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    Faddeev calculation of pentaquark Θ+\Theta^+ in the Nambu-Jona-Lasinio model-based diquark picture

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    A Bethe-Salpeter-Faddeev (BSF) calculation is performed for the pentaquark Θ+\Theta^+ in the diquark picture of Jaffe and Wilczek in which Θ+\Theta^+ is a diquark-diquark-sˉ{\bar s} three-body system. Nambu-Jona-Lasinio (NJL) model is used to calculate the lowest order diagrams in the two-body scatterings of sˉD{\bar s}D and DDD D. With the use of coupling constants determined from the meson sector, we find that sˉD{\bar s}D interaction is attractive in s-wave while DDDD interaction is repulsive in p-wave. With only the lowest three-body channel considered, we do not find a bound 12+ \frac 12^+ pentaquark state. Instead, a bound pentaquark Θ+\Theta^+ with 12− \frac 12^- is obtained with a unphysically strong vector mesonic coupling constants.Comment: 22 pages, 11 figures, accepted version in Phys. Rev. C. Summary of main changes/corrections: 1. "which only holds at tree level" below the eq. (23) is added. 2. In the last paragraph of p.23 we added a remark that the coupling constant obtained from Lambda mass is different from the estimate as obtained from the meson spectru
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