haruspex said:
The objection (which I share) is to using the same symbol to mean two different things. (Funnily enough, I've been having just this discussion with another HomeworkHelper.) E.g. in sin(x) = ∫cos(x).dx , the x on the right is a dummy variable, so cannot mean the same as the x on the left.
You are confusing the antiderivative (##\int \cos x\,dx = \sin x + C##) with the definite integral (##\int_0^x \cos t\,dt = \sin x##). They are rather different mathematical concepts that are connected to one another via the fundamental theorem of calculus.
What that equation intends is sin(x) = ∫xcos(x).dx, …
That is just as bad notation as we have been accusing Jhenrique of making. That doesn't make a bit of sense.
------------------------------------------------------------------------------------------
Your notation is rather bizarre, Jhenrique.
Nonetheless, I think I know what you are going after here, which is the concept of an inverse difference. First let's look at a difference table. I'll use forward differences, ##\Delta f_i = f_{i+1}-f_i##. Backward differences (##\nabla f_i = f_i - f_{i-1}##) and central differences (##\partial f_i = f_{i+1/2}-f_{i-1/2}##) yield analogous results.
<br />
\begin{matrix}<br />
n & f_n & \Delta^1 f_n\\<br />
0 & f_0 & f_1 - f_0 \\<br />
1 & f_1 & f_2 - f_1 \\<br />
2 & f_2 & f_3 - f_2 \\<br />
3 & f_3 & f_4 - f_3 \\<br />
\cdots & \cdots & \cdots \\<br />
N & f_N & f_{N+1} - f_N \\<br />
\cdots & \cdots & \cdots<br />
\end{matrix}<br />
This table can be extended to the right via ##\Delta^k f_n = \Delta^{k-1} f_{n+1} - \Delta^{k-1} f_n##. It can also be extended to the left, and this is what you want. Almost all that is needed is ##\Delta f^0 f_n##, and this is just the identity operator: ##\Delta^0 f_n##.
That's not quite all that is needed. Just as ##\int f(x)\,dx## involves an arbitrary constant, so do their difference calculus equivalents. With these arbitrary constants, the difference table takes the form
<br />
\begin{matrix}<br />
n & \cdots & \Delta^{-2} & \Delta^{-1} & \Delta^0 & \Delta^1 & \Delta^2 & \cdots \\<br />
0 & \cdots<br />
& c_2<br />
& c_1<br />
& f_0 <br />
& f_1 - f_0 <br />
& \Delta^1 f_1 - \Delta^1 f_0 <br />
& \cdots \\<br />
1 & \cdots<br />
& c_2 + c_1<br />
& c_1 + f_0<br />
& f_1 <br />
& f_2 - f_1 <br />
& \Delta^1 f_2 - \Delta^1 f_1 <br />
& \cdots \\<br />
2 & \cdots<br />
& c_2 + 2c_1 + f_0<br />
& c_1 + f_0 + f_1<br />
& f_2 <br />
& f_3 - f_2 <br />
& \Delta^1 f_3 - \Delta^1 f_2 <br />
& \cdots \\<br />
3 & \cdots<br />
& c_2 + 3c_1 +2 f_0+f_1<br />
& c_1 + f_0 + f_1 + f_2<br />
& f_3 <br />
& f_4 - f_3 <br />
& \Delta^1 f_4 - \Delta^1 f_3 <br />
& \cdots \\<br />
\cdots & \cdots & \cdots & \cdots & \cdots & \cdots & \cdots & \cdots \\<br />
N & \cdots<br />
& \text{your job}<br />
& \text{your job}<br />
& f_N <br />
& f_{N+1} - f_N <br />
& \Delta^1 f_{N+1} - \Delta^1 f_N<br />
& \cdots \\<br />
\cdots & \cdots & \cdots & \cdots & \cdots & \cdots & \cdots & \cdots<br />
\end{matrix}<br />
What you want is that ##\Delta^{-2}## column.