The finite singularities are square-root branch points at z=±1. Choose the cut between them and the branch f(z)∼z at infinity. The two banks then have values +i1−x2 above and −i1−x2 below. A counterclockwise loop around the cut traverses its upper bank right-to-left, so its integral is −2iI, where I is the required real integral. At large radius,Therefore I=π/2. Infinity is not another square-root branch point: this branch has an ordinary pole there on its sheet. Small detours about the finite endpoints vanish as their radius to power 3/2.
f(z)=z−2z1+O(z−3),∮f(z)dz=−πi.
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