Abstract
In this chapter, we discuss the present results focusing on the narrowness of the width which is the most peculiar property to the \(\varTheta ^+\) pentaquark. The mechanism of the \(\pi ^-p \rightarrow K^-\varTheta ^+\) reaction was theoretically discussed using the KEK-E522 and E559 results. Knowing that the t-channel and contact term contributions are very small, the s-channel contribution is important in the \(\pi ^-p \rightarrow K^-\varTheta ^+\) reaction. Since the s-channel amplitude is related to the \(\varTheta ^+\) decay width through the \(KN\varTheta \) coupling constant, we can estimate the upper limit of the width from the cross section measured in the experiment. Using both the 2010 and 2012 data together with a theoretical calculation using the effective Lagrangian approach, the upper limits of the width were estimated to be 0.36 and 1.9 MeV for the \(\varTheta ^+\) spin-parity of \(1/2^+\) and \(1/2^-\), respectively. These widths are compared with the past experimental results.
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Notes
- 1.
The approximate error is estimated by using the curvature at the minimum of the \(\chi ^2\) function and assuming a parabolic shape [7].
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Moritsu, M. (2016). Discussion. In: Search for the Pentaquark Θ+ via the π−p → K−X Reaction at J-PARC. Springer Theses. Springer, Singapore. https://doi.org/10.1007/978-981-10-0012-6_5
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DOI: https://doi.org/10.1007/978-981-10-0012-6_5
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