The Taylor series of a smooth function (at a given point ) is a formal power series (in ) whose partial sums are the Taylor polynomials of (at ). As the Taylor polynomials are approximations of by polynomials (up to a given degree), so the Taylor series is an approximation of by an analytic function (or at least an asymptotic expansion that attempts to be this).
See also Taylor's theorem for error estimates in the convergence of Taylor series.
Let a smooth function with th derivative and let be a real number.
The Taylor series of at is the formal power series
For a smooth function with th derivative , its Maclaurin series is its Taylor series at zero:
Similar definitions apply to functions on any Cartesian space or smooth manifold.
Recall that a (partial) function is analytic at (in the interior of ) if there exists a power series at and a neighbourhood of such that, for all , converges to .
If is analytic at , then the only power series witnessing this is the Taylor series of at (so in particular, the Taylor series exists; analytic functions are smooth).
In contrast, a smooth function need not be analytic; the classic counterexample is a bump function. In fact, the Taylor series of at might not converge to anywhere except at , either because the Taylor series has vanishing radius of convergence or because it converges to something else (an analytic function with the same jet as but a different germ). However, we can say this:
(Taylor series is asymptotic series)
The Taylor series of a smooth function is always an asymptotic expansion of .
This follows from the Hadamard lemma, see this exampleeries#TaylorSeriesOfSmoothFunctionIsAsymptoticSeries) for details.
In particular, every power series in one real variable is the Taylor series of some smooth function on the real line (even if it has vanishing radius of convergence and so is not the Taylor series of any analytic function).
The proof is reproduced for instance in MSIA, I, 1.3
See more at Borel's theorem.
Examples of sequences of local structures
Last revised on November 21, 2023 at 01:13:49. See the history of this page for a list of all contributions to it.