Let's say we want to approximate a second order differential:
$$ \partial_{aa} V(a)$$
Now, say we have a grid of values for $A$, where the step size is $\Delta$, $i$ is the index on this A grid, and we define the short hand notation
$$V_i \equiv V(A_i)$$
Achdou et al (page 13, equation 35) then compute the approximation to the second order differential on the grid at a point $i$ as
$$\partial_{AA} v_i = \frac{v_{i+1} - 2v_i + v_{i-1}}{\Delta^2}$$
They don't explain why, and I can't follow here. Could someone provide me with the rough ansatz for why this is the case?