000) A.V.Efremov, K.Goeke, M.V.Polyakov, D.Urbano Azimuthal Asymmetries in Deep Inelastic Scattering NUCLEAR REACTIONS 1H(e, e'π+X), (e, e'π-X), E not given; calculated pion azimuthal asymmetries; deduced proton transversity distribution. Effective chiral quark soliton model, comparison with data.
doi: 10.1016/S0370-2693(00)00296-3
2000FR09 Nucl.Phys. A663-664, 995c (2000) Effective Weak Chiral Lagrangian from the Instanton Vacuum
doi: 10.1016/S0375-9474(99)00752-6
2000GO10 Nucl.Phys. A666-667, 18c (2000) The Instanton Based Chiral Quark Soliton Model: Form factors and (skewed) parton distributions
doi: 10.1016/S0375-9474(00)00003-8
2000KI12 Phys.Rev. D61, 114006 (2000) H.-C.Kim, M.Praszalowicz, K.Goeke Hyperon Semileptonic Decays and Quark Spin Content of the Proton NUCLEAR STRUCTURE 1H, 1n; analyzed spin structure, hyperon semileptonic decays. 1H deduced quark content of spin. Chiral-quark soliton model calculations.
doi: 10.1103/PhysRevD.61.114006
2000PO24 Eur.Phys.J. A 9, 115 (2000) M.V.Polyakov, A.Sibirtsev, K.Tsushima, W.Cassing, K.Goeke On the Search for a Narrow Penta-quark Z+-baryon in NN Interactions NUCLEAR REACTIONS 1H(p, X), E=threshold+100, 200 MeV; calculated neutron-kaon invariant mass spectra; deduced possiblilty of penta-quark Z+-baryon detection.
doi: 10.1007/s100500070061
2000SI25 Nucl.Phys. A675, 637 (2000) A.Silva, D.Urbano, T.Watabe, M.Fiolhais, K.Goeke The Electroproduction of the Δ(1232) in the Chiral Quark-Soliton Model
doi: 10.1016/S0375-9474(00)00195-0
2000UR03 Prog.Part.Nucl.Phys. 44, 211 (2000) D.Urbano, A.Silva, M.Fiolhais, T.Watabe, K.Goeke E2/M1 and C2/M1 for the Electroproduction of the Δ(1232) in the Chiral Quark-Soliton Model NUCLEAR REACTIONS 1H(e, X), E not given; calculated Δ resonance production amplitudes.
doi: 10.1016/S0146-6410(00)00072-7
1999BA16 Phys.Rev. D59, 056005 (1999) Electric Dipole Moment of the Neutron in the Chiral Quark Soliton Model NUCLEAR STRUCTURE 1n; calculated electric dipole moment.
doi: 10.1103/PhysRevD.59.056005
1999PO01 Phys.Rev. D59, 034024 (1999) P.V.Pobylitsa, M.V.Polyakov, K.Goeke, T.Watabe, C.Weiss Isovector Unpolarized Quark Distribution in the Nucleon in the Large-Nc Limit NUCLEAR STRUCTURE 1n, 1H; calculated quark distributions. Effective chiral theory.
doi: 10.1103/PhysRevD.59.034024
1999PR02 Nucl.Phys. A647, 49 (1999) M.Praszalowicz, T.Watabe, K.Goeke Quantization Ambiguities of the SU(3) Soliton NUCLEAR STRUCTURE 1n, 1H; calculated electric, magnetic form factors. Chiral quark soliton model, SU(2), SU(3) versions. Comparison with data.
doi: 10.1016/S0375-9474(99)00008-1
1998BR32 Phys.Lett. 438B, 242 (1998) W.Broniowski, M.Polyakov, H.-C.Kim, K.Goeke Tensor Susceptibilities of the Vacuum from Constituent Quarks
doi: 10.1016/S0370-2693(98)01048-X
1998WA04 Nucl.Phys. A629, 152c (1998) Nucleon Described by the Chiral Soliton in the Chiral Quark Soliton Model NUCLEAR STRUCTURE 1n, 1H; analyzed form factor data; deduced quark structure features. Chiral quark soliton model.
