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36 Integrals with Coalescing SaddlesProperties

§36.11 Leading-Order Asymptotics

With real critical points (36.4.1) ordered so that

36.11.1 t1⁡(𝐱)<t2⁡(𝐱)<⋯<tjmax⁡(𝐱),

and far from the bifurcation set, the cuspoid canonical integrals are approximated by

36.11.2 ΨK⁡(𝐱)=2⁢π⁢∑j=1jmax⁢(𝐱)exp⁡(i⁢(ΦK⁡(tj⁡(𝐱);𝐱)+14⁢π⁢(−1)j+K+1))×|∂2ΦK⁡(tj⁡(𝐱);𝐱)∂t2|−1/2⁢(1+o⁡(1)).

Asymptotics along Symmetry Lines

36.11.3 Ψ2⁡(0,y)={π/y⁢(exp⁡(14⁢i⁢π)+o⁡(1)),y→+∞,π/|y|⁢exp⁡(−14⁢i⁢π)⁢(1+i⁢2⁢exp⁡(−14⁢i⁢y2)+o⁡(1)),y→−∞.
36.11.4 Ψ3⁡(x,0,0) =2⁢π(5⁢|x|3)1/8⁢{exp⁡(−2⁢2⁢(x/5)5/4)⁢(cos⁡(2⁢2⁢(x/5)5/4−18⁢π)+o⁡(1)),x→+∞,cos⁡(4⁢(|x|/5)5/4−14⁢π)+o⁡(1),x→−∞.
36.11.5 Ψ3⁡(0,y,0) =Ψ3⁡(0,−y,0)¯=exp⁡(14⁢i⁢π)⁢π/y⁢(1−(i/3)⁢exp⁡(32⁢i⁢(2⁢y/5)5/3)+o⁡(1)),
y→+∞.
36.11.6 Ψ3⁡(0,0,z) =Γ⁡(13)|z|1/3⁢3+{o⁡(1),z→+∞,2⁢π⁢51/4(3⁢|z|)3/4⁢(cos⁡(23⁢(3⁢|z|5)5/2−14⁢π)+o⁡(1)),z→−∞.
36.11.7 Ψ(E)⁡(0,0,z) =πz⁢(i+3⁢exp⁡(427⁢i⁢z3)+o⁡(1)),
z→±∞,
36.11.8 Ψ(H)⁡(0,0,z) =2⁢πz⁢(1−i3⁢exp⁡(127⁢i⁢z3)+o⁡(1)),
z→±∞.