32 Painlevé TranscendentsProperties

§32.5 Integral Equations

Let K⁡(z,ζ) be the solution of

32.5.1 K⁡(z,ζ)=k⁢Ai⁡(z+ζ2)+k24⁢∫z∞∫z∞K⁡(z,s)⁢Ai⁡(s+t2)⁢Ai⁡(t+ζ2)⁢ds⁢dt,

where k is a real constant, and Ai⁡(z) is defined in §9.2. Then

32.5.2 w⁡(z)=K⁡(z,z),

satisfies PII with α=0 and the boundary condition

32.5.3 w⁡(z)∼k⁢Ai⁡(z),
z→+∞.