Step 1: Recall Maxwell's equations in magnetostatics (no currents, no time-varying fields).
\[
\nabla \cdot \vec{B} = 0, \qquad \nabla \times \vec{B} = \mu_0 \vec{J} = 0 \quad (\text{since } \vec{J} = 0)
\]
Thus, both divergence and curl of $\vec{B}$ vanish in this region.
Step 2: Check Option (A).
If $\nabla \times \vec{B} = 0$, the field is irrotational. An irrotational field can be expressed as the gradient of a scalar potential:
\[
\vec{B} = - \nabla \phi
\]
Hence, Option (A) is correct.
Step 3: Check Option (B).
Saying $\vec{B}$ is "rotational" means $\nabla \times \vec{B} \neq 0$. But in the given case, $\nabla \times \vec{B} = 0$.
So, Option (B) is incorrect.
Step 4: Check Option (C).
As derived from Ampère's law without current,
\[
\nabla \times \vec{B} = 0
\]
Thus, Option (C) is correct.
Step 5: Check Option (D).
From Gauss's law for magnetism,
\[
\nabla \cdot \vec{B} = 0
\]
Hence, Option (D) is correct.
Final Answer:
Correct statements are (A), (C), and (D).
\[
\boxed{\text{Correct Answer: (A), (C), (D)}}
\]