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What is so special about $\alpha=-1$ in the integral of $x^\alpha$?
We all know the rule to find primitives (=antiderivatives) of powers of $x$:
$$ \int x^\alpha dx = \frac{x^{\alpha +1}}{\alpha +1}+C$$
whenever $\alpha \in \mathbb{R} \setminus \{-1\}$. In this case we know a primitive is given by the natural logarithm:
$$ \int \frac{1}{x} dx = \ln(x)+C$$
Doesn't this upset you? I mean, for every other power the rule is "algebraic" in some sense: you just get a different power and a coefficient. But for $\alpha = -1$ you get something trascendental! where does this "exception" come from? I can observe that the order of the pole at the origin is the same as the dimension of the space I'm integrating on...but I'm not satisfied enough with this.
I was not aware of this previous question
What is so special about $\alpha=-1$ in the integral of $x^\alpha$?
when I asked mine, I apologize. Anyway, all the answers to that question are "just" a collection of ways to see and say $\it{that}$ the case $\alpha =-1$ is different, but nothing substantial came out of that discussion, from my point of view. I was looking for something deeper, that could shed some light on $\it{why}$ the simples power has the hardest primitive.
To give you a taste of what I was thinking about, let me talk about something that maybe has nothing to do with this. If one wonders about the square-root function, he sees it is not well defined, because for example both $2$ and $-2$ are square roots of $4$. Saying that things just go like this, or that one has to choose a branch of the square-roots, is something you can do. But a better explanation would be talking about Riemann surfaces and considering the function not on $\mathbb{C}$ but on the sphere $\mathbb{CP}^1$. I was hoping something "like this" (or like something else, I don't know) was lurking beneath the surface...something more interesting that a bunch of computations.