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In mathematics, Riemann's differential equation, named after Bernhard Riemann, is a generalization of the hypergeometric differential equation, allowing the regular singular points to occur anywhere on the Riemann sphere, rather than merely at 0, 1, and . The equation is also known as the Papperitz equation. The hypergeometric differential equation is a second-order linear differential equation which has three regular singular points, 0, 1 and . That equation admits two linearly independent solutions; near a singularity , the solutions take the form , where is a local variable, and is locally holomorphic with . The real number is called the exponent of the solution at . Let ''α'', ''β'' and ''γ'' be the exponents of one solution solution at 0, 1 and & respectively; and let ''α''', ''β''' and ''γ''' be that of the other. Then : By applying suitable changes of variable, it is possible to transform the hypergeometric equation: Applying Möbius transformations will adjust the positions of the RSPs, while other transformations (see below) can change the exponents at the RSPs , subject to the exponents adding up to 1. ==Definition== The differential equation is given by : :: ■ウィキペディアで「Riemann's differential equation」の詳細全文を読む スポンサード リンク
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