An analysis of and $B^+ \to K_{\rm \scriptscriptstyle S}^0 K^+$ decays is performed with the LHCb experiment. The collision data used correspond to integrated luminosities of and collected at centre-of-mass energies of and $\sqrt{s}=8\mathrm{,Te\kern -0.1em V}$, respectively. The ratio of branching fractions and the direct {\it CP} asymmetries are measured to be $(B^+ \to K_{\rm \scriptscriptstyle S}^0 K^+)/(B^+ \to K_{\rm \scriptscriptstyle S}^0 \pi^+) = 0.064 \pm 0.009 \pm 0.004^{\it CP}(B^+ \to K_{\rm \scriptscriptstyle S}^0 \pi^+) = -0.022 \pm 0.025 \pm 0.010^{\it CP}(B^+ \to K_{\rm \scriptscriptstyle S}^0 K^+) = -0.21 \pm 0.14 \pm 0.01\sqrt{s}=7\mathrm{,Te\kern -0.1em V}B_c^+ \to K_{\rm \scriptscriptstyle S}^0 K^+(f_c\cdot(B_c^+ \to K_{\rm \scriptscriptstyle S}^0 K^+))/(f_u\cdot(B^+ \to K_{\rm \scriptscriptstyle S}^0 \pi^+)) < 5.8\times10^{-2}\textrm{at 90% confidence level}f_cf_u\bar{b}B_c^+B^+$ meson, respectively.

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