Put with . The chain rule gives
and hence
After substitution and division by , the ordinary differential equation becomes
Comparison with the Gauss hypergeometric equation gives, up to interchanging and ,
At and , the coefficient of has at most a simple pole and that of has at most a double pole, so both are regular singular points. The regular singular point at infinity criterion gives the same conclusion at infinity. The corresponding Papperitz symbol is
Indeed, the exponent pairs are at zero, at one, and at infinity; their sum also satisfies the Fuchs relation.
The solution of with and is . Near , the map has the local inverse , so this solution is analytic in , corresponds to exponent zero at , and has value one there. Uniqueness of the normalized local solution of the Gauss hypergeometric equation therefore gives the hypergeometric cosine identity
or, when on the chosen local branch,
Since , the second local hypergeometric solution is
Under , it must be a constant multiple of the independent elementary solution . As , both and are asymptotic to one another, while . Matching the normalized hypergeometric factor, whose value at zero is one, gives
Consequently the hypergeometric sine identity is

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