A Riemann (definite) integral ∫abf(x)dx requires a finite interval [a,b] with f finite throughout. An improper integral of the first kind relaxes the finiteness of the interval — one or both limits of integration are ±∞ — and is defined as a limit of ordinary Riemann integrals:
∫a∞f(x)dx=limt→∞∫atf(x)dx,∫−∞af(x)dx=limt→−∞∫taf(x)dx,∫−∞∞f(x)dx=limt→∞∫−ttf(x)dx.
If the limit exists (and is finite), the improper integral is said to converge; otherwise it diverges. By the Second Fundamental Theorem, if F is an anti-derivative of f, then ∫a∞f(x)dx=limt→∞[F(t)−F(a)] — so in practice one finds F, substitutes t for the infinite endpoint, and takes the limit termwise.
Recurring limiting facts used throughout this chapter:
- t→∞limtan−1t=2π, so ∫0∞a2+x2dx=2aπ for a>0. …