$\Upsilon(1S)-->\gamma(\eta',\eta,f_2(1270))$ decays

$\Upsilon(1s)\to\gamma(\eta',\eta, f_2(1270))$ are studied by an approach in which the glueball components of these mesons play dominant role. Strong dependence on quark mass has been found in the decays $(J/\psi, \Upsilon(1s))\to\gamma(\eta',\eta)$. Very small decay rates of $\Upsilon(1s)\to\gamma(\eta',\eta)$ are predicted. d-wave dominance has been found in $\Upsilon(1s)\to\gamma f_2(1270)$, which leads to larger $B(\Upsilon(1s)\to\gamma f_2(1270)).$