  We revisit Munshi's proof of the $t$-aspect subconvex bound for $\rm GL(3)$
$L$-functions, and we are able to remove the `conductor lowering' trick. This
simplification along with a more careful stationary phase analysis allows us to
improve Munshi's bound to, $$ L(1/2+it, \pi) \ll_{\pi, \epsilon}
(1+|t|)^{3/4-3/40+\epsilon}. $$