doi: 10.1016/S0375-9474(97)00679-9
1997KI05 Nucl.Phys. A616, 606 (1997) Strange Vector Form Factors of the Nucleon in the SU(3) Chiral Quark-Soliton Model with the Proper Kaon Cloud
doi: 10.1016/S0375-9474(96)00486-1
1997KI26 Phys.Rev. D55, 5698 (1997) H.-C.Kim, M.V.Polyakov, K.Goeke Weak Electricity of the Nucleon in the Chiral Quark-Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated pseudotensor constant. Chiral Quark-Soliton model.
doi: 10.1103/PhysRevD.55.5698
1996BL17 Phys.Rev. D53, 485 (1996) A.Blotz, M.Praszalowicz, K.Goeke Axial-Vector Properties of the Nucleon with 1/N(c) Corrections in the Solitonic SU(3)-NJL Model
doi: 10.1103/PhysRevD.53.485
1996BR17 Z.Phys. A354, 421 (1996) W.Broniowski, G.Ripka, E.N.Nikolov, K.Goeke Analytic Structure of Meson Propagators in the Proper-Time Regularized Nambu-Jona-Lasinio Model
doi: 10.1007/s002180050065
1996DO12 Nucl.Phys. A603, 415 (1996) F.Doring, C.Schuren, E.Ruiz-Arriola, T.Watabe, K.Goeke Analytical Continuation of the Fermion Determinant with a Finite Cut-Off
doi: 10.1016/0375-9474(96)80009-G
1996KI02 Nucl.Phys. A596, 415 (1996) H.-C.Kim, A.Blotz, C.Schneider, K.Goeke Strangeness in the Scalar Form Factor of the Nucleon
doi: 10.1016/0375-9474(95)00404-1
1996KI03 Nucl.Phys. A598, 379 (1996) H.-C.Kim, M.V.Polyakov, A.Blotz, K.Goeke Magnetic Moments of the SU(3) Octet Baryons in the Semibosonized SU(3) Nambu-Jona-Lasinio Model NUCLEAR STRUCTURE 1,1n; calculated μ vs constituent quark mass. Framework of SU(3) semibosonized Nambu-Jona-Lasinio model.
doi: 10.1016/0375-9474(95)00506-4
1996NI08 Nucl.Phys. A608, 411 (1996) E.N.Nikolov, W.Broniowski, C.V.Christov, G.Ripka, K.Goeke Meson Loops in the Nambu-Jona-Lasinio Model
doi: 10.1016/S0375-9474(96)00231-X
1995BL03 Nucl.Phys. A585, 21c (1995) A.Blotz, M.Praszalowicz, K.Goeke Hyperons in Effective Chiral Quark Models
doi: 10.1016/0375-9474(94)00538-X
1995CH30 Phys.Rev. C52, 425 (1995) Chr.V.Christov, K.Goeke, P.V.Pobylitsa 1/N(c) Rotational Corrections to g(A) in the Nambu-Jona-Lasinio Model and Charge Conjugation
doi: 10.1103/PhysRevC.52.425
1995CH41 Nucl.Phys. A592, 513 (1995) Chr.V.Christov, A.Z.Gorski, K.Goeke, P.V.Pobylitsa Electromagnetic Form Factors of the Nucleon in the Chiral Quark Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated μ, rms radii, mass difference, form factors.
doi: 10.1016/0375-9474(95)00309-O
1995RU12 Nucl.Phys. A591, 561 (1995) E.Ruiz Arriola, P.Alberto, K.Goeke, J.N.Urbano The Projected Chiral Soliton Model with Vector Mesons NUCLEAR STRUCTURE 1n, 1H; calculated mass difference. Projected chiral soliton model.
