A search for charmless three-body decays of and mesons with a meson in the final state is performed using the collision data, corresponding to an integrated luminosity of , collected at a centre-of-mass energy of recorded by the LHCb experiment. Branching fractions of the $B_{(s)}^0 \to K_{\rm S}^0 h^{+} h^{\prime -}h^{(\prime)} = \pi, K$), relative to the well measured decay, are obtained. First observation of the decay modes and and confirmation of the decay $B^0 \to K_{\rm S}^0 K^{\pm} \pi^{\mp}$ are reported. The following relative branching fraction measurements or limits are obtained \begin{eqnarray*} \nonumber \frac{{\cal B}(B^0 \to K_{\rm S}^0 K^{\pm} \pi^{\mp})}{{\cal B}(B^0 \to K_{\rm S}^0 \pi^{+} \pi^{-})} &=& 0.128 \pm 0.017 , ({\rm stat.}) \pm 0.009 , ({\rm syst.}) ,, \ \nonumber \frac{{\cal B}(B^0 \to K_{\rm S}^0 K^{+} K^{-} )}{{\cal B}(B^0 \to K_{\rm S}^0 \pi^{+} \pi^{-})} &=& 0.385 \pm 0.031 , ({\rm stat.}) \pm 0.023 , ({\rm syst.}) ,, \ \nonumber \frac{{\cal B}(B_s^0 \to K_{\rm S}^0 \pi^{+} \pi^{-} )}{{\cal B}(B^0 \to K_{\rm S}^0 \pi^{+} \pi^{-})} &=& 0.29\phantom{0} \pm 0.06\phantom{0} , ({\rm stat.}) \pm 0.03\phantom{0} , ({\rm syst.}) \pm 0.02 , (f_s/f_d) ,, \ \nonumber \frac{{\cal B}(B_s^0 \to K_{\rm S}^0 K^{\pm} \pi^{\mp})}{{\cal B}(B^0 \to K_{\rm S}^0 \pi^{+} \pi^{-})} &=& 1.48\phantom{0} \pm 0.12\phantom{0} , ({\rm stat.}) \pm 0.08\phantom{0} , ({\rm syst.}) \pm 0.12 , (f_s/f_d) ,, \ \nonumber \frac{{\cal B}(B_s^0 \to K_{\rm S}^0 K^{+} K^{-} )}{{\cal B}(B^0 \to K_{\rm S}^0 \pi^{+} \pi^{-})} &\in& [0.004;0.068] ; {\rm at ;; 90% ; CL} ,. \end{eqnarray*}

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