Your minimal polynomial argument is sufficient to show that the degree of the extension is 8. However, unless you have been given reason to believe that the extension is Galois, the Galois group of a splitting field of $f$ might have more than 8 elements.
In this case the extension is Galois, and there are fewer valid automorphisms than immediately apparent, due to hidden algebraic relations. For instance, if $\alpha = \sqrt{(2+\sqrt{2})(3+\sqrt{3})}$ and $\beta = \sqrt{(2-\sqrt{2})(3-\sqrt{3})}$, then we have $\alpha\beta = 2\sqrt{3}$. This tells us that $\alpha$ and $\beta$ can't be sent to arbitrary roots of $f$, in particular $\sigma(\alpha)\sigma(\beta) = \pm 2\sqrt{3}$. Going further, you can write $2\sqrt{3}$ as a polynomial in $\alpha$, giving an expression for $\beta$ in terms of $\alpha$ with rational coefficients. Thus, $\sigma(\beta)$ is uniquely determined by $\sigma(\alpha)$. Similar arguments show that $\sigma(\alpha)$ uniquely determines $\sigma$.
To do this explicitly, you might wish to save effort. For instance, consider the intermediate field $\Bbb Q(\sqrt{2}, \sqrt{3})$. Over this field $f$ factors into irreducibles as $(x^2-\alpha^2)(x^2-\beta^2)(x^2-\gamma^2)(x^2-\delta^2)$. The nontrivial automorphism $\sigma$ fixing this field must therefore satisfy $$\sigma(\alpha) = -\alpha, \sigma(\beta) = -\beta, \sigma(\gamma) = -\gamma, \sigma(\delta) = -\delta.$$ Note that the previous paragraph's argument implies that no nontrivial automorphism fixes any root of $f$, since all of these roots generate the whole field.
Next, we wish to examine the element $\psi$ satisfying $\psi(\alpha) = \beta$. We expand the polynomial $$(x^2-\alpha^2)(x^2-\beta^2) = x^4 -(12+2\sqrt{6}) + 12.$$ This tells us that the four Galois automorphisms fixing $\Bbb Q(\sqrt{6})$ send $\alpha$ to $\pm \alpha, \pm \beta$. Thus, $\psi$ fixes $\sqrt{6}$ and in turn we know $\psi(\sqrt{2}) = -\sqrt{2}, \psi(\sqrt{3}) = -\sqrt{3}$, since $\psi$ can't fix all of $\Bbb Q(\sqrt{2}, \sqrt{3})$. Thus, we infer from $\beta\psi(\beta) = \psi(\alpha\beta) = \psi(2\sqrt{3}) = -2\sqrt{3})$ that $\psi(\beta) = -\alpha$. To determine the action on the other roots, we fix $\gamma = \sqrt{(2-\sqrt{2})(3+\sqrt{3})}$ and $\delta = \sqrt{(2+\sqrt{2})(3-\sqrt{3})}$. Now we have the relations $\alpha/\gamma = \delta/\beta = 1+\sqrt{2}$. This lets us compute
$$\frac{\beta}{\psi(\gamma)} = \frac{\psi(\delta)}{-\alpha} = 1-\sqrt{2}$$
Solving these equations gives $\psi(\gamma) = -\delta, \psi(\delta) = \gamma$.