doi: 10.1016/0375-9474(95)00204-E
1995WA12 Phys.Lett. 349B, 197 (1995) T.Watabe, Chr.V.Christov, K.Goeke E2/M1 Ratio for the γN → Δ Transition in the Quark Soliton Model
doi: 10.1016/0370-2693(95)00227-C
1994BL11 Acta Phys.Pol. B25, 1443 (1994) A.Blotz, K.Goeke, M.Praszalowicz Isospin Mass Splittings and the m(s) Corrections in the Semibosonized SU(3)-Nambu-Jona-Lasinio Model
1994CH25 Phys.Lett. 325B, 467 (1994) Chr.V.Christov, A.Blotz, K.Goeke, P.Pobilitsa, V.Petrov, M.Wakamatsu, T.Watabe 1/N(c) Rotational Corrections to g(A) and Isovector Magnetic Moment of the Nucleon
doi: 10.1016/0370-2693(94)90041-8
1994FI03 Nucl.Phys. A570, 782 (1994) Nucleon Form Factors in a Projected Chiral Soliton Model with Dynamical Confinement NUCLEAR STRUCTURE 1H, 1n; calculated magnetic, electric form factors. Projected chiral soliton model with dynamical confinement.
doi: 10.1016/0375-9474(94)90083-3
1994NI07 Nucl.Phys. A579, 398 (1994) E.N.Nikolov, W.Broniowski, K.Goeke Electric Polarizability of the Nucleon in the Nambu-Jona-Lasinio Model
doi: 10.1016/0375-9474(94)90915-6
1994SI04 Nucl.Phys. A569, 629 (1994) P.Sieber, M.Praszalowicz, K.Goeke Dependence of Baryonic Observables on the Quark-Axial-Vector Coupling in the Chiral Quark Model
doi: 10.1016/0375-9474(94)90377-8
1994WU04 Z.Phys. A348, 111 (1994) R.Wunsch, K.Goeke, Th.Meissner On Size and Shape of the Average Meson Fields in the Semibosonized Nambu and Jona-Lasinio Model
1993BL01 Phys.Lett. 302B, 151 (1993) A.Blotz, M.V.Polyakov, K.Goeke The Spin of the Proton in the Solitonic SU(3) NJL Model NUCLEAR STRUCTURE 1H; calculated spin ' crisis ' features. Solitonic SU(3) Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(93)90375-R
1993CH27 Nucl.Phys. A556, 641 (1993) Chr.V.Christov, E.Ruiz Arriola, K.Goeke Nucleon Properties and Restoration of Chiral Symmetry at Finite Density and Temperature in an Effective Theory NUCLEAR STRUCTURE 1H, 1n; calculated rms radius, electric form factor. 1H; calculated μ, magnetic form factor. Soliton, Nambu-Jona-Lasinio model.
doi: 10.1016/0375-9474(93)90474-C
1993NE05 Nucl.Phys. A560, 909 (1993) T.Neuber, M.Fiolhais, K.Goeke, J.N.Urbano Nucleon Description in a Projected Chiral Soliton Model with Dynamical Confinement NUCLEAR STRUCTURE 1n, 1H; calculated μ, charge radii. Projected chiral soliton model, dynamical confinement.
doi: 10.1016/0375-9474(93)90138-N
1992GO02 Phys.Lett. 278B, 24 (1992) A.Z.Gorski, F.Grummer, K.Goeke Nucleon Electric Form Factors and Quark Sea Polarization in the Nambu-Jona-Lasinio Model NUCLEAR STRUCTURE 1n, 1H; calculated electric form factor vs momentum transfer, charge distribution. Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(92)90705-9
1992NE06 Phys.Lett. 281B, 202 (1992) Peierls-Yoccoz Linear and Angular Momentum Projected Observables in the Linear Chiral Sigma Model NUCLEAR STRUCTURE 1n, 1H; calculated μ, rms charge radii. Linear chiral sigma model, Gell-Mann-Levi lagrangian.
