$$\nabla \times V= \hat{e_x}\space(\frac{\partial}{\partial{y}} V_z-\frac{\partial}{\partial{z}} V_y)+\hat{e_y}\space(\frac{\partial}{\partial{z}} V_x-\frac{\partial}{\partial{x}} V_z)+\hat{e_z}\space(\frac{\partial}{\partial{x}} V_y-\frac{\partial}{\partial{y}} V_x)$$
In the above provided equation, I have understood "$\nabla \times V$" to be just a notation (which is defined to have above value) and not to indicate any cross product.
Reference: Is $\nabla$ a vector?
The following has been extracted from the book "Mathematical methods for Physicists" by Arfken, Weber, and Harris:
Another possible operation with the vector operator r is to take its cross product with a vector. Using the established formula for the cross product, and being careful to write the derivatives to the left of the vector on which they are to act, we obtain $$\nabla \times V= \hat{e_x}\space(\frac{\partial}{\partial{y}} V_z-\frac{\partial}{\partial{z}} V_y)+\hat{e_y}\space(\frac{\partial}{\partial{z}} V_x-\frac{\partial}{\partial{x}} V_z)+\hat{e_z}\space(\frac{\partial}{\partial{x}} V_y-\frac{\partial}{\partial{y}} V_x)$$
$$= \begin{array}{|ccc|} \hat{e_x} & \hat{e_y} & \hat{e_z} \\ \frac{\partial}{\partial{x}} & \frac{\partial}{\partial{y}} & \frac{\partial}{\partial{z}} \\ V_x & V_y & V_z \end{array} \\\\\space Eq (3.58)$$
This vector operation is called the curl of V. Note that when the determinant in Eq. (3.58) is evaluated, it must be expanded in a way that causes the derivatives in the second row to be applied to the functions in the third row (and not to anything in the top row); we will encounter this situation repeatedly, and will identify the evaluation as being from the top down.
I have trouble in understanding the above passage. I feel the determinant equivalent of the curl of V to be wrong, because we don't get the curl of V when we solve that determinant. Is it right to write in determinant form?