I have read about this related question, Tautological 1-form on the cotangent bundle and have asked some professor and is still being confused.
So let $M=\mathbb{R^2}$, $N=\mathbb{R}$. $F:M\rightarrow N$ by $F(x_1,x_2)=x_1\in N$. Given $\alpha(y)=\xi(y)d y\in C^\infty(N; T^*N)$, we can pull it back as $$(F^*\alpha)(x_1,x_2)=\xi(x_1)d x_1,$$ which we can thinking of it as a field of arrow on the $\mathbb{R}^2$ plane pointing in the $x_1$ direction with its norm independent of $x_2$.
Now SUDDENLY, let's make $M\equiv T^*N= T^*\mathbb{R}=\mathbb{R}^2$ (therefore $F$ can also be called $\pi$), so $\xi$, as $\alpha(\partial_{x_1})$, is actually $x_2$. But to distinguish it from the coordinate, let's call it $\hat{x_2}$: $$F^*\alpha(x_1,x_2)=\xi(x_1)d x_1=\hat{x_2}(x_1)d x_1,$$ $\xi(x_1)$ or $\hat{x_2}(x_1)$ is still a function of $x_1$ (actually, a function of the 2-dimensional coordinate $(x_1,x_2)$, but no dependence on $x_2$). We define $$\theta=F^*\alpha\equiv \xi(x_1)d x_1$$ Can anybody tell me why the simplectic form on $T^*N=T^*\mathbb{R}=\mathbb{R}^2$ can be defined by the following way: $$\omega=d \theta=d\xi\wedge d x_1\equiv d x_2\wedge dx_1,$$ rather than $d \theta=\partial_{x_1}\xi(x_1)d x_1\wedge d x_1=0$? I haven been stuck on this problem for several days (not that that's the only thing I have been doing), really appreciate it if anyone can help me!