doi: 10.1016/0370-2693(92)91129-W
1992NI03 Phys.Lett. 281B, 208 (1992) E.N.Nikolov, M.Bergmann, Chr.V.Christov, K.Goeke, A.N.Antonov, S.Krewald Nucleon Properties in a Medium and Quasielastic Electron Scattering NUCLEAR REACTIONS 12C, 40,48Ca, 56Fe, 208Pb(e, e'X), E not given; calculated longitudinal, transverse response functions. Relativistic Fermi gas model.
doi: 10.1016/0370-2693(92)91130-2
1991FI09 Phys.Lett. 268B, 1 (1991) M.Fiolhais, T.Neuber, K.Goeke, P.Alberto, J.N.Urbano Linear and Angular Momentum Projected Observables in the Chiral Chromodielectric Model of the Nucleon NUCLEAR STRUCTURE 1H, 1n; calculated μ, rms charge radii. Chiral chromodielectric model lagrangian.
doi: 10.1016/0370-2693(91)90912-A
1991FI10 Phys.Lett. 269B, 43 (1991) M.Fiolhais, C.Christov, T.Neuber, M.Bergmann, K.Goeke Neutron-Proton Mass Difference in a Baryonic Medium and the Nolen-Schiffer Anomaly NUCLEAR STRUCTURE 1n, 1H; calculated mass difference; deduced Nolen-Schiffer anomaly implications. Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(91)91449-6
1990AL20 Z.Phys. A336, 449 (1990) P.Alberto, E.Ruiz Arriola, M.Fiolhais, K.Goeke, F.Grummer, J.N.Urbano Form Factors in the Projected Linear Chiral Sigma Model NUCLEAR STRUCTURE 1H; calculated magnetic, electric form factors, quark, pion, total isospin density vs r, charge distribution. 1n; calculated magnetic, electric form factors, charge distribution. Linear chiral soliton model.
1990AL31 Phys.Lett. 247B, 210 (1990) P.Alberto, E.Ruiz Arriola, J.N.Urbano, K.Goeke Form Factors in the Projected Chiral Soliton Model with Vector Mesons NUCLEAR STRUCTURE 1H; calculated electric, magnetic form factors. Projected chiral soliton model.
doi: 10.1016/0370-2693(90)90883-8
1990BE22 Phys.Lett. 243B, 185 (1990) M.Bergmann, K.Goeke, S.Krewald Medium Effects in Quasi-Elastic Electron Scattering NUCLEAR REACTIONS 40Ca(e, e'), E not given; calculated longitudinal, transverse response function. Nambu-Jona-Lasinio model form factors.
doi: 10.1016/0370-2693(90)90837-V
1990CH15 Nucl.Phys. A510, 689 (1990) Chr.V.Christov, E.Ruiz Arriola, K.Goeke Properties of the Nucleon in the Nuclear Medium within a Chiral Quark-Meson Theory NUCLEAR STRUCTURE 1H, 1n; calculated μ, rms radii. Chiral quark-meson theory of nuclear medium.
doi: 10.1016/0375-9474(90)90355-P
1990CH28 Phys.Lett. 243B, 191 (1990) Chr.V.Christov, E.Ruiz Arriola, K.Goeke σ and π Meson Properties and Delocalization of the Nucleon in a Hot and Dense Nuclear Medium NUCLEAR STRUCTURE 1H; calculated rms radius. Hot baryon medium, Nambu-Jona-Lasinio model.
doi: 10.1016/0370-2693(90)90838-W
1990SL01 J.Phys.(London) G16, 395 (1990) B.Slavov, F.Grummer, K.Goeke, R.Gissler, V.I.Dimitrov, Ts.Venkova Comparison of Quantised ATDHF and GCM Theory with Application to the 12C + 20Ne System NUCLEAR REACTIONS, ICPND 20Ne(12C, X), E(cm) ≈ 0-10 MeV; calculated astrophysical S-factor vs E. One parameter generator coordinate method, quantized adiabatic TDHF.
