State Watson's lemma, describing the asymptotic behaviour of the integral
I(λ)=∫0Ae−λtf(t)dt,A>0
as λ→∞, given that f(t) has the asymptotic expansion
f(t)∼tαn=0∑∞antnβ
as t→0+, where β>0 and α>−1.
Give an account of Laplace's method for finding asymptotic expansions of integrals of the form
J(z)=∫−∞∞e−zp(t)q(t)dt
for large real z, where p(t) is real for real t.
Deduce the following asymptotic expansion of the contour integral
∫−∞−iπ∞+iπexp(zcosht)dt=21/2iezΓ(21)[z−1/2+81z−3/2+O(z−5/2)]
as z→∞.