This is the improper integral we want to look at:
I=∫a∞f(x)dx.I will show that for the integral to coverge (exist), f(x) must decline faster than 1/x for large x. (This only works for monotonically decaying functions. Functions like xsinx or sin(x2) won’t apply. My note is very unrigorous.)
We can split an integral into two parts:
I=∫abf(x)dx+∫b∞f(x)dx.Because the first term is a finite integral, saying I exists is equivalent as saying ∫b∞f(x)dx exists, for any large b.
Notice that
∫b∞xpdx={1+px1+p∣b∞ln(x)∣b∞,p=−1,p=−1.When p=−1, the integral is limx→∞ln(x)−ln(b), which diverge. If something declines slower than x−1=1/x, it of course diverge, too!
If p ≥ -1, ∫b∞xpdxdiverges.When p<−1,
∫b∞xpdx=x→∞lim1+px1+p−b1+p.Since p<−1⇔1+p<0,
x→∞limx1+p=0⟹∫b∞xpdx=−1+pb1+p=constant.We thus proved that, for an integral ∫a∞f(x)dx to converge, plus f(x) is monotonically decaying function, we must have
f(x)∼xa1,a>1,for large x.One cannot in general deduce that “f(x) decays faster than 1/x” from the convergence of ∫a∞f(x)dx alone. For example, if f oscillates (e.g. f(x)=sinx/x) or if f has sparse narrow spikes whose areas sum to a finite total, the integral may converge while xf(x) does not tend to zero.