Step 1: Check if the velocity field is one-dimensional.
The velocity components are
\[
u = 4xy,\qquad v = 2(x^2 - y^2).
\]
Both depend on both variables \(x\) and \(y\).
A one-dimensional field would depend on only one spatial variable.
Hence, the velocity field is not one-dimensional.
Statement (A) is incorrect.
Step 2: Check incompressibility using
\[
\nabla \cdot \vec{V} = \frac{\partial u}{\partial x} + \frac{\partial v}{\partial y}.
\]
Compute each term:
\[
\frac{\partial u}{\partial x} = \frac{\partial (4xy)}{\partial x} = 4y,
\]
\[
\frac{\partial v}{\partial y} = \frac{\partial (2(x^2 - y^2))}{\partial y} = -4y.
\]
Thus,
\[
\nabla \cdot \vec{V} = 4y - 4y = 0.
\]
Zero divergence implies an incompressible flow.
Statement (B) is correct.
Step 3: Check irrotationality using vorticity
\[
\omega_z = \frac{\partial v}{\partial x} - \frac{\partial u}{\partial y}.
\]
Compute each derivative:
\[
\frac{\partial v}{\partial x} = \frac{\partial (2(x^2 - y^2))}{\partial x} = 4x,
\]
\[
\frac{\partial u}{\partial y} = \frac{\partial (4xy)}{\partial y} = 4x.
\]
So,
\[
\omega_z = 4x - 4x = 0.
\]
Since the vorticity is zero everywhere, the flow is irrotational.
Statement (C) is correct.
Step 4: Check acceleration at $(x=0, y=0)$.
Fluid acceleration is
\[
\vec{a} = (u \frac{\partial}{\partial x} + v \frac{\partial}{\partial y})\vec{V}.
\]
At the point \((0,0)\):
\[
u(0,0) = 4(0)(0) = 0,\qquad v(0,0) = 2(0 - 0) = 0.
\]
If both velocity components are zero at that point, then
\[
\vec{a}(0,0) = 0.
\]
Thus, acceleration is zero at the origin.
Statement (D) is correct.
Final Answer: (B), (C), (D)