Pion-nucleon and kaon-nucleon scattering lengths in QCD sum rules

Y. Kondo, O. Morimatsu, and Y. Nishino
Phys. Rev. C 53, 1927 – Published 1 April 1996
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Abstract

The pion-nucleon and kaon-nucleon scattering lengths are studied in the QCD sum rule. We show that the leading and next-to-leading order terms of the operator product expansion (OPE) give rise to the Tomozawa-Weinberg and σ terms, respectively in the pion-nucleon and kaon-nucleon scattering lengths. We discuss phenomenological contributions which should be added to the experimental scattering lengths to be compared with the theoretical calculation by the OPE: we estimate the Λ(1405) contribution in the kaon-nucleon channel by using the effective coupling strength determined by the analysis of the scattering data. We also estimate the continuum contribution above the threshold in the pion-nucleon channel by using the nonlinear σ model. It turns out that the results of the QCD sum rule for the pion-nucleon scattering lengths are consistent with those of the low energy theorem and therefore with experiments and those for the kaon-nucleon scattering lengths differ from the results of naive partial conservation of axial-vector current–plus-current-algebra approach by the contribution from Λ(1405). © 1996 The American Physical Society.

  • Received 13 October 1995

DOI:https://doi.org/10.1103/PhysRevC.53.1927

©1996 American Physical Society

Authors & Affiliations

Y. Kondo

  • Suzuka University of Medical Science and Technology, 1001-1 Kishioka, Suzuka, Mie 510-02, Japan

O. Morimatsu

  • Institute for Nuclear Study, University of Tokyo, Midori-cho, Tanashi, Tokyo 188, Japan

Y. Nishino

  • Research Center for Nuclear Physics, Osaka University, Mihogaoka, Ibaraki, Osaka 567, Japan

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Issue

Vol. 53, Iss. 4 — April 1996

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