tangent vector fields as linear partial differential operators
The vector field X is defined as X(f) = (∂f/∂x_i)v_i where X(x_i) = v_i. Also the directional derivative of f in the direction of v is defined as df(v) = (∂f/∂x_i)v_i. I am using einstein's summation notation so both X(f) and df(v) are sums.
From this we can see that X(f) = df(v). The operator X is defined as
X = (∂/∂x_i)v_i. The source of my confusion comes from the fact that i see df(X) written instead of df(v) where they take ∂/∂x_i to be the basis vectors. I'm confused about why vectors are denoted by ∂/∂x_i which is just an operator? i don't quite understand how an operator X can also act as a vector.
for these operators to be vectors it must be true that they satisfy the properties defining a vector space for all differentiable functions right?
When on a manifold do we always work in this basis of operators?