Let $\mathcal{M}$ be a real, compact, orientable manifold and let $X$ be a vector field on $\mathcal{M}$. Consider the functional


$$E(f) = \int\_{\mathcal{M}} X\_p(f)^2 dV$$


where $X\_p(f)$ is the directional (Lie) derivative of $f$ along $X$ at the point $p$ and $dV$ is a volume form on $\mathcal{M}$ -- this functional essentially measures the total amount of change in $f$ along $X$ over all of $\mathcal{M}$ in the $L^2$ sense. Then $\delta E(f)$ is a differential operator whose eigenspectrum


$$\delta E(f) = \lambda f$$


(for $\lambda \in \mathbb{R}$) yields the critical points of $E$ over the set of functions with unit norm. Is there an established name for this operator (or functional) and/or its corresponding eigenspectrum?


The prototype for this operator is Dirichlet's energy


$$\int\_{\mathcal{M}} ||\nabla f||^2 dV$$


which has as its (unit-norm) critical points the Laplacian eigenspectrum


$$\nabla^2 f = \lambda f,$$


the main difference being that Dirichlet's energy measures the total *gradient*, i.e., the change in all directions, rather than just the change along a particular direction at each point.



Is there a name for this differential operator and/or its corresponding spectrum?
There is an simple explicit formula for your operator in terms of known operators. To see this, note that $\delta E\_f(g)$ (the differential of $E$ at the function $f$ in the direction $g$) is equal to
$$
2 \int X(f) X(g) dV = 2\int \left[L\_X(g X(f) dV )-g\left(X(X(f)) dV+X(f)L\_X(dV)\right)\right]
$$
where $L\_X$ is the Lie deriviative with respect to $X$. Now, $\int L\_X(\alpha) = 0$ for any top degree form $\alpha$, so we get
$$
\delta E\_f(g) = - 2 \int\_X g \left[X(X(f)) + X(f) div(X)\right]dV
$$
where the divergence of $X$ is defined by $div(X)= L\_X(dV)/dV$. So, using the $L^2$-inner product on functions, we can interpret the 1-form $\delta E$ as the differential operator
$$
D :f \mapsto - X(X(f)) - X(f) div(X).
$$
(This is the same way that the differential of Dirichlet energy is seen as the Laplacian.) 


Note that the leading order part of D is just $X^2$ and so, in particular, $D$ is not elliptic. You'd expect this, of course, because $E$ only sees the change of $f$ in the $X$-direction.