doi: 10.1088/0954-3899/16/3/011
1989RU03 Phys.Lett. 225B, 22 (1989) E.Ruiz Arriola, Chr.V.Christov, K.Goeke Medium Effects on Nucleon Properties NUCLEAR STRUCTURE 1n, 1H; calculated μ, rms radii, electric form factor, charge distribution. Medium effects.
doi: 10.1016/0370-2693(89)91002-2
1988AL21 Phys.Lett. 208B, 75 (1988) P.Alberto, E.Ruiz Arriola, M.Fiolhais, F.Grummer, J.N.Urbano, K.Goeke Nucleon Form Factors in the Projected Linear Chiral Soliton Model NUCLEAR STRUCTURE 1H, 1n; calculated electromagnetic, axial form factors.
doi: 10.1016/0370-2693(88)91206-3
1988FI03 Nucl.Phys. A481, 727 (1988) M.Fiolhais, K.Goeke, F.Grummer, J.N.Urbano The Generalized Hedgehog and the Projected Chiral Soliton Model NUCLEAR STRUCTURE 1H, 1n; calculated μ, rms radii. Generalized hedgehog, projected chiral soliton models.
doi: 10.1016/0375-9474(88)90723-3
1987FI06 Phys.Lett. 194B, 187 (1987) M.Fiolhais, A.Nippe, K.Goeke, F.Grummer, J.N.Urbano The Goldberger-Treiman Relation and the Chiral Soliton Model NUCLEAR STRUCTURE 1n, 1H; calculated rms radii, μ. Chiral soliton model.
doi: 10.1016/0370-2693(87)90525-9
1987GO18 Z.Phys. A326, 339 (1987) K.Goeke, M.Harvey, U.-J.Wiese, F.Grummer, J.N.Urbano Solution of Symmetry Conserving Chiral Soliton Model for Nucleon and Delta NUCLEAR STRUCTURE 1n, 1H; calculated μ, rms charge radii. Linear chiral soliton model.
1987PR01 Ann.Phys.(New York) 174, 202 (1987) D.Provoost, F.Grummer, K.Goeke Quantized ATDHF and Angular Momentum Projection: Three-dimensional applications to heavy ion scattering NUCLEAR STRUCTURE 8Be, 12C, 20Ne; calculated levels, Γα. Adiabatic time-dependent Hartree-Fock theory. NUCLEAR REACTIONS 4He(α, α), 16O(α, α), E ≈ 30 MeV; calculated scattering phase shifts. Abiabatic time-dependent Hartree-Fock theory.
doi: 10.1016/0003-4916(87)90084-4
1987RE04 Rep.Prog.Phys. 50, 1 (1987) The Generator Coordinate Method and Quantised Collective Motion in Nuclear Systems NUCLEAR REACTIONS 40Ca(α, α), E=5-10 MeV; compiled resonances. 16O(16O, 16O), E=9-19 MeV; compiled reflection coefficients. 16O(16O, 32S), E=6-10 MeV; 20Ne(12C, 32S), E ≤ 10 MeV; compiled σ(E), S factors. 16O(α, α), 4He(α, α), E ≤ 30 MeV; compiled phase shifts. Generator coordinate method. NUCLEAR STRUCTURE 20Ne, 24Mg, 70Zn, 130Ce; compiled levels, J, π. 4He; compiled transition form factor. 32S; compiled zero-point energies. Generator coordinate method.
