In mathematics, an analytic manifold, also known as a C ω {\displaystyle C^{\omega }} manifold, is a differentiable manifold with analytic transition maps. The term usually refers to real analytic manifolds, although complex manifolds are also analytic. In algebraic geometry, analytic spaces are a generalization of analytic manifolds such that singularities are permitted.

For U R n {\displaystyle U\subseteq \mathbb {R} ^{n}} , the space of analytic functions, C ω ( U ) {\displaystyle C^{\omega }(U)} , consists of infinitely differentiable functions f : U R {\displaystyle f:U\to \mathbb {R} } , such that the Taylor series

T f ( x ) = | α | 0 D α f ( x 0 ) α ! ( x x 0 ) α {\displaystyle T_{f}(\mathbf {x} )=\sum _{|\alpha |\geq 0}{\frac {D^{\alpha }f(\mathbf {x_{0}} )}{\alpha !}}(\mathbf {x} -\mathbf {x_{0}} )^{\alpha }}

converges to f ( x ) {\displaystyle f(\mathbf {x} )} in a neighborhood of x 0 {\displaystyle \mathbf {x_{0}} } , for all x 0 U {\displaystyle \mathbf {x_{0}} \in U} . The requirement that the transition maps be analytic is significantly more restrictive than that they be infinitely differentiable; the analytic manifolds are a proper subset of the smooth, i.e. C {\displaystyle C^{\infty }} , manifolds. There are many similarities between the theory of analytic and smooth manifolds, but a critical difference is that analytic manifolds do not admit analytic partitions of unity, whereas smooth partitions of unity are an essential tool in the study of smooth manifolds. A fuller description of the definitions and general theory can be found at differentiable manifolds, for the real case, and at complex manifolds, for the complex case.

See also

  • Complex manifold
  • Analytic variety
  • Algebraic geometry § Analytic geometry

References



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