I'm beginning to study $4$-dimensional Riemannian manifolds, in particular the decomposition induced by the Hodge $\star$-operator on the space of the differential two-forms. I'm considering $\mathbb{R}^4$ as an example: I understood that $\Lambda^2 \mathbb{R}^4=\Lambda_{+}\oplus \Lambda_{-}$, where $\Lambda_{\pm}$ is the eigenspace of $\star$ relative to the eigenvalue $\pm 1$.
The group $SO(4)$ acts on $\Lambda^2 \mathbb{R}^4$ in the standard way induced by the action of $SO(4)$ on $\mathbb{R}^4$, i.e. if $X\in SO(4)$ and $a\wedge b$ is a two-form, then $X(a\wedge b)=Xa\wedge Xb$. I've got three questions:
$1)$ Since $\Lambda^2 \mathbb{R}^4\cong so(4)$ (the Lie algebra of $SO(4)$), are there some relations between the action of $SO(4)$ on $\Lambda^2 \mathbb{R}^4$ and the adjoint action of $SO(4)$ on $so(4)$?
$2)$ What is the action of $SO(4)$ on $\Lambda^2 \mathbb{R}^4$ when restricted to $\Lambda_{\pm}$? I know that $so(4)\cong so(3)\oplus so(3)$, so I thought it could be useful to compute the action, but I don't know how to do it.
$3)$ I read that the restriction of the action to $\Lambda_{\pm}$ induces a surjective homomorphism $\phi:SO(4)\rightarrow SO(3)\times SO(3)$ which is two to one. How can I prove this and compute the homomorphism? I understood that there is a surjective homomorphism from $SU(2)$ to $SO(3)$ and that $SU(2)\times SU(2)$ is the universal cover of $SO(4)$ (a double cover, in particular): could it be useful?