Step 1: Set up the impedances.
At frequency $\omega$, the reactance is $X_c$ and the impedance is $Z = \sqrt{R^2 + X_c^2}$. At $\tfrac{\omega}{3}$ the reactance triples to $3X_c$, so $Z' = \sqrt{R^2 + 9X_c^2}$.
Step 2: Use the current drop.
The current halves, so the impedance doubles: $Z' = 2Z$.
Step 3: Square and simplify.
$R^2 + 9X_c^2 = 4(R^2 + X_c^2)$, which gives $5X_c^2 = 3R^2$, so $\tfrac{X_c^2}{R^2} = \tfrac{3}{5} = 0.6$.
Step 4: Take the root.
$\tfrac{X_c}{R} = \sqrt{0.6}$.
\[ \boxed{\sqrt{0.6}} \]