Suppose $C$ is a scalar, $\mathcal{Y}$ is one-form and there is the equation
$$ dC\wedge \mathcal{Y}=0 \quad (1)$$
What is the most general solution of this equation?
Using the geometrical interpretation of the wedge product I would say that there is a solution $$ \mathcal{Y}=f(C)dC,\quad (2)$$ but is this the most general one? Probably the answer is no, but I would like to know other opinions.
In the tensorial form the equation (1) is $$\partial_s C Y_t - Y_s \partial_t C=0,\quad (3)$$ here $\mathcal{Y}=Y_adx^a$. Obviously (2) is a solution, but again it is not clear that (2) is the most general one.
There is the theorem (Theorem 3 in Wedge Product) saying that $v_1\wedge v_2\wedge \cdots \wedge v_k=0$ if and only if $$v_j=\sum_{i=1,i\ne j} a_i v_i$$ for some $j$, $j\le 1\le k$. Applying it to (1) we get the most general solution in the form $$\mathcal{Y}=f dC,$$ with some arbitrary function $f$. The solution (2) is correct ONLY if we require additionally $d\mathcal{Y}=0$, which gives $f=f(C)$.