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Using the data obtained with SKAT bubble chamber, the total yields of $K^+(892)$, $Sigma^+(1385)$ and $Sigma^0$ are estimated for the first time in neutrino-induced reactions at moderate energies ($<E_{ u}>$ = 10.4 GeV). It is shown, that the recently observed cite{ref1,ref2} enhancement of the $K^0$ and $Lambda$ yields in $ u A$ interactions (as compared to $ u N$ interactions) is contributed only slightly by the $K^+(892)$ and $Sigma^+(1385)$ production, respectively. The decay contribution to the $K^0$ and $Lambda$ yields is found to be in qualitative agreement with higher energy ($<E_ u> geq$ 40 GeV) data. It is shown, that the energy dependence of the $K^+(892)$ mean multiplicity in $ u N$ interactions is approximately linear in the range of $<E_{ u}> approx$ 10-60 GeV, while that for $Sigma^0$ in $ u A$ interactions (for $A$ = 20-21) is approximately logarithmic in the range of $<E_{ u}> approx$ 10-150 GeV.
The total yields of the all well-established light mesonic resonances (up to the $phi$(1020) meson) are estimated in neutrinonuclear interactions at < E_nu > = 10 GeV, using the data obtained with SKAT bubble chamber. For some resonances, the yields
Differential cross sections for $gamma p to K^+Lambda(1405)$ and $gamma p to K^+Sigma^0(1385)$ reactions have been measured in the photon energy range from 1.5 to 2.4 GeV and the angular range of $0.8<cos(Theta)<1.0$ for the $K^+$ scattering angle in
The aim of the present analysis is to determine the relative production cross sections of the $Lambda$(1405) and $Sigma(1385)^{0}$ resonances in p+p collisions at E$_{kin}$=3.5 GeV measured with HADES. Upper and lower limits have been determined for
We report branching fraction measurements of four decay modes of the $Lambda_{c}^{+}$ baryon, each of which includes an $eta$ meson and a $Lambda$ baryon in the final state, and all of which are measured relative to the $Lambda_{c}^{+} rightarrow p K
Using a data sample of 980 fb$^{-1}$ collected with the Belle detector at the KEKB asymmetric-energy $e^+e^-$ collider, we study the processes of $Xi^0_cto Lambdabar K^{*0}$, $Xi^0_cto Sigma^0bar K^{*0}$, and $Xi^0_cto Sigma^+K^{*-}$ for the first ti