That equation admits two linearly independent solutions; near a singularity
Let α, β and γ be the exponents of one solution at 0, 1 and
Then By applying suitable changes of variable, it is possible to transform the hypergeometric equation: Applying Möbius transformations will adjust the positions of the regular singular points, while other transformations (see below) can change the exponents at the regular singular points, subject to the exponents adding up to 1.
The differential equation is given by The regular singular points are a, b, and c. The exponents of the solutions at these regular singular points are, respectively, α; α′, β; β′, and γ; γ′.
As before, the exponents are subject to the condition The solutions are denoted by the Riemann P-symbol (also known as the Papperitz symbol) The standard hypergeometric function may be expressed as The P-functions obey a number of identities; one of them allows a general P-function to be expressed in terms of the hypergeometric function.
It is In other words, one may write the solutions in terms of the hypergeometric function as The full complement of Kummer's 24 solutions may be obtained in this way; see the article hypergeometric differential equation for a treatment of Kummer's solutions.
The P-function possesses a simple symmetry under the action of fractional linear transformations known as Möbius transformations (that are the conformal remappings of the Riemann sphere), or equivalently, under the action of the group GL(2, C).
Given arbitrary complex numbers A, B, C, D such that AD − BC ≠ 0, define the quantities and then one has the simple relation expressing the symmetry.
If the Moebius transformation above moves the singular points but does not change the exponents, the following transformation does not move the singular points but changes the exponents: [2] [3]