For vector bundles $E$ and $F$ on a manifold $M$ I have seen here that a linear differential operator $L:\Gamma(E)\to\Gamma(F)$ of order $k$ can locally be written in the form $L=\sum_{\alpha\leq k}l_{\alpha}\partial^{\alpha}$, $l_{\alpha}:E\to F$ is a bundle homomorphism.
- How do I calculate $\partial^{\alpha}S$ when $S\in\Gamma(E)$? Do I simply pick a basis/frame for $E$ and apply $\partial^{\alpha}$ to the component functions?
The symbol of $L$ in the direction of a one-form $\omega$ is the differential operator obtained by only summing over those $\alpha$ for which $\lvert\alpha\rvert=k$ and replacing $\partial^{\alpha}$ by $\omega^{\alpha}=\omega_1^{\alpha_1}\dots\omega_n^{\alpha_n}$, with $(\omega_i)_{i=1}^n$ being the components of $\omega$ in dual basis/frame. In other words, $\text{Principal symbol}(L)(\omega)=\sum_{\lvert\alpha\rvert=k}\omega^{\alpha}l_{\alpha}.$ In a calculation from this answer here, covariant derivatives, rather than derivatives, were replaced with the components of the one-form (in this one they use $\xi$ instead of $\omega$).
- How does the definition of the principle symbol coincide with the answer posted there?