Well, sometimes these expressions are hard to find, especially for the degree of approximation your looking for.
I should note that I led you down the most direct approach for computing these expressions. There are other methods, some of them using readily available expressions and a more theoretical result that leads to a surprisingly and (relatively) easy construction for any degree for any order of accuracy.
Let's consider another construction to the first derivative. Recall the Taylor expression:
<br />
f_{-1} = f_{0} - h\,f' + \frac{1}{2!}h^2\,f'' - \frac{1}{3!}h^3\,f''' + \frac{1}{4!}h^4\,f^{(4)} + \cdots<br />
From here, solve for h\,f' in the truncated series to yield
<br />
h\,f' = (f_{0} - f_{-1}) + \frac{1}{2!}h^2\,f'' - \frac{1}{3!}h^3\,f''' + \frac{1}{4!}h^4\,f^{(4)}<br />
Now, to complete our task, all we need are suitable approximations to f'' and f'''. By "suitable", we mean that the approximations must be of sufficient degree of accuracy to yield an acceptable overall degree of accuracy when used in the equation (remember, we will be dividing by h). Thus, we want to see oders of approximation within the terms of the expression for h\,f' that are of O(h^4).
This means we need:
a) a 2nd order (O(h^2)) approx for f''
b) a 1st order (O(h)) approx for f'''
If we had those, we could substitute into the expression for h\,f' to yield the final expression.
From available sources, we have the following:
<br />
h^2\,f'' = 2\,f_{0} - 5\,f_{-1} + 4\,f_{-2} - f_{-3} + O(h^4)<br />
<br />
h^3\,f''' = f_{0} - 3\,f_{-1} + 3\,f_{-2} - f_{-3} + O(h^4)<br />
Substituting these into the expression and collecting terms, we see that we can once again yield our result
<br />
6h\,f' = 11\,f_{0} - 18\,f_{-1} + 9\,f_{-2} - 2\,f_{-3}<br />
We can perform a similar construction for f''. We now have
<br />
\frac{h^2}{2!}\,f'' = (f_{-1} - f_{0}) + h\,f' + \frac{1}{3!}h^3\,f''' - \frac{1}{4!}h^4\,f^{(4)}<br />
and we require approximations
a) O(h^4) approx for f'
b) O(h^2) approx for f^{(3)}
c) O(h) approx for f^{(4)}
From sources, we have
<br />
12h\,f' = 25\,f_{0} - 48\,f_{-1} + 36\,f_{-2} - 16\,f_{-3} + 3\,f_{-4} + O(h^5)<br />
<br />
2h^3\,f''' = 5\,f_{0} - 18\,f_{-1} + 24\,f_{-2} - 14\,f_{-3} + 3\,f_{-4} + O(h^5)<br />
<br />
h^4\,f^{(4)} = f_{0} - 4\,f_{-1} + 6\,f_{-2} - 4\,f_{-3} + f_{-4} + O(h^5)<br />
Substituting into the expression, collecting terms, and solving for f'' yields
<br />
f'' = \frac{ 35\,f_{0} - 104\,f_{-1} + 114\,f_{-2} - 56\,f_{-3} + 11\,f_{-4} }{12\,h^2} + O(h^3)<br />
Unfortunately, continuing this approach for the third derivative requires fifth order approximation to f' which may not be so readily available. In summary, the required approximations are:
a) O(h^5) approx for f'
b) O(h^4) approx for f^''
c) O(h^2) approx for f^{(4)}
d) O(h) approx for f^{(5)}
Instead of pursuing this approach, we should look at the last technique, ie, the technique/results of finite difference calculus. I won't get into it, but just simply reference the results (cf, eg, Hildebrand, Introduction to Numerical Analysis).
But - let's take a break - I'll post some more about this a little later. Just to suffice, I present what I think is the third derivative (this needs to be checked).
<br />
f^{(3)} \approx \frac{ 17\,f_{0} - 71\,f_{-1} + 118\,f_{-2} - 98\,f_{-3} + 41\,f_{-4} + 7\,f_{-5} }{4\,h^3} + O(h^3)<br />