Power series
Analytic functions

A function f defined on some open subset U of R or C is called analytic if it is locally given by a convergent power series. This means that every a ∈ U has an open neighborhood V ⊆ U, such that there exists a power series with center a that converges to f (x) for every x ∈ V.

Every power series with a positive radius of convergence is analytic on the interior of its region of convergence. All holomorphic functions are complex-analytic. Sums and products of analytic functions are analytic, as are quotients as long as the denominator is non-zero.

If a function is analytic, then it is infinitely differentiable, but in the real case the converse is not generally true. For an analytic function, the coefficients a can be computed as a n = f (n) (c) n ! {\displaystyle a_{n}={\frac {f^{\left(n\right)}\left(c\right)}{n!}}}

where f (n) (c) {\displaystyle f^{(n)}(c)} denotes the n th derivative of f at c, and f (0) (c) = f (c) {\displaystyle f^{(0)}(c)=f(c)}. This means that every analytic function is locally represented by its Taylor series.

The global form of an analytic function is completely determined by its local behavior in the following sense: if f and g are two analytic functions defined on the same connected open set U, and if there exists an element c ∈ U such that f (c) = g (c) for all n ≥ 0, then f (x) = g (x) for all x ∈ U.

If a power series with radius of convergence r is given, one can consider analytic continuations of the series, i.e. analytic functions f which are defined on larger sets than { x | | x − c | < r } and agree with the given power series on this set. The number r is maximal in the following sense: there always exists a complex number x with | x − c | = r such that no analytic continuation of the series can be defined at x.

The power series expansion of the inverse function of an analytic function can be determined using the Lagrange inversion theorem.
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