1. Current in terms of drift velocity
$$ I = nAv_d q $$
Where:
2. Area relation with diameter $d$
$$ A = \pi \left(\frac{d}{2}\right)^2 = \frac{\pi d^2}{4} $$
So, $A \propto d^2$
Therefore:
$$ I \propto d^2 v_d $$
For same material, $n$ and $q$ are constant.
3. Comparing two cases
Let initial: diameter = $d$, current = $I$, drift velocity = $v_d$
New: diameter = $d' = \frac{d}{2}$, current = $I' = 2I$, drift velocity = $v_d'$
$$ \frac{I'}{I} = \frac{d'^2 v_d'}{d^2 v_d} $$
$$ \frac{2I}{I} = \frac{\left(\frac{d}{2}\right)^2 v_d'}{d^2 v_d} $$
$$ 2 = \frac{\frac{d^2}{4} \cdot v_d'}{d^2 v_d} = \frac{v_d'}{4 v_d} $$
$$ v_d' = 2 \times 4 \, v_d = 8 v_d $$
$$ \therefore v_d' = 8v $$