@VJ123 Well, this has something to do with a kind of fundamental asymmetry we often see in measure theory. If $f$ is a non-negative, measurable function, the integral $\int f$ always makes sense, but it may be infinite. To deal with not necessarily non-negative measurable functions, we split them up into a positive part, $f^+$, and a negative part, $f^-$, for which the integrals are defined as previously and then define $\int f=\int f^+-\int f^-$.
For this to work out nicely, we require both integrals on the RHS to be finite (we don't want something like $\infty-\infty$ to stand there) and …