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NSR database version of April 11, 2024.

Search: Author = K.Goeke

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2009GO10      Phys.Rev. C 79, 035210 (2009)

K.Goeke, V.Guzey, M.Siddikov

Leading twist nuclear shadowing, nuclear generalized parton distributions, and nuclear deeply virtual Compton scattering at small x

doi: 10.1103/PhysRevC.79.035210
Citations: PlumX Metrics

2008GO13      Eur.Phys.J. A 36, 49 (2008)

K.Goeke, V.Guzey, M.Siddikov

Deeply Virtual Compton Scattering on nucleons and nuclei in the Generalized Vector Meson Dominance model

doi: 10.1140/epja/i2008-10549-x
Citations: PlumX Metrics

2008LE22      Nucl.Phys. A811, 353 (2008)

T.Ledwig, H.-C.Kim, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2005SI18      Nucl.Phys. A755, 290c (2005)

A.Silva, D.Urbano, K.Goeke

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
Citations: PlumX Metrics

2004AZ03      Eur.Phys.J. A 21, 501 (2004)

Ya.I.Azimov, K.Goeke

Decay properties of new D-mesons

doi: 10.1140/epja/i2004-10010-4
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2004SI31      Eur.Phys.J. A 22, 481 (2004)

A.Silva, H.-Ch.Kim, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2003SI18      Nucl.Phys. A721, 417c (2003)

A.Silva, H.-C.Kim, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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)

M.Franz, H.-C.Kim, K.Goeke

ΔS = 1, 2 Effective Weak Chiral Lagrangian from the Instanton Vacuum

doi: 10.1016/S0375-9474(01)01275-1
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

2000FR09      Nucl.Phys. A663-664, 995c (2000)

M.Franz, H.-C.Kim, K.Goeke

Effective Weak Chiral Lagrangian from the Instanton Vacuum

doi: 10.1016/S0375-9474(99)00752-6
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1999BA16      Phys.Rev. D59, 056005 (1999)

J.Balla, A.Blotz, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1998WA04      Nucl.Phys. A629, 152c (1998)

T.Watabe, K.Goeke

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
Citations: PlumX Metrics

1997KI05      Nucl.Phys. A616, 606 (1997)

H.-C.Kim, T.Watabe, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1994FI03      Nucl.Phys. A570, 782 (1994)

M.Fiolhais, T.Neuber, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

1992NE06      Phys.Lett. 281B, 202 (1992)

T.Neuber, K.Goeke

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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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
Citations: PlumX Metrics

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
Citations: PlumX Metrics

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
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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
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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
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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
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1987RE04      Rep.Prog.Phys. 50, 1 (1987)

P.-G.Reinhard, K.Goeke

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
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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
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1986NI01      Z.Phys. A323, 27 (1986)

M.Niklas, K.Goeke, F.Grummer

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
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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
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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
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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
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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
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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
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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
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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
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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
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1979CA05      Phys.Lett. 82B, 160 (1979)

B.Castel, K.Goeke

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
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1979GO01      Phys.Rev. C19, 201 (1979)

K.Goeke, B.Castel

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
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1977CA25      Phys.Rev. C16, 2092 (1977)

B.Castel, K.Goeke

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
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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
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1976CA07      Phys.Rev. C13, 1765 (1976)

B.Castel, K.Goeke

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
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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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