Abstract

The neutrinoproduction of ϕϕ and Ds+D^+_s mesons is studied, using the data obtained with the SKAT bubble chamber at the Serpukhov accelerator. It is found that the ϕϕ production occurs predominantly in the forward hemisphere of the hadronic c.m.s. (at xF>0x_F > 0, xFx_F being the Feynman variable), with the mean yield strongly exceeding the expected yield of directly produced ϕϕ mesons and varying from <nΦ(xF>0)>=(0.92±0.34)⋅10−2<n_Φ(x_F > 0) > = (0.92\pm0.34) \cdot 10^{-2} at W>W > 2 GeV up to (1.23±0.53)⋅10−2(1.23\pm0.53) \cdot 10^{-2} at W>W > 2.6 GeV and (1.44±0.69)⋅10−2(1.44\pm0.69) \cdot 10^{-2} at W>W > 2.9 GeV, WW being the invariant mass of the hadronic system. The yield of leading Ds+D^+_s mesons carrying more than z=0.85z = 0.85 of the current cc- quark energy is estimated: at W>2.9W > 2.9 GeV, <nDs+(z>0.85)>=(6.64±1.91)⋅10−2<n_{D^+_s}(z > 0.85) > = (6.64\pm1.91) \cdot 10^{-2}. It is shown, that the shape of the ϕϕ meson differential spectrum on xFx_F is reproduced by that expected from the Ds+→ϕXD^+_s \to ϕX decays which, however, can account for only the half of the measured ϕϕ yield.

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