Let $N$ be a von Neumann algebra and let $(\phi_\lambda)$ be a net of normal states on $N$ so that $\phi_\lambda\to\phi$ in the weak-* topology, i.e. $\phi_\lambda(x)\to\phi(x)$ for all $x\in N$. What can we infer about $\phi$ in this case? Of course, $\phi$ is going to be a state on $N$, since $\phi(x^*x)=\lim_\lambda\phi_\lambda(x^*x)\geq0$ and $\phi(1_N)=\lim_\lambda\phi_\lambda(1_N)=1$.
But can we say anything more about $\phi$? If not, can we prove that the normal states on $N$ are dense in the weak-* topology in the state space $S(N)$?
I was thinking that, if this density is true, it suffices to prove it for the case of $\mathcal{B(H)}$. Indeed, if this is true for those von Neumann algebras, then we take an arbitrary von Neumann algebra $N$ and concretely represent it on some Hilbert space, i.e. we have an inclusion of von Neumann algebras $N\subset\mathcal{B(H)}$. Now normal states of von Neumann subalgebras extend to normal states and, in general, states extend to states (in the $C^*$-algebraic setting). So we take a state $\phi$ on $N$, we extend it on a state $\Phi$ on $\mathcal{B(H)}$ and then we approximate $\Phi$ in the weak-* sense by normal states on $\mathcal{B(H)}$. We restrict those to $N$ and these are normal states on $N$ approximating $\phi$ weak-* on $N$.
I have no idea on how to prove this though, any help is appreciated.