The integral ∫ e^{N·f(z)} dz is dominated, for large N, by the saddle point z* where f'(z*)=0. The Gaussian integral around z* gives the approximation e^{N·f(z*)}·√(2π/N|f''(z*)|). Applied to n!, this yields Stirling's formula. The steepest descent contour passes through the saddle where Im(f) is constant.