If $\alpha\wedge d\alpha$ is a volume form, there exists a vector field $X$ such that $i_X\alpha\equiv1$ and $i_X (d\alpha)\equiv0$.

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I'm currently stuck on the following problem:

Let $\alpha$ be a 1-form on a connected 3-manifold $M$ such that $\alpha\wedge d\alpha$ is a volume form. Show that there exists a vector field $X$ on $M$ such that $i_X\alpha\equiv1$ and $i_X(d\alpha)\equiv0$.

I believe there are a few routes to solve this problem, but I keep getting stuck at each step. Working locally, I first wrote $$\alpha=\alpha_1dx+\alpha_2dy+\alpha_3dz$$ and noticed that $\alpha$ is non-vanishing. Indeed, if not, there exists a point $p\in M$ such that $\alpha_i(p)=0$ for $i=1,2,3$. Computing $\omega=\alpha\wedge d\alpha$, it follows that $\omega_p=0$, a contradiction. Thus, because $\alpha\neq0$, we get (by a theorem about $\alpha\wedge d\alpha$) that $\ker\alpha$ is not involutive, but I'm really not sure what I can do from here. I suppose that if we choose appropriate vector fields $X,Y\in\ker\alpha$, we do get that

$$d \alpha(X, Y)=X(\alpha(Y))-Y(\alpha(X))-\alpha([X, Y])=-\alpha([X,Y])$$

is non-zero.

Alternatively, there is the usual expansion

$$i_X(\alpha\wedge d\alpha)=i_X\alpha\wedge d\alpha-\alpha\wedge i_Xd\alpha,$$ which connects both the conditions that $i_X\alpha\equiv1$ and $i_Xd\alpha\equiv0$ with the contraction of a volume form, but again I'm not able see where this leads me.

I'd really appreciate any help towards a full solution. I'm reviewing my knowledge of smooth manifold theory, so this problem is not homework (although it's from an old exam at my university). Thank you!

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If you're not already aware, the vector field $X$ is called the Reeb vector field associated to $\alpha$.

The key piece of the construction is Jacobi's theorem, which states that the determinant of an odd-dimensional skew-symmetric matrix is zero. This implies that a skew 2-form such as $d\alpha$ has nonzero kernel when viewed as a map $T_pM\to T^*_pM$ given by $v\to\iota_vd\alpha$.

Since $\alpha\wedge d\alpha$ is a volume form, we must have that $\ker\alpha\cap\ker d\alpha=0$, and thus $\ker d\alpha$ is one dimensional and $\alpha|_{\ker d\alpha}$ is nonvanishing. The Reeb field $X$ is exactly the preimage of $\{1\}$ under $\alpha|_{\ker d\alpha}$