I write $\Bbb E^x$ and $\Bbb P^x$ to indicate the initial condition $X_0=x$.
Define $u(x):=\Bbb E^x\left[\int_0^\infty e^{-t} 1_{\{X_t=y\}}dt\right]$. Then $\delta:=\inf\{u(x):x\in E\}>0$. Choose $b>0$ so large that $e^{-b}<\delta/2$. Writing $T_y:=\inf\{t>0:X_t=y\}$, you have
$$
\eqalign{
v(x) &\le\Bbb E^x\left[\int_0^b e^{-t}1_{\{X_t=y\}}dt\right]+e^{-b}\cr
&=\Bbb E^x\left[\int_0^b e^{-t}1_{\{X_t=y\}}1_{\{T_y\le b\}}dt\right]+e^{-b}\cr
&\le\Bbb E^x\left[\int_0^b e^{-t}1_{\{T_y\le b\}}dt\right]+e^{-b}\cr
&=(1-e^{-b})\Bbb P^x\left[T_y\le b\right]+e^{-b}\cr
&\le\Bbb P^x\left[T_y\le b\right]+e^{-b}\cr
}
$$
It follows that
$$
\Bbb P^x[T_y>b]\le 1-\delta/2,\qquad\forall x.
$$
Noting that $\{T_y>2b\} =\{T_y>b\}\cap\{\inf\{t>b:X_t=y\}>b\}$, and using the Markov property at time $b$:
$$
\eqalign{
\Bbb P^x[T_y>2b]
&=\Bbb E^x\left[ 1_{\{T_y>b\}}\Bbb P^{X_b}[T_y>b]\right]\cr
&\le\Bbb E^x\left[ 1_{\{T_y>b\}}\cdot(1-\delta/2)\right]\cr
&\le(1-\delta/2)^2.
}
$$
Repeating this you see that
$$
\Bbb P^x[T_y>nb]\le(1-\delta/2)^n,\qquad n=1,2,\ldots, x\in E.
$$
It follows easily from this that there is a constant $C>0$ such that
$$
\Bbb P^x[T_y>t]\le Ce^{-\rho t},\qquad t>0, x\in E,
$$
where $\rho:=-[\log(1-\delta/2)]/b$. This implies that $T_y$ has finite moments of all orders; indeed
$$
\Bbb E^x[\exp(\alpha T_y)]<\infty,\qquad x\in E,
$$
provided $\alpha<\rho$.