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Origin of Dynamically Generated Baryon Rsonances

T.Hyodo D.Jido A.Hosaka

T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. 原子核物理评论, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001
引用本文: T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. 原子核物理评论, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001
T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. Nuclear Physics Review, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001
Citation: T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. Nuclear Physics Review, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001

Origin of Dynamically Generated Baryon Rsonances

doi: 10.11804/NuclPhysRev.26.S1.001

Origin of Dynamically Generated Baryon Rsonances

  • 摘要: We study the origin of baryon resonances which are dynamically generated in the chiral unitary approach. We propose a natural renormalization scheme for the dynamical generation of resonances using the low energy chiral interaction and a general feature of the scattering theory. A deviation of a phenomenological scattering amplitude from the natural one is interpreted by an effective pole term interaction of genuine nature which can not be described by the mesonbaryon dynamics, reminiscent of the CDD pole. Applying the present method to physical mesonbaryon scatterings, we find that the Λ(1405) resonance is dominated by a mesonbaryon component forming a KNπΣ molecularlike structure, while the N(1535) resonance requires some pole contribution.

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出版历程
  • 收稿日期:  1900-01-01
  • 修回日期:  1900-01-01
  • 刊出日期:  2020-05-11

Origin of Dynamically Generated Baryon Rsonances

doi: 10.11804/NuclPhysRev.26.S1.001

摘要: We study the origin of baryon resonances which are dynamically generated in the chiral unitary approach. We propose a natural renormalization scheme for the dynamical generation of resonances using the low energy chiral interaction and a general feature of the scattering theory. A deviation of a phenomenological scattering amplitude from the natural one is interpreted by an effective pole term interaction of genuine nature which can not be described by the mesonbaryon dynamics, reminiscent of the CDD pole. Applying the present method to physical mesonbaryon scatterings, we find that the Λ(1405) resonance is dominated by a mesonbaryon component forming a KNπΣ molecularlike structure, while the N(1535) resonance requires some pole contribution.

English Abstract

T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. 原子核物理评论, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001
引用本文: T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. 原子核物理评论, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001
T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. Nuclear Physics Review, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001
Citation: T.Hyodo, D.Jido, A.Hosaka. Origin of Dynamically Generated Baryon Rsonances[J]. Nuclear Physics Review, 2009, 26(5): 1-6. doi: 10.11804/NuclPhysRev.26.S1.001

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