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:
[tex]
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[/tex]
From here, solve for [itex]h\,f'[/itex] in the truncated series to yield
[tex]
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)}[/tex]
Now, to complete our task, all we need are suitable approximations to [itex]f''[/itex] and [itex]f'''[/itex]. 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 [itex]h[/itex]). Thus, we want to see oders of approximation within the terms of the expression for [itex]h\,f'[/itex] that are of [itex]O(h^4)[/itex].
This means we need:
a) a 2nd order ([itex]O(h^2)[/itex]) approx for [itex]f''[/itex]
b) a 1st order ([itex]O(h)[/itex]) approx for [itex]f'''[/itex]
If we had those, we could substitute into the expression for [itex]h\,f'[/itex] to yield the final expression.
From available sources, we have the following:
[tex]
h^2\,f'' = 2\,f_{0} - 5\,f_{-1} + 4\,f_{-2} - f_{-3} + O(h^4)[/tex]
[tex]
h^3\,f''' = f_{0} - 3\,f_{-1} + 3\,f_{-2} - f_{-3} + O(h^4)[/tex]
Substituting these into the expression and collecting terms, we see that we can once again yield our result
[tex]
6h\,f' = 11\,f_{0} - 18\,f_{-1} + 9\,f_{-2} - 2\,f_{-3}[/tex]
We can perform a similar construction for [itex]f''[/itex]. We now have
[tex]
\frac{h^2}{2!}\,f'' = (f_{-1} - f_{0}) + h\,f' + \frac{1}{3!}h^3\,f''' - \frac{1}{4!}h^4\,f^{(4)}[/tex]
and we require approximations
a) [itex]O(h^4)[/itex] approx for [itex]f'[/itex]
b) [itex]O(h^2)[/itex] approx for [itex]f^{(3)}[/itex]
c) [itex]O(h)[/itex] approx for [itex]f^{(4)}[/itex]
From sources, we have
[tex]
12h\,f' = 25\,f_{0} - 48\,f_{-1} + 36\,f_{-2} - 16\,f_{-3} + 3\,f_{-4} + O(h^5)[/tex]
[tex]
2h^3\,f''' = 5\,f_{0} - 18\,f_{-1} + 24\,f_{-2} - 14\,f_{-3} + 3\,f_{-4} + O(h^5)[/tex]
[tex]
h^4\,f^{(4)} = f_{0} - 4\,f_{-1} + 6\,f_{-2} - 4\,f_{-3} + f_{-4} + O(h^5)[/tex]
Substituting into the expression, collecting terms, and solving for [itex]f''[/itex] yields
[tex]
f'' = \frac{ 35\,f_{0} - 104\,f_{-1} + 114\,f_{-2} - 56\,f_{-3} + 11\,f_{-4} }{12\,h^2} + O(h^3)[/tex]
Unfortunately, continuing this approach for the third derivative requires fifth order approximation to [itex]f'[/itex] which may not be so readily available. In summary, the required approximations are:
a) [itex]O(h^5)[/itex] approx for [itex]f'[/itex]
b) [itex]O(h^4)[/itex] approx for [itex]f^''[/itex]
c) [itex]O(h^2)[/itex] approx for [itex]f^{(4)}[/itex]
d) [itex]O(h)[/itex] approx for [itex]f^{(5)}[/itex]
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).
[tex]
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)[/tex]