Part $1$ follows immediately from (one formulation of) Frobenius' theorem. Specifically, if $\xi$ is integrable, then $\alpha \wedge d\alpha = 0$. Since $\alpha$ is a $1$-form, that implies (take local coordinates, for example) that $d\alpha = \alpha \wedge \omega$ for some $\omega\in \Omega^1(M)$.
For part $2$, suppose $d\alpha = \alpha\wedge \omega'$. Then $\alpha \wedge (\omega - \omega') = 0$, forcing $\omega - \omega' = f\alpha$ for some $f\in C^\infty(M)$ (again, local coordinates might clarify the last equality).