doi: 10.1088/0034-4885/50/1/001
1986GI03 Phys.Lett. 166B, 385 (1986) R.Gissler, D.Provoost, F.Grummer, K.Goeke The Importance of α-Transfer in Subbarrier Fusion Processes NUCLEAR REACTIONS, ICPND 20Ne(12C, X), E(cm) ≈ 0-10 MeV; analyzed sub-barrier fusion σ(E), astrophysical S-factor vs E; deduced α-transfer role in fusion. Adiabatic TDHF.
doi: 10.1016/0370-2693(86)91584-4
1986NI01 Z.Phys. A323, 27 (1986) Deformation Effects in the 12C - 12C System NUCLEAR REACTIONS 12C(12C, X), E(cm) ≈ 0.25-6 MeV; calculated integrated density distributions vs cluster distances, interaction potentials, subbarrier fusion astrophysical factor S(E). Quantized adiabatic TDHF.
1986SL01 Nucl.Phys. A454, 392 (1986) B.Slavov, V.I.Dimitrov, K.Goeke, F.Grummer, P.-G.Reinhard A Measure of Adiabaticity for Nuclear Collective Motion NUCLEAR REACTIONS 16O(16O, X), E not given; calculated collective potential, validity measure vs ion-ion distance.
doi: 10.1016/0375-9474(86)90276-9
1984PR09 Nucl.Phys. A431, 139 (1984) D.Provoost, F.Grummer, K.Goeke, P.-G.Reinhard Quantized ATDHF Calculations for the α + 16O → 20Ne, 20Ne → α + 16O System NUCLEAR STRUCTURE 4He, 16O; calculated total binding energy. 20Ne; calculated proton rms radius, intrinsic quadrupole moment, ground state rotational band. Quantized adiabatic TDHF. NUCLEAR REACTIONS 16O(α, α), E(cm)=8.04, 14.7 MeV; calculated σ(θ), phase shifts. Quantized adiabatic TDHF.
doi: 10.1016/0375-9474(84)90058-7
1984RE08 Z.Phys. A317, 339 (1984) P.-G.Reinhard, F.Grummer, K.Goeke Collective Mass Parameters and Linear Response Techniques in Three-Dimensional Grids NUCLEAR STRUCTURE 32S; calculated rotational, transverse inertia parameters vs 16O cluster separation. Generator coordinate method, adiabatic TDHF. NUCLEAR REACTIONS 16O(16O, 16O), E not given; calculated rotational, translational inertia parameters vs ion distance. Adiabatic TDHF, generator coordinate method.
doi: 10.1007/BF01438367
1984RE09 Phys.Rev. C30, 878 (1984) P.-G.Reinhard, J.Friedrich, K.Goeke, F.Grummer, D.H.E.Gross Dynamics of the 16O + 16O → 32S Fusion Process NUCLEAR STRUCTURE 4He, 12C, 16O, 20Ne, 24Mg, 32S, 40Ca; calculated binding energy, diffraction, rms radii, surface width. 16O; calculated charge density. Quantized adiabatic TDHF. NUCLEAR REACTIONS, ICPND 16O(16O, X), E(cm)=2-50 MeV; calculated subbarrier, above barrier fusion σ(E), astrophysical S-factor vs E. 16O(e, e), E not given; calculated form factor. Quantized adiabatic TDHF.
doi: 10.1103/PhysRevC.30.878
1983GO08 Phys.Lett. 124B, 21 (1983) K.Goeke, F.Grummer, P.-G.Reinhard Quantized ATDHF Calculations for Subbarrier Fusion of Heavy Ions NUCLEAR REACTIONS, ICPND 16O(16O, X), E(cm)=0.5-10 MeV; calculated fusion σ, astrophysical S-factor vs E. Subbarrier fusion, adiabatic TDHF.
doi: 10.1016/0370-2693(83)91394-1
1983GO25 Ann.Phys.(New York) 150, 504 (1983) K.Goeke, F.Grummer, P.-G.Reinhard Three-Dimensional Nuclear Dynamics in the Quantized ATDHF Approach NUCLEAR REACTIONS 4He(α, α), 12C(12C, 12C), 16O(16O, 16O), E(cm) ≈ 1-9 MeV; calculated collective mass, potential vs ion-ion distance, subbarrier fusion σ(E), astrophysical S-factor vs E. Adiabatic TDHF theory.
