Step 1: Establish the condition for an electrostatic field.
A vector field \(\vec{F}\) qualifies as an electrostatic field if its curl is zero:
\[
\nabla \times \vec{F} = 0.
\]
Step 2: Verify the curl of \(\vec{F_1}\).
The given field is \(\vec{F_1} = A(\hat{i}y + \hat{j}x)\). Its curl is:
\[
\nabla \times \vec{F_1} =
\begin{vmatrix}
\hat{i} & \hat{j} & \hat{k} \\
\frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\
Ay & Ax & 0
\end{vmatrix}.
\]
Expanding the determinant gives:
\[
\nabla \times \vec{F_1} = \hat{i}(0 - 0) - \hat{j}(0 - 0) + \hat{k}\left(\frac{\partial Ax}{\partial y} - \frac{\partial Ay}{\partial x}\right).
\]
The \(z\)-derivatives vanish as the terms are independent of \(z\), and the \(x\)- and \(y\)-derivatives cancel:
\[
\nabla \times \vec{F_1} = \hat{k}(A - A) = 0.
\]
Thus, \(\vec{F_1}\) satisfies the electrostatic condition.
Step 3: Verify the curl of \(\vec{F_2}\).
The given field is \(\vec{F_2} = A(\hat{i}y - \hat{j}x)\). Its curl is:
\[
\nabla \times \vec{F_2} =
\begin{vmatrix}
\hat{i} & \hat{j} & \hat{k} \\
\frac{\partial}{\partial x} & \frac{\partial}{\partial y} & \frac{\partial}{\partial z} \\
Ay & -Ax & 0
\end{vmatrix}.
\]
Expanding the determinant gives:
\[
\nabla \times \vec{F_2} = \hat{i}(0 - 0) - \hat{j}(0 - 0) + \hat{k}\left(\frac{\partial (-Ax)}{\partial x} - \frac{\partial Ay}{\partial y}\right).
\]
Simplifying:
\[
\nabla \times \vec{F_2} = \hat{k}(-A - A) = \hat{k}(-2A).
\]
Since the curl is nonzero, \(\vec{F_2}\) is not an electrostatic field.
Final Answer:
\[
\boxed{(2) Only \(\vec{F_1}\) is an electrostatic field.}
\]