There seems to be a major inconsistency (perhaps due to my lack of understanding) between what Folland calls a "characteristic" and what I had previously thought was a characteristic.
For example, Folland says that the characteristics of the equation $\partial_x u = 0$ are $\{ \xi : \xi_1 = 0\}$ (in $\mathbb{R}^2$). This confuses me to no end since I thought the characteristic hypersurface was the $x_1$ axis here? According to this definition it's the orthogonal compliment to this. The same issue arises with the heat operator $L=u_t-u_{xx}$ where he says the characteristics are $\{\xi \neq 0 : \xi_x = 0\}$. Aren't the characteristics $t=$ cosntant which are orthogonal to these?
Sorry if this question is elementary but it's given me a real headache and I'm not sure what it is I'm missing here.

