Solution

ID: past-exam-of-the-short-options-paper-shared-by-prelims-and-parts-a-and-b-of-the-physics-course-of-the-university-of-oxford/2018/s1/1/solution

A branch point is a point around which analytic continuation changes the value of a multivalued function. For , one circuit around zero changes the sign. A branch cut removes paths producing this ambiguity; for example gives a single holomorphic square root off the nonpositive real axis. The position of a cut is a convention, while the branch point is intrinsic.
Set . For outside the closed segment joining to , avoids the nonpositive real axis. Therefore the principal square root of defines a holomorphic function there, with the normalization . The endpoints are branch points. Expanding at infinity,
For a positively oriented contour surrounding the cut, its integral equals the integral on a sufficiently large positively oriented circle, since the intervening annulus is holomorphic. Thus
On the upper and lower banks, and . The upper bank is traversed from to , and the lower bank from to . Their sum is times the required real integral. Small endpoint arcs vanish because their singularities have exponent less than one. Consequently
For , use with the same normalization. Its expansion is , and its bank values are . Equating the contour integral with times the real integral gives
The condition ensures endpoint integrability. Choosing the other square-root branch reverses , but also reverses both bank values, leaving the real integral unchanged.

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