Denote by $N$ the jump measure of the Lévy process, i.e. $$N_t(B) := N([0,t] \times B) := \sharp \\{s \in [0,t]; \Delta X_s := X_s-X_{s-} \in B\\},$$ and by $\
u$ its Lévy measure. It is widely known that $(N_t(B))_{t \geq 0}$ is a Poisson process with intensity $\
u(B)$. In particular, we have
$$\mathbb{P}(N_t(B) >0) = 1- \mathbb{P}(N_t(B)=0)= 1-e^{-\
u(B) t}.$$
For any set $B$ such that $0<\
u(B)<\infty$ this implies
$$\mathbb{P}(\exists s \in [0,t]: \Delta X_s \in B) = \mathbb{P}(N_t(B) >0) \stackrel{t \to \infty}{\to} 1.$$
Applying this for $B = [n,n+1)$, we get
$$\mathbb{P}(\exists t \geq 0: \Delta X_t \in [n,n+1)) = 1.$$
Hence,
$$\mathbb{P}(\forall N \geq 1 \exists t \geq 0: \Delta X_t \geq N) = 1.$$
This shows that the jump heights are (almost surely) unbounded.
**Remark:** The proof applies to any Lévy process with unbounded Lévy measure.