Mesonic decays of the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>ψ</mml:mi><mml:mn/><mml:mo>(</mml:mo><mml:mn>3095</mml:mn><mml:mo>)</mml:mo><mml:mn/></mml:math>

We present branching ratios for several mesonic decay modes of the $\ensuremath{\psi}(3095)$. The two-body and quasi-two-body final states have branching ratios that follow the general pattern of behavior expected for the decay of an SU(3) singlet via an SU(3)-symmetric interaction. The ${\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}$ and ${K}^{+}{K}^{\ensuremath{-}}$ mass spectra in $\ensuremath{\omega}\ensuremath{\pi}\ensuremath{\pi}$, $\ensuremath{\omega}\mathrm{KK}$, $\ensuremath{\varphi}\ensuremath{\pi}\ensuremath{\pi}$, and $\ensuremath{\varphi}\mathrm{KK}$ final states show remarkable differences that are most readily interpretable in terms of the Okubo-Zweig-Iizuka rule.