Solution

ID: past-exam-of-the-mathematics-course-of-the-university-of-cambridge/2006/ii/paper-3/14e/a/solution

Write the Papperitz symbol by listing pairs of exponents at . For they are , , and . Under the points in the -plane correspond respectively to in the -plane. Thus the pulled-back exponents are at zero, at one, and at infinity.
Multiplication by shifts the exponents at one by and those at infinity by , yielding
This is the original Gauss hypergeometric equation. Both functions are analytic and normalized to one at zero, so uniqueness of that normalized local solution proves the Pfaff transformation
Continue the identity using the branch . As usual, the parameters must admit the normalized hypergeometric solution; excluded singular parameter values are treated only when their limiting solution exists.

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