doi: 10.1016/0003-4916(83)90025-8
1981UR01 Nucl.Phys. A370, 329 (1981) J.N.Urbano, K.Goeke, P.-G.Reinhard Dynamical and Quantum Mechanical Corrections to Heavy-Ion Potentials NUCLEAR MOMENTS 16O(16O, 16O), E(cm)=16, 20 MeV; calculated σ(θ), barrier penettration properties. Heavy ion potentials, dynamical, quantum mechanical corrections.
doi: 10.1016/0375-9474(81)90080-4
1980CA06 Phys.Lett. 91B, 185 (1980) B.Castel, G.R.Satchler, K.Goeke Core Polarization Effects and Giant Quadrupole Resonances in the A = 90 Region NUCLEAR STRUCTURE A ≈ 90; calculated proton, neutron effective charges. Linearized Hartree-Fock, macroscopic GQR excitation models.
doi: 10.1016/0370-2693(80)90426-8
1980GO05 Nucl.Phys. A339, 377 (1980) K.Goeke, B.Castel, P.-G.Reinhard Isovector Giant Monopole Resonances: A Sum-Rule Approach NUCLEAR STRUCTURE 16O, 40Ca, 56Ni, 90Zr, 208Pb; calculated T=1, giant monopole resonance sum rules. Adiabatic time-dependent Hartree-Fock, Skyrme interacion.
doi: 10.1016/0375-9474(80)90022-6
1979CA05 Phys.Lett. 82B, 160 (1979) Calculation of Nuclear RMS Radii Using a Skyrme Interaction with a State Dependent Effective Mass NUCLEAR STRUCTURE 40,48Ca; calculated properties of valence orbits. Modified Skyrme interaction, local enhancement of effective mass at Fermi surface.
doi: 10.1016/0370-2693(79)90724-X
1979GO01 Phys.Rev. C19, 201 (1979) Calculation of Giant Monopole Resonances in the Adiabatic Time-Dependent Hartree-Fock Theory NUCLEAR STRUCTURE 16O, 40Ca, 90Zr, 208Pb; calculated GMR. time-dependent Hartree-Fock with Skyrme interactions.
doi: 10.1103/PhysRevC.19.201
1977CA25 Phys.Rev. C16, 2092 (1977) Effective Charges and Isoscalar Shifts in the Linearized Hartree-Fock Model NUCLEAR STRUCTURE 207,208Pb, 209Bi, 89Y, 90Zr; calculated change in rms radii. Skyrme interaction.
doi: 10.1103/PhysRevC.16.2092
1977MU05 Phys.Rev. C15, 1467 (1977) H.Muther, K.Goeke, K.Allaart, A.Faessler Single-Particle Degrees of Freedom and the Generator-Coordinate Method NUCLEAR STRUCTURE 46,50Ti, 52Cr, 54Fe; calculated levels, B(E2).
doi: 10.1103/PhysRevC.15.1467
1976CA07 Phys.Rev. C13, 1765 (1976) Prolate-Oblate Energy Difference and Shape Variation in the f-p Shell NUCLEAR STRUCTURE 48Ti, 50,52Cr, 54,56Fe, 64Zn, 72Ge; calculated prolate-oblate energy differences. Generator-coordinate method.
doi: 10.1103/PhysRevC.13.1765
1976DI12 Phys.Rev. C14, 1189 (1976) M.Didong, H.Muther, K.Goeke, A.Faessler Coupling of Two-Quasiparticle and Collective Excitations in Ge and Zn Isotopes NUCLEAR STRUCTURE 72,74Ge, 70Zn; calculated levels, B(E2).
doi: 10.1103/PhysRevC.14.1189
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