How does a vector field transform under an infinitesimal coordinate transformation? If I have a vector $X^{\mu}(x)$, and then I consider an infinitesimal coordinate transformation of the form $x^{\mu} \to x^{\mu} + v^{\mu}(x)$, then how does my vector $X^{\mu}(x)$ transform?
From some reading online, it seems like the answer is along the lines of:
$$
X^{\mu}(x) \ \to \ X^{\mu}(x) + v^{\sigma}(x) \partial_{\sigma} X^{\mu}(x) - X^{\sigma}(x) \partial_{\sigma} v^{\mu}(x)
$$
I'm not really understanding where this is coming from though...is it because we're taking a Taylor expansion of $X^{\mu}(x+v)$? The minus sign is particularly unsettling for me. 
 A: If $X^\mu(x)$ is a vector field, in terms of coordinates $\{x^\mu\}$ and we consider an infinitesimal shift,
$$x^\mu \to x^\mu + v^\mu(x)$$
then the vector field $X^\mu$ changes according to the Lie derivative w.r.t. to the vector $v^\mu$, that is, we have that,
$$\delta X^\mu = \mathcal L_v X^\mu = v^\nu \nabla_\nu X^\mu - X^\nu \nabla_\nu v^\mu$$
by simplying applying the rules of Lie differentiation of a tensor. If the manifold is entirely flat, then covariant derivatives are demoted to partial derivatives,
$$\delta X^\mu = v^\nu \partial_\nu X^\mu - X^\nu \partial_\nu v^\mu$$
recovering the expression given by the OP. Notice that $v^\nu \partial_\nu$ is the same as the vector $v^\mu$ expressed as a derivation.$^\dagger$ As such, we can write,
$$\mathcal L_v X = [v,X]$$
with the Lie bracket, where $v$ and $X$ are the fields expressed as derivations, i.e. operators.

$\dagger$ A vector as a derivation can be thought of as a directional derivative. Specifically, for a vector $v$ and a map $f : \mathbb R^n \to \mathbb R$, we have that,
$$D_v f(x) = \frac{d}{d\lambda} f(x + \lambda v) \bigg\rvert_{\lambda = 0} = v^\mu \partial_\mu f (x).$$
A case of interest is when $v$ is a vector along a curve, that is, it is the vector tangent along a path, in which case one may define differentiation of a map along a path on the manifold.
