PutThe two endpoints and both contribute. Near , set . ThenExpanding the last amplitude in powers of and applying the Complex Watson lemma after rotating onto a decaying endpoint ray gives one exponential series. Repeating at gives the other. After multiplication by the prefactor in the integral representation, the two endpoint contributions combine aswhereSeparating the even and odd powers gives the large-argument asymptotic expansion of the Bessel function of the first kind:Its first terms areFor fixed , the expansion is uniform in every closed sectorwith . The exclusion of the negative real axis fixes the branch of and stays away from its Stokes boundary.
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