Production ofK+K−pairs in proton-proton collisions below theϕmeson threshold

Q. J. Ye,M. Hartmann,D. Chiladze,S. Dymov,A. Dzyuba,H. Gao,R. Gebel,V. Hejny,A. Kacharava, B. Lorentz,D. Mchedlishvili, S. Merzliakov, M. Mielke, S. Mikirtytchiants, H. Ohm,M. Papenbrock, A. Polyanskiy, V. Serdyuk,H. J. Stein, H. Ströher, S. Trusov,Yu. Valdau,C. Wilkin, P. Wüstner

Physical Review C(2013)

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摘要
The $pp\ensuremath{\rightarrow}pp{K}^{+}{K}^{\ensuremath{-}}$ reaction was measured below the $\ensuremath{\phi}$ threshold at a beam energy of 2.568 GeV using the COSY-ANKE magnetic spectrometer. By assuming that the four-body phase space is distorted only by the product of two-body final-state interactions, fits to a variety of one-dimensional distributions permit the evaluation of differential and total cross sections. The shapes of the distributions in the $Kp$ and $Kpp$ invariant masses are reproduced only if the ${K}^{\ensuremath{-}}p$ interaction is even stronger than that found at higher energy. The cusp effect in the ${K}^{+}{K}^{\ensuremath{-}}$ distribution at the ${K}^{0}{\overline{K}}^{0}$ threshold is much more clear and some evidence is also found for coupling between the ${K}^{\ensuremath{-}}p$ and ${\overline{K}}^{0}n$ channels. However, the energy dependence of the total cross section cannot be reproduced by considering only a simple product of such pairwise final-state interactions.
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