TITLE: Elliptic operators corresponds to non vanishing vector fields
QUESTION [11 upvotes]: Added, June 19, 2019:   The  main  motivation of  this  post is  to  associate an  index  to  differential operator  associated to  a  dynamical  system such that the index  has  an interesting  dynamical interpretation. For  example we  hope that  the  index can help  us  to  find  an  upper  bound for the  number of  attractors  of  a dynamical  system.   According to  comment  conversations in this post we realize  that ellipticity or  hypoelipticity is  a very relevant or  perhaps  a  necessary  conditions  for  existence of  "Index".  Now  the  subject and  materials  of  this recently hold  conference, "Fredholm theory of  Non  elliptic  operatores seems to be  related to this  post. 

Let $X$ be  a  non vanishing  vector  field on  a compact  manifold $M$. The only differential operator associated with $X$ which I am aware of, is the derivational operator $D(g)=X.g$. Unfortunately this operator is not an elliptic operator.
From the  dynamical view point,what type of elliptic operators, or  at  least  Fredholm diff. operators, can be associated with $X$?
I mean, for  a  given non vanishing vector  field $X$, what interesting elliptic operator $D$ can be constructed such that its  fredholm index contains some information about the dynamical behavior of $X$. For example: the number of attractores, or the number of isolated compact invariant sets, etc.. 
EditL: For  a  possible related post see the following:
How to compute the index of such operator?

REPLY [10 votes]: Perhaps you would be interested in Witten's proof of the Poincare-Hopf theorem.  Given a smooth nondegenerate vector field $V$ on a smooth closed manifold $M$, the theorem asserts that the Euler characteristic of $M$ is equal to the sum of the signs of the critical points of $V$.  Perhaps this isn't as interesting as the dynamical behavior that you mentioned in your question, but it's a start.
Witten's approach is to use $V$ to perturb the de Rham complex by replacing the de Rham differential $d$ with the operator
$$d_t = d + t i_v \colon\: \Omega^*(M) \to \Omega^*(M)$$
where $t$ is a real number and $i_V$ is the interior product with $V$.  He looked at the corresponding perturbed de Rham operator $D_t = d_t + d_t^*$ (where the adjoint is defined using a choice of Riemannian metric) and as usual viewed it as a graded Dirac-type operator on the graded Clifford module $\Omega^*(M)$.  $D_t$ is elliptic and hence Fredholm, and since the index of an operator is determined by its symbol class the index of $D_t$ is just the index of the usual de Rham operator $D$ which is the Euler characteristic of $M$.
On the other hand, one can calculate that
$$D_t^2 = D^2 + t^2 ||V||^2 + t T$$
where $T$ is some bundle map.  For large values of $t$ the potential term $t^2 ||V||^2$ becomes very large except in a tiny neighborhood of the critical set of $V$, so one can show that the eigenvectors of $D_t$ concentrate near the critical set.  Combining this observation with the McKean-Singer formula for the index of $D_t$ and some asymptotic analysis proves the Poincare-Hopf theorem.
There are a variety of generalizations of this result in the literature - perturbing other operators, relaxing the nondegeneracy assumption, etc.  I don't know this literature too well and so I don't quite know how much dynamics to expect, but it's worth a look.