Or another way. f(x) = 0 , for your f is very easy to solve - your f has been factorised already for you. So you have got a value of f for which there are two points, two values of x. Call them x1 and x2 to be more general. So if f is symmetrical it has to be symmetrical for these two points. I.e. it has to be symmetrical around what x-value (call it xm)? That would be true for any function f. The converse is not true for any function in general but it is true in general that an axis of symmetry can't be any other value of x than xm the one found as above*, so you will narrow it down vastly by finding that. Once you have you can probably show that x = xm is a line of symmetry for your whole function in your case (sufficiency as well as necessity).
To know what I'm talking about it may be better to draw a graph of you function. Quite an important problem because it is the start of more general and extensive principles.
*i.e. the condition is necessary but not sufficient