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DONG Yu-bing, HE Jun. Electromagnetic Transition Amplitudes of Nucleon Negative parity Resonance by OPE and OGE Quark Models[J]. Nuclear Physics Review, 2004, 21(2): 157-158. doi: 10.11804/NuclPhysRev.21.02.157
Citation: DONG Yu-bing, HE Jun. Electromagnetic Transition Amplitudes of Nucleon Negative parity Resonance by OPE and OGE Quark Models[J]. Nuclear Physics Review, 2004, 21(2): 157-158. doi: 10.11804/NuclPhysRev.21.02.157

Electromagnetic Transition Amplitudes of Nucleon Negative parity Resonance by OPE and OGE Quark Models

doi: 10.11804/NuclPhysRev.21.02.157
  • Received Date: 1900-01-01
  • Rev Recd Date: 1900-01-01
  • Publish Date: 2004-06-20
  • Electromagnetic transition amplitudes of negative parity resonances are calculated based on onepion exchange (OPE) model and one gluon exchange (OGE) model, respectively. The configuration mixing caused by the hyperfine interactions of the two models is discussed. Calculated results for the
    amplitudes indicate that baryon wave functions of OGE are more reasonable
    than those of OPE.
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    沈阳化工大学材料科学与工程学院 沈阳 110142

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Electromagnetic Transition Amplitudes of Nucleon Negative parity Resonance by OPE and OGE Quark Models

doi: 10.11804/NuclPhysRev.21.02.157

Abstract: Electromagnetic transition amplitudes of negative parity resonances are calculated based on onepion exchange (OPE) model and one gluon exchange (OGE) model, respectively. The configuration mixing caused by the hyperfine interactions of the two models is discussed. Calculated results for the
amplitudes indicate that baryon wave functions of OGE are more reasonable
than those of OPE.

DONG Yu-bing, HE Jun. Electromagnetic Transition Amplitudes of Nucleon Negative parity Resonance by OPE and OGE Quark Models[J]. Nuclear Physics Review, 2004, 21(2): 157-158. doi: 10.11804/NuclPhysRev.21.02.157
Citation: DONG Yu-bing, HE Jun. Electromagnetic Transition Amplitudes of Nucleon Negative parity Resonance by OPE and OGE Quark Models[J]. Nuclear Physics Review, 2004, 21(2): 157-158. doi: 10.11804/NuclPhysRev.21.02.157

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