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NSR database version of May 3, 2024.

Search: Author = T.Watabe

Found 11 matches.

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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

2000WA26      Phys.Rev. D62, 054009 (2000)

M.Wakamatsu, T.Watabe

Spin and Orbital Angular Momentum Distribution Functions of the Nucleon

NUCLEAR STRUCTURE 1n, 1H; calculated spin and orbital angular momentum distribution functions. Chiral quark soliton model.

doi: 10.1103/PhysRevD.62.054009
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

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

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

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

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

1991HI10      Phys.Rev. C44, 1467 (1991)

D.Hirata, H.Toki, T.Watabe, I.Tanihata, B.V.Carlson

Relativistic Hartree Theory for Nuclei Far from the Stability Line

NUCLEAR STRUCTURE 36,40,44,48,52,56,60,64,68,38,42,46,50,54,58,62,66,70Ca; calculated binding energy per particle, p, n, charge radii, single particle spectra. Relativistic Hartree theory.

doi: 10.1103/PhysRevC.44.1467
Citations: PlumX Metrics

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